Abstract:
A method of making a semiconductor device, including the steps of forming, upon a substrate, a semiconductor film, an insulating film, and a conductive film. Part of the upper surface of the conductive film is covered with a resist pattern so that the semiconductor film protrudes from the edges of the resist pattern. Then, the conductive film is etched using the resist pattern as a mask to leave a patterned conductive film, whereby side wall additives of reaction byproducts are generated. Next, the insulating film is etched using the patterned conductive film and side wall additives as a mask, and the side wall additives are removed. Then, impurities are implanted in the semiconductor film using the patterned conductive film as a mask so that impurities transmit through the insulating film, which expose on both sides of the patterned conductive film after removing the side wall additives. Finally, the resist pattern is removed.

Description:
This is a divisional, of application Ser. No. 09/651,876, filed Aug. 30, 2000 now U.S. Pat. No. 6,628,349. 
   This application is based on Japanese Patent Applications HEI 11-309850 filed on Oct. 29, 1999, HEI 11-245324 filed on Aug. 31, 1999, and 2000-213685 filed on Jul. 14, 2000, the entire contents of which are incorporated herein by reference. 

   BACKGROUND OF THE INVENTION 
   a) Field of the Invention 
   The present invention relates to a thin film transistor, a liquid crystal display substrate, a MIS type field effect transistor (MISFET), and their manufacture methods, and more particularly to a transistor having a lightly doped drain structure, a liquid display substrate having such transistors, and their manufacture methods. 
   b) Description of the Related Art 
   Thin film transistors (TFT) are used as switching elements of pixels of an active matrix type liquid crystal display device. A small off-current of TFT is necessary for holding electric charges accumulated by a pixel electrode. The off-current can be reduced by adopting a lightly doped drain (LDD) structure. 
   If both the source and drain regions of TFT have the LDD structure, an on-current reduces. In order to reduce the off-current and retain a sufficient on-current, it can be considered preferable if the LDD structure is formed only on the drain side. 
   For example, in order to form the LDD structure in only the drain region, first impurity ions are implanted into the drain and source regions at a low concentration. Thereafter, the area in the drain region at the low concentration is covered with a resist mask and impurity ions are implanted at a relatively high concentration. The source region is not covered with the resist mask. If the gate length is short, a high precision of position alignment is required when a resist mask is formed to cover the low concentration region on the drain side and expose the source region. 
   A TFT using a polysilicon thin film has a carrier mobility higher than a TFT using amorphous silicon. Therefore, by using polysilicon TFT, an image display area and its driver circuit can be formed on the same substrate. A larger on-current is required for TFT in the peripheral circuit than a switching TFT of each pixel. In this context, it may occur that the LDD structure is adopted for TFT in the pixel area and not for TFT in the peripheral circuit. 
   If the LDD structure is adopted for the source and drain regions of TFT in the pixel area and not adopted for TFT in the peripheral circuit, the number of photolithography processes increases more than if the LDD structure is adopted for all TFTs. An increase in the number of photography processes results in a higher manufacture cost and a lower manufacture yield. 
   SUMMARY OF THE INVENTION 
   It is an object of the present invention to provide TFT having a small off-current and not requiring a high alignment precision even if the gate length is short. 
   It is another object of the present invention to provide a liquid crystal display substrate in which TFT in an image display area has a small off-current and TFT in a peripheral circuit has a large on-current, and a method of manufacturing such a substrate. 
   It is another object of the present invention to provide a method of manufacturing TFT or MISFET having the LDD structure, capable of suppressing an increase in the number of manufacture processes as small as possible. 
   According to one aspect of the present invention, there is provided a thin film transistor comprising: a current path pattern defining a current path, the current path pattern being made of semiconductor material and formed on an insulating principal surface of a substrate; a gate pattern three-dimensionally crossing the current path pattern at least in first and second cross areas, the gate pattern defining a channel region of the current path pattern in an area superposed upon by the gate pattern; and a gate insulating film disposed between the current path pattern and the gate pattern in the first and second cross areas, wherein the current path pattern has an LDD structure on both sides of the channel region in the first cross area, the LDD structure including low concentration regions in contact with the channel region and high concentration regions in contact with the low concentration regions, and has an impurity concentration in areas in contact with the channel region in the second cross area higher than an impurity concentration of the low impurity concentration regions. 
   Since the LDD structure is formed on both sides of the channel region in the first contact area, it is not necessary to mask only one side of the gate during manufacture. Accordingly, a high position alignment precision is not required even if the gate length is short. Since the LDD structure is formed in one of the first and second cross areas, an off-current can be made small. 
