The present invention contains subject matter related to Japanese Patent Application JP 2005-049716 filed with the Japanese Patent Office on Feb. 24, 2005, the entire contents of which being incorporated herein by reference.
The present invention relates to a thin film semiconductor device and a method of manufacturing the same, and to an active matrix type display configured by use of the thin film semiconductor device. Particularly, the invention relates to a semiconductor thin film crystallizing technology for forming device regions of a thin film semiconductor device. More particularly, the invention relates to a lateral crystal growth technology for creating a temperature difference between different regions of a semiconductor thin film by laser annealing and inducing crystal growth in the film plane direction (lateral direction) by utilizing the temperature difference.
A thin film semiconductor device has thin film transistors as main component devices. The thin film transistor uses a semiconductor thin film as an active layer. As the semiconductor thin film, for example, a silicon film is generally used. In recent years, a technology of forming a polycrystalline silicon film on an inexpensive glass substrate as an active layer of a thin film transistor has been developed progressingly.
As a technology for forming a polycrystalline silicon film on a glass substrate at a low temperature, there has been developed a crystallizing technology based on irradiation with laser light. The crystallization by irradiation with laser light (hereinafter referred to as “laser annealing” in some cases) is a technology in which the energy of laser light is absorbed into an amorphous silicon film, whereby only the film is instantaneously melted, and recrystallization is achieved during the cooling process.
Recently, a technology of obtaining a polycrystalline silicon film with a high crystallinity by use of a continuously oscillated laser light has been publicly reported. In this technology, an amorphous silicon film is scanned with a continuously oscillated laser beam so that a solid-liquid interface in the semiconductor thin film is moved in a lateral direction, whereby a temperature difference is created in the film, and lateral crystal growth is induced in the silicon film by utilizing the temperature difference. However, the process margin of this technology is narrow in that, if the scanning speed is low, the film itself is lost through bumping, and, if the scanning speed is high, the speed would exceed the moving velocity of the solid-liquid interface, resulting in an insufficient lateral crystal growth.
A crystal growth technology utilizing a pulsedly oscillated laser beam in place of the continuously oscillated laser beam has also been developed, as described for example in Japanese Patent Laid-open No. 2003-318108 (hereinafter referred to as Patent Document 1). In the technology as described in Patent Document 1, an amorphous silicon film is formed on a substrate, and a metallic film is formed on a part of the amorphous silicon film. A first irradiation with laser beam from the upper side of the amorphous silicon film is conducted using the metallic film as a mask, whereby the part, other than the part masked by the metallic film, of the amorphous silicon film is crystallized. Thereafter, the metallic film is removed, and a second irradiation with laser beam from the upper side of the amorphous silicon film is conducted, to crystallize a part of the amorphous silicon. The polycrystalline silicon film crystallized by the second irradiation with laser beam is used as a channel region of a thin film transistor.
However, in the crystallization technology disclosed in Patent Document 1, the irradiation with laser beam is carried out two times, and the metallic film mask used in the first irradiation with laser beam is removed, before carrying out the second irradiation with laser beam. Therefore, the process for crystallization is complicated, which is undesirable from the viewpoint of productivity. In addition, since the irradiation with laser beam is carried out dividedly in two runs, it is difficult for a uniform lateral crystal growth to take place, and it is difficult to obtain a good crystallinity.
Thus, there is a need to induce lateral crystal growth by a single run of irradiation with laser beam and thereby to form a semiconductor thin film having a uniform crystal structure. In order to fulfill the above need, according to one embodiment of the present invention, there is provided a method of manufacturing a thin film semiconductor device, including a light absorbing layer forming step for forming a light absorbing layer on the face side of a transparent substrate, a patterning step for patterning the light absorbing layer into a predetermined shape, an insulation film forming step for covering the patterned light absorbing layer with an insulation film, a semiconductor thin film forming step for forming a semiconductor thin film on the insulation film, and a laser annealing step for irradiating the substrate with laser light pulsedly oscillated from the back side of the substrate so as to crystallize the semiconductor thin film, wherein the laser annealing step includes: a first process in which an external region of the semiconductor thin film located on the outer side relative to the pattern of the light absorbing layer is thermally melted, and the light absorbing layer is heated, without melting an internal region of the semiconductor thin film located on the inner side relative to the pattern of said light absorbing layer; a second process in which the molten semiconductor thin film is cooled and microcrystal grains are produced in the vicinity of the boundary between the external region and the internal region; a third process in which a first lateral growth progresses from the boundary between the external region and the internal region toward the outer side with the microcrystal grains as nuclei so that polycrystal grains greater than the microcrystal grains are produced in the area of the external region adjacent to the boundary; and a fourth process in which heat is transferred from the heated light absorbing layer to the semiconductor thin film through the insulation film, whereby the internal region is melted, and thereafter a second lateral growth progresses from the boundary toward the inner side with the polycrystal grains as nuclei so that further enlarged polycrystal grains are produced in the internal region.
