Source: http://www.google.com/patents/US7662703?dq=7,339,580
Timestamp: 2015-04-27 23:22:17
Document Index: 5935442

Matched Legal Cases: ['art 421', 'art 421', 'art 421', 'art 421', 'art 421', 'art 421']

Patent US7662703 - Method for manufacturing crystalline semiconductor film and semiconductor device - Google PatentsSearch Images Maps Play YouTube News Gmail Drive More »Sign inAdvanced Patent SearchPatentsThere is provided a method for manufacturing a crystalline semiconductor film. An insulating film is formed over a substrate; an amorphous semiconductor film is formed over the insulating film; a cap film is formed over the amorphous semiconductor film; the amorphous semiconductor film is scanned and...http://www.google.com/patents/US7662703?utm_source=gb-gplus-sharePatent US7662703 - Method for manufacturing crystalline semiconductor film and semiconductor deviceAdvanced Patent SearchPublication numberUS7662703 B2Publication typeGrantApplication numberUS 11/892,968Publication dateFeb 16, 2010Filing dateAug 28, 2007Priority dateAug 31, 2006Fee statusPaidAlso published asUS20080318398Publication number11892968, 892968, US 7662703 B2, US 7662703B2, US-B2-7662703, US7662703 B2, US7662703B2InventorsTomoaki Moriwaka, Koichiro TanakaOriginal AssigneeSemiconductor Energy Laboratory Co., Ltd.Export CitationBiBTeX, EndNote, RefManPatent Citations (45), Non-Patent Citations (2), Referenced by (6), Classifications (14), Legal Events (2) External Links: USPTO, USPTO Assignment, EspacenetMethod for manufacturing crystalline semiconductor film and semiconductor device
US 7662703 B2Abstract
There is provided a method for manufacturing a crystalline semiconductor film. An insulating film is formed over a substrate; an amorphous semiconductor film is formed over the insulating film; a cap film is formed over the amorphous semiconductor film; the amorphous semiconductor film is scanned and irradiated with a continuous wave laser beam or a laser beam with a repetition rate of greater than or equal to 10 MHz, through the cap film; and the amorphous semiconductor film is melted and crystallized. At that time, an energy period in a length direction in a laser beam spot of the laser beam is 0.5 μm to 10 μm, preferably, 1 μm to 5 μm; an energy distribution in a width direction in a laser beam spot of the laser beam is a Gaussian distribution; and the amorphous semiconductor film is scanned with the laser beam so as to be irradiated with the laser beam for a period of greater than or equal to 5 microseconds and less than or equal to 100 microseconds per region.
1. A method for manufacturing a crystalline semiconductor film, comprising the steps of:
forming a film over the semiconductor film;
irradiating the semiconductor film with a continuous wave laser beam through the film; and
melting and crystallizing the semiconductor film to form a crystalline semiconductor film having a crystal grain with a parallel boundary and a width of greater than or equal to 0.5 μm and less than or equal to 10 μm,
wherein an energy period of the laser beam is greater than or equal to 0.5 μm and less than or equal to 10 μm, and
wherein the semiconductor film is irradiated with the laser beam for a period of greater than or equal to 5 microseconds and less than or equal to 100 microseconds per region.
2. A method for manufacturing a crystalline semiconductor film according to claim 1, wherein the laser beam having the energy period of greater than or equal to 0.5 μm and less than or equal to 10 μm has a wavy energy distribution in a direction perpendicular to a scan direction of the laser beam.
3. A method for manufacturing a crystalline semiconductor film according to claim 2, wherein the laser beam is formed using a diffractive optical element.
4. A method for manufacturing a crystalline semiconductor film according to claim 2, wherein the laser beam is formed by splitting a laser beam emitted from one laser device and combining the split laser beams.
5. A method for manufacturing a crystalline semiconductor film according to claim 2, wherein a plurality of the laser beams are arranged in a direction perpendicular to a scan direction of the laser beam.
6. A method for manufacturing a crystalline semiconductor film according to claim 1, wherein the cap film has a region transmitting the laser beam having an energy capable of crystallizing the semiconductor film and a region which does not transmit the laser beam having an energy capable of crystallizing the semiconductor film, which form stripes, the laser beams are scanned in a direction parallel to the stripes.
7. A method for manufacturing a crystalline semiconductor film according to claim 6,
wherein an anti-reflective film is formed in the region transmitting the laser beam having an energy capable of crystallizing the semiconductor film, and a reflective film is formed in the region which does not transmit the laser beam having an energy capable of crystallizing the semiconductor film.
8. A method for manufacturing a crystalline semiconductor film according to claim 6, wherein an anti-reflective film is formed in the region transmitting the laser beam having an energy capable of crystallizing the semiconductor film, and a film absorbing the laser beam is formed in the region which does not transmit the laser beam having an energy capable of crystallizing the semiconductor film.
9. A method for manufacturing a crystalline semiconductor film according to claim 6, wherein the cap film has irregularities in a striped pattern.
10. A method for manufacturing a crystalline semiconductor film according to claim 6, wherein the laser beam has a trapezoid energy distribution in a direction perpendicular to a scan direction of the laser beam.
11. A method for manufacturing a crystalline semiconductor film according to claim 1, wherein an energy of the laser beam is higher than an energy adequate for melting the semiconductor film.
12. A method for manufacturing a crystalline semiconductor film according to claim 1, wherein a thickness of the semiconductor film is 30 nm to 200 nm.
13. A method for manufacturing a crystalline semiconductor film according to claim 1, wherein the cap film is a silicon nitride film containing 0.1 atomic % to 10 atomic % of oxygen, in which a composition ratio of nitrogen to silicon is 1:1.3 to 1.5.
14. A method for manufacturing a crystalline semiconductor film according to claim 1, wherein the semiconductor film is an amorphous silicon film.
15. A method for manufacturing a crystalline semiconductor film,
wherein a semiconductor element is formed using a crystalline semiconductor film formed in accordance with claim 1.
16. A method for manufacturing a crystalline semiconductor film, comprising the steps of:
wherein a half-width of an energy of the laser beam agrees with the width of the crystal grains.
17. A method for manufacturing a crystalline semiconductor film according to claim 16, wherein an energy of the laser beam is higher than an energy adequate for melting the semiconductor film.
18. A method for manufacturing a crystalline semiconductor film according to claim 16, wherein a thickness of the semiconductor film is 30 nm to 200 nm.
19. A method for manufacturing a crystalline semiconductor film according to claim 16, wherein the cap film is a silicon nitride film containing 0.1 atomic % to 10 atomic % of oxygen, in which a composition ratio of nitrogen to silicon is 1:1.3 to 1.5.
20. A method for manufacturing a crystalline semiconductor film according to claim 16, wherein the semiconductor film is an amorphous silicon film.
21. A method for manufacturing a crystalline semiconductor film,
wherein a semiconductor element is formed using a crystalline semiconductor film formed in accordance with claim 16.
22. A method for manufacturing a crystalline semiconductor film, comprising the steps of:
irradiating the semiconductor film with a laser beam with a repetition rate of greater than or equal to 10 MHz through the film; and
23. A method for manufacturing a crystalline semiconductor film according to claim 22, wherein the laser beam having the energy period of greater than or equal to 0.5 μm and less than or equal to 10 μm has a wavy energy distribution in a direction perpendicular to a scan direction of the laser beam.
24. A method for manufacturing a crystalline semiconductor film according to claim 23, wherein the laser beam is formed using a diffractive optical element.
25. A method for manufacturing a crystalline semiconductor film according to claim 23, wherein the laser beam is formed by splitting a laser beam emitted from one laser device and combining the split laser beams.
26. A method for manufacturing a crystalline semiconductor film according to claim 23, wherein a plurality of the laser beams are arranged in a direction perpendicular to a scan direction of the laser beam.
27. A method for manufacturing a crystalline semiconductor film according to claim 22, wherein the cap film has a region transmitting the laser beam having an energy capable of crystallizing the semiconductor film and a region which does not transmit the laser beam having an energy capable of crystallizing the semiconductor film, which form stripes, the laser beams are scanned in a direction parallel to the stripes.
28. A method for manufacturing a crystalline semiconductor film according to claim 27,
29. A method for manufacturing a crystalline semiconductor film according to claim 27, wherein an anti-reflective film is formed in the region transmitting the laser beam having an energy capable of crystallizing the semiconductor film, and a film absorbing the laser beam is formed in the region which does not transmit the laser beam having an energy capable of crystallizing the semiconductor film.
30. A method for manufacturing a crystalline semiconductor film according to claim 27, wherein the cap film has irregularities in a striped pattern.
31. A method for manufacturing a crystalline semiconductor film according to claim 27, wherein the laser beam has a trapezoid energy distribution in a direction perpendicular to a scan direction of the laser beam.
32. A method for manufacturing a crystalline semiconductor film according to claim 22, wherein an energy of the laser beam is higher than an energy adequate for melting the semiconductor film.
33. A method for manufacturing a crystalline semiconductor film according to claim 22, wherein a thickness of the semiconductor film is 30 nm to 200 nm.
34. A method for manufacturing a crystalline semiconductor film according to claim 22, wherein the cap film is a silicon nitride film containing 0.1 atomic % to 10 atomic % of oxygen, in which a composition ratio of nitrogen to silicon is 1:1.3 to 1.5.
35. A method for manufacturing a crystalline semiconductor film according to claim 22, wherein the semiconductor film is an amorphous silicon film.
36. A method for manufacturing a crystalline semiconductor film,
wherein a semiconductor element is formed using a crystalline semiconductor film formed in accordance with claim 22.
37. A method for manufacturing a crystalline semiconductor film, comprising the steps of:
38. A method for manufacturing a crystalline semiconductor film according to claim 37, wherein an energy of the laser beam is higher than an energy adequate for melting the semiconductor film.
39. A method for manufacturing a crystalline semiconductor film according to claim 37, wherein a thickness of the semiconductor film is 30 nm to 200 nm.
40. A method for manufacturing a crystalline semiconductor film according to claim 37, wherein the cap film is a silicon nitride film containing 0.1 atomic % to 10 atomic % of oxygen, in which a composition ratio of nitrogen to silicon is 1:1.3 to 1.5.
41. A method for manufacturing a crystalline semiconductor film according to claim 37, wherein the semiconductor film is an amorphous silicon film.
42. A method for manufacturing a crystalline semiconductor film,
wherein a semiconductor element is formed using a crystalline semiconductor film formed in accordance with claim 37. Description
The present invention relates to a method for manufacturing a semiconductor film having a crystal structure by using a laser crystallization technique and a semiconductor device such as a thin film transistor (hereinafter, TFT) including the semiconductor film. More specifically, the present invention relates to a method for manufacturing a crystalline semiconductor film having crystal grains in which crystal grain boundaries are almost parallel to each other and the widths of the crystal grains are controlled, and a semiconductor device including the crystalline semiconductor film.
In recent years, a laser crystallization technique of irradiating an amorphous semiconductor film formed over a glass substrate with a laser beam to form a semiconductor film having a crystal structure (hereinafter referred to as a crystalline semiconductor film) has been widely researched, and a large number of suggestions are given.
Since a crystalline semiconductor film has higher mobility than an amorphous semiconductor film, the crystalline semiconductor film is utilized for TFTs. Consequently, TFTs using the crystalline semiconductor film are used for an active matrix type liquid crystal display device, an organic EL display device, and the like in which, over a glass substrate, TFTs are formed for a pixel portion or for a pixel portion and a driver circuit.
As a crystallization method, other than laser crystallization, there are a thermal annealing method using an annealing furnace and a rapid thermal annealing (RTA) method. However, when the laser crystallization is used, heat is absorbed only by the semiconductor film and crystallization can be performed without increasing temperature of the substrate too much. Therefore, a substance such as glass, plastic, or the like that has a low melting point can be used as the substrate. As a result, a glass substrate which is inexpensive and is easily processed even in a large area can be used; thus, production efficiency can be drastically improved by the laser crystallization.
Attention has been focused on excellent characteristics of such a crystallization method and a semiconductor film has been tried to be manufactured by laser crystallization. Consequently, the development of many techniques has succeeded. Among the successful techniques, there is a technique of obtaining a crystalline semiconductor film having excellent semiconductor characteristics, particularly high mobility, by the steps of irradiating an amorphous semiconductor film in which the concentration of oxygen, nitrogen, and carbon is reduced with a laser beam and subjecting the amorphous semiconductor film to a melting step and a recrystallization step (Patent Document 1: Japanese Published Patent Application No. H5-299339). In this technique, it is suggested that in laser beam irradiation, a protective film is preferably formed over the amorphous semiconductor film, and by the placement of the protective film, an impurity can be prevented from mixing into the semiconductor film.
It is an object of the present invention to provide a method for manufacturing a crystalline semiconductor film as to which the directions of crystal grain boundaries and the widths of crystal grains can be controlled, and further, a method for manufacturing a crystalline semiconductor film which has a specific crystal structure and as to which the directions of crystal grain boundaries and the widths of crystal grains can be controlled. In addition, it is another object of the present invention to provide a method for manufacturing a semiconductor device having excellent electric characteristics and fewer variations in electric characteristics among semiconductor elements.
As described above, one aspect of the present invention is to provide a method for manufacturing a crystalline semiconductor film and a semiconductor device. In the method for manufacturing a crystallize semiconductor film, an insulating film is formed over a substrate; an amorphous semiconductor film is formed over the insulating film; a cap film is formed over the amorphous semiconductor film; a continuous wave laser beam or a laser beam with a repetition rate of greater than or equal to 10 MHz, which is transmitted through the cap film, is scanned so that the amorphous semiconductor film is irradiated with the laser beam; and the amorphous semiconductor film is melted and crystallized. At this time, an energy period in a length direction in a laser beam spot of the laser beam is 0.5 μm to 10 μm, preferably, 1 μm to 5 μm; an energy distribution in a width direction in a laser beam spot of the laser beam is a Gaussian distribution; and the laser beam is scanned so that the amorphous semiconductor film is irradiated with the laser beam for a period of greater than or equal to 5 microseconds and less than or equal to 100 microseconds per region.
Further, one aspect of the present invention is to provide a method for manufacturing a crystalline semiconductor film, a semiconductor device, and the method for manufacturing a crystalline semiconductor film is as the following. In the method for manufacturing a crystalline semiconductor film, an insulating film is formed over a substrate, an amorphous semiconductor film is formed over the insulating film, and a cap film is formed over the amorphous semiconductor film. Further, a continuous wave laser beam or a laser beam with a repetition rate of 10 MHz or more which are transmitted by the cap film is scanned to melt the amorphous semiconductor film, and then the amorphous semiconductor film is crystallized. Here, the cap film is formed so that a region of the amorphous semiconductor film, which is irradiated with a laser beam having an energy capable of crystallizing an amorphous semiconductor film and another region of the amorphous semiconductor film, which is irradiated with a laser beam having an energy which does not crystallize an amorphous semiconductor film form stripes, and the laser beam is scanned in parallel to the stripes. Further, the region of the amorphous semiconductor film, which is irradiated with a laser beam having an energy capable of crystallizing an amorphous semiconductor film and the other region of the amorphous semiconductor film, which is irradiated with a laser beam having an energy which does not crystallize an amorphous semiconductor film are defined here as one period. One period here is 0.5 μm to 10 μm, preferably 1 μm to 5 μm, and a laser beam is scanned to irradiate on a region of the amorphous silicon film for 5 microseconds to 100 microseconds.
A part of the energy of the laser beam is higher than energy that melts the amorphous semiconductor film. The thickness of the amorphous semiconductor film is greater than or equal to 30 nm and less than or equal to 200 nm. The interval between crystal boundaries in the crystalline semiconductor film is greater than or equal to 0.5 μm and less than or equal to 10 μm. The cap film may be a silicon nitride film containing oxygen at 0.1 atomic % to 10 atomic % and having a composition ratio of nitrogen to silicon of 1 to greater than or equal to 1.3 and less than or equal to 1.5. Further, the amorphous semiconductor film may be an amorphous silicon film.
With the above structure, a crystalline semiconductor film having crystal grains with a width of greater than or equal to 0.5 μm and less than or equal to 10 μm, preferably greater than or equal to 1 μm and less than or equal to 5 μm with parallel crystal grain boundaries can be manufactured. Further, a crystalline semiconductor film can be manufactured, in which crystal surface orientations at three surfaces perpendicular to one another are aligned with a certain ratio or more, crystal grain boundaries are parallel to each other, and which has a crystal grain with a width of greater than or equal to 0.5 μm and less than or equal to 10 μm, preferably greater than or equal to 1 μm and less than or equal to 5 μm.
Here, the laser beam is moved in a width direction of the laser beam spot. The width of a crystal grain is in a direction which crosses a scanning direction of the laser beam at 90�, that is, the length of a crystal grain in the same direction as the length of the laser beam spot. In other words, it is the length of a crystal grain in a direction crossing a crystal grain boundary at about 90�.