   According to another aspect of the present invention, there is provided a liquid crystal display substrate comprising: a plurality of gate bus lines extending in a row direction and formed on an insulating principal surface of a substrate; a plurality of drain bus lines extending in a column direction and formed on the principal surface of the substrate, the drain bus line being electrically insulated from the gate bus line in a cross area in which the gate bus line and the drain bus line cross each other; a pixel electrode disposed in each of cross areas between the gate bus line and the drain bus line; a current path pattern disposed in and along each cross area between the gate bus line and the drain bus line, the current path pattern being made of semiconductor material and three-dimensionally crossing a corresponding one of the gate bus lines at least in two cross areas, a channel region of the current path pattern being formed in an area superposed upon by the gate bus line, a first end portion of the current path pattern being electrically connected to a corresponding one of the drain bus lines, and a second end portion of the current path pattern being electrically connected to a corresponding one of the pixel electrodes; and a gate insulating film disposed between the gate bus line and the current path pattern in the cross area, wherein the current path pattern has an LDD structure on both sides of the channel region nearer to the first end portion, the LDD structure including low concentration regions in contact with the channel region and high concentration regions in contact with the low concentration regions, and has an impurity concentration in areas in contact with the channel region nearer to the second end portion higher than an impurity concentration of the low impurity concentration regions. 
   Since the LDD structure is formed on both sides of the channel region nearer to the first end portion, it is not necessary to mask only one side of the gate during manufacture. Accordingly, a high position alignment precision is not required even if the gate length is short. Since the LDD structure is formed in one of the first and second cross areas, an off-current can be made small. 
   If the substrate is rotated by 90°, the row direction and the column direction are replaced with each other. Namely, in the present specification, the row direction and the column direction mean the two directions intersecting with each other and do not necessarily mean horizontal and vertical directions. 
   According to another aspect of the present invention, there is provided a method of manufacturing a semiconductor display substrate, comprising the steps of: preparing a substrate having an insulating principal surface, and an image display area and a peripheral circuit area defined in a plane of the principal surface, the peripheral circuit area being disposed at a side of the image display area; forming a plurality of first current path patterns distributed in a matrix shape on the principal surface of the substrate in the image display area and a second current path pattern in the peripheral circuit area, in such a manner that each of the first current path patterns includes a portion flowing current at least in a column direction and the second current path patter includes a portion flowing current at least in a row direction; covering the first and second current path patterns with a gate insulating film; forming a plurality of gate patterns on the gate insulating film in such a manner that the gate pattern crosses the column directionally flowing current portion of the first current path pattern in the image display area and crosses the row directionally flowing current portion of the second current path pattern in the peripheral circuit area; implanting impurity ions into the first and second current path patterns by using the gate patterns as a mask; and irradiating an energy beam into the first and second current path patterns along an oblique direction relative to a plane of the principal surface to activate doped impurities so that the energy beam is irradiated in the first current path pattern in a shaded state of one of both sides of the gate pattern and irradiated in the second current pattern on both sides of the gate pattern. 
   The energy beam is not irradiated in a region of the shaded state of one of both sides of the gate bus line, and impurities are not activated. The region whose impurities are not activated serves as the low concentration region of the LDD structure. If two TFTs are formed having gates whose extension directions are shifted by 90°, one TFT can have a one-side LDD structure, and the other TFT can have a both-side LDD structure. 

   
     BRIEF DESCRIPTION OF THE DRAWINGS 
       FIG. 1  is a plan view of a TFT according to a first embodiment. 
       FIGS. 2A  to  2 D are cross sectional views of a substrate illustrating a manufacture method for the TFT of the first embodiment. 
       FIGS. 3A and 3B  are graphs showing on-current and off-current of TFTs of various types. 
       FIGS. 4A  to  4 I are schematic plan views of TFTs of various types whose on-current and off-current were evaluated. 
       FIG. 5  is a plan view showing another example of the structure of a multi-gate TFT. 
       FIG. 6  is a cross sectional view of a TFT used in a liquid crystal display substrate according to a second embodiment. 
       FIG. 7  is a schematic plan view of the liquid crystal display substrate of the second embodiment, and enlarged plan views of TFTs. 
       FIGS. 8A  to  8 E are plan views showing other examples of the structure of a multi-gate TFT. 
       FIGS. 9A  to  9 E are cross sectional views of a substrate illustrating a method of manufacturing TFTs according to a third embodiment. 
       FIGS. 10A and 10B  are cross sectional views of a substrate illustrating a method of manufacturing TFTs according to a fourth embodiment. 
   

   DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS 
   With reference to FIG.  1  and  FIGS. 4A  to  4 I, a TFT and a liquid crystal display substrate using TFTs according to the first embodiment of the invention will be described. 