According to another embodiment of the present invention, there is provided a method of manufacturing a thin film semiconductor device, including a semiconductor thin film forming step for forming a semiconductor thin film on a substrate, an insulation film forming step for forming an insulation film thereon, a light absorbing layer forming step for forming a light absorbing layer on the upper side of the semiconductor thin film, with the insulation film therebetween, a patterning step for pattering the light absorbing layer into a predetermined shape, and a laser annealing step for irradiating the substrate with laser light pulsedly oscillated from the upper side of the substrate so as to crystallize the semiconductor thin film, wherein the laser annealing step includes: a first process in which an external region of the semiconductor thin film located on the outer side relative to the pattern of the light absorbing layer is thermally melted, and the light absorbing layer is heated, without melting an internal region of the semiconductor thin film located on the inner side relative to the pattern of the light absorbing layer; a second process in which the molten semiconductor thin film is cooled and microcrystal grains are produced in the vicinity of the boundary between the external region and the internal region; a third process in which a first lateral growth progresses from the boundary between the external region and the internal region toward the outer side with the microcrystal grains as nuclei so that polycrystal grains greater than the microcrystal grains are produced in the area of the external region adjacent to the boundary; and a fourth process in which heat is transferred from the heated light absorbing layer to the semiconductor thin film through the insulation film, whereby the internal region is melted, and thereafter a second lateral growth progresses from the boundary toward the inner side with the polycrystal grains as nuclei so that further enlarged polycrystal grains are produced in the internal region.
Preferably, the laser annealing step includes irradiating the substrate with laser light having a wavelength range of from 520 to 540 nm. The laser annealing step may include irradiating the substrate with the pulsedly oscillated laser light while scanning in such a range that irradiated regions overlap with each other. Preferably, the light absorbing layer forming step includes forming the light absorbing layer by use of a conductive film, and the patterning step includes pattering the conductive material so as to produce a wiring including a gate electrode. In this case, preferably, a high melting point metal or an alloy or silicide containing a high melting point metal as a constituent thereof is used as the conductive material for forming the light absorbing layer.
According to a further embodiment of the present invention, there is provided a thin film semiconductor device including an insulating substrate provided integratedly with thin film transistors, wherein each of the thin film transistors includes a semiconductor thin film and a gate electrode laminated, with a gate insulation film therebetween; the semiconductor thin film includes a channel region overlapping with the gate electrode, and a source region and a drain region which are located respectively on both sides of the channel region; the semiconductor thin film is a polycrystalline layer crystallized by laser annealing, and is divided along the boundary of a predetermined pattern into an internal region and an external region; the external region has a first lateral growth region containing polycrystal grains laterally grown from the boundary toward the outer side by the laser annealing; the internal region has a second lateral growth region containing polycrystal grains laterally grown from the boundary toward the inner side with the polycrystalline contained in the first lateral growth region as nuclei; and the channel region is formed in the second lateral growth region.
