Method for fabricating single crystal silicon film

The present invention relates to a method for fabricating a single crystal silicon thin film at the desired location to the desired size from an amorphous or polycrystalline thin film on a substrate using laser irradiation and laser beam movement along the substrate having the semiconductor thin films being irradiated. This method comprises the steps of: forming a semiconductor layer or a metal thin film on a transparent or semi-transparent substrate; forming a single crystal seed region on the substrate of the desired size by a crystallization method using laser irradiation; and converting the desired region of the semiconductor layer or metal thin film into a single crystal region, using the single crystal seed region.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to a method for fabricating a semiconductor thin film, and more particularly to a method for fabricating a single crystal silicon thin film at the desired location to the desired size from an amorphous or polycrystalline thin film on a substrate using laser irradiation and laser beam movement along the substrate having the semiconductor thin films being irradiated.

2. Description of the Prior Art

Generally, a thin film transistor (hereinafter, referred to as TFT), a core switching device, which is used in LCD or OLED using organic EL material, is the most important semiconductor device for the performance of a flat panel display (hereinafter, referred to as FPD).

Mobility or leakage current, a measure of the TFT performance, greatly varies depending on the state or structure of a silicon (Si) thin film, which forms an active layer, a channel for charge carrier transport. In the case of a currently commercially available LCD, the active layer of most TFTs is made of an amorphous silicon (a-Si) thin film.

Since a-Si TFT using a-Si has a very low mobility of about 0.5 cm2/Vs, there is a limitation in making all switching devices required in LCD, using a-Si TFT. This is because a switching device for a peripheral circuit of LCD needs to be operated at a very high speed, but this high speed cannot be achieved with a-Si TFT.

Thus, switching parts for the peripheral circuit, such as a driver circuit, various controllers, and a digital-analogue-converter (DAC), etc., are formed of switching devices integrated on single crystal Si to cope with a high-speed requirement for the LCD driving. On the other hand, since a-Si TFT has a switching function while showing a characteristic of low-leakage current required for ensuring image quality, it is used as a pixel-switching device.

TFT using poly-crystal Si has a high mobility of several tens to several hundreds cm2/Vs and thus can exhibit high driving speed suitable for the periphery circuit. Thus, formation of poly-Si on a glass substrate allows a pixel region and also a peripheral circuit region to be realized.

Accordingly, in the case of poly-Si TFT, separate part mounting processes required for the formation of the peripheral circuit are not required and the peripheral circuit can be formed simultaneously with a pixel region, so that a reduction in part costs for the peripheral circuit can be expected.

In addition, because of high mobility, poly-Si allows TFT to be produced at a smaller size than existing a-Si and enables the peripheral circuit and the pixel region to be formed by an integration process. Thus, making linewidth fine becomes easier so that poly-Si TFT can realize high resolution as compared to a-Si TFT-LCD.

Furthermore, poly-Si TFT can show a high-current characteristic and thus is suitable for use in OLED, a current drive type display of the next generation FDP. Thus, studies to form poly-Si and fabricate TFT on a glass substrate are actively conducted at the most recent.

In order to form poly-Si on a glass substrate, a method is typically used, in which a-Si is deposited and then crystallized into poly-Si by thermal treatment. Since the glass substrate is deformed at a higher temperature than 600° C., excimer laser annealing (hereinafter, referred to as ELA) which crystallize only a-Si without causing damage to the substrate is typically used for crystallization. Generally, upon crystallization using ELA, a-Si is irradiated with a laser so that it is melted and re-solidified to produce poly-Si. Upon crystallization, grains are randomly formed such that they have various sizes ranging from several tens nm to a few μm depending on laser irradiation conditions.

Generally, as the size of grains is increased, the mobility of a TFT device is increased and the range of parts, which can be integrated upon the integration of the peripheral circuit, becomes wider. Thus, it is preferred to obtain ELA conditions where the greatest possible size of grains can be obtained, but the greater the size of grains, the worse the uniformity of grain distribution. This causes a degradation in uniformity of device characteristics, and as a result, causes a problem in view of reliability.

Accordingly, in applying ELA-crystallized poly-Si in LCD, there is applied poly-Si having grains of a suitable size in a range where uniformity is ensured. In this case, however, poly-Si TFT having high mobility can not be fabricated due to a limitation on grain size, and thus, there is necessarily a limitation in integrating the peripheral circuit.