In accordance with the present invention, a crystalline semiconductor film can be formed, which has large crystal grains as to which crystal grain boundaries are parallel to each other, and the widths of crystal grains are greater than or equal to 0.5 μm and less than or equal to 10 μm, preferably greater than or equal to 1 μm and less than or equal to 5 μm, by crystal growth of a semiconductor film in a predetermined direction through laser beam irradiation. Further, a crystalline semiconductor film having large crystal grains with a width of 0.5 μm to 10 μm, preferably 1 μm to 5 μm with parallel crystal grain boundaries, in which crystal surface orientations at three surfaces perpendicular to one another are aligned to a certain extent can be formed. The crystalline semiconductor films can have excellent semiconductor characteristics.
When a semiconductor element is formed using the crystalline semiconductor film, a semiconductor device with excellent characteristics, such as excellent electric characteristics and fewer variations in electric characteristics among adjacent semiconductor elements, can be manufactured. In particular, when a thin film transistor is formed as a semiconductor element, by controlling the position of a semiconductor layer so that crystal grain boundaries and a moving direction of carries are parallel, the position of a crystal grain boundary crossing a channel can be controlled, and a thin film transistor having high electric characteristics such as high field effect mobility can be obtained.
FIGS. 2A to 2D are a top view of a substrate at a time when a semiconductor film is irradiated with a laser beam and perspective views illustrating energy distributions of the laser beam and a semiconductor layer formed using a crystalline semiconductor film;
FIG. 3 is a schematic view showing a laser irradiation apparatus applicable to the present invention;
FIGS. 4A and 4B are diagram illustrating an example of interference of a laser beam on an irradiation surface in the present invention;
FIGS. 5A to 5F are cross-sectional views illustrating a method for manufacturing a semiconductor device of the present invention;
FIGS. 6A and 6B are a top view of a substrate at a time when a semiconductor film is irradiated with a laser beam and a perspective view illustrating an energy distribution of the laser beam;
FIGS. 7A to 7C are cross-sectional views illustrating a method for manufacturing a semiconductor device of the present invention;
FIGS. 8A and 8B are top views each illustrating a substrate at a time when a semiconductor film is irradiated with a laser beam;
FIGS. 9A to 9D are cross-sectional views illustrating a method for manufacturing a semiconductor device of the present invention;
FIGS. 10A to 10C are cross-sectional views illustrating a method for manufacturing a semiconductor device of the present invention;
FIGS. 12A to 12E are cross-sectional views each illustrating a structure of a light-emitting element which can be applied to the present invention;
FIG. 13 is a diagram illustrating an equivalent circuit of a light-emitting element which can be applied to the present invention;
FIGS. 14A to 14E are cross-sectional views illustrating a method for manufacturing a semiconductor device of the present invention;
FIGS. 15A to 15D are cross-sectional views illustrating a method for manufacturing a semiconductor device of the present invention;
FIGS. 16A to 16C are cross-sectional views illustrating a method for manufacturing a semiconductor device of the present invention;
FIGS. 17A to 17D are cross-sectional views illustrating a method for manufacturing a semiconductor device of the present invention;
FIG. 18 is a diagram explaining a structure of a semiconductor device of the present invention;
FIGS. 19A to 19F are views illustrating applications of a semiconductor device of the present invention;
FIGS. 20A to 20F are views illustrating electronic devices using a semiconductor device of the present invention;
FIG. 21 is a diagram illustrating a structure of an electronic appliance using a semiconductor device of the present invention;
FIG. 22 is an exploded view of an electronic appliance using a semiconductor device of the present invention;
FIGS. 23A and 23B are top views explaining a semiconductor device of the present invention;
FIGS. 24A and 24B are diagrams showing temperature of a semiconductor film irradiated with a conventional pulsed laser beam and temperature of a semiconductor film irradiated with a continuous wave laser beam;
FIG. 25 is a view illustrating a laser irradiation apparatus which can be applied to the present invention; and
FIG. 26 is a perspective view illustrating a crystal surface orientation of a crystalline semiconductor film of the present invention.
Hereinafter, embodiment modes of the present invention will be described. Note that the present invention can be implemented in various modes, and it is easily understood by those skilled in the art that modes and details thereof can be modified in various ways without departing from the spirit and scope of the present invention. Therefore, the present invention should not be construed as being limited to the following description of the embodiment modes.
In Embodiment Mode 1, first, a manufacturing process of a crystalline semiconductor film of the present invention will be briefly described with reference to FIGS. 1A to 4B, and FIGS. 24A and 24B.
First, for example, a glass substrate having a thickness of 0.7 mm is used as a substrate 100 having an insulating surface as shown in FIG. 1A. On one surface thereof, a silicon nitride film containing oxygen which has a thickness of 50 nm to 150 nm and a silicon oxide film containing nitrogen which has a thickness of 50 nm to 150 nm are formed as an insulating film 101 functioning as a base film. Further, as a semiconductor film 102, an amorphous semiconductor film is formed by a plasma CVD method over the insulating film 101 to have a thickness of greater than or equal to 20 nm and less than or equal to 200 nm, preferably greater than or equal to 20 nm and less than or equal to 100 nm, more preferably greater than or equal to 20 nm and less than or equal to 80 nm.
As the substrate 100, a glass substrate made of aluminoborosilicate glass, barium borosilicate glass, quartz, or the like can be used. Besides, a plastic substrate made of PET (polyethylene terephthalate), PEN (polyethylene naphthalate), PES (polyethersulfone), or polypropylene, or a substrate made of a synthetic resin such as acrylic can be used.
The insulating film 101 functioning as a base film may be provided as needed. When the substrate 100 is a glass substrate, the insulating film 101 prevents an impurity from glass from diffusing into the semiconductor film 102, but when the substrate 100 is a quartz substrate, the insulating film 101 functioning as a base film is not necessarily provided. Moreover, a separation layer may be provided between the insulating film 101 and the substrate 100 to separate a semiconductor element that will be formed later from the substrate 100 after the process.
As for the semiconductor film 102, amorphous silicon is used in this embodiment mode; however, polycrystalline silicon, silicon germanium (Si1-xGex(0<x<0.1)), or silicon carbide (SiC) in which a single crystal has a diamond structure can also be used.
This embodiment mode shows an example in which the semiconductor film 102 is formed of amorphous silicon, but polycrystalline silicon may also be used. For example, polycrystalline silicon can be formed as follows: an amorphous silicon film is deposited, a slight amount of an element such as nickel, palladium, germanium, iron, cobalt, platinum, or gold is added to the amorphous silicon film, and heat treatment is performed on the amorphous silicon film at 550� C. for 4 hours.
In addition, after the semiconductor film 102 is formed, it may be heated in an electrical furnace at 500� C. for 1 hour. In this heat treatment, the amorphous silicon film is dehydrogenated. Note that the dehydrogenation is performed to prevent a hydrogen gas from jetting out from the semiconductor film 102 when it is irradiated with a laser beam, and this heat treatment may be omitted if the amount of hydrogen contained in the semiconductor film 102 is small.
Next, a cap film 103 having a thickness greater than or equal to 200 nm and less than or equal to 1000 nm is formed over the semiconductor film 102. The cap film 103 is preferably formed to have a thickness of greater than or equal to 200 nm and less than or equal to 1000 nm, because, if the cap film 103 is too thin, it will become difficult to control a crystal surface orientation of a crystalline semiconductor film that will be formed later. In addition, it is preferable that the cap film 103 have sufficient transmissivity with respect to a wavelength of a laser beam and thermal values such as a thermal expansion coefficient and a value such as ductility that are similar to those of the adjacent semiconductor film. Further, it is preferable that the cap film 103 be a hard and dense film like a gate insulating film of a thin film transistor that will be formed later. Such a hard and dense film can be formed by, for example, reducing the deposition rate. The deposition rate may be greater than or equal to 1 nm/min and less than or equal to 400 nm/min, preferably greater than or equal to 1 nm/min and less than or equal to 100 nm/min.
Note that when much hydrogen is contained in the cap film, heat treatment is performed for dehydrogenation in a similar manner to the semiconductor film 102.
The cap film 103 can be formed of a single layer structure of a silicon nitride film, a silicon oxide film containing nitrogen, a silicon nitride film containing oxygen, or the like. In addition, a cap film in which a silicon oxide film containing nitrogen and a silicon nitride film containing oxygen are sequentially stacked, or a cap film in which a silicon nitride film containing oxygen and a silicon oxide film containing nitrogen are sequentially stacked can be used. Further, a plurality of films may be stacked as a cap film, and an interference effect of light due to a thin film may be utilized, so that light-absorption efficiency of the semiconductor film 102 can be enhanced. With the use of the cap film having such a structure, the semiconductor film 102 can be crystallized with a laser beam with low energy; thus, the cost can be reduced.
Here, as the cap film 103, a silicon nitride film is formed, which has a thickness of greater than or equal to 200 nm and less than or equal to 1000 nm, contains oxygen at 0.1 atomic % to 10 atomic %, and has a composition ratio of nitrogen to silicon of 1 to greater than or equal to 1.3 and less than or equal to 1.5.
In this embodiment mode, as the cap film 103, a silicon nitride film containing oxygen which has a thickness of 300 nm is formed by a plasma CVD method using monosilane, ammonia, and nitrous oxide as a reaction gas. Note that nitrous oxide is used as an oxidizer, and instead of nitrous oxide, oxygen which has an oxidizing effect may also be used.
The following shows a relation between time of irradiation with a laser beam and the width of a crystal grain that is formed when the semiconductor film is irradiated with a continuous wave laser beam or a pulsed laser beam with a repetition rate of greater than or equal to 10 MHz.
In the crystallization process of the semiconductor film, it is considered that an influence of convection due to a temperature gradient in the semiconductor film or convection generated by a pressure difference such as a surface tension is small, and melting time of the semiconductor film is more closely related to crystal growth distance than the above factors. Note that the melting time of the semiconductor film is time from the start of melting of the semiconductor film to the completion of solidification thereof.
In FIG. 24A, a dashed line 114 represents a change of an energy distribution of a pulsed laser beam over time, and a solid line 115 represents a change of temperature of a semiconductor film irradiated with a laser beam over time. As shown in FIG. 24A, when irradiation with a conventional pulsed laser beam is performed, almost all energy of the laser beam is absorbed by the surface of the semiconductor film, and thus, the semiconductor film is heated. Note that the pulse width of a conventional pulsed laser beam is as short as 1 nanosecond to 100 nanoseconds; therefore, the energy of the laser beam with which the semiconductor film is irradiated is absorbed by the surface of the semiconductor film, and the energy becomes heat to heat the semiconductor film rapidly. After that, the heat is transmitted to the semiconductor film and the insulating film 101 functioning as a base film, and thus, the semiconductor film is cooled. Accordingly, the semiconductor film can be heated to greater than or equal to the melting point in a short time. In addition, the temperature of the semiconductor film (solid line 115) is kept at a constant temperature, and then gradually decreased to less than or equal to the melting point of the semiconductor film. In the crystallization using the conventional pulsed laser beam, although melting time 117 of the semiconductor film is a little longer than a pulse width 116, the melting time 117 of the semiconductor film can approximate to the pulse width 116. In the crystallization process of the semiconductor film using a conventional pulsed excimer laser beam, the pulse width 116 is several tens of nanoseconds to several hundreds of nanoseconds; therefore, the melting time 117 of the semiconductor film can also be several tens of nanoseconds to several hundreds of nanoseconds.
The width of a crystal grain of a crystalline semiconductor film that is formed when the semiconductor film is irradiated with a laser beam having the above pulse width is several tens of nanometers to a hundred and several tens of nanometers. The width of a crystal grain can be regarded as a crystal growth distance. According to an experiment, it is found that the crystal grain becomes larger with the longer pulse width. Given that the melting time of the semiconductor film is in proportion to the crystal growth distance, it can be said that the crystal grain grows by 1 nanometer per nanosecond of irradiation time of a laser beam.
The above proportional relation is applied to the case where the semiconductor film is irradiated with a continuous wave laser beam or a pulsed laser beam with a repetition rate of 10 MHz to form a crystalline semiconductor film.
In FIG. 24B, a dashed line 124 represents a change of an energy distribution of a continuous wave laser beam over time, and a solid line 125 represents a change of temperature of a semiconductor film irradiated with a laser beam over time. As shown in FIG. 24B, time 126 during which a certain region of the semiconductor film is irradiated with a continuous wave laser beam is greater than or equal to 5 microseconds and less than or equal to 100 microseconds, preferably greater than or equal to 10 microseconds and less than or equal to 50 microseconds. This can be calculated using the width of a beam spot in a scanning direction of a continuous wave laser beam and the scanning speed. For example, here, the width of a beam spot is to be greater than or equal to 5 μm and less than or equal to 15 μm, and the scanning speed is to be greater than or equal to 300 mm/sec and less than or equal to 700 mm/sec.
Meanwhile, time of irradiation with the continuous wave laser beam of the present invention is longer than the irradiation time of the conventional pulsed laser beam, for example, greater than or equal to 5 microseconds and less than or equal to 100 microseconds, preferably greater than or equal to 10 microseconds and less than or equal to 50 microseconds. Therefore, when the semiconductor film is irradiated with a laser beam, the energy of the laser beam becomes heat, and the heat is transferred to the semiconductor film (the energy that is transferred to the semiconductor film at this time is E1) and transmitted from the semiconductor film to the insulating film 101 functioning as a base film (the energy at this time is E2). In the case where E1 is larger than E2, the energy distribution (dashed line 124) of the laser beam is increased, and the heat due to the energy of the laser beam is transferred to the substrate and the insulating film in addition to the semiconductor film. As a result, as shown in FIG. 24B, the temperature (solid line 125) of the semiconductor film is not increased rapidly but the semiconductor film is heated gradually in a heating period 128.
Next, a period during which the temperature of the semiconductor film is greater than or equal to the melting point is a melting period 127. Then, after the melting period 127 in which the temperature becomes greater than or equal to the melting point of the semiconductor film, the temperature of the semiconductor film is gradually decreased in the case where E2 is larger than E1. This period is referred to as a cooling period 129. Accordingly, even when a certain region of the semiconductor film is irradiated with a laser beam continuously for a period of greater than or equal to 5 microseconds and less than or equal to 100 microseconds, preferably greater than or equal to 10 microsecond and less than or equal to 50 microseconds, the melting period 127 in which the semiconductor film is melted is considered to be substantially about a tenth of the time.
Therefore, it is considered that when the semiconductor film is irradiated with a continuous wave laser beam, the semiconductor film is melted continuously for a period of greater than or equal to 0.5 microseconds and less than or equal to 10 microseconds, preferably greater than or equal to 1 microsecond and less than or equal to 5 microseconds in a certain region of the semiconductor film.
A relation between a crystal growth distance and melting time of the semiconductor film at a time when the semiconductor film is irradiated with a conventional pulsed laser beam is applied to a crystal grain that is formed by irradiating the semiconductor film with a continuous wave laser beam. At that time, the crystal growth distance is greater than or equal to 0.5 μm and less than or equal to 10 μm, preferably greater than or equal to 1 μm and less than or equal to 5 μm. That is, in a crystalline semiconductor film in which crystal grains are adjacent, the width of the crystal is greater than or equal to 0.5 μm and less than or equal to 10 μm, preferably greater than or equal to 1 μm and less than or equal to 5 μm.
Further, in the present invention in, as shown in FIG. 2B, the period of an energy distribution 132 a in the direction of a length 130 a of a beam spot 130 of a laser beam is 0.5 μm to 10 μm, preferably 1 μm to 5 μm. In addition, the value of the energy distribution 132 a of the laser beam is equal to or higher than an energy adequate to melt the semiconductor film. By scanning such a laser beam in one direction, grain boundaries are formed in a direction parallel to a scan direction of the laser beam. Further, crystal width 0.5 μm to 10 μm, preferably 1 μm to 5 μm. It is considered that the crystal growth distance is determined in accordance with the melting time of the semiconductor film at this time; thus, a crystal grain boundary is included even between the adjacent crystal grains with the same surface orientations.
The following will describe the crystal surface orientation and the crystal grain boundaries of the semiconductor film, which is obtained through laser crystallization using the cap film 103.
By providing the cap film 103 over the semiconductor film 102, energy at an interface between the semiconductor film 102 and the cap film 103 is minimized. Accordingly, when the melted semiconductor film 102 is solidified, crystal surface orientations of the semiconductor film can be easily aligned in one direction. Since the crystal growth rate of the semiconductor film is influenced by the crystal surface orientations, the crystal growth rate of the crystals is almost the same when the crystal surface orientations are aligned in one direction. Therefore, the crystal growth time of the crystals is almost the same, and the crystal growth distance of the crystals are almost the same. Further, coagulation of a melted semiconductor begins from a part where the temperature is low. Therefore, coagulation of a beam spot of the laser beam begins at a part where the energy is low, and ends at a part where the energy is high. Since the energy distribution in the length direction of a beam spot of the laser beam is periodic, grain boundaries are formed along the energy distribution on the beam spot of the laser beam.