Preferably, the semiconductor thin film is a polycrystalline layer crystallized by the laser annealing conducted by irradiation with laser light through a light absorbing layer formed in a predetermined pattern, and is formed through: a first process in which the external region located on the outer side relative to the pattern of the light absorbing layer is thermally melted, and the light absorbing layer is heated, without melting the internal region located on the inner side relative to the pattern of the light absorbing layer; a second process in which the molten semiconductor thin film is cooled and microcrystal grains are produced in the vicinity of the boundary between the external region and the internal region; a third process in which a first lateral growth progresses from the boundary between the external region and the internal region toward the outer side with the microcrystal grains as nuclei so that polycrystal grains greater than the microcrystal grains are produced in the area of the external region adjacent to the boundary; and a fourth process in which heat is transferred from the heated light absorbing layer to the semiconductor thin film through the gate insulation film, whereby the internal region is melted, and thereafter a second lateral growth progresses from the boundary toward the inner side with the polycrystal grains as nuclei so that further enlarged polycrystal grains are produced in the internal region. In addition, preferably, the light absorbing layer used in the laser annealing includes a conductive material, and the gate electrode is formed from the conductive material either directly or through a processing. The gate electrode may be formed by using a high melting point metal or an alloy or silicide containing a high melting point metal as a constituent thereof, as the conductive material. Preferably, the source region and the drain region range into at least a part of the first lateral growth region. The first lateral growth region in which the source region and the drain region are formed may range over a distance of at least 2 μm from the boundary toward the outer side. Preferably, the thin film transistor includes an LDD region lower in impurity concentration than the drain region between the channel region and at least the drain region, and the LDD region is formed in the first lateral growth region or the second lateral growth region.
According to yet another embodiment of the present invention, there is provided a display including an insulating substrate provided integratedly with pixels and thin film transistors for driving the pixels, wherein each of the thin film transistors includes a semiconductor thin film and a gate electrode laminated, with a gate insulation film therebetween; the semiconductor thin film includes a channel region overlapping with the gate electrode, and a source region and a drain region which are located respectively on both sides of the channel region; the semiconductor thin film is a polycrystalline layer crystallized by laser annealing, and is divided along the boundary of a predetermined pattern into an internal region and an external region; the external region has a first lateral growth region containing polycrystal grains laterally grown from the boundary toward the outer side by the laser annealing; the internal region has a second lateral growth region containing polycrystal grains laterally grown from the boundary toward the inner side with the polycrystal grains contained in the first lateral growth region as nuclei; and the channel region is formed in the second lateral growth region.
Preferably, the semiconductor thin film is a polycrystalline layer crystallized by the laser annealing conducted by irradiation with laser light through a light absorbing layer formed in a predetermined pattern, and is formed through: a first process in which the external region located on the outer side relative to the pattern of the light absorbing layer is thermally melted, and the light absorbing layer is heated, without melting the internal region located on the inner side relative to the pattern of the light absorbing layer; a second process in which the molten semiconductor thin film is cooled and microcrystal grains are produced in the vicinity of the boundary between the external region and the internal region; a third process in which a first lateral growth progresses from the boundary between the external region and the internal region toward the outer side with the microcrystal grains as nuclei so that polycrystal grains greater than the microcrystal grains are produced in the area of the external region adjacent to the boundary; and a fourth process in which heat is transferred from the heated light absorbing layer to the semiconductor thin film through the gate insulation film, whereby the internal region is melted, and thereafter a second lateral growth progresses from the boundary toward the inner side with the polycrystal grains as nuclei so that further enlarged polycrystal grains are produced in the internal region. Besides, each of the pixels may include an organic electroluminescence device. Alternatively, each of the pixels may include a pixel electrode connected to the thin film transistor, a counter electrode opposed to the pixel electrode, and a liquid crystal held between the electrodes.
In accordance with the present invention, the pattern of the light absorbing layer used for the gate electrode or the like is formed on the amorphous semiconductor thin film, to divide the semiconductor thin film into the internal region covered with the pattern and the external region surrounding the internal region. With the pattern of the light absorbing layer as a mask, irradiation with laser light is carried out once so as to achieve uniform crystallization. By the one run of irradiation with laser light, the lateral crystal growth in the external region and the lateral crystal growth in the internal region can be performed sequentially, with a delay time of not more than 10 μs. In the present invention, the generation of a delay from the external region which is melted immediately upon direct irradiation with the laser light is tactfully utilized for melting the internal region by heat transfer to the semiconductor thin film after the light absorbing layer is heated by irradiation with the laser light. Since it suffices to carry out only one run of irradiation with laser light, the laser light irradiation apparatus itself may be simple in configuration, and the throughput is remarkably enhanced from the viewpoint of process also.