     FIG. 1  is a plan view showing one pixel area of a liquid crystal display substrate according to the first embodiment. On an insulating principal surface of a glass substrate, a plurality of gate bus lines  1  and drain bus lines  2  are formed. Each gate bus line  1  extends in a row direction in  FIG. 1 , and each drain bus line extends in a column direction in FIG.  1 . The gate bus line  1  and drain bus line  2  are electrically insulated in their cross areas. 
   In each cross area between the gate bus line  1  and drain bus line  2 , a current path pattern  3  made of polysilicon is disposed. One end portion  3   a  of the current path  3  is electrically connected to a corresponding drain bus line  2  via a contact hole  4   a . The current path pattern  3  extends along the drain bus line  2  from the end portion  3   a  to a cross area  10  between the drain bus line  2  and gate bus line  1 . 
   In this cross area  10 , the current path pattern  3  crosses a corresponding gate bus line  1 . The current pattern  3  extends in parallel to the corresponding gate bus line  1  and again crosses the corresponding gate bus line  1  in a cross area  11 . Namely, a multi-gate type TFT is formed in which the current path pattern  3  crosses the gate bus line in the two cross areas  10  and  11 . The other end portion  3   b  of the current path pattern  3  is electrically connected to a pixel electrode  5  via a contact hole  4   b.    
   On both sides of a channel layer  3 ′ of the current path pattern  3  in the cross area  10 , the LDD structure is formed which has a low concentration region in contact with the channel layer and a high concentration region in contact with the low concentration region. In areas in contact with the channel layer  3 ″ in the cross area  11 , a low concentration region is not formed. Namely, the high concentration regions are in direct contact with this channel layer. This high concentration region has an impurity concentration higher than that of the low concentration region in the cross area  10 . 
   Next, with reference to  FIGS. 2A  to  2 D, the cross sectional structure of the liquid crystal display substrate shown in FIG.  1  and its manufacture method will be described.  FIGS. 2A  to  2 D are cross sectional views taken along one-dot chain line A 2 —A 2  shown in FIG.  1 . 
   As shown in  FIG. 2A , on the surface of a glass substrate  20 , an underlie SiO 2  film  21  is formed by plasma enhanced chemical vapor deposition (PE-CVD). On this underlie SiO 2  film  21 , a polysilicon film  3   c  is formed to a thickness of 50 nm. In place of a lamination substrate of the glass substrate  20  and underlie SiO 2  film  21 , another substrate having an insulating principal surface may be used. A method of forming the polysilicon film  3   c  will be described briefly. 
   On the underlie SiO 2  film  21 , an amorphous silicon film is first deposited by PE-CVD. A XeCl excimer laser is applied to the amorphous silicon film to polycrystallize it. The excimer laser is exposed to a narrow stripe area on the substrate surface. This narrow stripe exposure area is moved at each one shot along a direction perpendicular to the longer axis direction of the exposure area to apply the laser to almost the whole area of the amorphous silicon film. For example, the energy density of the laser in the laser exposure area is 400 mJ/cm 2 , and an overlap factor during exposure area movement is 90% or higher. 
   As shown in  FIG. 2B , the polysilicon film  3   c  is patterned to leave a current path pattern  3 . For example, the polysilicon film  3   c  is etched through reactive ion etching using mixture gas of CF 4  and O 2 . The plan shape of the current path pattern  3  has been described with reference to  FIG. 1. A  gate insulating film  22  of SiO 2  is deposited to a thickness of 100 nm on the current path pattern  3  and exposed underlie SiO 2  film  21 . For example, the gate insulating film  22  is deposited by PE-CVD using SiH 4  and N 2 O as source gas. 
   On this gate insulating film  22 , an aluminum (Al) film  1   a  is deposited to a thickness of 300 nm. For example, the Al film  1   a  is deposited by sputtering. 
   Next, the processes of forming the structure shown in  FIG. 2C  will be described. The Al film  1   a  is patterned to leave the gate bus line  1 . The plan shape of the gate bus line  1  has been described with reference to FIG.  1 . In the cross area  10 , a resist pattern  30  is formed covering a partial surface area of the gate insulating film  22  continuous with the sides of the gate bus lines  1 . 
   By using the resist pattern  30  as a mask, the gate insulating film  22  is etched. A gate insulating film  22   a  is therefore left under the resist pattern  30 . The gate insulating film  22   a  outward projects from the sides of the gate bus line  1 . The length of this outward projected area is, for example, 0.5 μm. In the cross area  11 , the gate bus line  1  serves as a mask so that a gate insulating film  22   b  is left between the gate bus line  1  and current path pattern  3 . After the gate insulating film  22  is etched, the resist pattern  30  is removed. 