Accordingly, when the cap film is provided over the semiconductor film and laser crystallization is performed, a semiconductor film having a crystal grain with a width of greater than or equal to 0.5 μm and less than or equal to 10 μm, preferably greater than or equal to 1 μm and less than or equal to 5 μm can be formed. Further, a semiconductor film which has a crystal grain with a width of greater than or equal to 0.5 μm and less than or equal to 10 μm, preferably greater than or equal to 1 μm and less than or equal to 5 μm and in which crystal surface orientations are aligned in one direction or can be regarded as being substantially in the same direction can be formed. In other words, a semiconductor film having characteristics similar to those of a single crystal can be formed.
Next, a laser device and an optical system for forming a beam spot, which are used for the crystallization of the amorphous semiconductor film by laser beam irradiation, will be described.
As shown in FIG. 25, as each of laser devices 11 a and 11 b, a laser device emitting a laser beam having a wavelength that is absorbed by the semiconductor film 102 by several tens of % or more is used. Typically, the second harmonic or the third harmonic can be used. Here, an LD (Laser Diode) pumped continuous wave laser (Nd: YVO4, the second harmonic (wavelength: 532 nm)) with the maximum total output of 20 W is prepared. It is not necessary to particularly limit the wavelength of the laser beam to the second harmonic; however, the second harmonic is superior to other higher-order harmonics in terms of energy efficiency.
Laser power used in the present invention is within a range which can completely melt the semiconductor film and within a range which can form a crystalline semiconductor film having aligned crystal surface orientations. When laser power that is lower than this range is used, the semiconductor film cannot be completely melted, and a crystalline semiconductor film in which crystal grains are small and crystal surface orientations are not aligned in one direction is formed. On the other hand, when laser power higher than this range is used, many crystal nuclei are generated in the semiconductor film, and from the crystal nuclei, disordered crystal growth is generated, and thus, a crystalline semiconductor film with uneven position, size, and surface orientations of crystal grains is formed.
When the semiconductor film 102 is irradiated with the continuous wave laser beam, energy is continuously applied to the semiconductor film 102; therefore, when the semiconductor film is once brought to a melted state, the melted state can be kept. In FIG. 1B, a semiconductor film 107 being irradiated with a laser beam 105 is melted. Further, a solid-liquid interface of the semiconductor film is moved by scanning the semiconductor film with the continuous wave laser beam to grow a crystal grain laterally. Thus, a crystal grain, which is elongated in one direction along the moving direction and has a width of greater than or equal to 0.5 μm and less than or equal to 10 μm, preferably greater than or equal to 1 μm and less than or equal to 5 μm, in which crystal grains are parallel, can be formed. FIG. 2A is a perspective view of what is shown in FIG. 1B. FIG. 2B is an enlarged view of a region irradiated with the laser beam 105 of FIG. 2A, which illustrates an energy distribution 132 a in a length direction of a beam spot 110 of the laser beam. FIG. 2C shows an enlarged view of a region irradiated with the laser beam 105 of FIG. 2A and an energy distribution 132 b in a width direction of the beam spot 110 of the laser beam. In the semiconductor film which is scanned with a laser beam, a crystal grain 133 that is elongated from the beam spot 130 in the laser scanning direction is formed and its width is greater than or equal to 0.5 μm and less than or equal to 10 μm, preferably greater than or equal to 1 μm and less than or equal to 5 μm. Further, grain boundaries are formed in a region irradiated with a part of laser beam of an energy distribution where the energy intensity is low. Further, since crystal growth begins at a part where the energy distribution of the laser beam is low, the grain boundaries are formed at a part where the energy distribution of the laser beam is low. In other words, an energy distribution of a laser beam is periodic; thus, grain boundaries are also periodic and the grain boundaries are parallel.
A solid laser is used at that time because, as compared to a gas laser or the like, its output has high stability and stable process is expected. Note that, without limitation to the continuous wave laser, it is possible to use a pulsed laser with a repetition rate of greater than or equal to 10 MHz.
When a pulsed laser with a high repetition rate is used, the semiconductor film can always be kept melting through the whole thickness, as long as a pulse interval of the laser beam is shorter than time from melting to solidification of the semiconductor film. Thus, a semiconductor film having a crystal grain that is elongated in one direction by the movement of the solid-liquid interface can be formed. In this case, the pulse width of the laser beam is significantly small compared to the melting time of the semiconductor film exceptionally, and laser characteristics are almost the same as those of a continuous wave laser; therefore, the pulsed laser can be treated similarly to the continuous wave laser. In the case of FIG. 25, two laser devices are prepared; however, when the output is sufficiently high, one oscillator may be used.
In this embodiment mode, a Nd: YVO4 laser is used for the laser devices 11 a and 11 b; however, other continuous wave lasers and pulsed lasers having a repetition rate of greater than or equal to 10 MHz can also be used. For example, as a gas laser, there is an Ar laser, a Kr laser, a CO2 laser, or the like. As a solid-state laser, there is a YAG laser, a YLF laser, a YAlO3 laser, a GdVO4 laser, a KGW laser, a KYW laser, an alexandrite laser, a Ti: sapphire laser, a Y2O3 laser, a Nd: YVO4 laser, or the like. A YAG laser, a Y2O3 laser, a GdVO4 laser, or a Nd: YVO4 laser is also called a ceramic laser. As a metal vapor laser, there is a helium cadmium laser or the like.
In addition, as for the laser devices 11 a and 11 b, the laser beam can be emitted with oscillation of TEM00 (a single transverse mode). In such a case, the light-condensing property of a linear beam spot that is obtained on the surface to be irradiated can be increased and an energy density can be increased, which is preferable. Further, using a beam homogenizer such as a lens array or a diffractive optical element, the light-condensing property of a beam spot in a length direction can be improved to improve energy density.
Optical treatment to a laser beam emitted from these laser devices will be briefly described as follows. Laser beams 12 a and 12 b are emitted with the same energy from the laser devices 11 a and 11 b, respectively. A polarization direction of the laser beam 12 b emitted from the laser device 11 b is changed through a wavelength plate 13 because the two laser beams having polarization directions different from each other are combined at a polarizer 14.
After the laser beam 12 b passes through the wavelength plate 13, the laser beam 12 b is reflected by a mirror 22 and made to enter the polarizer 14. Then, the laser beam 12 a and the laser beam 12 b are combined at the polarizer 14 to form a laser beam 12. The wavelength plate 13 and the polarizer 14 are adjusted so that the beam that has been transmitted through the wavelength plate 13 and the polarizer 14 has appropriate energy. Note that, in this embodiment mode, the polarizer 14 is used for combining the laser beams; however, other optical elements such as a polarization beam splitter may also be used.
The laser beam 12 that is synthesized by the polarizer 14 is reflected by a mirror 15, and a cross-section of the laser beam is formed into a linear shape on the surface to be irradiated 18 by a cylindrical lens 16 having a focal length of, for example, 150 mm, and a cylindrical lens 17 having a focal length of, for example, 20 mm. The mirror 15 may be provided depending on an arrangement condition of an optical system of a laser irradiation apparatus.
Further, an optical system for obtaining a wavy energy distribution in the direction of a length direction of the laser spot of the laser beam, which is formed on the surface to be irradiated 18, that is, a period of 0.5 μm to 10 μm, preferably 1 μm to 5 μm, is provided between surface to be irradiated 18 and the cylindrical lens 17. As such an optical system, a diffractive optical element or the like can be used.
Note that the width of the laser beam formed into a linear shape is preferably made small as possible to make the cross section of the laser beam linear, which increases the energy density of the laser beam on the semiconductor film; thus, the processing time can be reduced.
In order to elongate the cross-sectional shape of the laser beam formed into a linear shape thinly, an optical system for thinly concentrating a laser beam may be provided separately. For example, in order to make the cross section of a laser beam linear, a cylindrical lens array, a diffractive optical element, an optical waveguide, or the like can be used.
Further, when a laser medium having a rectangular shape is used, the cross-sectional shape of the laser beam can be made linear at an emission phase.
In the present invention, as described above, a ceramic laser can be used. When the ceramic laser is used, a shape of a laser medium can be shaped relatively freely; therefore, the ceramic laser is suitable for forming such a laser beam.
Then, an irradiation method of the laser beam will be described. Since the surface to be irradiated 18, where the semiconductor film 102 covered with the cap film 103 is formed, is moved at a relatively high speed, the surface to be irradiated 18 is fixed to a suction stage 19. The suction stage 19 can be moved in X and Y directions in a plane parallel to the surface to be irradiated 18 by a single-axis robot for the X-axis 20 and a single-axis robot for the Y axis 21. The one-axis robots are arranged so that the length direction of the linear beam spot corresponds to the Y axis.
Next, the surface to be irradiated 18 is made to move along the width direction of the beam spot, that is, along the X axis, and the surface to be irradiated 18 is irradiated with the laser beam. Here, a scanning speed of the single-axis robot for the X axis 20 is 35 cm/sec, and the laser beam having an energy of 7.0 W is emitted from each of the two laser devices. The laser output after combining the laser beams is 14 W. A region where the semiconductor film is completely melted is formed by irradiation with the laser beam. Through a solidification process, a crystalline semiconductor film of the present invention can be formed, which has a crystal grain with a width of greater than or equal to 0.5 μm and less than or equal to 10 μm, preferably greater than or equal to 1 μm and less than or equal to 5 μm, and in which a crystal is grown in one orientation.
An appropriate scanning speed for the single-axis robot for the X axis 20 is approximately several cm/sec to several hundreds of cm/sec. The speed may be determined as appropriate by a worker in accordance with the output of the laser devices.
Note that, in this embodiment mode, a method is used, in which the semiconductor film 102 which is the surface to be irradiated 18 is moved using the single-axis robot for the X axis 20 and the single-axis robot for the Y axis 21, but the present invention is not limited thereto, and the laser beam can be scanned using a method moving an irradiation system, in which the surface to be irradiated 18 is fixed while an irradiation position of the laser beam is moved; a method moving a surface to be irradiated, in which the irradiation position of the laser beam is fixed while the surface to be irradiated 18 is moved; or a method in which these two methods are combined.
Further, the single-axis robot for the Y axis 21 is moved by a distance equal to the width of the crystalline semiconductor film that is formed, and the single-axis robot for the X axis 20 is rescanned at a predetermined speed, which is 35 cm/sec here. By repeating a series of such operations, the entire surface of the semiconductor film can be efficiently crystallized.
Further, the laser beam may be interfered using a laser irradiation apparatus as shown in FIG. 3 to form a laser beam having an energy period in a length direction of the beam spot is 0.5 μm to 10 μm, preferably 1 μm to 5 μm.
The laser irradiation apparatus shown in FIG. 3 is an example of laser irradiation apparatuses capable of making a period of interference of the laser beam 0.5 μm to 10 μm, preferably 1 μm to 5 μm. A laser beam emitted from a laser device 171 is converted into a harmonic by a nonlinear optical element 172, and split into a plurality of laser beams by a mirror 173 which is a splitting means. The laser beams are reflected by mirrors 174 a and 174 b which are forming means of a laser beam having a periodic energy distribution and reach a substrate 176. On the substrate 176, interference occurs when a plurality of laser beams are combined, and a laser beam having a periodic energy distribution is formed. The substrate 176 is set on a movable stage 177 which is a relative moving means of a substrate to a laser beam. By moving the stage 177, even a large substrate can be irradiated with a laser beam. Further, cylindrical lenses 175 a and 175 b are desirably provided to increase an energy density on an irradiation surface.
Note that a laser device the same as the laser devices 11 a and 11 b shown in FIG. 25 can be suitably selected for the laser device 171. The shape of a laser beam emitted from a laser differs depending on the kinds of the lasers, for example, is circle in the case where the rod shape is cylindrical, and rectangular in the case of a slab shape.
Here, an aspect of interference of a laser beam on an irradiation surface at a time of irradiation with a laser beam using a laser irradiation apparatus shown in FIG. 3 will be described with reference to FIGS. 4A and 4B.
As shown in FIG. 4A, interference occurs when a plurality of laser beams having a wavelength of λ are superimposed on an irradiation surface at an incidence angle of θ. The energy density distribution here is a wavy periodic distribution in which parts of high energy density and parts of low energy density appear alternately as shown in FIG. 4B. Focusing attention on only a part of high energy density, a plurality of spot laser beams can be regarded as being arranged in a line. When such laser beams are used for irradiation, much more efficient irradiation with the laser beam can be performed than a case of using one spot laser beam. That is particularly effective in the case of annealing a semiconductor film using a laser beam having a high energy density, which is emitted from a high output laser. Further, it is quite advantageous because a periodic energy density distribution can be formed by causing interference on an irradiation surface even when a highly coherent laser beam is used.
Further, as shown in FIG. 4A, the plurality of laser beams are incident on the irradiation surface in a symmetrical manner. Therefore, reflection of a laser beam 1 follows an optical path of a laser beam 2 incident on the irradiation surface, and reflection of the laser beam 2 follows an optical path of the laser beam 1 incident on the irradiation surface. In other words, each reflected light behaves in the same way as the return light; thus, bad influences such as variations in the output of the laser device or frequency of the laser beam, rod breakage, or the like are probably caused. Therefore, an isolator is preferably provided to eliminate reflected light and stable the laser.
Next, the cap film 103 is removed by etching. Then, a resist is applied to the crystalline semiconductor film, exposed to light, and developed, whereby the resist is formed into a desired shape. Furthermore, etching is performed using the resist that is formed here as a mask, and the crystalline semiconductor film, which is exposed by the development, is removed. Through this process, an island-like semiconductor film 141 is formed over the insulating film 101 as shown in FIG. 2D. By using this island-like semiconductor film, a semiconductor device having a semiconductor element such as a thin film transistor, a diode, a resistor, a capacitor, or a CCD can be manufactured. Here, as shown in FIG. 1D, a thin film transistor 150 is formed as one mode.
Next, a crystal surface orientation of the crystalline semiconductor film which can be manufactured in this embodiment mode will be described.
In this embodiment mode, the position, size, and a surface orientation of crystal grains of the crystalline semiconductor film 106 from which the cap film 103 thereover has been removed by etching are measured by EBSP (Electron Back Scatter Diffraction Pattern) measurement. First, basic points of EBSP will be described, and then, supplemental explanation is added to describe surface orientations in a crystal semiconductor film in this embodiment mode will be described while complementary explanation is being added.
EBSP refers to a method in which an EBSP detector is connected to a scanning electron microscope (SEM), an orientation of a diffraction image (an EBSP image) of each crystal, which is generated when a sample that is highly tilted in the scanning electron microscope is irradiated with a convergent electron beam, is analyzed, and a crystal surface orientation of a sample is measured according to orientation data and position information of a measurement point (x, y).
When an electron beam is incident to a crystalline semiconductor film, inelastic scatterings occur also at the back, and a linear pattern, which is peculiar to a crystal surface orientation by Bragg diffraction, can also be observed in the sample. Here, this linear pattern is generally referred to as a Kikuchi line. In an EBSP method, a crystal surface orientation of a crystalline semiconductor film is obtained by analyzing a Kikuchi line reflected in a detector.
In a sample having a polycrystalline structure, each crystal grain has a different surface orientation. Thus, every time the irradiated position of the crystalline semiconductor film is moved, the sample is irradiated with the electron beam and the crystal surface orientation in each irradiated position is analyzed. In such a manner, the crystal surface orientation or arrangement information of a crystalline semiconductor film having a flat surface can be obtained. As a measurement region is broader, the tendency of the crystal surface orientations of the entire crystalline semiconductor film can be obtained better; and as there are more measurement points, the more information on the crystal surface orientations in the measurement region can be obtained in detail.
However, a surface orientation within a crystal cannot be determined only by a surface orientation measured from one observation surface of the crystal. This is because, even when crystal surface orientations are aligned in one direction only at one observation surface, it cannot be said that the surface orientations are aligned within the crystals unless the surface orientations are aligned at other observation surfaces. Therefore, in order to determine the surface orientation within the crystal, the surface orientations observed from at least two surfaces are needed, and as more information is obtained from more surfaces, the precision gets higher.
Therefore, when a proportion of a specific crystal surface orientation is relatively high and this orientation is the same at three surfaces in the measurement region, a crystal can be approximately regarded as a single crystal. Actually, as shown in FIG. 26, the surface orientation within the crystal can be specified with high precision by putting together pieces of information on three surfaces (an observation surface A, an observation surface B, and an observation surface C) where each of three vectors perpendicular to one another (a vector a, a vector b, and a vector c) is a normal vector.