The melting of the internal region covered with the pattern of the light absorbing layer would need a higher laser energy density (area density) than that for the melting of the semiconductor thin film in the external region. The reason lies in that the light absorbing layer to be used as the mask is formed of a high melting point metal or the like, which has a high heat capacity, and the melting thereof needs a greater amount of heat accordingly. An additional reason lies in that, in the case of a bottom gate structure, the transfer of heat to the semiconductor thin film is accompanied by dissipation of heat into the glass substrate. For ensuring that the light absorbing layer is sufficiently heated by one run of irradiation with laser light and not any excessive thermal energy is applied to the external region of the semiconductor thin film, it is effective to use laser light having a wavelength range of from 520 to 540 nm. The laser light with this green color wavelength is the so-called green laser, which is characterized by a lower absorptivity in absorption into a silicon film, as compared with UV excimer laser. The green laser is absorbed by the silicon film only partly, which makes it possible to heat the pattern of the light absorbing layer in a high energy density and, on the other hand, to heat the other external region in a low energy density. For example, at room temperature, only 5 to 10% of green laser is absorbed by a silicon film. With the green laser used, it is possible to first induce the first lateral crystal growth in the external region and thereafter to induce the second lateral crystal growth in the internal region, with a predetermined delay.
In accordance with the manufacturing method of the present invention, the lateral crystal growth is controlled according to the pattern of the light absorbing layer which is formed prior to the laser annealing. This makes it possible to control the size and position of the polycrystalline silicon grain boundary in the internal region, whereby uniformity is enhanced remarkably. With this internal region used for the channel region of the thin film transistor, it is possible to conspicuously improve the characteristics of the thin film transistor. In addition, since crystallization is tactfully carried out by one run of irradiation with laser light in the present invention, the processing rate is enhanced by a simply calculated factor of about 10 to 20 times, as compared with the case where about 10 to 20 runs of irradiation are carried out per one location according to the related art. Furthermore, since the size and position of the crystal grains are little changed even in the case where the irradiated regions partly overlap with each other, the substrate can be irradiated with pulsedly oscillated laser light while scanning in such a range that the irradiated regions partly overlap with each other. For example, crystallinity is little changed even when irradiation with line beams having a longitudinal irradiation region shape is conducted so that the line beams overlap with each other in the major axis direction. Therefore, when the irradiation is conducted so that the line beams partly overlap with each other, a device having a width exceeding the width of the line beam can uniformly be treated to be crystallized.
Now, embodiments of the present invention will be described in detail below, referring to the drawings.
The laser annealing step constituting a characteristic part of the present invention includes first to fourth processes. In the first process, irradiation with the laser light 106 is conducted, whereby an external region (107, 108) of the semiconductor thin film 105 located on the outer side relative to the pattern of the light absorbing layer 103 is thermally melted, and the light absorbing layer 103 is heated, without melting an internal region (109) of the semiconductor thin film 105 located on the inner side relative to the pattern of the light absorbing layer 103. In the subsequent second process, the molten semiconductor thin film 105 is cooled, and microcrystal grains S, P are formed in the external region (107, 108). In the second process, the semiconductor thin film once heated to or above the melting point thereof by the irradiation with the laser light is brought into a supercooled state, and random nucleation upon the supercooling provides seeds for crystallization, so that the crystal grains are fine in diameter.
In the third process shown in
In the fourth process shown in
Preferably, the laser annealing step includes irradiating the substrate 101 with green laser light 106 having a wavelength range of from 520 to 540 nm. In addition, the laser annealing step in some cases includes irradiating the substrate 101 with pulsedly oscillated laser light 106 while scanning in such a range that the irradiation regions overlap with each other. Besides, in the light absorbing layer forming step, the light absorbing layer 103 may be formed by use of a conductive material, and, in the patterning step, the conductive material may be patterned, to produce a wiring including a gate electrode of a thin film transistor, for example. Furthermore, in the light absorbing layer forming step, a high melting point metal or an alloy or silicide containing a high melting point metal as a constituent thereof may be used as the conductive material for forming the light absorbing layer 103.