   By using the gate bus line  1  as a mask, a first phosphorous ion doping is performed. This first phosphorous ion doping is performed under the conditions of hydrogen diluted PH 3  as an ion source, an acceleration energy of 70 keV and a dose of 1×10 14  cm −2 . As different from ion implantation used by semiconductor manufacture processes, mass spectrometry of an ion beam emitted from an ion source is not performed. With this ion doping, phosphorous ions are doped into the current path pattern  3  under the gate insulating film  22   a  to form low concentration regions  3   d . Phosphorous ions are not doped just under the gate bus line  1 . 
   Next, by using the gate bus line  1  and gate insulating film  22   a  as a mask, a second phosphorous ion doping is performed. The second phosphorous ion doping is performed under the conditions of an acceleration energy of 10 keV and a dose of 5×10 15  cm −2 . In the cross area  11 , high concentration regions  3   e  are therefore formed on both sides of the channel layer  3 ″ just under the gate bus line  1 . In the cross area  10 , a high concentration region  3   e  in contact with the low concentration region  3   d  is therefore formed. 
   After the second phosphorous ion doping, laser annealing is performed to activate the doped phosphorous ions. The laser used is an XeCl excimer laser and the energy density is 200 to 300 mJ/cm 2 . 
   As shown in  FIG. 2D , an interlayer insulating film  23  is formed over the whole substrate surface, the interlayer insulating film having a two-layered structure of an SiO 2  film and an SiN film. The thickness of the interlayer insulating film  23  is, for example, 400 to 500 nm. Contact holes  4   a  and  4   b  are formed through the interlayer insulating film  23 . The upper surface of the end portion of the current path pattern  3  on the side of the cross area  10  is exposed at the bottom of the contact hole  4   a . The upper surface of the end portion of the current path pattern  3  on the side of the cross area  11  is exposed at the bottom of the contact hole  4   b.    
   A drain bus line  2  and an interlayer connection member  2   a  respectively having a three-layer structure of Ti/Al/Ti are formed on the interlayer insulating film  23 . The drain bus line  2  is therefore connected to the one end portion of the current path pattern  3  via the contact hole  4   a , and the interlayer connection member  2   a  is therefore connected to the other end portion of the current path pattern  3  via the contact hole  4   b.    
   A passivation film  24  is formed on the interlayer insulating film  23 , covering the drain bus line  2  and interlayer connection member  2   a . For example, the passivation film  24  is made of SiN. A contact hole  4   c  is formed through the passivation film  24  to expose an upper surface of the interlayer connection member  2   a . A pixel electrode  5  made of indium tin oxide (ITO) is formed on the passivation film  24 . The pixel electrode  5  is therefore connected to the interlayer connection member  2   a  via the contact hole  4   c.    
   As shown in  FIG. 2D , the current path pattern  3  has, on both sides of the channel layer in the cross area  10 , the low concentration regions  3   d  in contact with the channel layer and the high concentration regions  3   e  in contact with the low concentration regions  3   d , constituting the LDD structure. The channel layer  3 ″ in the cross area  11  is in direct contact with the high concentration regions  3   e  having an impurity concentration higher than that of the low concentration region  3   d.    
   TFTs of the first embodiment and other TFTs of various types for comparison were formed and on-current and off-current were measured. The measurement results will be described with reference to  FIGS. 3A and 3B  and  FIGS. 4A  to  4 I. 
     FIGS. 4A  to  4 I are schematic plan views of TFTs of various types whose on-current and off-current were evaluated. TFTs shown in  FIGS. 4A  to  4 C are single-gate TFTs having one gate G, a source S and a drain D. TFTs shown in  FIGS. 4D  to  4 F are two-gate TFTs having two gates G, a source S and a drain D. TFTs shown in  FIGS. 4G  to  4 I are triple-gate TFTs having three gates G, a source S and a drain D. The gate length of the single gate TFT is 2 μm, the gate length of the double-gate TFT is 4 μm in total, and the gate length of the triple-gate TFT is 6 μm in total. 
   TFT shown in  FIG. 4A  has the LDD structure having a low concentration region LDD on the source side of the channel layer, TFT shown in  FIG. 4B  has the LDD structure on the drain side, TFT shown in  FIG. 4C  has the LDD structure on both the source and drain sides. 
   TFTs shown in  FIGS. 4D and 4G  have the LDD structure on both sides of a gate G nearest to the source. TFTs shown in  FIGS. 4E and 4H  have the LDD structure on both sides of a gate G nearest to the source. TFTs shown in  FIGS. 4F and 4I  have the LDD structure on both sides of gates G at both ends. In addition to TFTs shown in  FIGS. 4A  to  4 I, single-gate TFTs, double-gate TFTs and triple-gate TFTs respectively having no LDD structure were also formed. 