U.S. Pat. Nos. 6,368,945 and 6,322,625 disclose a crystallization method where large sizes of grains are obtained while ensuring uniformity. The principle of this method which is called “sequential lateral solidification” (SLS) will now be described.

FIG. 1is a schematic view of a laser system for carrying out a SLS process. As shown inFIG. 1, a substrate110deposited with an a-Si film120is placed on a stage100and first irradiated with a laser beam130through a mask140. In this case, there can be various patterns in the mask140.

A typical example of this mask is a slit-shaped mask200as shown inFIG. 2a. In the mask200, slits210having a width220and a length230are patterned. As laser beam is irradiated through the mask, the laser beam passed through the mask is irradiated in a beamlet form, and the irradiated laser beam has such energy that a-Si can be completely melted.

FIG. 3ais an enlarged view of one slit. InFIG. 3ashowing a condition before laser irradiation, the reference numeral310represents the width of a region exposed through a slit330, and a-Si320is present before exposure to laser irradiation.FIG. 3bshows a condition immediately after laser was irradiated through a slit (condition where laser was irradiated for several tens nanoseconds and then cut-off). In this case, an exposed region was melted into a liquid silicon360, the boundary between the liquid silicon360and the a-Si silicon340is formed at the edge of the slit, and a fine poly-Si350is formed at the boundary. With the passage of time, the growth of grains is progressed toward the slit center, using the poly-Si350as a seed. In a growth process of grains, the growth of grains having slow growth rate is inhibited by grains having fast growth rate so that only some grains are continued to grow. The interface380between poly-Si and liquid Si-is continued to move, and ultimately, the poly-Si and the liquid Si meet with each other at the slit center as shown inFIG. 3d. In this case, the grown grain size320is approximately a half of the slit width. If the slit width is larger or the supercooling rate of the melted silicon after laser irradiation is fast, nucleation can occur within the liquid silicon361before the grains grown from both edges of the slit meet with each other at the boundary381.

Since this circumstance is undesired, it is important that the laser irradiation conditions, the substrate temperature and the form of a slit are optimized so that the nucleation does not occur.

After the first laser irradiation was completed, a location for laser beam irradiation is shifted by a length of450as shown inFIG. 4a, and then, second laser irradiation is conducted through a slit. After the second laser irradiation, silicon between slit boundaries420,421is converted into a liquid silicon460, and a poly-Si region440which was formed after the first irradiation remains intact and is re-crystallized. In this case, at the boundary421, a fine poly-Si region is formed, and then the growth of grains is progressed using the formed poly-Si as a seed, but at the boundary420, the growth of grains is progressed using a region excluding the grains melted after the second irradiation among the grains formed after the first irradiation. as a seed. As a result, a structure as shown inFIG. 4cis obtained. In other words, a boundary470which is formed by progressing the grain growth from both sides of the slit after the second irradiation is moved by a distance491which was shifted from the original location for the second irradiation.

By this procedure, the grain size becomes larger due to an increase in grain length in the scanning direction. Furthermore, upon the second irradiation, since the seed crystal and a new crystal undergo continuous growth in a state where crystal orientation is not changed, a boundary480disappears.

FIG. 5ashows a condition after the laser beam was moved in any length while the above procedure was repeated. The lower portion ofFIG. 5ashows a procedure where grains, which have been continued to grow in one direction, are present as an elongated form, and growing interfaces520,521of grains, which have been grown from slit boundaries510,511(,FIG. 5A) after exposure to a slit at a front stage of growth, are grown into a liquid silicon530.

Then, the scanning procedure is progressed to a point551, and an a-Si region550is crystallized, thereby giving a structure as shown inFIG. 5b. The scanned distance is approximately equal to the reference numeral580, and the length of the grown grains corresponds to the scanned distance580. Since the slit is patterned according to the mask, movement of the laser beam by a given scanned distance results in formation of poly-Si patterns as shown inFIGS. 2band2c. The respective poly-Si patterns have a grain structure as shown inFIG. 5b. As shown inFIG. 5b, at the initial region where scanning was initiated, there is a region having many fine grains, i.e., a region shown by the reference numeral560, since many grains competitively grow. Above the region560, there is a region having elongated grains, i.e., a region shown by the reference numeral570. The results of actual experiments indicate that the region560is smaller than 1 μm that is negligibly small in a patterned region of poly-Si (“Sequential lateral solidification of thin silicon films on SiO2”, R.S. Sposil and James S. Im, Appl. Phys. Lett., 69(19), 2864(1996)).