Continuedly referring to
On the other hand, the pattern of the light absorbing layer 103 formed of a metal or the like is also directly heated by the irradiation with the laser light 106, and the heat is transferred to the thermal buffer layer 102 therebeneath and the insulation film 104 on the upper side. The heat transferred to the insulation film 104 is transferred to the internal region (109) composed of an unmelted amorphous silicon thin film, with a time delay of typically within 10 μs, to melt the amorphous silicon. It should be noted here that, by the time when the melting of the amorphous silicon begins, the first lateral crystal growth has already begun, or, depending on the conditions, has been completed and the polycrystal grains L1 have been formed. Therefore, the amorphous silicon in the internal region (109) is melted in the state of containing a part of the crystal grains L1 formed in the first lateral growth region 107, so that when temperature is lowered due to the subsequent dissipation of heat, the second lateral crystal growth with the unmelted crystal grains L1 as nuclei starts progressing from the outer peripheral portion of the pattern of the light absorbing layer 103 toward the inner side, and the polycrystal grains L2 are grown. The polycrystal grains L2 collide on each other at the center of the second lateral growth region, to form the major grain boundary R. Incidentally, in the case where the width of the pattern of the light absorbing layer 103 is shorter than two times the distance where lateral crystal growth is possible (typically, 1 to 10 μm), the major grain boundary R is not formed, and random nucleation attendant on the lowering in the temperature of the silicon melt occurs in the vicinity of the center in the width direction of the second lateral growth region 109, before the fronts of lateral crystal growth progressing from both sides of the pattern toward the inner side collide on each other. In this case, a microcrystalline region with a crystal grain diameter of 0.1 μm or less is formed along the center of the internal region (109), but there arises no special problem in using only the second lateral growth region 109 for forming a channel region.
As is clear from the foregoing, according to the present invention, the melting of the external region of the semiconductor thin film located on the outside of a gate electrode pattern and the melting of the internal region of the semiconductor thin film located on the inside of the gate electrode pattern can be sequentially performed with a delay time of within 10 μs, by one run of irradiation with laser light. Thus, the generation of a time delay during the process in which the metallic gate electrode is heated by irradiation with laser light and then the heat is transferred to the silicon film with the result of melting of silicon is tactfully utilized. Therefore, the treatment needs only one simple run of uniform irradiation, so that the irradiation apparatus can be simplified, and the throughput is enhanced remarkably.
Incidentally, the melting of the internal region located on the inside of the gate electrode requires a higher laser light energy density (area density), as compared with the melting of silicon in the external region located on the outside of the gate electrode. This is because the metallic gate electrode has a great heat capacity, so that a greater amount of heat is needed accordingly, and because the transfer of heat to the silicon layer is accompanied by dissipation of heat into the glass substrate. Taking this into consideration, green laser light is used in the present invention. The green laser light shows less absorption into a silicon layer, as compared with UV excimer laser light. For example, at room temperature, green laser light incident on a silicon layer is absorbed into the silicon layer in a proportion of only 5 to 10%. With the green laser light thus utilized, the metallic gate electrode can be heated in a high energy density, while the external region on the outside of the gate electrode pattern can be heated in a low energy density. As a result, the first lateral crystal growth and the second lateral crystal growth can be induced sequentially. In consideration of the use of the semiconductor thin film as a thin film transistor, the internal region on the inside of the gate electrode pattern has a high crystal uniformity, so that the internal region can be used for forming a channel region. In addition, polycrystal grains are orderly arrayed in a width of about 2 μm along the outer periphery of the gate electrode pattern. This portion can be used for forming an LDD region of a thin film transistor, which is very convenient on a device design basis.
According to the method of the present invention, the size of polycrystalline silicon grains and the position of the polycrystalline silicon grain boundary can both be controlled according to the metallic wiring pattern such as the gate electrode formed prior to the crystal growth, and, when the region of the polycrystalline silicon grains is used for forming a channel region of a thin film transistor, the characteristics of the transistor and the uniformity thereof are conspicuously enhanced. In addition, it suffices to conduct only one run of irradiation with laser light, which promises an enhancement of treatment rate by a factor of about 10 to 20 times, as compared with the repeated irradiation treatment according to the prior art in which the irradiation is carried out about 10 to 20 times per one location. Furthermore, the crystallinity and thin film transistor characteristics are little changed even where the irradiation is carried out two times instead of once, so that the irradiation treatment can be conducted while scanning in such a manner that the laser light irradiation regions partly overlap with each other. In this case, a semiconductor thin film larger in area than the irradiation region can be crystallized uniformly.