     FIG. 3A  is a graph showing the on-current of each TFT, and  FIG. 3B  is a graph showing the off-current of each TFT. The measurement conditions of the on-current were a gate voltage of 10 V and a drain voltage of 1 V, and the measurement conditions of the off-current were a gate voltage of −10 V and a drain voltage of 1 V. The abscissa of  FIGS. 3A and 3B  represents single-gate TFTs, double-gate TFTs and triple-gate TFTs sequentially in this order from left. In  FIGS. 3A and 3B , a circle symbol represents a TFT without the LDD structure, a triangle symbol represents a ITFT having a one-side LDD structure with the LDD region only on the source side shown in  FIGS. 4A ,  4 D and  4 G. A cross symbol represents a TFT having a one-side. LDD structure with the LDD region only on the drain side shown in  FIGS. 4B ,  4 E and  4 H. A square symbol represents a TFT having a both-side LDD structure with the LDD region on both the source and drain sides shown in  FIGS. 4C ,  4 F and  4 I. 
   Although TFTs having the both-side LDD structure can reduce the off-current more than TFTs having no LDD structure as indicated by the square symbols in  FIG. 3B , the on-current also reduces as indicated by the circle symbols in FIG.  3 A. Although TFTs having no LDD structure can obtain a larger on-current than TFTs having the both-side LDD structure as indicated by the circle symbols in  FIG. 3A , the off-current increases as shown in FIG.  3 B. 
   TFTs having the one-side LDD structure with the double-gate or triple-gate can obtain an on-current not so smaller than TFTs having no LDD structure, and an off-current not so larger than TFTs having the both-side LDD structure. 
   TFT having a single gate and the one-side LDD structure has the LDD structure only on one side of the gate. In forming the LDD structure only on one side of the gate, in the process shown in  FIG. 2C , the resist pattern  30  covers only one side of the gate bus line  1 . Therefore, as the gate length becomes short and the gate bus line  1  becomes narrow, a high alignment precision is required. 
   In contrast, TFT having double gates or triple gates and the one-side LDD structure has the LDD structure on both sides of one of the gates. Therefore, even if the gate length becomes short, a high alignment precision in forming the LDD structure is not required. Manufacture yield can be prevented from being lowered by misalignment. 
   As shown in  FIGS. 4D ,  4 E,  4 G and  4 H, the both-side LDD structure on the source or drain side having double gates or triple gates can realize a large on-current and a small off-current and can improve manufacture yield. 
   In  FIGS. 4D  to  4 I, one gate bus line is branched and each branch crosses the current path pattern between the source and drain. Instead, as shown in  FIG. 1 , the gate bus line  1  may be disposed linearly and the current path pattern  3  is bent to make the gate bus line  1  and current path pattern  3  cross twice. 
     FIG. 5  shows another example of the structure of a gate bus line and a current path pattern. A gate bus line  1  is disposed linearly and a current path pattern  3  is bent in an S-character shape, and both cross in three areas. Of these three cross areas, the cross area on the side of an end portion  3   a  connected to a drain bus line is formed with the LDD structure on both sides thereof. The current path pattern  3  may be formed linearly and the gate bus line  1  is bent to make both cross each other in a plurality of cross areas. 
   Next, with reference to  FIGS. 6 and 7 , a liquid crystal display substrate according to the second embodiment will be described. 
     FIG. 6  is a cross sectional view of a TFT used with the liquid crystal display substrate of the second embodiment. The principal surface of a glass substrate  20  has an underlie SiO 2  film  21  formed thereon. A partial surface area of the underlie SiO 2  film has a current path pattern  3  of polysilicon formed therein. The gate bus line  1  three-dimensionally crosses the current path pattern  3 . A gate insulating film  22  is disposed between the gate bus line  1  and current path pattern  3 . This structure is formed by the same processes as the processes up to the process of forming the gate bus line shown in  FIG. 2C  of the first embodiment. 
   Next, by using the gate bus line  1  as a mask, phosphorous ions are doped. The phosphorous ion doping conditions are the same as the conditions of the second phosphorous ion doping described with  FIG. 2C  of the first embodiment. 
   After phosphorous ions are doped, a laser beam  31  is applied obliquely relative to the substrate surface to activate doped phosphorous ions. The laser used is a XeCl excimer laser and the energy density is 200 to 300 mJ/cm 2 . The incidence plane of the laser beam  31  is perpendicular to the extension direction of the gate bus line  1 . In this case, the laser beam does not reach a portion of the current path pattern  3  shaded by the gate bus line  1 . Therefore, a region  3   f  in which phosphorous ions are not activated is left on one side of the gate bus line. This region  3   f  with phosphorous ions not activated serves as the low concentration region of the LDD structure. 
   As described earlier, by the annealing with an obliquely irradiated laser beam, the low concentration region of the LDD structure can be formed in self-alignment with the gate bus line. 