The SLS method is advantageous in that various shapes are obtained according to the shape of a mask, and for some masks, a single crystal Si island region can be selectively formed at a portion where a channel region of TFT is formed (U.S. Pat. No. 6,322,625).

Thus, the use of this method allows a poly-Si structure, the uniformity of device characteristics, and improvement in device performance to be obtained.

However, in a Si thin film obtained by SLS, if a regularity in the formation of a single crystal Si array having rectangular or hexagonal arrangement, and a single crystal Si island, does not coincide with the design of pixel and peripheral circuit arrangements, the uniformity of device characteristics is adversely affected.

Thus, in the existing SLS method, there can be a limitation in view of a design since a mask design for crystallization must match with pixel and peripheral circuit designs.

Furthermore, a method of making a single crystal among the SLS methods is to form a single crystal Si island in the strict sense and thus grain boundaries are present in several places of a substrate. Thus, if the pixel or the peripheral circuit is configured around the grain boundaries, excellent device characteristics and uniformity can be expected.

As a result, an ultimate solution to ensure excellent device characteristics and uniformity in any design scheme will be a method wherein single crystal silicon is formed over the entire substrate, or single crystal Si is grown only on a peripheral circuit portion and the remaining pixel region is kept at the state of a-Si so that single crystal Si having an excellent switching property for the peripheral circuit is formed outside the pixel region having low leakage current, thereby fundamentally preventing formation of the grain boundaries capable of causing non-uniformity.

For this purpose, according to the present invention, a method in which single crystal Si is easily formed at the desired location to the desired size using a simpler mask is proposed.

SUMMARY OF THE INVENTION

Accordingly, an object of the present invention is to provide a method for fabricating a single crystal silicon film, by which the crystallinity of low temperature poly-silicon silicon as an active layer of a thin film transistor, a pixel or peripheral circuit-driving device applied in LCD or OLED, can be increased, thereby forming single crystal silicon.

To achieve the above-mentioned object, the present invention provides a method for fabricating a single crystal silicon film, which comprises forming a single crystal region through a laser irradiation after forming a semiconductor layer or a metal thin film on a transparent or semi-transparent substrate, which comprises the steps of: forming a single crystal seed region on the substrate of the desired size by a crystallization method using laser irradiation; and converting the desired region of the semiconductor layer or metal thin film into a single crystal region, using the single crystal seed region.

Furthermore, the method of the present invention comprises the step of: irradiating the substrate of the desired size with a laser in a specific shape through a mask so that the laser-irradiated portion is firstly crystallized; conducting a first scanning process which comprises moving the laser by the desired distance so that a grain in the firstly crystallized portion is grown by the desired distance; completing the first scanning process after it was progressed by the desired distance, thereby forming a poly-crystal island region; conducting a second scanning process which comprises 90° turning the laser at the end of the first scanning process and scanning the seed grain formed in an elongated shape in the scanning direction during the first scanning process, so that the seed grain is grown to form a single crystal region; and irradiating the laser onto a portion of a single crystal seed region formed after progressing the second scanning process by the desired distance, thereby extending the single crystal region.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

Hereinafter, a method for fabricating a single crystal silicon film according to the present invention will be described in detail with reference to the accompanying drawings.

In order to enhance crystallinity and also to ensure uniformity in forming a polycrystalline silicon (poly-Si) thin film on an amorphous substrate such as a glass or plastic insulator, a single crystal or a single-crystal tile whose location was precisely controlled is formed over the entire substrate according to the present invention. This allows problems of the prior art to be fundamentally solved. A typical method for this purpose is designed in the present invention, and the crystallization of a-Si will be described herein by way of example.

In a principle to realize the present invention, a poly-Si island pattern, which undergone the prior SLS process, is subjected to an additional laser scanning process in a perpendicular direction to a direction in which grains of the island pattern were grown. This results in formation of a single crystal Si seed region. Then, according to a SLS process using this seed region, a single crystal Si region or a single crystal Si tile is formed over the entire substrate or formed on a certain region of the substrate, such as a region where a panel is formed, or a peripheral circuit region, in order to shorten process time.

FIG. 6shows the arrangement of a poly-Si island610having a width660and a length670completed inFIG. 5band a laser beam630having a length640and a width650for use in the second scanning. The laser beam630is moved in the x-direction perpendicular to the first scanning direction, starting from one edge of the poly-Si island pattern610.

It is preferred that the laser beam length640for the second scanning is approximately equal to the length670of the poly-Si island pattern610. After the first scanning but before the second scanning, a mask is turned by 90° or the sample is turned by 90°.

