In a method of forming a polycrystalline silicon film in a process of manufacturing an LCD, a hydrogenated amorphous silicon film is formed on a glass substrate by plasam CVD throughout areas serving as the pixel portion and driver unit of the LCD. A laser beam is radiated on a selected region of the film on the area serving as the driver unit. The energy of the laser beam is set such that hydrogen in the film is discharged without crystallizing the film and damaging the film. The energy of the laser beam is gradually increased to gradually discharge hydrogen from the film. The energy of the laser beam is finally set such that the film is transformed into a polycrystalline silicon film. The amorphous silicon film can be poly-crystallized without damaging the film by the discharge of hydrogen.
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1. A method of forming a polycrystalline silicon film for the manufacture of a liquid crystal display (LCD) having a pixel portion and a driver unit, comprising:
(a) forming a hydrogenated amorphous silicon film (α a-Si:H film) on a surface of a glass substrate in areas of said substrate corresponding to said pixel portion and said driver unit, (b) determining a minimum energy density of a laser beam which, when irradiated on the surface of said α a-Si:H film causes hydrogen therein to explosively discharge from said α a-Si:H film, which energy density value is termed a ceiling value, (c) repeatedly irradiating said α a-Si:H film corresponding to said driver unit with a laser beam having an energy density value below said ceiling value, measuring the amount of hydrogen released after each said irradiation, and increasing the energy density of said repeated laser beam irradiations whenever consecutive irradiations give a measured amount of hydrogen released which decreases after said consecutive irradiations, and (d) crystallizing said repeatedly irradiated α a-Si:H film corresponding to said driver unit by irradiation with a laser beam having an energy density above said ceiling value and sufficient to cause silicon in said repeatedly irradiated α a-Si:H film to crystallize into a the polycrystalline silicon film.
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7. A method according to
8. A method according to
9. A method according to
10. A method according to
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12. A method according to
radiating a test light on said repeatedly irradiated film; spectroscopically detecting a reflected light of the test light from said repeatedly irradiated film to obtain detection data concerning a band gap spectroscopic reflectance distribution of said repeatedly irradiated film and comparing reference data concerning a band gap spectroscopic reflectance distribution of a polysilicon film and responding to the detection data with the detection data to evaluate a crystallized state of said repeatedly irradiated film to determine whether said irradiated film changes to a crystallized state polysilicon film; and stopping the irradiation of the laser beam onto the film, if the amorphous silicon film changes to the crystallized state polysilicon film, and continuing the irradiation of the film if the amorphous silicon film does not change to the crystallized polysilicon film.
13. A method according to
14. A method according to
15. A method according to
16. A method for forming a polycrystalline silicon film according to
heating the repeatedly irradiated amorphous silicon film so that said amorphous silicon film changes to the polycrystalline silicon film; radiating a test light onto the film during or after the heating of said repeatedly irradiated amorphous silicon film; spectroscopically detecting a reflected light of the test light from said heated silicon film to obtain detection data concerning band gap spectroscopic reflectance distribution of said heated silicon film; and comparing reference data concerning band gap spectroscopic reflectance distribution of a polycrystalline sample silicon film, having a reference level of crystallinity, with the detection data to evaluate a crystallized state of the heated silicon film to detect whether the crystallized state of the silicon film reaches the reference level; and stopping the heating of the heated silicon film, if the crystallized state of the heated silicon film reaches the reference level, and continuing the heating of the heated silicon film, if the crystallized state of the film does not reach the reference level.
17. A method according to
spectroscopic reflectance distribution. 19. A method for forming a polycrystalline silicon film according to claim 1 further comprising determining crystallinity of the repeatedly irradiated amorphous silicon film by steps of: heating the repeatedly irradiated amorphous silicon film so that said amorphous silicon film changes to the polycrystalline silicon film; radiating a test light onto the silicon film during the heating of the repeatedly irradiated amorphous silicon film, spectroscopically detecting a reflected light of the test light from said heated silicon film to obtain detection data concerning band gap spectroscopic reflectance distribution of said heated silicon film, comparing reference data concerning band gap spectroscopic reflectance distribution of a polycrystalline silicon sample film, having a reference level of crystallinity, with the detection data to evaluate the crystallized state of the heated silicon film to detect whether the crystallized state of the heated silicon film reaches the reference level, stopping the heating of the film, if the crystallized state of the heated silicon film reaches the reference level, and continuing the heating of the heated silicon film, if the crystallized state of the film does not reach the reference level. 20. A method according to claim 19, wherein said heating includes a step of irradiating a laser beam onto the repeatedly irradiated amorphous silicon film, while adjusting an energy of said laser beam according to the crystallized state as evaluated in the comparing step. 21. A method according to claim 20, wherein the energy of said laser beam is gradually increased until the crystallized state of the repeatedly irradiated amorphous silicon film reaches said reference level. |
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1. Field of the Invention
The present invention relates to a method of forming a polycrystalline silicon (i.e., polysilicon) film in a process of manufacturing an LCD (Liquid Crystal Display).
2. Description of the Related Art
An LCD using a TFT (Thin-Film Transistor) has received a great deal of attention because the LCD provides very excellent picture quality.