     FIG. 7  is a schematic plan view of the liquid crystal display substrate of the second embodiment, and enlarged plan views of TFTs. An image display area  35  is defined on a principal surface of the glass substrate  20 . A peripheral circuit area  36  is defined in upper and right side areas of the image display area  35 . In the image display area  35 , gate bus lines  1  and drain bus lines  2  such as shown in  FIG. 1  are disposed in a lattice shape, and pixel electrodes  5  are disposed in a matrix shape. In the peripheral circuit area  36 , a peripheral circuit is disposed for applying drive signals to the gate bus lines  1  and drain bus lines  2 . 
   A TFT  40  in the image display area  35  is constituted of the current path pattern  3 , an end portion  3   a  on the drain side, an end portion  3   b  on the source side, and the gate bus line  1 . The end portion  3   a  of the drain side is connected to the drain bus line  2 , and the end portion  3   b  on the source side is connected to the pixel electrode  5 . The current path pattern  3  has a U-character bent shape and includes a portion in which current flows in the column direction (vertical direction in FIG.  7 ). The gate bus line  1  extends in the row direction (horizontal direction in  FIG. 7 ) and crosses the column directionally flowing current portion in two cross areas. The end portion  3   a  on the drain side and the end portion  3   b  on the source side are disposed in an area lower than the gate bus line  1  as viewed in FIG.  7 . 
   A p-channel type TFT  41  in the peripheral circuit area  36  is constituted of a current path pattern  41 C, an end portion  41 S on the source side, an end portion  41 D on the drain side, and a gate electrode  41 G. The current path pattern  41 C includes a portion in which current flows in the row direction. The gate electrode  41 G extends in the row direction and crosses the column directionally flowing current portion of the current path pattern  41 C. 
   An n-channel type TFT  42  is constituted of a current path pattern  42 C, an end portion  42 S on the source side, an end portion  42 D on the drain side, and a gate electrode  42 G. The current path pattern  42 C includes a portion in which current flows in the column direction. The gate electrode  42 G extends in the row direction and crosses the column directionally flowing current portion of the current path pattern  42 C. 
   TFT  40  has the LDD structure only in the area lower than the gate bus line  1  as viewed in FIG.  7 . TFT  42  also has the LDD structure only in the area lower than the gate electrode  42 G. TFT  41  has no LDD structure. 
   Such LDD structure can be formed by obliquely applying a laser as described with  FIG. 6  to activate impurity ions. In forming the liquid crystal display substrate of the second embodiment shown in  FIG. 7 , the optical axis of a laser beam is inclined so as to shade the area lower than the gate bus line  1  as viewed in FIG.  7 . Since the gate electrode  42 G of TFT  42  is disposed in parallel to the gate bus line  1 , the shaded area is formed in an area lower than the gate electrode  42 G as viewed in FIG.  7 . Since the gate electrode  41 G of TFT  41  is in parallel to the incidence plane of a laser beam, this beam is applied to the areas on both sides of the gate electrode and no shaded area is formed. 
   TFT  40  in the image display area  35  has the double-gate structure and the LDD structure on the source side of the gate near the source and on the drain side of the gate near the drain. Therefore, as compared to a TFT with no LDD structure, the off-current can be reduced more. In the peripheral circuit area, desired TFTs are provided with the one-side LDD structure, and other TFTs are not provided with the LDD structure. For example, n-channel type TFTs are provided with the one-side LDD structure and p-channel type TFTs are not provided with the LDD structure. In this manner, the reliability of n-channel type TFTs can be improved and the on-current of p-channel type TFTs can be prevented from being lowered. 
   In the manufacture of the liquid crystal display substrate shown in  FIG. 7 , the LDD structure is formed in a desired area by obliquely applying a laser beam. Since a photography process for the LDD structure is not necessary, the number of processes can be prevented from being increased. 
   Although single-gate type TFTs and double-gate type TFTs have been described with reference to  FIG. 7 , the method of activating impurity ions by obliquely applying a laser beam described with  FIG. 6  is also applicable to TFTs having triple gates or more gates. 
     FIG. 8A  is a schematic plan view showing a triple-gate type TFT formed by using the method of obliquely applying a laser beam. This TFT is constituted of a current path pattern C, a source side end portion S, a drain side end portion D, and a gate electrode G. The current path pattern C has an S-character bent shape. The gate electrode G crosses the current path pattern C in three cross areas. In each cross area, a low concentration area LDD of the LDD structure is formed only on one side of the gate electrode. 
   In TFT shown in  FIG. 8A , the current path pattern C is bent and the gate electrode G is straight. The current path pattern may be made straight, and the gate electrode may be branched to form a multi-gate type TFT. 
     FIG. 8B  shows a double-gate type TFT with a gate electrode G having two branches. The gate electrode G is branched into two branches. Each of the branched two gate electrodes crosses the current path pattern C. In each cross area, a low concentration area LDD of the LDD structure is formed only on the drain side of the gate electrode. 