FIGS. 7a,7band7cconcretely show the second scanning process. For SLS, the laser beam width650is generally a few μm, and the width of an elongated grain in the poly-Si island pattern610is in the range of 1 to several μm.FIG. 7aschematically shows a state where grains are present in one edge of the poly-Si island pattern. A grain710is formed in an elongated shape in the first scanning process, and a grain711is not grown in the initial growth process.

As described above, the grain711has a very small size of about 1 μm. Since the accuracy of aligning of a laser beam in a SLS system is about sub-μmw, the laser beam can be aligned such that it melts only a portion of the grain710as shown inFIG. 7b. Of course, parts or all of the grain730can be melted. And more important, the size (length and width) of the grain, which was grown in an elongated form over the entire poly-Si island pattern, is similar to the dimension level of the laser beam.

Thus, the region730is liquefied after the first irradiation in the second scanning process, and the liquefied region is re-solidified. At this time, the grain710and the grain731, which have very small sizes, serve as seeds, and the grain710forms most of the seeds. Thus, when the second scanning is progressed toward a poly-Si region740, the poly-Si region740inFIG. 7bis converted into a single crystal Si region as shown inFIG. 7cvia melting and solidification processes. When the grain731is partially melted upon the first irradiation in the second scanning, it can be grown in the scanning process, but its size is very small and its growth rate is slower than the grain710as found in the scanning process, and thus, the size of a newly grown region751is negligible. The boundary760between a portion melted upon the first irradiation of the second scanning and the remaining portion will disappear. This is because the seed region710and the crystallized region750have the same orientation.

There can be caused the worst where the aligning of the laser beam is inaccurate or pluralities of elongated grains are present in the seed region. If small grains formed at a lower portion in the first scanning process (e.g., grain731) are ignored, seed crystals will be two crystals having similar growth rates.

FIGS. 8aand8bshow the second scanning process under this condition. As two initial seed crystals820,821are scanned with a laser beam830while removing a poly-Si region810, a grain boundary800remaining before scanning extends while the poly-Si island pattern consists of two grains.

In this case, the growth of a grain870is superior to the growth of a grain871so that a region of the grain870is larger than the grain871. Even in this case, such grains sufficiently act as a single crystal seed layer for converting the remaining substrate region or certain region into a single crystal region. This is because the size of the respective grain regions850,851,880,881is about several tens μm sufficiently larger than the width of a laser beam passed through a slit, and thus, a grain suitably chosen from such grains may be applied as a seed crystal for the subsequent crystallization.

FIGS. 11ato11dshow a method of forming a single crystal Si region over the entire substrate in the above-mentioned manner.

FIG. 11ashows that a laser beam1130is irradiated starting from one edge of a poly-Si island1120formed upon the first scanning, and the second scanning is progressed to one edge of a substrate1110in the scanning direction shown in the figure.

As a laser beam1160reaches the opposite edge of the substrate1110after the second scanning, a single crystal Si seed region1150of a rectangular shape is formed and the remaining region remains at a-Si.

Following this, the laser beam is irradiated onto a portion of the single crystal Si seed region1150as shown inFIG. 11C, thereby repeating melting and solidification. The laser irradiation is conducted in the order of1170,1171, . . .1180, in a direction shown by the reference numeral1190. In this way, a single crystal Si region is formed over the entire substrate as shown inFIG. 11d.

The respective irradiation steps1170,1171inFIG. 11cmay be conducted on several places at the same time such that process time can be shortened. For example, the irradiation steps1170and1172are conducted at the same time, and then, the irradiation steps1171and1173are conducted at the same time.

This method has the following differences from a “2 shot SLS process” (U.S. Pat. No. 6,368,945), which was recently proposed by James Im et al. In the present invention, a single crystal Si region is formed by the first scanning in the x-direction and the second scanning in the y-direction. Particularly in the case of the second scanning, since seed crystals are of small number (about one or two), the second scanning from crystals of small number allows single crystal seed regions to be formed. Once such seed regions are formed, crystallization is conducted in the same manner as the “2 shot SLS process” proposed by James Im et al. As a result, in the “2 shot SLS process”, a structure where poly-Si regions are arranged as shown inFIG. 3is obtained, but in the present invention, a single crystal Si region is formed. Namely, in the present invention, a process of forming the single crystal Si region at an initial stage is added so that the microstructure of a final thin film is greatly changed. In the present invention, additional processes (first and second scanning processes) are required to form the single crystal regions, but the present invention is advantageous in that the resulting structure provides very high uniformity and degree of freedom of design as compared to the “2 shot SLS process” The additional processes can be partially improved as in other embodiments of the present invention which will be described later.