Referring now to
Next, as shown in
Next, the glass substrate 101 is irradiated once with a second harmonic output type laser light 106 pulsedly oscillated from a solid state laser, from the back side through an appropriate irradiation optical system. As the solid state laser, there may be used the second harmonic outputs of pulse oscillation Q switch Nd:YAG laser and Nd:YLF laser. The wavelengths of these harmonic outputs are 532 nm and 527 nm, respectively. The laser diode excitation and flash lamp excitation may be similarly adopted; from the viewpoints of output stability and excitation light source replacement cycle, however, the laser diode excitation is preferred. Examples of the solid state laser which can be used include the Evolution Series (oscillation wavelength: 527 nm) and the CORONA Series (oscillation wavelength: 532 nm), both produced by Coherent, USA. In this embodiment, Evolution 30 by Coherent, USA, was used in the oscillation conditions of a repetition frequency of 1 kHz, a pulse width of about 150 nm, and a pulse energy of 20 mJ. As for the irradiation system, a line form beam processed by a uniformizing optical system composed of a condenser lens, a fly eye lens and the like to uniformize the light intensity distribution in an irradiation spot to within ±5% and then shaped by a shaping optical system composed of a cylindrical lens, a slit and a condenser lens into a shape having a length of 2 mm and a width of 0.3 mm, was used. The energy density was set to within the range of 1 to 2 J/cm2. By scanning with the line form beam in the width direction, a semiconductor thin film having a large area can be crystallized.
By the irradiation with the laser beam, the portion, directly above the gate electrode pattern 103, of the semiconductor thin film 105 is converted into a second lateral growth region 109. On the other hand, the portion, surrounding the outer periphery of the gate electrode pattern 103, of the semiconductor thin film 105 becomes a first lateral growth region 107. The outside portion, beyond the first lateral growth region 107, of the semiconductor thin film 105 becomes an ordinary polycrystalline region 108 composed of microcrystal grains. As has been described above, the growth directions of the first lateral growth region 107 are indicated by arrows A. On the other hand, the growth directions of the second lateral growth region 109 are indicated by arrows B. The directions of transfer of heat for inducing the second lateral crystal growth are indicated by arrows C.
Subsequently, as shown in
Next, an insulating stopper film 110 is formed on the semiconductor thin film 105, which has been crystallized in the preceding step, in the state of being matched to the gate electrode 103. In this case, an SiO2 film is first formed in a thickness of about 100 to 300 nm by plasma CVD. Here, for example, silane gas SiH4 and nitrous oxide N2O are subjected to plasma dissociation, thereby building up the SiO2 film. Then, the SiO2 film is patterned into a predetermined shape, to obtain the stopper film 110. In this case, the stopper film 110 is patterned in such a manner as to achieve self-alignment with the gate electrode 103, by use of a back exposure technique. Incidentally, the portion, located beneath the stopper film 110, of the semiconductor thin film 105 is protected as a channel region 111. As has been described above, B+ ions have preliminarily been implanted into the channel region 111 in a comparatively low dose by the Vth ion implantation.
Subsequently, with the stopper film 110 as a mask, an impurity (P+ ion) is implanted into the semiconductor thin film 105 by ion doping 120, to form LDD regions 112. In this case, for example, the dose is 5×1012 to 1×1013/cm2, and the acceleration voltage is 10 keV. Further, a photoresist (omitted in the figure) is formed and patterned so as to cover the stopper film 110 and the LDD regions 112 on both sides thereof, then, with the photoresist pattern as a mask, an impurity 120 (e.g., P+ ion) is implanted into the semiconductor thin film 105 in a high concentration, to form a source region 105S and a drain region 105D. For example, ion doping 120 (ion shower) can be used for the impurity implantation. This technique resides in implanting the impurity by electric field acceleration, without applying mass separation; for example, the impurity is implanted in a dose of about 1×1015/cm2, to form the source region 105S and the drain region 105D. The acceleration voltage is 10 keV, for example.
Following to the foregoing, the impurities implanted into the semiconductor thin film 105 are activated by RTA (Rapid Thermal Anneal) using a UV lamp. Thereafter, unrequired portions of he semiconductor thin film 105 and the gate insulation film 104 are removed by patterning, to form bottom gate type thin film transistors and to separate the thin film transistors on a device basis.