In the crystalline semiconductor film that is formed in this embodiment mode, the vectors a to c are set as described below. The vector c is parallel to a scanning direction of the laser beam (i.e., a growth direction of a crystal grain) and the substrate surface; the vector a is perpendicular to the substrate surface and the vector c; and the vector b is parallel to the substrate surface, perpendicular to a crystal growth direction of a crystal grain, and perpendicular to the vectors a and c. According to the information from these three observation surfaces A to C, the crystal surface orientation of the crystalline semiconductor film (direction of a crystal axis in the direction perpendicular to the observation surface) can be specified with high precision.
In a crystalline semiconductor film formed in this embodiment mode, crystal grains on each of the observation surfaces A to C are mostly aligned in certain directions can be formed. For example, a crystalline semiconductor film in which most crystal grains are aligned in the <100> direction at the observation surface A, most crystal grains are aligned in the <310> direction at the observation surface B, and most crystal grains are aligned in the <310> direction at the observation surface C can be formed. Thus, the crystal surface orientations are aligned in one direction with a high proportion at each of the three observation surfaces. In other words, it is found that a crystal which is approximate to a single crystal, in which crystal surface orientations are regarded as being aligned in one direction, is formed in a crystallized region.
In this embodiment mode, a crystalline semiconductor film can be formed, in which the width of crystal grains is greater than or equal to 0.5 μm and less than or equal to 10 μm, preferably greater than or equal to 1 μm and less than or equal to 5 μm, and the crystal surface orientations are aligned in one direction or in directions that can be regarded as substantially the same direction. In other words, the crystalline semiconductor film has characteristics similar to those of a single crystal. By using such a semiconductor film, performance of a semiconductor device can be considerably improved. For example, when a TFT is formed using this crystalline semiconductor film, electric field-effect mobility equivalent to that of a semiconductor device using a single crystalline semiconductor can be obtained.
Further, in such a TFT, it is possible to reduce variations in ON current value (a value of a drain current that flows when a TFT is in an ON state), OFF current value (a value of a drain current that flows when a TFT is in an OFF state), threshold voltage, subthreshold swing, and electric field-effect mobility. Since there is such an advantageous effect, electric characteristics of a TFT are improved, and operational characteristics and reliability of a semiconductor device using such a TFT are improved. Thus, a semiconductor device capable of high-speed operation with high current driving capability and fewer variations in performance among a plurality of elements can be manufactured.
While a semiconductor film is irradiated with a laser beam having an energy distribution in which a period is 0.5 μm to 10 μm, preferably 1 μm to 5 μm in Embodiment Mode 1; this embodiment mode will describe a case where a cap film is formed so that when a region where a laser beam with energy sufficient for crystallizing the semiconductor film is transferred to the semiconductor film and a region where the laser beam with energy sufficient for crystallizing the semiconductor film is not transferred to the semiconductor film are collectively defined as one period, the period is 0.5 μm to 10 μm, preferably 1 μm to 5 μm.
FIGS. 5A, 5C, and 5E are cross-sectional views of a substrate taken parallel to the scan direction of a laser beam with which a semiconductor film is irradiated. FIGS. 5B, 5D, and 5F are cross-sectional view of a substrate taken perpendicular to the scan direction of the laser beam with which a semiconductor film is irradiated. Further, FIG. 6A is a top view of what is shown in FIGS. 5C and 5D, FIG. 6B illustrates an energy distribution of a beam spot of a laser beam in a length direction and a width direction. Note that a cross-sectional view of FIG. 6A taken along A-B corresponds to FIG. 5C, and a cross-sectional view taken along C-D in FIG. 6A corresponds to FIG. 5D.
As shown in FIGS. 5A and 5B, an insulating film 101 is formed over a substrate 100 as in Embodiment Mode 1, and a semiconductor film is formed over the insulating film 101. Next, a cap film 161 having regions with different transmissivities with respect to a laser beam is formed over the semiconductor film 102. As shown in a top view of a substrate in FIG. 6A, a region 161 a which transmits energy sufficient for crystallizing a semiconductor film and a region 161 b which does not transmit energy sufficient for crystallizing the semiconductor film are provided to form stripes. That is, the region 161 a which transfers energy sufficient for crystallizing the semiconductor film to the semiconductor film and the region 161 b which does not transfer energy sufficient for crystallizing the semiconductor film to the semiconductor film are provided to form stripes. In other words, the region 161 a which imparts energy sufficient for crystallizing the semiconductor film for the semiconductor film to absorb and the region 161 b which does not impart energy sufficient for crystallizing the semiconductor film for the semiconductor film to absorb are provided to form stripes. Further, a laser beam 131 is scanned so that the stripes and the scan direction of the laser beam 131 are parallel. Here, in the case where a region which transmits energy sufficient for crystallizing a semiconductor film and a region which does not transmit energy sufficient for crystallizing the semiconductor film are collectively defined as one period, the period is 0.5 μm to 10, preferably 1 μm to 5 μm. Typically, the width of the region 161 a which transmits energy sufficient for crystallizing a semiconductor film semiconductor film is one to ten times the width of the region 161 b which does not transmit energy sufficient for crystallizing the semiconductor film. When the width of the region 161 a which transmits energy sufficient for crystallizing a semiconductor film is 1 μm to 10 μm, the crystal grains to be later formed can have a width of 0.5 μm to 10 μm, preferably 1 μm to 5 μm.
In a case of using a laser beam having a wavelength which can be absorbed in a semiconductor film, as a method for forming the cap film having regions with different transmissivities with respect to the laser beam, when the cap film 161 is formed of a material which transmits light, the thicknesses of regions which transmit the laser beam and the thicknesses of regions which do not transmit laser beams are differentiated in accordance with the wavelength of the laser beam to form stripes. Thus, regions having a thickness to serve as anti-reflective films and regions having a thickness to serve as reflective films can be provided in accordance with the wavelength of the laser beam to form stripes of alternate elevations and depressions. Here, crystal grain boundaries are formed in parts of the semiconductor film in contact with the region of the cap film 161 which has a thickness to serve as the anti-reflective film, and crystal grains are formed in parts of the semiconductor film in contact with the region for the cap film 161 which has a thickness to serve as the reflective film.
Further, in the case of using a laser beam having a wavelength, which can be absorbed in the semiconductor film (for example, visible light, UV light), films which reflect the laser beam may be formed to form stripes in contact with a cap film 161 having a uniform thickness instead of forming films which absorb the laser beam to form stripes. Crystal grains are formed in parts of the semiconductor film which overlap with the films reflecting the laser beam, and crystal grain boundaries are formed in parts of the semiconductor film which overlap with the films which do not reflect the laser beam.
Alternatively, films which absorb the laser beam may be formed to form stripes in contact with the cap film 161 having a uniform film thickness. In that case, the cap film 161 is formed of a material having a band gap which is greater than the energy of the laser beam, and the films which absorb the laser beam are formed from a material having band gap energy smaller than the energy of the laser beam. In the case of forming a silicon nitride oxide film as the cap film 161, the films which absorb the laser beam may be formed of metal; conductive metal oxide such as ITO, which is doped with phosphorus, boron, or a rare gas element; an organic resin in which a colorant is dispersed; or the like. Due to the relation of the heat conductivities between the laser beam and the films which absorb the laser beam, crystal grain boundaries are formed in parts of the semiconductor film which overlap with the films which absorb the laser beam, and crystal grains are formed in parts of the semiconductor film which overlap with regions which are not provided with the films which absorb the laser beam.
Further, when a film which absorbs a laser beam is formed using a laser beam having a wavelength, which is not absorbed in a semiconductor film (for example, infrared light) is used and films which absorb the laser beam are formed in contact with the cap film 161 having a uniform thickness to form stripes, the temperature of the films which absorb the laser beam rises, and the heat is transferred to the semiconductor film. As a result, crystal grains are formed in parts of the semiconductor film which overlap with the films which absorb the laser beam, and grain boundaries are formed in parts of the semiconductor film which do not overlap with the film which absorb the laser beam.
Here, the cap film 161 is formed to have different film thicknesses to form stripes. Regions in the cap film 161 which have a thickness to serve as reflective films are regions which do not transmit a laser beam having energy sufficient for crystallizing a semiconductor film, and regions of the cap film 161 which have a thickness to serve as anti-reflective films are regions which transmit the laser beam having energy sufficient for crystallizing a semiconductor film. Further, as the laser beam, visible light is used.
Next, as show in FIGS. 5C and 5D and FIG. 6A, the semiconductor is irradiated with a laser beam 105. Here, as shown in FIG. 6B, the irradiation is preferably performed using the laser beam having an energy distribution in a length direction of the laser beam 131 which has a trapezoidal shape 132. When the irradiation is performed using a laser beam having such an energy distribution, the energy distribution of a laser beam transferred to the semiconductor film has a curve 162 shown in FIGS. 5C and 5D. As compared to the regions 161 a which easily transmit a laser beam, energy of the regions 161 b which hardly transmit the laser beam is damped, and a period of the laser beam at the cap film 161 is 0.5 μm to 10 μm, preferably 1 μm to 5 μm. By scanning such a laser beam in one direction, grain boundaries can be made parallel, and the widths of crystal grains can be 0.5 μm to 10 μm, preferably 1 μm to 5 μm.
As a manner of irradiation using the laser beam 131 with an energy distribution having the trapezoidal shape 132, a diffractive optical element, an optical waveguide, or the like may be provided between a surface to be irradiated and a cylindrical lens 17 in a laser irradiation apparatus shown in FIG. 25.
By scanning the laser beam entirely over the semiconductor film 102, as shown in FIGS. 5E and 5F, a crystalline semiconductor film 106 can be formed. In the crystalline semiconductor film 106, crystal grain boundaries 106 a are formed in parallel to a scan direction of the laser beam 105. Further, the distance between the crystal grain boundaries, that is, the width of the crystal grains is 0.5 μm to 10 μm, preferably 1 μm to 5 μm.
In this embodiment mode, a crystalline semiconductor film can be formed, in which the width of crystal grains is greater than or equal to 0.5 μm and less than or equal to 10 μm, preferably greater than or equal to 1 μm and less than or equal to 5 μm, and the crystal surface orientations are aligned in one direction or in directions that can be regarded as substantially the same direction. In other words, the crystalline semiconductor film has characteristics similar to those of a single crystal. With the use of such a semiconductor film, performance of a semiconductor device can be considerably improved. For example, when a TFT is formed using this crystalline semiconductor film, electric field-effect mobility equivalent to that of a semiconductor device using a single crystalline semiconductor can be obtained.
In this embodiment mode, a manner of irradiation with a laser beam, which is different from the above embodiment mode will be described with reference to FIGS. 7A to 8B.
FIGS. 7A to 7C each show a cross-sectional view of a substrate taken along a direction parallel to a scan direction of a laser beam for irradiating a semiconductor film, and FIG. 8A is a top view of what is shown in FIG. 7B.
As shown in FIG. 7A, the insulating film 101 is formed over the substrate 100 as in Embodiment Mode 1, the semiconductor film 102 is formed over the insulating film 101, and the cap film 103 is formed over the semiconductor film 102.
Next, as shown in FIG. 7B, the semiconductor film 102 is irradiated with a laser beam 191. Here, the laser beam 191 has a beam spot 192 with a length of 0.5 μm to 10 μm, preferably 1 μm to 5 μm in a length direction. In addition, the half-width of the energy of the laser beam 191 is 0.5 μm to 10 μm, preferably 1 μm to 5 μm. Further, the energy of the laser beam is an energy capable of melting the semiconductor film. By scanning such a laser beam in one direction, a crystalline semiconductor film 106 in which crystal grain boundaries 106 a are parallel and the widths of the crystal grains are 0.5 μm to 10 μm, preferably 1 μm to 5 μm can be formed in a region irradiated with the laser beam as shown in FIG. 8A. In this embodiment mode, the crystal grains and grain boundaries 106 a of the crystalline semiconductor film 106 are formed along the scan mark of the beam spot 192 of the scan laser beam.
As a manner of irradiation with a laser beam having the beam spot 192 of which length is 0.5 μm to 10 μm, preferably 1 μm to 5 μm in a length direction, which has an energy capable of melting a semiconductor film a cylindrical lens or the like may be used as an optical system of the laser irradiation apparatus shown in FIG. 25.
In FIG. 8A, a mode in which the semiconductor film is irradiated with one laser beam is shown; however, the present invention is not limited thereto. For example, a plurality of laser beams may be arranged in a line in a direction crossing a scan direction of the laser beam at 90�. FIG. 8B illustrates a mode in which simultaneous scanning with the five beam spots 192 a to 192 e arranged in a line is performed. The simultaneous scanning with the plurality of beam spots 192 a to 192 d arranged in a line can improve throughput. Further, the crystalline semiconductor film 106 in which the grain boundaries 106 a which are parallel to the width of the beam spots are formed, and the widths of the grains are 0.5 μm to 10 μm, preferably 1 μm to 5 μm can be formed.
In this embodiment mode, a liquid crystal display device which is an example of a semiconductor device will be described with reference to FIGS. 9A to 9D, and 10A to 10C.
As shown in FIG. 9A, in a similar manner to Embodiment Mode 1, an insulating film 101 is formed over a substrate 100, a semiconductor film 102 is formed over the insulating film 101, and a cap film 103 is formed over an amorphous semiconductor film.
Here, as the substrate 100, an AN 100 substrate with a thickness of 0.7 mm is used. As the insulating film 101, a silicon nitride film containing oxygen which has a thickness of 40 nm to 60 nm and a silicon oxide film containing nitrogen which has a thickness of 80 nm to 120 nm are formed by a plasma CVD method. In addition, an amorphous semiconductor film which has a thickness of 20 nm to 80 nm is formed as the semiconductor film 102 by a plasma CVD method. Further, as the cap film 103, a silicon nitride film which has a thickness of greater than or equal to 200 nm and less than or equal to 1000 nm, contains oxygen at 0.1 atomic % to 10 atomic %, and has a composition ratio of nitrogen to silicon of 1 to greater than or equal to 1.3 and less than or equal to 1.5 is formed by a plasma CVD method.
Next, the substrate 100 is heated. Here, heating is performed so that hydrogen contained in the amorphous semiconductor film formed over the substrate 100 is removed. Thus, the substrate 100 is heated at 500� C. for 1 hour and then heated at 550� C. for 4 hours.
Next, as shown in FIG. 9B, the semiconductor film 102 is irradiated with a laser beam 104, and then, the cap film 103 is removed. At that time, as for the laser beam 104, a laser beam having energy that can melt the semiconductor film 102 is selected. A wavelength that can be absorbed by the semiconductor film 102 is selected for the laser beam 104. As a result, a crystalline semiconductor film 106 can be formed over the insulating film 101. Here, as the laser beam 104, the second harmonic of a Nd: YVO4 laser is used. As a method for removing the cap film 103, dry etching, wet etching, polishing, or the like can be used. Here, the cap film 103 is removed by dry etching.
Next, as shown in FIG. 9C, the crystalline semiconductor film 106 is selectively etched to form semiconductor films 201 to 203. As a method for etching the crystalline semiconductor film 106, dry etching, wet etching, or the like can be used. Here, after a resist is applied to the crystalline semiconductor film 106, light-exposure and development are performed to form a resist mask. With the use of the resist mask, a dry etching method in which a flow ratio of SF6:O2 is set to be 4:15 is performed to selectively etch the crystalline semiconductor film 106, and then, the resist mask is removed.
Next, as shown in FIG. 9D, a gate insulating film 204 is formed over the semiconductor films 201 to 203. The gate insulating film is formed using silicon nitride, silicon nitride containing oxygen, silicon oxide, silicon oxide containing nitrogen, or the like with a single layer structure or a layered structure. Here, silicon oxide containing nitrogen which has a thickness of 115 nm is formed by a plasma CVD method.
Then, gate electrodes 205 to 208 are formed. The gate electrodes 205 to 208 can be formed using a metal or a polycrystalline semiconductor doped with an impurity having one conductivity type. In the case of using a metal, tungsten (W), molybdenum (Mo), titanium (Ti), tantalum (Ta), aluminum (Al), or the like can be used. Moreover, metal nitride obtained by nitriding the above metal can also be used. Alternatively, a structure in which a first layer including the metal nitride and a second layer including the metal are stacked may be used. Further, a paste including fine particles is discharged on the gate insulating film by a droplet discharge method, and the paste is dried and baked, and thereby the gate electrode can be formed. Furthermore, a paste including fine particles is formed over the gate insulating film by a printing method, and the paste is dried and baked, and thereby the gate electrode can be formed. Typical examples of the fine particles are fine particles containing, as its main component, any of gold, silver, copper, an alloy of gold and silver, an alloy of gold and copper, an alloy of silver and copper, and an alloy of gold, silver, and copper. Here, after a tantalum nitride film having a thickness of 30 nm and a tungsten film having a thickness of 370 nm are formed over the gate insulating film 204 by a sputtering method, a resist mask formed by a photolithography process is used to etch the tantalum nitride film and the tungsten film selectively, and the gate electrodes 205 to 208 each having a shape, in which the width of the tantalum nitride film is larger than that of the tungsten film, are formed.