At the end of crystallization, as shown inFIG. 9d, a single crystal region961and a poly-Si region960are met with each other at a boundary962. Thus, the size of the single crystal region is increased by a distance931moved in the reverse y-direction, thereby extending the single crystal region. In this case, the laser irradiation is conducted in such a manner that there is no grain formed by nucleation in the melted Si region952ofFIG. 9cbefore the reference numerals961and960are formed. Since the newly formed single crystal region961was grown from the region900, an original single crystal region, a boundary963is not substantially observed.

Thereafter, the laser beam is moved in the x-direction and irradiated. In this case, as shown inFIG. 9e, a region970, which is irradiated with a laser beam970, overlaps with a portion of the previously formed region as shown by the reference numeral972, thereby removing a boundary effect. The irradiated region971is melted, and as shown inFIG. 9f, there are a region981growing from the single crystal region, and a region980growing from the a-Si region. At the end of growth, as shown inFIG. 9g, a single crystal region991and a poly-Si region990are met with each other. It is believed that the boundary992between the previously formed single crystal region994and the newly formed single crystal region991, and the boundary993between the original single crystal region900and these single crystal regions, are not substantially observed.

This is because such boundaries992,993are not boundaries formed by meeting of grains having different orientations, and have the same crystal orientation. When scanning in the x-direction is continued in this way, the size of the single crystal region becomes larger, and at the end of the scanning in the x-direction, scanning in the reverse y-direction is progressed with laser irradiation. This state is shown inFIG. 10. After scanning in the x-direction was completed, a laser irradiation region is shifted in the reverse y-direction and laser irradiation is conducted in such a manner that a single crystal region1020acts as a seed, and at the same time, a poly-Si region1030is melted.

In this way, a region1050irradiated with a laser1040is melted and crystallized again. When this scanning is conducted as shown inFIG. 11c, a single crystal Si region is finally formed over the entire substrate as shown inFIG. 11d.

The above-mentioned crystallization method results in formation of the single crystal Si region over the entire substrate. In this method, process time is somewhat increased as compared to the existing SLS process, due to the additional processes required to form the initial single crystal seed region. To solve this shortcoming, the following embodiments of the present invention are described.

FIGS. 12aand12bshow a method of forming several single crystal Si seed regions by the first and second scanning processes at the same time. An a-Si film1210is deposited on a substrate1200, and irradiated with a laser through a mask where slit patterns were formed. Since several slit patterns are formed in the mask, poly-Si islands1221,1222,1223,1224having a width1230and a length1220are formed upon the first laser scanning at the same time, and irradiated with a laser upon the second scanning in the x-direction at the same time. This laser irradiation is conducted in the reverse y-direction, using the single crystal Si regions formed by the second scanning as a seed, to produce single crystal Si tiles1231,1232,1233,1234as shown inFIG. 12b. Although this method is disadvantageous in that the boundaries between the Si tiles1231,1232,1233,1234occur due to a difference in orientation between such Si tiles, it allows process time to be reduced by about ¼ as compared to the above-mentioned method where the single crystal Si film is formed over the entire substrate. This embodiment is advantageously applied for products having a panel region smaller than single crystal Si tile regions.

FIGS. 13ato13eshow another embodiment of the present invention. An a-Si film is first deposited on a substrate1300, and then irradiated with a laser beam through a mask1304having slit patterns therein. In the mask1304, slits having a length1306and a width1305are regularly arranged at an interval1360from each other. A distance moved by the first scanning is shown by the reference numeral1301.

At the end of the first scanning, poly-Si islands1311are formed in the respective regions at regular intervals, and the reference numeral1312remains at the state of a-Si. Then, after a laser beam is aligned such that it is placed near a boundary1310perpendicularly to the first scanning direction upon the second scanning, the second scanning is conducted in the x-direction. In this case, the scanning distance is adjusted such that it is as long as the reference numeral1302.

Thus, the growth of single crystal Si is progressed toward a-Si regions1312, using a certain grain within the respective poly-Si islands as a seed, so that tiles consisting of poly-Si islands and single crystal Si regions1322are formed over the entire substrate as shown inFIG. 13b.