Thereafter, as shown in
In the above-mentioned manner, a thin film semiconductor device having the thin film transistor provided on the insulating substrate 101 is completed. As has been described above, the thin film transistor includes the semiconductor thin film 105 and the gate electrode 103 laminated, with the gate insulation film 104 therebetween. The semiconductor thin film 105 has the channel region 111 overlapping with the gate electrode 103, and the source region 105S and the drain region 105D which are located respectively on both sides of the channel region 111. The semiconductor thin film 105 is a polycrystalline layer crystallized by laser annealing, and is divided along the boundary of a predetermined pattern into the internal region and the external region (
The semiconductor thin film 105 is a polycrystalline layer polycrystallized by the laser annealing conducted by irradiation with the laser light 106 through the light absorbing layer formed in the predetermined pattern. As shown in
Now, referring to
Subsequently, the semiconductor thin film 105 is patterned into an island-like shape. On the semiconductor thin film 105 thus patterned, SiO2 is grown to a thickness of 10 to 400 nm (here, for example, 100 nm) by plasma CVD, normal pressure CVD, reduced pressure CVD, ECR-CVD, sputtering or the like, to form a gate insulation film 104.
Next, a film of a high melting point metal such as Ti, Mo, W, Ta, etc. or an alloy thereof is formed in a thickness of 100 to 800 nm on the gate insulation film 104, and is patterned into a predetermined shape, to form a gate electrode 103. The portion, located beneath the gate electrode 103, of the semiconductor thin film 105 is a portion which will later be a channel region. As has been described above, B+ ions have been preliminarily implanted into this portion in a comparatively low dose by the Vth ion implantation.
Subsequently, as shown in
Subsequently, as shown in
Thereafter, the dopant implanted into the polycrystalline silicon semiconductor thin film 105 is activated. The activating treatment can be conducted by RTA (Rapid Thermal Anneal) using a UV lamp, in the same manner as in manufacturing the bottom gate type thin film transistor.
Thereafter, as shown in
As a result, a top gate type thin film transistor is completed. The thin film transistor has the channel region 111 formed in the second lateral growth region 109. On the other hand, the source region 105S and the drain region 105D are formed in the first lateral growth region 107. In addition, the LDD regions 112 are formed in the first lateral growth region 107 or the second lateral growth region 109. Incidentally, in the case of the top gate type thin film transistor, the upper side of the semiconductor thin film is closed with the metallic gate electrode, so that the release path for the hydrogen gas generated attendant on the melting of silicon is smaller, as compared with the case of the bottom gate type thin film transistor. Therefore, it is important for the dehydrogenating treatment of the semiconductor thin film to be preliminarily carried out with special care.
Finally,
On the other hand, the TFT is produced according to the present invention, and is composed of a gate electrode 103 formed on a substrate 101 composed of a glass or the like, a gate insulation film 104 laminated thereon, and a semiconductor thin film 105 formed on the upper side of the gate electrode 103, with the gate insulation film 104 therebetween. The semiconductor thin film 105 is composed of a thin film of polycrystalline silicon laterally grown according to the present invention. The thin film transistor TFT includes a source S, a channel Ch and a drain D, which constitute a path for a current supplied to the OLED. The channel Ch is located just above the gate electrode 103. The TFT in this bottom gate structure is covered with a layer insulation film 116, on which are formed a source electrode 113S and a drain electrode 113D. On these electrodes is formed the above-mentioned OLED, with another layer insulation film 114 therebetween. A contact hole is opened in the layer insulation film 114, and the transparent electrode 130 of the OLED is electrically connected to the drain electrode 113D of the TFT through the contact hole. Incidentally, while each pixel is composed of the organic electroluminescence device OLED in this embodiment, this is not limitative. For example, the pixel can be composed of a pixel electrode connected to a thin film transistor TFT, a counter electrode opposed thereto, and a liquid crystal held between the electrodes.
It should be understood by those skilled in the art that various modifications, combinations, sub-combinations and alterations may occur depending on design requirements and other factors insofar as they are within the scope of the appended claims or the equivalents thereof.
Number | Date | Country | Kind |
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P2005-049716 | Feb 2005 | JP | national |