Next, using the gate electrodes 205 to 208 as masks, an impurity element which imparts n-type conductivity and an impurity element which imparts p-type conductivity are added to the semiconductor films 201 to 203, and source regions and drain regions 209 to 214 and a high-concentration impurity region 215 are formed. In addition, low-concentration impurity regions 216 to 223 overlapping with parts of the gate electrodes 205 to 208 are formed. Further, channel regions 201 c to 203 c and 203 d overlapping with the gate electrodes 205 to 208 are formed. Here, the source regions and drain regions 209, 210, 213, and 214; the high concentration impurity region 215; and the low concentration impurity regions 216, 217, and 220 to 223 are doped with boron which is an impurity element imparting p-type conductivity. In addition, source regions and drain regions 211, 212, and the low concentration impurity regions 218 and 219 are doped with phosphorus which is an impurity element imparting n-type conductivity.
Then, heat treatment is performed in order to activate the impurity element that is added to the semiconductor film. Here, heating in a nitrogen atmosphere at 550� C. for 4 hours is performed. Through the above steps, thin film transistors 225 to 227 are formed. In addition, as the thin film transistors 225 and 227, p-channel thin film transistors are formed, and as the thin film transistor 226, an n-channel thin film transistor is formed. In addition, a driver circuit is configured with the p-channel thin film transistor 225 and the n-channel thin film transistor 226, and the p-channel thin film transistor 227 functions as an element applying voltage to a pixel electrode.
Next, as shown in FIG. 10A, a first interlayer insulating film for insulating the gate electrodes and wirings of the thin film transistors 225 to 227 is formed. Here, as the first interlayer insulating film, a silicon oxide film 231, a silicon nitride film 232, and a silicon oxide film 233 are stacked. Then, wirings 234 to 239 connecting to source and drain regions of the thin film transistors 225 and 227 and a connecting terminal 240 are formed over the silicon oxide film 233 which is a part of the first interlayer insulating film. Here, after a Ti film having a thickness of 100 nm, an Al film having a thickness of 300 nm, and a Ti film having a thickness of 100 nm are sequentially formed by a sputtering method, with the use of a resist mask formed by a photolithography process, etching is selectively performed, and the wirings 234 to 239 and the connecting terminal 240 are formed. After that, the resist mask is removed.
Next, a second interlayer insulating film 241 is formed over the first interlayer insulating film, the wirings 234 to 239, and the connection terminal 240. As the second interlayer insulating film 241, an inorganic insulating film such as a silicon oxide film, a silicon nitride film, or a silicon oxide nitride film can be used, and these insulating films are formed with a single layer structure or a layered structure including two or more layers. In addition, as a method for forming the inorganic insulating film, a sputtering method, an LPCVD method, a plasma CVD method, or the like may be used. Here, after forming a silicon nitride film containing oxygen which has a thickness of 100 nm to 150 nm by a plasma CVD method, the silicon nitride film containing oxygen is selectively etched with the use of a resist mask formed by a photolithography process to form a contact hole reaching the wiring 239 of the thin film transistor 227 and the connection terminal 240, and at the same time, the second interlayer insulating film 241 is formed. After that, the resist mask is removed.
As in this embodiment mode, when the second interlayer insulating film 241 is formed, TFTs, wirings, and the like of a driver circuit portion can be prevented from being exposed, and the TFTs can be protected from contaminants.
Next, a first pixel electrode 242 connecting to the wiring 239 of the thin film transistor 227 and a conductive film 244 connecting to the connection terminal 240 are formed. When a liquid crystal display device is a transmissive type liquid crystal display device, the first pixel electrode 242 is formed of a light-transmitting conductive film. In addition, when a liquid crystal display device is a reflective type liquid crystal display device, the first pixel electrode 242 is formed of a reflective conductive film. Here, the first pixel electrode 242 and the conductive film 244 are formed in such a way that after ITO containing silicon oxide having a thickness of 125 nm is formed by a sputtering method, etching is selectively performed with the use of a resist mask formed by a photolithography process.
Next, an insulating film 243 functioning as an alignment film is formed, and the insulating film 243 is formed in such a way that after a film of a high molecular compound such as polyimide, polyvinyl alcohol, or the like is formed by a roll coating method, a printing method, or the like, rubbing is performed. In addition, the insulating film 243 can be formed by deposition of SiO from an oblique angle to a substrate. Alternatively, the insulating film 243 can be formed by polymerizing a photo-reactive type high molecular compound by irradiation of the photo-reactive type high molecular compound with polarized UV light. Here, the insulating film 243 is formed by the steps of printing a high molecular compound film such as a layer of polyimide, polyvinyl alcohol, or the like, and baking and rubbing the film.
Next, as shown in FIG. 10B, a second pixel electrode 253 is formed on a counter substrate 251, and an insulating film 254 functioning as an alignment film is formed on the second pixel electrode. Note that a colored film 252 may be formed between the counter substrate 251 and the pixel electrode 253.
The counter substrate 251 can be formed by selecting a substrate similar to the substrate 100. In addition, the second pixel electrode 253 can be formed in a similar manner to the first pixel electrode 242. The insulating film 254 functioning as an alignment film can be formed in a similar manner to the insulating film 243. Moreover, the colored film 252 is a film which is necessary when color display is performed, and in RGB mode, a colored film in which dye or pigment corresponding to each color of red, green, and blue is dispersed is formed corresponding to each pixel.
Next, the substrate 100 and the counter substrate 251 are bonded together using a sealant 257. Further, a liquid crystal layer 255 is formed between the substrate 100 and the counter substrate 251. Furthermore, the liquid crystal layer 255 can be formed by using a vacuum injection method which utilizes capillarity to inject a liquid crystal material into a region which is surrounded by the insulating films 243 and 254 which serve as alignment films and the sealant 257. Alternatively, the liquid crystal layer 255 can be formed by the steps of forming a sealant 157 over one surface of the counter substrate 251, dropping a liquid crystal material to a region enclosed by the sealant, and attaching the counter substrate 251 and the substrate 100 together by pressure bonding using the sealant, under reduced pressure.
As the sealant 257, a thermosetting epoxy resin, a UV-curable acrylic resin, a thermoplastic nylon, polyester, or the like can be formed using a dispensing method, a printing method, a thermocompression method, or the like. Note that by dispersing a filler in the sealant 257, the distance between the substrate 100 and the counter substrate 251 can be maintained. Here, a thermosetting epoxy resin is used for the sealant 257.
Further, in order to maintain the distance between the substrate 100 and the counter substrate 251, spacers 256 may be provided between the insulating films 243 and 254 which serve as alignment films. The spacers can be formed by applying an organic resin and etching the organic resin into a desired shape; representatively, a columnar shape or a cylindrical shape. Further, spacer beads may be used as the spacers. Here, spacer beads are used as the spacers 256.
Further, although not shown, one or both of the substrate 100 and the counter substrate 251 are provided with a polarizing plate.
Next, as shown in FIG. 10C, in a terminal portion 263, a connection terminal which is connected to a gate wiring or a source wiring of a thin film transistor (in FIG. 10C, the connection terminal 240 which is connected to a source wiring or a drain wiring is shown) is provided. An FPC (flexible printed circuit) 262 which serves as an external input terminal is connected to the connection terminal 240 through the conductive film 244 and an anisotropic conductive film 261. The connection terminal 240 receives video signals and clock signals through the conductive film 244 and the anisotropic conductive film 261.
A circuit which drives a pixel, such as a source driver or a gate driver, is formed in a driver circuit portion 264. Here, the n-channel thin film transistor 226 and the p-channel thin film transistor 225 are provided. Note that the n-channel thin film transistor 226 and the p-channel thin film transistor 225 form a CMOS circuit.
A plurality of pixels are formed in a pixel portion 265, and a liquid crystal element 258 is formed in each pixel. The liquid crystal element 258 is a portion in which the first pixel electrode 242, the second pixel electrode 253, and the liquid crystal layer 255, which fills the gap between the first pixel electrode 242 and the second pixel electrode 253, overlap with one another. The first pixel electrode 242 included in the liquid crystal element 258 is electrically connected to the thin film transistor 227.
A liquid crystal display device can be manufactured through the above-described process. As to the liquid crystal display device shown in this embodiment mode, cracks to be in a layer over a substrate or on a substrate can be reduced in a manufacturing process. Therefore, liquid crystal display devices can be manufactured with high yield.
As shown in FIG. 11A, thin film transistors 225 to 227 are formed over a substrate 100 with an insulating film 101 therebetween using similar steps to those in Embodiment Mode 4. Further, a silicon oxide film 231, a silicon nitride film 232, and a silicon oxide film 233 are stacked as a first interlayer insulating film which insulates gate electrodes and wirings of the thin film transistors 225 to 227. Further, wirings 308 to 313 which are connected to semiconductor films of the thin film transistors 225 to 227, and a connection terminal 314 are formed over the silicon oxide film 233, which is a part of the first interlayer insulating film.
Next, a second interlayer insulating film 315 is formed over the first interlayer insulating film, the wirings 308 to 313, and the connection terminal 314. Then, a first electrode 316 which is connected to the wiring 313 of the thin film transistor 227 and a conductive film 320 which is connected to the connection terminal 314 are formed. To form the first electrode 316 and the conductive film 320, ITO containing silicon oxide is formed by a sputtering method to a thickness of 125 nm, and then is selectively etched using a resist mask formed by a photolithography process.
By forming the second interlayer insulating film 315 as in this embodiment mode, exposure of the TFTs, wirings, and the like of a driver circuit portion can be prevented, and the TFTs can be protected from contaminants.
Next, an organic insulating film 317 which covers an end portion of the first electrode 316 is formed. Here, photosensitive polyimide is applied and baked. Then, exposure and development are performed to form the organic insulating film 317 such that a driver circuit, the first electrode 316 in a pixel region, and the second interlayer insulating film 315 on the periphery of the pixel region are exposed.
Next, a layer 318 containing a light-emitting substance is formed by an evaporation method over a part of the first electrode 316 and the organic insulating film 317. The layer 318 containing a light-emitting substance is formed of an organic or inorganic compound having a light-emitting property. Further, the layer 318 containing a light-emitting substance may be formed of both an organic compound having a light-emitting property and an inorganic compound having a light-emitting property. Moreover, a red-light-emitting pixel, a blue-light-emitting pixel, and a green-light-emitting pixel can be formed by using a red-light-emitting substance, a blue-light-emitting substance, and a green-light-emitting substance, respectively, for the layer 318 containing a light-emitting substance.
When the layer 318 containing a light-emitting substance is formed using a layer which uses an organic compound and has a light-emitting function (hereinafter referred to as a light-emitting layer 343), the light-emitting element 321 functions as an organic EL element.
As an organic compound with a light-emitting property, for example, 9,10-di(2-naphthyl)anthracene (abbr.: DNA); 2-tert-butyl-9,10-di(2-naphthyl)anthracene (abbr.: t-BuDNA); 4,4′-bis(2,2-diphenylvinyl)biphenyl (abbr.: DPVBi); coumarin 30; coumarin 6; coumarin 545; coumarin 545T; perylene; rubrene; periflanthene; 2,5,8,11-tetra(tert-butyl)perylene (abbr.: TBP); 9,10-diphenylanthracene (abbr.: DPA); 5,12-diphenyltetracene; 4-(dicyanomethylene)-2-methyl-6-[p-(dimethylamino)styryl]-4H-pyran (abbr.: DCM1); 4-(dicyanomethylene)-2-[2-(julolidin-9-yl)ethenyl]-6-methyl-4H-pyran (abbr.: DCM2); 4-(dicyanomethylene)-2,6-bis[p-(dimethylamino)styryl]-4H-pyran (abbr.: BisDCM); or the like may be used. Further, the following compounds capable of emitting phosphoresce can also be used: bis[2-(4′,6′-difluorophenyl)pyridinato-N,C2′](picolinato)iridium (abbr.: FIrpic); bis{2-[3′,5′-bis(trifluoromethyl)phenyl]pyridinato-N,C2′}(picolinato)iridium (abbr.: Ir(CF3 ppy)2(pic)); tris(2-phenylpyridinato-N,C2′)iridium (abbr.: Ir(ppy)3); (acetylacetonato)bis(2-phenylpyridinato-N,C2′)iridium (abbr.: Ir(ppy)2(acac)); (acetylacetonato)bis[2-(2′-thienyl)pyridinato-N,C3′]iridium (abbr.: Ir(thp)2(acac)); (acetylacetonato)bis(2-phenylquinolinato-N,C2′)iridium (abbr.: Ir(pq)2(acac)); (acetylacetonato)bis[2-(2′-benzothienyl)pyridinato-N,C3′]iridium (abbr.: Ir(btp)2(acac)); and the like.
Further, as shown in FIG. 12A, the light-emitting element 321 may include the first electrode 316, and also the layer 318 containing a light-emitting substance and the second electrode 319, which are formed over the first electrode 316. The layer 318 containing a light-emitting substance includes a hole-injecting layer 341 formed of a material with a hole-injecting property, a hole-transporting layer 342 formed of a material with a hole-transporting property, the light-emitting layer 343 formed of an organic compound with a light-emitting property, an electron-transporting layer 344 formed of a material with an electron-transporting property, and an electron-injecting layer 345 formed of a material with an electron-injecting property.
As the material with a hole-transporting property, phthalocyanine (abbr.: H2Pc); copper phthalocyanine (abbr.: CuPc); vanadyl phthalocyanine (abbr.: VOPc); 4,4′,4″-tris(N,N-diphenylamino)triphenylamine (abbr.: TDATA); 4,4′,4″-tris[N-(3-methylphenyl)-N-phenylamino]triphenylamine (abbr.: MTDATA); 1,3,5-tris[N,N-di(m-tolyl)amino]benzene (abbr.: m-MTDAB); N,N′-diphenyl-N,N′-bis (3-methylphenyl)-1,1′-biphenyl-4,4′-diamine (abbr.: TPD); 4,4′-bis[N-(1-naphthyl)-N-phenylamino]biphenyl (abbr.: NPB); 4,4′-bis{N-[4-di(m-tolyl)amino]phenyl-N-phenylamino}biphenyl (abbr.: DNTPD); 4,4′-bis[N-(4-biphenylyl)-N-phenylamino]biphenyl (abbr.: BBPB); 4,4′,4″-tri(N-carbazolyl)triphenylamine (abbr.: TCTA); and the like may be used. Note that the present invention is not limited thereto. Among the above compounds, an aromatic amine compound typified by TDATA, MTDATA, m-MTDAB, TPD, NPB, DNTPD, BBPB, TCTA, NPB or the like is preferable as the organic compound because it easily generates holes. The substances mentioned here generally have a hole mobility of 10−6 cm2/Vs or more.
As a material with a hole-injecting property, the aforementioned materials with a hole-transporting property can be used. Further, a chemically-doped conductive high-molecular compound can also be used. For example, polyaniline (abbr.: PAni); polyethylene dioxythiophene (abbr.: PEDOT) doped with polystyrene sulfonate (abbr.: PSS); or the like can also be used. Further, a thin film of an inorganic semiconductor such as molybdenum oxide, vanadium oxide, or nickel oxide, or an ultrathin film of an inorganic insulator such as aluminum oxide is also effective.
Here, a material with an electron-transporting property may be a material including a metal complex with a quinoline skeleton or a benzoquinoline skeleton, or the like, such as tris(8-quinolinolato)aluminum (abbr.: Alq3), tris(4-methyl-8-quinolinolato)aluminum (abbr.: Almq3), bis(10-hydroxybenzo[h]-quinolinato)beryllium (abbr.: BeBq2), or bis(2-methyl-8-quinolinolato)-4-phenylphenolato-aluminum (abbr.: BAlq). Further, a metal complex having an oxazole ligand or a thiazole ligand, or the like can also be used, such as bis[2-(2-hydroxyphenyl)benzoxazolato]zinc (abbr.: Zn(BOX)2), or bis[2-(2-hydroxyphenyl)benzothiazolato]zinc (abbr.: Zn(BTZ)2). As an alternative to a metal complex, 2-(4-biphenylyl)-5-(4-tert-butylphenyl)-1,3,4-oxadiazole (abbr.: PBD), 1,3-bis[5-p-tert-butylphenyl)-1,3,4-oxadiazol-2-yl]benzene (abbr.: OXD-7), 3-(4-tert-butylphenyl)-4-phenyl-5-(4-biphenylyl)-1,2,4-triazole (abbr.: TAZ), 3-(4-tert-butylphenyl)-4-(4-ethylphenyl)-5-(4-biphenylyl)-1,2,4-triazole (abbr.: p-EtTAZ), bathophenanthroline (abbr.: BPhen), bathocuproin (abbr.: BCP), or the like can be used. The substances mentioned here generally have an electron mobility of 10−6 cm2/Vs or more.