Thereafter, when additional scanning is conducted using the single crystal regions1322as a seed, the regions which were made of the poly-Si islands are converted into single crystal Si regions1331as shown inFIG. 13cso that single crystal Si regions having a width1333and a length1334are formed in a tile shape over the entire substrate. In this case, the reference numeral1330, which was a boundary between the poly-Si island and the single crystal Si region inFIG. 13b, is not substantially observed. Depending on the scanning direction and the additional steps, various single-crystal Si tile shapes as shown inFIGS. 13dand13ecan be obtained.

This embodiment is advantageous in that process time is remarkably shortened, since the length of the second scanning over the entire substrate as shown inFIG. 11bis greatly reduced. This embodiment can be applied for a case where the entire substrate does not need to be made single-crystal according to the panel size, or a case where the reduction of cost is required for products where securing of the uniformity of a Si thin film is important without requiring a Si thin film of quality as high as single crystal Si.

In this embodiment, the size1302,1303of the tiles need to be sufficiently small such that it does not affect uniformity.

In another embodiment, the scanning direction and number are suitably controlled as shown inFIG. 14, so that only a portion1440(pixel region) for forming a panel1420, and a peripheral circuit region1430, on a substrate1400, are made of a single crystal, and the remaining portion is in the form of poly-Si tiles1410. This allows process time to be reduced while ensuring uniformity.

This embodiment can be applied for products where a peripheral circuit has high switching speed, and the size of a panel is large.

In another embodiment, as shown inFIG. 15, an a-Si film1520is deposited on a substrate1500, only a peripheral circuit region1530of a panel1510is made of a single crystal, and a pixel region1540remains at a-Si.

This embodiment can be applied in a case where a-Si TFT having low leakage current is disposed at a pixel region, and peripheral TFT requiring high-speed switching is made of a single crystal. This embodiment allows process time to be remarkably reduced while ensuring a characteristic of low leakage current.

All the above-mentioned methods can be realized by suitable coping of laser irradiation direction and mask alignment, and regarded as solutions to cope with costs, product characteristics and various designs.

As described above, according to the present invention, the single crystal Si seed region is formed by the additional laser irradiation process using one or two seed grains, which were formed in an elongated shape within a poly-Si, island formed by the prior SLS process. Starting from this seed region, the single crystal Si region can be formed over the entire substrate or a portion or certain region of the substrate.

Thus, the present invention allows the uniformity problem to be fundamentally solved, so that it is possible to cope with various product designs. Furthermore, in fabricating a panel on the single crystal Si region, it can cope with switching speed in a peripheral circuit.

In the embodiments of the methods disclosed herein, the insulating film is a silicon nitride or oxide film selected from SiOx, SiOxHy, SiNxand can be either bi-layer or multiple-layer or a film of nitride or oxide of a metal selected from Al, Cu, Ti and W. In the embodiments of the methods described herein, the semiconductor layer can be made of a material selected from either a-Si (amorphous silicon), a-Ge (amorphous germanium), a-Six,Gey(amorphous silicon germanium), poly-Si (poly-crystalline silicon), poly-Ge (poly-crystalline germanium) or poly-SixGey (poly-crystalline silicon-germanium). The metal film can be made of a metal selected from Al, Cu, Ti, W, Au or silver or compound of any of these metals and a semiconductor.

Accordingly, peripheral circuit parts are integrated to reduce the cost of module parts. Moreover, since single crystal silicon is applied unlike the existing process, sufficient switching speed allowing a drive circuit and also various interface parts to be integrated can be exhibited so that a system-on-panel can be ultimately formed. Thus, the present invention is applied for a wider range of products than existing LTPS TFT-LCD products.

Furthermore, according to the present invention, since a pixel region may also be formed of a-Si, products can be produced, which have a characteristic of low leakage current and where a peripheral circuit is integrated. Also, process costs can be greatly reduced.

Moreover, when a pixel region is made of single crystal silicon, it can exhibit high current so that it is suitable in OLED, a current drive type display, and low voltage driving becomes possible.

In addition, since the present invention can realize formation of single crystal Si on a large-sized glass substrate and also a small-sized substrate such as a Si wafer, it may also be applied in SOI (system-on-insulator) in a semiconductor memory integrated circuit process or in a three-dimensional integrated circuit process.

Finally, when laser crystallization is applied on wiring material, such as aluminum (Al) or copper (Cu), other than Si, to form a single crystal on the wiring material, bad wiring caused by electro-migration in an ultrahigh density integrated circuit can also be reduced.