     FIG. 8C  shows a TFT having a narrow gap between two branched gate electrodes. A low concentration region LDD formed on one side in one cross area reaches the border of the gate electrode G in the other cross area. The LDD structure is formed on both sides of the gate electrode in one cross area. By properly setting the incidence angle of an irradiated laser beam and the gap between the branched gate electrodes, the LDD structure can be formed on both sides in one cross area. The LDD structures on both sides of a channel layer can suppress a variation in element characteristics when the polarity of voltage applied to TFT is inverted. 
     FIG. 8D  is a schematic plan view of a triple-gate type TFT with the gate electrode G branched into three branches. In each cross area between the branched gate electrodes G and a current path pattern C, the LDD structure is formed on the drain side of the gate electrode G. As shown in  FIG. 8E , a gap between the two branched gate electrodes G of the three branched gate electrodes G may be narrowed to form the LDD structure on both side in one cross area. 
   Next, with reference to  FIGS. 9A  to  9 E, the third embodiment will be described. In the first embodiment, the end of the low concentration region  3   d  on the channel layer side is aligned with the border of the gate bus line  1 , and the end of the low concentration region  3   d  on the high concentration region  3   e  side is aligned with the border of the gate insulating film  22   a . Namely, both ends of the low concentration region  3   d  are defined by the photolithography processes. In the third embodiment to be described hereinunder, only one end of the low concentration region is defined by the photolithography process. 
   As shown in  FIG. 9A , an underlie SiO 2  film  21  is formed to a thickness of 200 nm on the surface of a glass substrate  20 . On this underlie SiO 2  film  21 , a current path pattern  3  of polysilicon is formed to a thickness of 50 nm. A gate insulating film  22  of SiO 2  is formed to a thickness of 120 nm on the underlie SiO 2  film  21 , covering the current path pattern  3 . The processes up to this are similar to those processes of forming the structure shown in  FIG. 2B  of the first embodiment. 
   A conductive film  1   a  of AlSc alloy is deposited to a thickness of 300 nm on the gate insulating film  22  by sputtering. On this conductive film  1   a , a resist pattern  51  having a plan shape corresponding to the gate bus line  1  shown in  FIG. 1  is formed. 
   As shown in  FIG. 9B , by using the resist pattern  51  as a mask, the conductive film  1   a  is etched. This etching is performed by using a two-frequency plasma etching system. For example, in this two-frequency plasma etching system, a voltage having a frequency of 4 MHz is applied via a capacitor to a substrate holder on which a substrate to be etched is placed, and an a.c. magnetic field having a frequency of 13.56 MHz is generated in the upper space of the substrate by using a coil. As etching gas, mixture gas of chlorine (Cl 2 ) and BCl 3  is used. For example, the flow rate of chlorine gas is set to 30 sccm, the flow rate of BCl 3  gas is set to 150 sccm, a pressure in the chamber is set to 8 Pa, and a power supplied to the coil is set to 1 kW. 
   It is preferable to make the power supplied to the coil at the frequency of 13.56 MHz be set larger than the power supplied to the substrate holder at the frequency of 4 MHz. By adjusting the powers in this manner, the ion impact effects can be reduced and a chemical reaction becomes dominant. Side wall additive  52  becomes, therefore, likely to be formed. Instead of generating the magnetic field in the upper space of the substrate by using the coil, a high frequency electric field may be generated by using plate electrodes. More generally, it is preferable to adjust powers so that the power supplied to a high frequency electric power supply means (corresponding to the coil or plate electrodes) disposed above the substrate is larger than the power supplied to another high frequency power supply means (corresponding to the substrate holder) disposed under the substrate. 
   With this etching, the conductive film  1   a  is patterned inheriting the shape of the resist pattern  51 , to leave a gate bus line  1 . The side wall additive  52  is also formed because reaction byproducts of AlSc material of the conductive film  1   a  and material of the resist pattern  51  reacted with etching gas are attached to the side walls of the gate bus line  1 . Under the above-described etching conditions, the thickness of the side wall additive  52  is about 100 nm. As the etching gas, instead of BCl 3 , gas such as SiCl 4 , HBr, HI, N 2 , CF 4  and HCl may be used. As the material of the conductive film  1   a , instead of AlSc, other material such as Al, AlTi, AlNd and AlCu may be used. 