As a material with an electron-injecting property, the aforementioned materials with an electron-transporting property may be used. Further, an ultrathin film of an insulator such as the following is often used: an alkali metal halide such as lithium fluoride or cesium fluoride; an alkaline-earth metal halide such as calcium fluoride; or an alkali metal oxide such as lithium oxide. Further, an alkali metal complex such as lithium acetyl acetonate (abbr.: Li(acac)) or 8-quinolinolato-lithium (abbr.: Liq) is also effective. Furthermore, a material mixed by, for example, co-evaporating the aforementioned material with an electron-transporting property and a metal with a low work function such as Mg, Li, or Cs can also be used.
As shown in FIG. 12B, the light-emitting element 321 may be formed using the first electrode 316, the layer 318 containing a light-emitting substance, and the second electrode 319. The layer 318 containing a light-emitting substance includes a hole-transporting layer 346 formed of an organic compound with a light-emitting property and an inorganic compound having an electron-accepting property with respect to the organic compound with a light-emitting property, a light-emitting layer 343 formed of an organic compound with a light-emitting property, and an electron-transporting layer 347 formed of an organic compound with a light-emitting property and an inorganic compound having an electron-donating property with respect to the organic compound with a light-emitting property.
As the organic compound for the hole-transporting layer 346 formed of the organic compound with a light-emitting property and the inorganic compound having an electron-accepting property with respect to the organic compound with a light-emitting property, the aforementioned organic compound with a hole-transporting property may be used as appropriate. Further, the inorganic compound may be any kind of inorganic compound as long as it can easily accept electrons from the organic compound. As the inorganic compound, various metal oxides or metal nitrides can be used. In particular, an oxide of a transition metal belonging to any of Group 4 to Group 12 in the periodic table is preferable because it is likely to exhibit an electron-accepting property. Specifically, titanium oxide, zirconium oxide, vanadium oxide, molybdenum oxide, tungsten oxide, rhenium oxide, ruthenium oxide, zinc oxide, or the like can be used. Among these metal oxides, oxides of transition metals belonging to any of Group 4 to Group 8 in the periodic table are preferable because many of them easily accept electrons. In particular, vanadium oxide, molybdenum oxide, tungsten oxide, and rhenium oxide are preferable because they can be formed by vacuum evaporation and are easy to be handled.
As the organic compound for the electron-transporting layer 347 formed of the organic compound with a light-emitting property and the inorganic compound having an electron-donating property with respect to the organic compound with a light-emitting property, the aforementioned organic compound with an electron-transporting property may be used as appropriate. Further, the inorganic compound may be any kind of inorganic compound as long as it can easily donate electrons to the organic compound. As the inorganic compound, various metal oxides or metal nitrides can be used. In particular, an alkali metal oxide, an alkaline-earth metal oxide, a rare-earth metal oxide, an alkali metal nitride, an alkaline-earth metal nitride, and a rare-earth metal nitride are preferable because they are likely to exhibit an electron-donating property. Specifically, lithium oxide, strontium oxide, barium oxide, erbium oxide, lithium nitride, magnesium nitride, calcium nitride, yttrium nitride, lanthanum nitride, and the like are preferable. In particular, lithium oxide, barium oxide, lithium nitride, magnesium nitride, and calcium nitride are preferable because they can be formed by vacuum evaporation and are easy to be handled.
The electron-transporting layer 347 and the hole-transporting layer 346 which are each formed of an organic compound with a light-emitting property and an inorganic compound are superior in electron injecting/transporting properties. Therefore, various materials can be used for the first electrode 316 and the second electrode 319 without limiting their work functions very much. Moreover, the drive voltage can be reduced.
Further, the light-emitting element 321 functions as an inorganic EL element by having a layer which uses an inorganic compound and has a light-emitting function (hereinafter referred to as a light-emitting layer 349) as the layer 318 containing a light-emitting substance. Inorganic EL elements are classified as dispersion-type inorganic EL elements or thin-film inorganic EL elements, depending on their structures. They differ from one another in that the former include a layer containing a light-emitting substance in which particles of a light-emitting material are dispersed in a binder and the latter include a layer containing a light-emitting substance formed of a thin film of a light-emitting material. However, they share the fact that they both need electrons accelerated by a high electric field. Further, mechanisms for obtaining light-emission include donor-acceptor recombination light emission, which utilizes a donor level and an acceptor level, and localized light emission, which utilizes a core electron transition of a metal ion. In many cases, dispersion-type inorganic EL elements utilize donor-acceptor recombination light emission, while thin-film inorganic EL elements utilize localized light emission. A structure of an inorganic EL element is described below.
A light-emitting material that can be used in this embodiment mode includes a base material and an impurity element which serves as a light-emitting center. By varying the impurity element that is included, various colors of light emission can be obtained. Various methods can be used to manufacture the light-emitting material, such as a solid phase method or a liquid phase method (e.g., a coprecipitation method). Further, a liquid phase method, such as a spray pyrolysis method, a double decomposition method, a method which employs a pyrolytic reaction of a precursor, a reverse micelle method, a method in which one or more of the above methods is combined with high-temperature baking, a freeze-drying method, or the like can be used.
In the solid phase method, a base material and an impurity element or a compound containing an impurity element are weighed, mixed in a mortar, and reacted by being heated and baked in an electric furnace. Thereby, the impurity element is included in the base material. Baking temperature is preferably 700� C. to 1500� C. This is because if the temperature is too low, the solid phase reaction will not proceed, and if the temperature is too high, the base material will decompose. The materials may be baked in powdered form. However, it is preferable to bake the materials in pellet form. Baking at a relatively high temperature is necessary in the solid phase method. However, due to its simplicity, this method has high productivity and is suitable for mass production.
The liquid phase method (e.g., a coprecipitation method) is a method in which a base material or a compound containing a base material, and an impurity element or a compound containing an impurity element, are reacted in a solution, dried, and then baked. Particles of the light-emitting material are distributed uniformly, and the reaction can proceed even if the particles are small and the baking temperature is low.
In the case of using a solid phase method to synthesize a light-emitting material for donor-acceptor recombination light-emission, a base material, a first impurity element or a compound containing the first impurity element, and a second impurity element or a compound containing the second impurity element are weighed, mixed in a mortar, then heated and baked in an electric furnace. Baking temperature is preferably 700� C. to 1500� C. This is because if the temperature is too low, the solid phase reaction will not proceed, and if the temperature is too high, the base material will decompose. The materials may be baked in powdered form. However, it is preferable to bake the materials in pellet form. As the base material, any of the above-mentioned base materials can be used. As the first impurity element or the compound containing the first impurity element, fluorine (F), chlorine (Cl), or aluminum sulfide or the like can be used, for example. As the second impurity element or the compound containing the second impurity element, copper, silver, copper sulfide, silver sulfide, or the like can be used, for example.
Further, in the case of employing a solid phase reaction, a compound including the first impurity element and the second impurity element may be used as an impurity element. In such a case, since the impurity elements diffuse readily and the solid phase reaction proceeds readily, a uniform light-emitting material can be obtained. Further, since an unnecessary impurity element does not enter the light-emitting material, a light-emitting material with high purity can be obtained. As a compound including the first impurity element and the second impurity element, for example, copper chloride, silver chloride, or the like can be used.
Note that the concentration of the impurity elements in the base material may be 0.01 atomic % to 10 atomic %, and is preferably in the range of 0.05 atomic % to 5 atomic %.
FIG. 12C shows a cross-section of an inorganic EL element in which the layer 318 containing a light-emitting substance is formed using a first insulating layer 348, a light-emitting layer 349, and a second insulating layer 350.
In the case of a thin film inorganic EL element, the light-emitting layer 349 includes the above-mentioned light-emitting material. As a method for forming the light-emitting layer 349, a resistive heating evaporation method, a vacuum evaporation method such as an electron-beam evaporation (EB evaporation) method, a physical vapor deposition (PVD) method such as a sputtering method, a chemical vapor deposition (CVD) method such as a metal organic CVD method or a low-pressure hydride transport CVD method, an atomic layer epitaxy (ALE) method, or the like can be used.
There is no particular limitation on the materials used for the first insulating layer 348 and the second insulating layer 350; however, preferably, they have a high insulating property and dense film quality. In addition, preferably, the materials of the insulating layers have a high dielectric constant. For example, silicon oxide, yttrium oxide, titanium oxide, aluminum oxide, hafnium oxide, tantalum oxide, barium titanate, strontium titanate, lead titanate, silicon nitride, zirconium oxide, or the like, or a mixed film or a stacked film containing two or more of these materials can be used. The first insulating layer 348 and the second insulating layer 350 can be formed by sputtering, an evaporation method, CVD, or the like. There is no particular limitation on the thickness of the first insulating layer 348 and the second insulating layer 350, but preferably it is in the range of 10 nm to 1000 nm. Note that a light-emitting element of this embodiment mode does not necessarily require hot electrons, and therefore has the advantages that a thin film can be formed and drive voltage can be reduced. Film thickness is preferably less than or equal to 500 nm, more preferably less than or equal to 100 nm.
Although not shown, a buffer layer may be provided between the light-emitting layer 349 and the insulating layers 348 and 350 or between the light-emitting layer 349 and the electrodes 316 and 319. The buffer layer facilitates carrier injection and suppresses mixture of the layers. There is no particular limitation on the material of the buffer layer. However, for example, zinc sulfide, selenium sulfide, tellurium sulfide, cadmium sulfide, calcium sulfide, strontium sulfide, barium sulfide, copper sulfide, lithium fluoride, calcium fluoride, barium fluoride, magnesium fluoride, or the like can be used.
Moreover, as shown in FIG. 12D, the layer 318 containing a light-emitting substance may be formed using a light-emitting layer 349 and a first insulating layer 348. In this case, in FIG. 12D, the first insulating layer 348 is provided between the second electrode 319 and the light-emitting layer 349. Note that the first insulating layer 348 may also be provided between the first electrode 316 and the light-emitting layer 349.
Further, the layer 318 containing a light-emitting substance may be formed using only the light-emitting layer 349. In other words, the light-emitting element 321 may be formed using the first electrode 316, the layer 318 containing a light-emitting substance, and the second electrode 319.
In the case of a dispersion-type inorganic EL element, a layer containing a light-emitting substance which is the form of a film is formed by dispersing particles of a light-emitting material in a binder. When particles with a desired size cannot be satisfactorily obtained by a method for manufacturing the light-emitting material, the material may be processed into particles by being crushed in a mortar or the like. A binder refers to a substance for fixing the dispersed particles of a light-emitting material in place and maintaining the shape of the layer containing a light-emitting substance. The light-emitting material is dispersed evenly throughout the layer containing a light-emitting substance and fixed in place by the binder.
In the case of the dispersion-type inorganic EL element, the layer containing a light-emitting substance can be formed by a droplet discharge method that can selectively form the layer containing a light-emitting substance, a printing method (such as screen printing or offset printing), a coating method such as a spin coating method, a dipping method, a dispensing method, or the like. There is no particular limitation on the thickness of the layer. However, it is preferably in the range of 10 nm to 1000 nm. Further, the proportion of the light-emitting material in the layer containing a light-emitting substance, which includes the light-emitting material and the binder, is preferably greater than or equal to 50 wt % and less than or equal to 80 wt %.
An element shown in FIG. 12E has a first electrode 316, a layer 318 containing a light-emitting substance, and a second electrode 319. The layer 318 containing a light-emitting substance is formed using an insulating layer 348 and a light-emitting layer in which a light-emitting material 352 is dispersed in a binder 351. FIG. 12E shows a structure in which the insulating layer 348 is in contact with the second electrode 319; however, a structure in which the insulating layer 348 is in contact with the first electrode 316 may also be used. Moreover, insulating layers may be formed in contact with each of the first electrode 316 and the second electrode 319 in the element. Further, the insulating layers in contact with the first electrode 316 and the second electrode 319 do not need to be provided in the element.
As a binder which can be used in this embodiment mode, an insulating material such as an organic material or an inorganic material can be used. A mixed material containing an organic material and an inorganic material may also be used. As an organic insulating material, a polymer with a relatively high dielectric constant, such as a cyanoethyl cellulose resin, or a resin such as polyethylene, polypropylene, a polystyrene based resin, a silicone resin, an epoxy resin, or vinylidene fluoride can be used. Further, a siloxane resin or a heat-resistant high molecular material such as aromatic polyamide or polybenzimidazole may also be used. A siloxane resin is a resin which includes a Si�O�Si bond. Siloxane is a material which has a skeleton structure formed of bonds of silicon (Si) and oxygen (O). As a substituent, an organic group containing at least hydrogen (for example, an alkyl group or aromatic hydrocarbon) can be used. Alternatively, a fluoro group may be used as a substituent. Further alternatively, both a fluoro group and an organic group containing at least hydrogen may be used as a substituent. Further, the following resin materials may also be used: a vinyl resin such as polyvinyl alcohol or polyvinylbutyral, a phenol resin, a novolac resin, an acrylic resin, a melamine resin, a urethane resin, an oxazole resin (e.g., polybenzoxazole), or the like. Further, a photocurable resin or the like can be used. Fine particles with a high dielectric constant, such as particles of barium titanate or strontium titanate, can be mixed with these resins as appropriate to adjust the dielectric constant.
Further, the inorganic insulating material used for the binder can be formed using silicon oxide, silicon nitride, silicon containing oxygen and nitrogen, aluminum nitride, aluminum containing oxygen and nitrogen, aluminum oxide, titanium oxide, barium titanate, strontium titanate, lead titanate, potassium niobate, lead niobate, tantalum oxide, barium tantalate, lithium tantalate, yttrium oxide, zirconium oxide, zinc sulfide, or other substances containing an inorganic insulating material. By including an inorganic material with a high dielectric constant in the organic material (by doping or the like), the dielectric constant of the layer containing a light-emitting substance, which includes the light-emitting material and the binder, can be further controlled, and the dielectric constant can be further increased.
Next, as shown in FIG. 11B, a protective film 322 is formed over the second electrode 319. The protective film 322 is to prevent moisture, oxygen, and the like from penetrating the light-emitting element 321. The protective film 322 is preferably formed using silicon nitride, silicon oxide, silicon nitride oxide, silicon oxide nitride, aluminum oxynitride, aluminum oxide, diamond-like carbon (DLC), carbon-containing nitrogen, or another insulating material, by a thin-film formation method such as a plasma CVD method or a sputtering method.
Further, when a sealing substrate 324 is attached to the second interlayer insulating film 315, which is formed over the substrate 100, by using a sealant 323, the light-emitting element 321 is provided in a space 325 which is surrounded by the substrate 100, the sealing substrate 324, and the sealant 323. The space 325 is filled with a filler, which may be an inert gas (such as nitrogen or argon) or the sealant 323.
Next, as shown in FIG. 11C, an FPC 327 is attached to the conductive film 320 which is in contact with the connection terminal 314 using an anisotropic conductive film 326, similarly to the above embodiment mode.
Here, FIG. 13 shows an equivalent circuit diagram of a pixel in the case of full-color display in this embodiment mode. In FIG. 13, a thin film transistor 332 which is surrounded by a dashed line corresponds to the thin film transistor 227 which drives a light-emitting element. A thin film transistor 331 controls the thin film transistor 332 to be turned on or off. Note that an organic EL element (hereinafter referred to as an OLED), in which a layer containing a light-emitting substance is formed using a layer containing a light-emitting organic compound, is used as the light-emitting element.
In a pixel which displays red color, an OLED 334R which emits red light is connected to a drain region of the thin film transistor 332, and a red anode-side power supply line 337R is provided in a source region of the thin film transistor 332. Further, the thin film transistor 331 for switching is connected to a gate wiring 336, and a gate electrode of the thin film transistor 332 for driving is connected to a drain region of the thin film transistor 331 for switching. The drain region of the thin film transistor 332 for switching is connected to a capacitor 338 which is connected to the red anode-side power supply line 337R.
In a pixel which displays green color, an OLED 334G which emits green light is connected to a drain region of the thin film transistor 332 for driving, and a green anode-side power supply line 337G is provided in a source region of the thin film transistor 332 for driving. The thin film transistor 331 for switching is connected to the gate wiring 336, and the gate electrode of the thin film transistor 332 for driving is connected to the drain region of the thin film transistor 331 for switching. Note that the drain region of the thin film transistor 331 for switching is connected to the capacitor 338 which is connected to the green anode-side power supply line 337G.
In a pixel displaying blue color, an OLED 334B which emits blue light is connected to a drain region of the thin film transistor 332 for driving, and a blue anode-side power supply line 337B is provided in a source region of the thin film transistor 332 for driving. The thin film transistor 331 for switching is connected to the gate wiring 336, and the gate electrode of the thin film transistor 332 for driving is connected to the drain region of the thin film transistor 331 for switching. Note that the drain region of the thin film transistor 332 for switching is connected to the capacitor 338 which is connected to the blue anode-side power supply line 337B.
Different voltages are applied to each of the pixels having different colors, depending on the material of the layer containing a light-emitting substance.
Further, for a light-emitting device using a digital video signal, driving methods include one in which video signals input to a pixel are ones with a constant voltage (CV) and one in which video signals input to a pixel are ones with a constant current (CC). Further, concerning the driving method which employs video signals with a constant voltage (CV), there is a system in which voltage of a signal which is applied to a light-emitting element is constant (CVCV), and a system in which current of a signal which is applied to a light-emitting element is constant (CVCC). Further, concerning the driving method which employs video signals with a constant current (CC), there is a system in which voltage of a signal which is applied to a light-emitting element is constant (CCCV), and a system in which current of a signal which is applied to a light emitting element is constant (CCCC).
Through the above steps, a light-emitting device having an active matrix light-emitting element can be manufactured. As to the light-emitting device shown in this embodiment mode, cracks to be in a layer over a substrate or on a substrate can be reduced in a manufacturing process. Therefore, light-emitting devices can be manufactured with high yield.
In this embodiment mode, a manufacturing process of a semiconductor device which is capable of non-contact data transmission will be described with reference to FIGS. 14A to 14E, 15A to 15D, 16A to 16C, and 17A to 17D. In addition, a structure of the semiconductor device will be described with reference to FIG. 18. Further, applications of the semiconductor device shown in this embodiment mode will be described with reference to FIGS. 19A to 19F.
As shown in FIG. 14A, a separation film 402 is formed over a substrate 401. Next, an insulating film 403 is formed over the separation film 402 as in Embodiment Modes 1 and 2, and a thin film transistor 404 is formed over the insulating film 403. Then, an interlayer insulating film 405 is formed to insulate a conductive film included in the thin film transistor 404, and source and drain electrodes 406 which are connected to the semiconductor film of the thin film transistor 404 are formed. After that, an insulating film 407 which covers the thin film transistor 404, the interlayer insulating film 405, and the source and drain electrodes 406 is formed. Then, a conductive film 408 which is connected to the source electrode or the drain electrode 406 with the insulating film 407 interposed therebetween is formed.
As the substrate 401, a substrate similar to the substrate 100 can be used. Further, a metal substrate or a stainless-steel substrate which has an insulating film formed on one surface, a plastic substrate which has heat resistance and can withstand the treatment temperature of this process, a ceramic substrate, or the like can be used. Here, a glass substrate is used as the substrate 401.
The separation film 402 is formed by a sputtering method, a plasma CVD method, a coating method, a printing method, or the like using an element such as tungsten (W), molybdenum (Mo), titanium (Ti), tantalum (Ta), niobium (Nb), nickel (Ni), cobalt (Co), zirconium (Zr), zinc (Zn), ruthenium (Ru), rhodium (Rh), palladium (Pd), osmium (Os), iridium (Ir), or silicon (Si); an alloy material containing the element as its main component; or a compound material containing the element as its main component, and has a single-layer or a stacked-layer structure. The crystal structure of a separation film including silicon that is the separation film 402 may be amorphous, microcrystalline, or polycrystalline.
When the separation film 402 has a single-layer structure, it is preferable to form a layer including tungsten or molybdenum, or a layer including a mixture of tungsten and molybdenum. Alternatively, a layer including an oxide of tungsten or an oxynitride of tungsten, a layer including an oxide of molybdenum or an oxynitride of molybdenum, or a layer including an oxide or an oxynitride of a mixture of tungsten and molybdenum is formed. The mixture of tungsten and molybdenum corresponds to, for example, an alloy of tungsten and molybdenum.
When the separation film 402 has a layered structure, a layer including tungsten or molybdenum or a layer including a mixture of tungsten and molybdenum is preferably formed as a first layer, and a layer including an oxide, a nitride, an oxynitride, or a nitride oxide of tungsten, molybdenum, or a mixture of tungsten and molybdenum is preferably formed as a second layer.
When the separation film 402 is formed as a layered structure including a layer which includes tungsten and a layer which includes an oxide of tungsten, the layer which includes tungsten may be formed and an insulating layer which includes an oxide may be formed thereover so that the layer which includes an oxide of tungsten is formed at the interface of the tungsten layer and the insulating layer. Further, the layer which includes an oxide of tungsten may be formed by processing a surface of the layer which includes tungsten using thermal oxidation treatment, oxygen plasma treatment, N2O plasma treatment, treatment using a solution with strong oxidizing power, such as ozone water, treatment using water to which hydrogen has been added, or the like. This also applies when forming a layer including a nitride of tungsten, a layer including an oxynitride of tungsten, or a layer including a nitride oxide of tungsten. After forming the layer which includes tungsten, a silicon nitride layer, a silicon oxynitride layer, or a silicon nitride oxide layer may be formed over the layer which includes tungsten.
Although the separation film 402 is formed such that it is in contact with the substrate 401 in the above process, the present invention is not limited to this process. An insulating film which serves as a base may be formed such that it is in contact with the substrate 401 and the separation film 402 may be provided such that it is in contact with the insulating film.
The insulating film 403 can be formed in a similar manner to the insulating film 101. Here, the insulating film is formed by generating plasma in the flow of an N2O gas to form a tungsten oxide film on a surface of the separation film 402, and then forming a silicon oxide film containing nitrogen by a plasma CVD method.
The thin film transistor 404 can be formed in a similar manner to the thin film transistors 225 to 227 shown in Embodiment Mode 4. The source and drain electrodes 406 can be formed similarly to the wirings 234 to 239 shown in Embodiment Mode 4.
The interlayer insulating film 405 and the insulating film 407 can be formed by applying and baking polyimide, acrylic, or a siloxane polymer. Alternatively, they may be formed using an inorganic compound by a sputtering method, a plasma CVD method, a coating method, a printing method, or the like as a single layer or a stacked layer. Representative examples of the inorganic compound include silicon oxide, silicon nitride, and silicon oxynitride.
Next, as shown in FIG. 14B, a conductive film 411 is formed over the conductive film 408. Here, a composition including gold particles is printed by a printing method and heated at 200� C. for 30 minutes so that the composition is baked. Thus, the conductive film 411 is formed.
Next, as shown in FIG. 14C, an insulating film 412 which covers the insulating film 407 and end portions of the conductive film 411 is formed. Here, the insulating film 412 which covers the insulating film 407 and end portions of the conductive film 411 is formed using an epoxy resin. An epoxy resin composition is applied by a spin coating method and heated at 160� C. for 30 minutes. Then, a part of the insulating film which covers the conductive film 411 is removed to expose the conductive film 411. Thus, the insulating film 412 having a thickness of 1 μm to 20 μm, preferably 5 μm to 10 μm, is formed. Here, a stacked-layer body including from the insulating film 403 to the insulating film 412 is referred to as an element-forming layer 410.
Next, as shown in FIG. 14D, the insulating films 403, 405, 407, and 412 are irradiated with a laser beam 413 to form opening portions 414 such as those shown in FIG. 14E, in order to facilitate a subsequent separation step. Next, an adhesive member 415 is attached to the insulating film 412. The laser beam used for irradiation to form the opening portions 414 is preferably a laser beam having a wavelength that is absorbed by the insulating films 403, 405, 407, and 412. Typically, a laser beam of an ultraviolet region, a visible region, or an infrared region is selected as appropriate and used for irradiation.
As a laser device capable of emitting such a laser beam, an excimer laser such as an ArF excimer laser, a KrF excimer laser, or a XeCl excimer laser, or a laser device similar to the laser devices 11 a and 11 b shown in Embodiment Mode 1 can be used as appropriate. Note that in the case of using a solid-state laser, preferably any one of the fundamental wave to the fifth harmonic is used, as appropriate. As a result of the laser irradiation, the insulating films 403, 405, 407, and 412 absorb the laser beam and melt, and thus, the opening portions are formed.
As a result of the laser irradiation, the insulating films 403, 405, 407, and 412 absorb the laser beam 413 and melt, and thus, the opening portions are formed. Note that when the process step of irradiating the insulating films 403, 405, 407, and 412 with the laser beam 413 is omitted, throughput can be improved.
Next, as shown in FIG. 15A, a part 421 of the element-forming layer is separated from the substrate 401 having the separation film by a physical means at a metal oxide film formed at the interface of the separation film 402 and the insulating film 403. A �physical means� here refers to a dynamic means or a mechanical means which changes some kind of dynamic energy (or mechanical energy). A typical physical means refers to the application of mechanical power (for example, pulling by a human hand or a gripping tool, or separating while rolling a roller).
In this embodiment mode, a method is used, in which a metal oxide film is formed between a separation film and an insulating film and a physical means is used to separate the element-forming layer 410 at the metal oxide film. However, the present invention is not limited thereto. A method can be used, in which a light-transmitting substrate is used as the substrate and an amorphous silicon layer containing hydrogen is used as the separation film. In such a method, after the step in FIG. 14E, the amorphous silicon film is irradiated with a laser beam from the substrate side to vaporize hydrogen contained in the amorphous silicon film, and separation occurs between the substrate and the separation film.
Further, after the step in FIG. 14E, alternatively, a method of removing the substrate by mechanical polishing, or a method of removing the substrate by using a solution such as HF which dissolves the substrate can be employed. In such a case, it is not necessary to use a separation film.
Further, a method can be used, in which, before attaching the adhesive member 415 to the insulating film 412 in FIG. 14E, a fluoride gas such as NF3, BrF3, or ClF3 is introduced into the opening portions 414 so that the separation film is etched away by the fluoride gas; then, the adhesive member 415 is attached to the insulating film 412; and then, the element-forming layer 410 is separated from the substrate.
Further, a method can be used, in which, before attaching the adhesive member 415 to the insulating film 412 in FIG. 14E, a fluoride gas such as NF3, BrF3, or ClF3 is introduced into the opening portions 414 so that the separation film is partially etched away by the fluoride gas; then, the adhesive member 415 is attached to the insulating film 412; and then, the element-forming layer 410 is separated from the substrate by a physical means.
Next, as shown in FIG. 15B, a flexible substrate 422 is attached to the insulating film 403 in the part 421 of the element-forming layer. Then, the adhesive member 415 is separated from the part 421 of the element-forming layer. Here, a film formed of polyaniline by a cast method is used as the flexible substrate 422.
Then, the flexible substrate 422 is attached to a UV sheet 431 of a dicing frame 432, as shown in FIG. 15C. Since the UV sheet 431 is adhesive, the flexible substrate 422 is fixed on the UV sheet 431. Then, the conductive film 411 may be irradiated with a laser beam to increase adhesiveness between the conductive film 411 and the conductive film 408.
Next, a connection terminal 433 is formed over the conductive film 411, as shown in FIG. 15D. By forming the connection terminal 433, alignment and adhesion with a conductive film which subsequently functions as an antenna can be performed easily.
Next, as shown in FIG. 16A, the part 421 of the element-forming layer is divided into parts. Here, the part 421 of the element-forming layer is divided into plural parts as shown in FIG. 16B, by irradiating the part 421 of the element-forming layer and the flexible substrate 422 with a laser beam 434. As the laser beam 434, any of the laser beams described above which may be used for the laser beam 413 can be used as appropriate. Here, preferably, a laser beam which can be absorbed by the insulating films 403, 405, 407, and 412, and the flexible substrate 422 is selected. Note that although the part of the element-forming layer is divided into plural parts by a laser cutting method here, a dicing method, a scribing method, or the like can be used instead as appropriate. The element-forming layer which has been divided into parts is shown as thin film integrated circuits 442 a and 442 b. Next, as shown in FIG. 16C, the UV sheet of the dicing frame 432 is irradiated with UV light to decrease the adhesiveness of the UV sheet 431. Then, the UV sheet 431 is supported by an expander frame 444. At this time, by supporting the UV sheet 431 with the expander frame 444 while stretching the UV sheet 431, the width of a groove 441 which is formed between the thin film integrated circuits 442 a and 442 b can be increased. Note that preferably, with an expanded groove 446, the size of an antenna substrate which is subsequently attached to the thin film integrated circuits 442 a and 442 b can be obtained.
Next, as shown in FIG. 17A, a flexible substrate 456 having conductive films 452 a and 452 b which function as antennas is attached to the thin film integrated circuits 442 a and 442 b using anisotropic conductive adhesives 455 a and 455 b. Note that the flexible substrate 456 having the conductive films 452 a and 452 b which function as antennas is provided with opening portions so as to partially expose the conductive films 452 a and 452 b. Accordingly, the flexible substrate 456 is attached to the thin film integrated circuits 442 a and 442 b while adjusting their positions such that the conductive films 452 a and 452 b which function as antennas are connected to connection terminals of the thin film integrated circuits 442 a and 442 b by conductive particles 454 a and 454 b which are included in the anisotropic conductive adhesives 455 a and 455 b. Here, the conductive film 452 a which functions as an antenna is connected to the thin film integrated circuit 442 a by the conductive particles 454 a within the anisotropic conductive adhesive 455 a, while the conductive film 452 b which functions as an antenna is connected to the thin film integrated circuit 442 b by the conductive particles 454 b within the anisotropic conductive adhesive 455 b. Then, as shown in FIG. 17B, the flexible substrate 456 and an insulating film 453 are divided into parts in a region where the conductive films 452 a and 452 b which function as antennas and the thin film integrated circuits 442 a and 442 b are not formed. Here, they are divided into parts by a laser cutting method in which the insulating film 453 and the flexible substrate 456 are irradiated with a laser beam 461.
Through the above steps, semiconductor devices 462 a and 462 b which are capable of non-contact data transmission can be manufactured as shown in FIG. 17C.
Note that a semiconductor device 464 such as the one shown in FIG. 17D may be manufactured in such a way that the flexible substrate 456 having the conductive films 452 a and 452 b which function as antennas is attached to the thin film integrated circuits 442 a and 442 b using the anisotropic conductive adhesives 455 a and 455 b in FIG. 17A; then, a flexible substrate 463 is provided so as to seal the flexible substrate 456 and the thin film integrated circuits 442 a and 442 b; and the region where the conductive films 452 a and 452 b which function as antennas and the thin film integrated circuits 442 a and 442 b are not formed is irradiated with the laser beam 461, as shown in FIG. 17B. In this case, the thin film integrated circuits are sealed by the flexible substrates 456 and 463 which have been divided into parts. Therefore, deterioration of the thin film integrated circuits can be suppressed.
Through the above steps, a thin and lightweight semiconductor device can be manufactured with high yield. As to the semiconductor device shown in this embodiment mode, cracks to be in a layer over a substrate or on a substrate can be reduced in a manufacturing process. Therefore, semiconductor devices can be manufactured with high yield.
Next, a structure of the above-mentioned semiconductor device which is capable of non-contact data transmission will be described with reference to FIG. 18.
The power supply portion 2002 includes a rectifier circuit 2021 which produces power based on a signal received from the outside through the antenna 2011, a storage capacitor 2022 for storing the produced power and a constant voltage circuit 2023 for generating a constant voltage to be supplied to each circuit.
The logic portion 2003 includes a demodulation circuit 2031 which demodulates a received signal, a clock generating/compensating circuit 2032 which generates a clock signal, a code recognition and determination circuit 2033, a memory controller 2034 which produces a signal for reading data from a memory based on a received signal, a modulation circuit 2035 for modulating an encoded signal to be transmitted, an encoder circuit 2037 which encodes the read data, and a mask ROM 2038 which stores data. Further, the modulation circuit 2035 has a resistor 2036 for modulation.
A code recognized and determined by the code recognition and determination circuit 2033 is a frame termination signal (EOF, End of Frame), a frame starting signal (SOF, Start of Frame), a flag, a command code, a mask length, a mask value, or the like. The code recognition and determination circuit 2033 also has a periodic redundancy check (CRC) function for detecting transmission errors.