   As shown in  FIG. 9C , by using as a mask the gate bus line  1  (or resist pattern  51 ) and side wall additive  52 , the gate insulating film  22  is etched to leave a patterned gate insulating film  22   a . The gate insulating film  22   a  has projection areas  22   b  outward projecting on both sides of the gate bus line  1  by an amount corresponding to the thickness of the side wall additive  52 . This etching is executed by using the two-frequency plasma etching system. As the etching gas, mixture gas of CF 4  and CHF 3  is used. For example, the flow rates of CH 4  gas and CHF 3  gas are both set to 50 sccm, the pressure in the chamber is set to 4 Pa and the power supplied to the coil is set to 1 kW. It is preferable to make the power supplied to the substrate holder under the substrate be set larger than the power supplied to the coil above the substrate. By adjusting the powers in this manner, the ion impact effects can be enhanced and etching with high anisotropy can be executed. More generally, it is preferable to adjust supply powers so that the power supplied to a high frequency power supply means (corresponding to the substrate holder) disposed under the substrate is larger than the power supplied to another high frequency electric power supply means (corresponding to the coil). 
   As shown in  FIG. 9D , the resist pattern  51  and side wall additive  52  are removed. This removal can be effected by a wet process using phenol containing remover and amine containing organic solvent. 
   As shown in  FIG. 9E , by using the gate bus line  1  as a mask, impurity ions are implanted into the current path pattern  3  under the conditions allowing impurity ions to transmit through the projection areas  22   b . More specifically, in the area where n-channel TFTs are formed, PH 3  ions are implanted under the conditions of an acceleration energy of 50 keV and a dose of 5×10 15  cm −2 , and in the area where p-channel TFTs are formed, BF 2  ions are implanted under the conditions of an acceleration energy of 50 keV and a dose of 5×10 15  cm −2 . 
   With the ion implantation under these conditions, the impurity concentration of a region of the current path pattern  3  under the projection areas  22   b  becomes lower than that of the exposed region. Therefore, low concentration regions  3   d  are formed under the projection areas  22   b  and high concentration regions  3   e  are formed outside of the low concentration regions  3   d.    
   The boundary between the low concentration region  3   d  and channel layer is defined by the border of the gate bus line  1 , and the boundary between the low concentration region  3   d  and high concentration region  3   e  is defined by the border of the gate insulating film  22   a . Since the border of the gate insulating film  22   a  is determined by the side wall of the side wall additive  52  shown in  FIG. 9B , the boundary between the low concentration region  3   d  and high concentration region  3   e  is determined in a self-alignment manner relative to the gate bus line  1 . 
   The length of the low concentration region  3   d  is determined by the thickness of the side wall additive  52 . This thickness depends upon the etching conditions for the conductive film  1   a  described with reference to FIG.  9 B. Therefore, by controlling the etching conditions, the length of the low concentration region  3   d  can be adjusted. 
   A method of forming the LDD structure in the cross area  10  shown in  FIG. 1  has been described with reference to  FIGS. 9A  to  9 E. With this method, however, the LDD structure is formed also in the cross area  11 . In order not to form the LDD structure in the cross area  11 , the projection areas  22   b  in the cross area  11  are removed prior to the ion implantation process described with reference to FIG.  9 E. This removal can be executed by RIE using mixture gas of CF 4  and CHF 3  by using a resist mask having an opening exposing the cross area  11  and nearby area. 
   In the first embodiment, the LDD structure and non-LDD structure are used in combination. If TFTs having only the LDD structure are to be formed on a glass substrate, it is not necessary to remove the projection areas  22   b.    
   Next, with reference to  FIGS. 10A and 10B , the fourth embodiment will be described. In the third embodiment, the LDD structure is formed for TFTs. This LDD structure forming method may be applied to MISFETs on a silicon single crystal substrate. In the fourth embodiment, MISFETs are formed on a silicon single crystal substrate. 
   The cross sectional view of a substrate during the manufacture processes shown in  FIG. 10A  corresponds to  FIG. 9A  referred to for the description of the third embodiment. The current pattern  3  shown in  FIG. 9A  is replaced by an active region  60  of a single crystal silicon substrate shown in  FIG. 10A , the gate insulating film  22  is replaced by a silicon oxide film  61  formed on the active region  60 , the conductive film  1   a  is replaced by a conductive film  62 , and the resist pattern  51  is replaced by a resist pattern  63 . 
   As the processes similar to those shown in  FIGS. 9B  to  9 E of the third embodiment are executed, a MISFET shown in  FIG. 10B  is obtained. This MISFET is constituted of source and drain regions  65 , a gate insulating film  61   a  made of silicon oxide, and a gate electrode  62  made of AlSc alloy. Each of the source and drain regions  65  has the LDD structure including a low concentration region  65   a  and a high concentration region  65   b.    
   According to a conventional MISFET manufacture method, an ion implantation process of forming a low concentration region and an ion implantation process of forming a high concentration region are executed independently. With the fourth embodiment method, both the low and high concentration regions can be formed by one ion implantation process. 
   The present invention has been described in connection with the preferred embodiments. The invention is not limited only to the above embodiments. It is apparent that various modifications, improvements, combinations, and the like can be made by those skilled in the art.