Next, applications of the above-described semiconductor device which is capable of non-contact data transmission will be described with reference to FIGS. 19A to 19F. The above-described semiconductor device which is capable of non-contact data transmission has a wide range of applications, such as bills, coins, securities, bearer bonds, documents (e.g., driver's licenses or resident's cards; refer to FIG. 19A), packaging containers (e.g., wrapping paper or bottles; refer to FIG. 19C), storage media (e.g., DVD software or video tapes; refer to FIG. 19B), means of transportation (e.g., bicycles; refer to FIG. 19D), personal belongings (e.g., shoes or glasses), food, plants, animals, human bodies, clothing, daily commodities, or tags on goods such as electronic devices or on bags (refer to FIGS. 19E and 19F). An electronic appliance is, for example, a liquid crystal display device, an EL display device, a television device (also referred to as simply a television, or as a TV receiver or a television receiver), a portable telephone, or the like.
Examples of electronic devices having a semiconductor device described in the above embodiment modes include television devices (also referred to as simply televisions, or as television receivers), cameras such as digital cameras or digital video cameras, portable telephone devices (also referred to as simply portable telephones, or mobile phones), portable information terminals such as PDAs, portable game machines, monitors for computers, computers, sound reproducing devices such as car audio devices, image reproducing devices equipped with a recording medium, such as home-use game machines, or the like. Specific examples of these are described with reference to FIGS. 20A to 20F.
A portable information terminal shown in FIG. 20A includes a main body 9201, a display portion 9202, and the like. By employing the semiconductor device shown in the above embodiment modes in the display portion 9202, a portable information terminal capable of high-definition display can be provided at a low price.
A digital video camera shown in FIG. 20B includes a display portion 9701, a display portion 9702, and the like. By employing the semiconductor device described in the above embodiment modes in the display portion 9701, a digital video camera capable of high-definition display can be provided at a low price.
A portable terminal shown in FIG. 20C includes a main body 9101, a display portion 9102, and the like. By employing the semiconductor device shown in the above embodiment modes in the display portion 9102, a portable terminal with high reliability can be provided at a low price.
A portable television device shown in FIG. 20D includes a main body 9301, a display portion 9302, and the like. By employing the semiconductor device shown in the above embodiment modes in the display portion 9302, a portable television device capable of high-definition display can be provided at a low price. Such a television device can be applied to a wide range of television devices, from small-sized devices that are mounted on portable terminals such as portable phones to medium-sized devices that are portable and large-sized devices (for example, 40 inches or more).
A portable computer shown in FIG. 20E includes a main body 9401, a display portion 9402, and the like. By employing the semiconductor device shown in the above embodiment modes in the display portion 9402, a portable computer capable of high-definition display can be provided at a low price.
A television device shown in FIG. 20F includes a main body 9501, a display portion 9502, and the like. By employing the semiconductor device shown in the above embodiment modes in the display portion 9502, a television device capable of high-definition display can be provided at a low price.
A structure of the television device will now be described with reference to FIG. 21.
FIG. 21 is a block diagram showing the main structure of the television device. A tuner 9511 receives a video signal and an audio signal. The video signal is processed through a video detection circuit 9512, a video signal processing circuit 9513 which converts the signal output from the video detection circuit 9512 into a color signal corresponding to red, green, or blue, and a control circuit 9514 for converting the video signal in accordance with input specifications of a driver IC. The control circuit 9514 outputs signals to a scanning line driver circuit 9516 and a signal line driver circuit 9517 of a display panel 9515. In the case where digital driving is used, a signal dividing circuit 9518 may be provided on a signal line side so that the input digital signal is divided into m number of signals to be supplied. The scanning line driver circuit 9516 and the signal line driver circuit 9517 are circuits for driving a pixel portion 9519.
Of the signals received by the tuner 9511, the audio signal is sent to an audio detection circuit 9521 and its output is supplied to a speaker 9523 through an audio signal processing circuit 9522. A control circuit 9524 receives control information on a receiving station (a receiving frequency), sound volume, and the like from an input portion 9525, and sends signals to the tuner 9511 and the audio signal processing circuit 9522.
Next, a portable phone appliance is described as a mode of an electronic appliance to which the semiconductor device of the present invention is mounted, with reference to FIG. 22. The portable phone appliance includes cases 2700 and 2706, a display panel 2701, a housing 2702, a printed wiring board 2703, operation buttons 2704, and a battery 2705 (refer to FIG. 22). The display panel 2701 is detachably incorporated into the housing 2702, and the housing 2702 is fitted to the printed wiring board 2703. The shape and size of the housing 2702 are changed as appropriate in accordance with the electronic appliance into which the display panel 2701 is incorporated. A plurality of semiconductor devices that are packaged are mounted on the printed wiring board 2703. The semiconductor device of the present invention can be used as one of them. The plurality of semiconductor devices mounted on the printed wiring board 2703 have functions such as the function of a controller, a central processing unit (CPU), a memory, a power supply circuit, an audio processing circuit, a sending/receiving circuit, and the like.
In the display panel 2701, a pixel portion and one or more peripheral driver circuits (in a plurality of driver circuits, the driver circuits which have a low operating frequency) may be formed over one substrate using TFTs, whereas some other peripheral driver circuits (in a plurality of driver circuits, the driver circuits which have a high operating frequency) may be formed over an IC chip. The IC chip may be mounted on the display panel 2709 using a COG (chip on glass) method, or the IC chip may be connected to a glass substrate by using a TAB (tape automated bonding) method or a printed board. Note that FIG. 23A shows an example of a structure of a display panel in which a pixel portion and one or more peripheral driver circuits are formed over one substrate and IC chips including some other peripheral driver circuits are mounted by a COG method or the like. The display panel shown in FIG. 23A includes a substrate 3900, a signal line driver circuit 3901, a pixel portion 3902, a scanning line driver circuit 3903, a scanning line driver circuit 3904, an FPC 3905, an IC chip 3906, an IC chip 3907, a sealing substrate 3908, and a sealant 3909. By employing such a structure, the power consumption of a display device can be reduced, and a portable phone appliance can be used for a longer period per charge. Further, the cost of a portable phone appliance can be reduced.
In order to further reduce power consumption, a pixel portion may be formed over a substrate using TFTs and all the peripheral driving circuits may be formed over an IC chip, and then the IC chip may be mounted on a display panel using a COG (chip on glass) method, or the like, as shown in FIG. 23B. A display panel shown in FIG. 23B includes a substrate 3910, a signal line driver circuit 3911, a pixel portion 3912, a scanning line driver circuit 3913, a scanning line driver circuit 3914, an FPC 3915, an IC chip 3916, an IC chip 3917, a sealing substrate 3918, and a sealant 3919.
As described above, the semiconductor device of the present invention is compact, thin, and lightweight. With these features, the limited space within the cases 2700 and 2706 of the electronic appliance can be used efficiently. Further, cost reduction is possible, and an electronic appliance having a semiconductor device with high reliability can be manufactured.
This application is based on Japanese Patent Application serial no. 2006-236018 filed in Japan Patent Office on Aug. 31, 2006, the entire contents of which are hereby incorporated by reference.
Patent CitationsCited PatentFiling datePublication dateApplicantTitleUS5313076Mar 17, 1992May 17, 1994Semiconductor Energy Laboratory Co., Ltd.Thin film transistor and semiconductor device including a laser crystallized semiconductorUS5643826Oct 25, 1994Jul 1, 1997Semiconductor Energy Laboratory Co., Ltd.Disposing crystallization promoting solution containing specified element in contact with amorphous silicon film on substrate, crystallizing by heatingUS5670793Sep 14, 1995Sep 23, 1997Hitachi, Ltd.Depositing pure silicon, then impurity layer at interface; heat treatmentUS5753542Mar 1, 1995May 19, 1998Semiconductor Energy Laboratory Co., Ltd.Method for crystallizing semiconductor material without exposing it to airUS5899547Nov 4, 1997May 4, 1999Semiconductor Energy Laboratory Co., Ltd.Liquid crystal displayUS5962869Jan 21, 1994Oct 5, 1999Semiconductor Energy Laboratory Co., Ltd.Semiconductor material and method for forming the same and thin film transistorUS6172380Nov 6, 1998Jan 9, 2001Sony CorporationSemiconductor materialUS6358766Jun 21, 2000Mar 19, 2002Semiconductor Energy Laboratory Co., Ltd.Method of fabricating a semiconductor deviceUS6423586Mar 9, 1998Jul 23, 2002Semiconductor Energy Laboratory Co., Ltd.Melting a noncrystal semiconductor film containing silicon, oxygen, nitrogen and carbon by irradiating with a laser beam to crystallize; specified raman shift; thin film transistorsUS6535535Feb 8, 2000Mar 18, 2003Semiconductor Energy Laboratory Co., Ltd.Laser irradiation method, laser irradiation apparatus, and semiconductor deviceUS6545320Jun 5, 2002Apr 8, 2003Semiconductor Energy Laboratory Co., Ltd.Electro-optical device and semiconductor deviceUS6787807Jun 18, 2001Sep 7, 2004Semiconductor Energy Laboratory Co., Ltd.Semiconductor deviceUS6808969Oct 25, 2002Oct 26, 2004Semiconductor Energy Laboratory Co., Ltd.Laser irradiation method and laser irradiation apparatus, and method for fabricating semiconductor deviceUS6881615Oct 18, 2001Apr 19, 2005Semiconductor Energy Laboratory Co., Ltd.Method for crystallizing semiconductor material without exposing it to airUS6908797Jul 8, 2003Jun 21, 2005Semiconductor Energy Laboratory Co., Ltd.Method of manufacturing a semiconductor deviceUS7112517Sep 9, 2002Sep 26, 2006Semiconductor Energy Laboratory Co., Ltd.Laser treatment device, laser treatment method, and semiconductor device fabrication methodUS7113527Dec 20, 2002Sep 26, 2006Semiconductor Energy Laboratory Co., Ltd.Method and apparatus for laser irradiation and manufacturing method of semiconductor deviceUS7125761Feb 27, 2004Oct 24, 2006Semiconductor Energy Laboratory Co., Ltd.Laser irradiation apparatus, laser irradiation method, and method for manufacturing semiconductor deviceUS7220627Apr 9, 2004May 22, 2007Semiconductor Energy Laboratory Co., Ltd.Method for manufacturing a semiconductor device where the scanning direction changes between regions during crystallization and processUS7384810 *May 26, 2006Jun 10, 2008Hitachi Displays, Ltd.Image display device and method for manufacturing the sameUS7397831 *Nov 15, 2004Jul 8, 2008Hitachi Displays, Ltd.Laser annealing apparatus and annealing method of semiconductor thin film using the sameUS20030085720Oct 25, 2002May 8, 2003Semiconductor Energy Laboratory Co., Ltd.Laser irradiation method and laser irradiation apparatus, and method for fabricating semiconductor deviceUS20030100169Sep 9, 2002May 29, 2003Koichiro TanakaLaser treatment device, laser treatment method, and semiconductor device fabrication methodUS20040069751Oct 6, 2003Apr 15, 2004Shunpei YamazakiIrradiating second harmonic of CW laser and a fundamental wave of CW laser at the same time to the same portion to improve annealing efficiencyUS20040119955Nov 26, 2003Jun 24, 2004Semiconductor Energy Laboratory Co. Ltd.Laser irradiation apparatus, laser irradiation method, and method for manufacturing a semiconductor deviceUS20040136416Dec 20, 2002Jul 15, 2004Koichiro TanakaMethod and apparatus for laser irradiation and manufacturing method of semiconductor deviceUS20040169023Feb 27, 2004Sep 2, 2004Semiconductor Energy Laboratory Co., Ltd.Laser irradiation apparatus, laser irradiation method, and method for manufacturing semiconductor deviceUS20040195222Dec 24, 2003Oct 7, 2004Semiconductor Energy Laboratory Co., Ltd.Laser irradiation method, laser irradiation apparatus, and method for manufacturing semiconductor deviceUS20040209410Apr 20, 2004Oct 21, 2004Semiconductor Energy Laboratory Co., Ltd.Beam irradiation apparatus, beam irradiation method, and method for manufacturing thin film transistorUS20040253838Mar 15, 2004Dec 16, 2004Semiconductor Energy Laboratory Co., Ltd.Laser irradiation apparatus, laser irradiation method, and method for manufacturing a semiconductor deviceUS20050003591 *May 28, 2004Jan 6, 2005Nec CorporationMethod of and apparatus for manufacturing semiconductor thin film, and method of manufacturing thin film transistorUS20050036190Apr 20, 2004Feb 17, 2005Semiconductor Energy Laboratory Co., Ltd.Beam irradiation apparatus, beam irradiation method, and method for manufacturing a thin film transistorUS20050037552Apr 9, 2004Feb 17, 2005Semiconductor Energy Laboratory Co., Ltd.Beam irradiation apparatus, beam irradiation method, and method for manufacturing semiconductor deviceUS20050037553Aug 5, 2004Feb 17, 2005Semiconductor Energy Laboratory Co., Ltd.Laser irradiation method, method for manufacturing a semiconductor device, and a semiconductor deviceUS20050115930Nov 29, 2004Jun 2, 2005Semiconductor Energy Laboratory Co., Ltd.Laser irradiation apparatus, laser irradiation method and method for manufacturing semiconductor deviceUS20050139786Dec 22, 2004Jun 30, 2005Semiconductor Energy Laboratory Co., Ltd.Laser irradiation method and method for manufacturing crystalline semiconductor filmUS20060003478 *Aug 24, 2005Jan 5, 2006Mikio HongoMethod of manufacturing display deviceUS20070087488Oct 12, 2006Apr 19, 2007Semiconductor Energy Laboratory Co., Ltd.Semiconductor device and manufacturing method thereofEP0651431A2Oct 31, 1994May 3, 1995Semiconductor Energy Laboratory Co., Ltd.Method of crystallizing a silicone layer and semiconductor devices obtained by using the methodJP2004179195A Title not availableJP2004327677A Title not availableJP2005191546A Title not availableJPH05299339A Title not availableJPH07135174A Title not availableJPH11145056A Title not available* Cited by examinerNon-Patent CitationsReference1Ohashi et al., TFTp5-4: "Crystalline Orientation of Large-Grain Poly-Si Thin Films Observed by Raman Spectroscopy", AM-LCD '04: International Workshop Active-Matrix Liquid-Crystal Displays, Issued Aug. 25, 2004, pp. 269-272.2Sotani et al., "Crystallization of Amorphous Si Films Using Indirect Heating by High Power CW-YAG Laser-Zone Melting for Film (III)", Extended Abstracts from the 50th Meeting of the Japan Society of Applied Physics and Related Societies, Issued Mar. 27, 2003, No. 2, pp. 925. (Full Translation).Referenced byCiting PatentFiling datePublication dateApplicantTitleUS8212254Aug 29, 2007Jul 3, 2012Semiconductor Energy Laboratory Co., Ltd.Thin film transistor, manufacturing method thereof, and semiconductor deviceUS8338278Nov 27, 2007Dec 25, 2012Semiconductor Energy Laboratory Co., Ltd.Method of manufacturing semiconductor device with crystallized semiconductor filmUS8349714Jan 10, 2008Jan 8, 2013Semiconductor Energy Laboratory Co., Ltd.Method of crystallizing semiconductor film and method of manufacturing semiconductor deviceUS8421080Oct 17, 2011Apr 16, 2013Panasonic CorporationThin-film transistor array device, organic EL display device, and method of manufacturing thin-film transistor array deviceUS8679907 *Apr 4, 2012Mar 25, 2014Panasonic CorporationThin-film transistor array manufacturing method, thin-film transistor array, and display deviceUS20130049004 *Apr 4, 2012Feb 28, 2013Panasonic CorporationThin-film transistor array manufacturing method, thin-film transistor array, and display device* Cited by examinerClassifications U.S. Classification438/487, 438/486, 438/166International ClassificationH01L21/20Cooperative ClassificationH01L21/02691, H01L29/4908, H01L21/02683, H01L21/02686, H01L21/02532, H01L27/1285European ClassificationH01L21/02K4C1A3, H01L21/02K4T8C8, H01L21/02K4T8C5P, H01L21/02K4T8C5CLegal EventsDateCodeEventDescriptionMar 14, 2013FPAYFee paymentYear of fee payment: 4Oct 10, 2007ASAssignmentOwner name: SEMICONDUCTOR ENERGY LABORATORY CO., LTD., JAPANFree format text: ASSIGNMENT OF ASSIGNORS INTEREST;ASSIGNORS:MORIWAKA, TOMOAKI;TANAKA, KOICHIRO;REEL/FRAME:019941/0676Effective date: 20071004Owner name: SEMICONDUCTOR ENERGY LABORATORY CO., LTD.,JAPANFree format text: ASSIGNMENT OF ASSIGNORS INTEREST;ASSIGNORS:MORIWAKA, TOMOAKI;TANAKA, KOICHIRO;US-ASSIGNMENT DATABASE UPDATED:20100216;REEL/FRAME:19941/676RotateOriginal ImageGoogle Home - Sitemap - USPTO Bulk Downloads - Privacy Policy - Terms of Service - About Google Patents - Send FeedbackData provided by IFI CLAIMS Patent Services