An LCD substrate used in the LCD is schematically shown in FIG. 1. A large number of pixel units U each of which is obtained by combining an TFT 102 to a pixel electrode 103 connected to the drain of the TFT 102 are arranged on a glass substrate 104. For example, several hundred thousands square pixel units U whose side has a length of about several hundreds μm are arranged. A transparent electrode 105 commonly used for the pixel units U is formed to oppose the pixel electrode 103 such that a liquid crystal 106 is formed between the pixel electrodes 103 and the transparent electrode 105, thereby forming a pixel portion 100 as shown in FIG. 2.
A large number of packaged IC chips 107 are arranged on the glass substrate 104 along the peripheral edge of the pixel portion 100. A driver unit 101 is formed by the IC chips 107. These IC chips are independently formed and then adhered to the glass substrate 104. The terminals of each of the IC chips 107 are connected to a source bus and a gate bus connected to each of the pixel units U of the pixel portion 100. For example, the number of gate buses and the number of source buses may reach 400 to 1,920. For this reason, a large number of wiring steps are required to connect the IC chips 107 to the pixel units. This is a factor of increasing the cost of an LCD.
The TFT of each pixel unit does not require its high-speed operation because the TFT causes the pixel of the pixel unit to be displayed as an image. For this reason, an amorphous silicon layer can be used as a semiconductor layer for the TFT. However, each transistor of the driver unit must have an operation speed considerably higher than that of the TFT because a circuit requiring a high-speed switching operation must be mounted on the driver unit. Therefore, a polysilicon film having a field-effect mobility higher than that of an amorphous silicon layer must be used as the semiconductor layer of the driver unit.
The film formation process must be performed at a temperature of about 600°C or more by, e.g., low-pressure CVD (LPCVD) to obtain a polysilicon layer. However, an inexpensive glass substrate has a thermal strain point of about 600°C A glass substrate which can withstand a high temperature of about 600°C is expensive.
Under the above circumstances, a common semiconductor layer which is used for constituting a driver unit, a pixel portion, and a wiring layer cannot be formed on the same glass substrate at the same time. Therefore, a cumbersome and costly operation of adhering IC chips for a driver unit to a glass substrate is inevitable at present.
It is, therefore, an object of the present invention to simplify the steps in a process of manufacturing an LCD and, more specifically, to form a polysilicon film at least for a driver unit using an amorphous silicon film commonly formed for the driver unit, a pixel portion, and a wiring layer.
According to the present invention, there is provided a method of forming a polycrystalline silicon film in a process of manufacturing an LCD having a pixel portion and a driver unit, comprising:
the step of preparing a glass substrate serving as a substrate of the LCD;
the step of forming a hydrogenated amorphous silicon film on the glass substrate throughout areas serving as the pixel portion and the driver unit;
the hydrogen discharging step of radiating a laser beam having a hydrogen discharging energy on a selected region of the film at least in the area serving as the driver unit, the hydrogen discharging energy being set such that hydrogen in the film is discharged without crystallizing the film and damaging the film; and
the crystallizing step of radiating a laser beam having a crystallizing energy on the selected region, the crystallizing energy being set to be higher than the hydrogen discharging energy such that the film is transformed into a polycrystalline silicon film.
More specifically, a hydrogenated amorphous silicon (a-Si:H) film having a large area is formed on a glass substrate by plasma CVD in an atmosphere of, e.g., about 300°C A laser beam is radiated on the amorphous silicon film of a driver unit and a pixel portion, if desired, to locally heat the amorphous silicon film to a surface temperature of about 1,000°C to 1,414°C In this manner, the amorphous silicon film is melted and poly-crystallized to form a polysilicon film for the driver unit.
A heating temperature in the step of forming an amorphous silicon film is lower than that of a polysilicon film. Annealing performed by a laser beam, i.e., laser annealing instantaneously heats the amorphous silicon film to poly-crystallize the amorphous silicon film, and the glass substrate is not heated to a high temperature accordingly. Therefore, the glass substrate does not require a high heat resistance, and an inexpensive material can be used as the glass substrate, so that a large-area transparent liquid crystal display can be manufactured.
An a-Si:H film formed by plasma CVD contains a considerably large amount of hydrogen. For this reason, when an energy required for poly-crystallizing the a-Si:H film is given to the a-Si:H film by using a laser beam, hydrogen is discharged from the film at once to degrade the film. Therefore, according to the present invention, the radiation energy of the laser beam is gradually increased to gradually discharge hydrogen frownwhen When the laser beam is radiated on the a-Si:H film, at the beginning, the output energy of the laser beam is set to be a lower energy than an energy required for polycrystallizing the a-Si:H film. The laser beam having the constant low energy, e.g., 160 mJ (a beam size is 0.9 cm×0.9 cm, and the transmittance of all the optical systems is 70%, thereby setting the energy density of the film surface to be 138 mJ/cm2) scans the a-Si:H film a plurality of times.
An amount of hydrogen is monitored by the mass spectrometer. After the amount of hydrogen is almost equal to the amount of the hydrogen in the immediately preceding scanning operation, the output energy is slightly increased to, e.g., 200 mJ (energy density: 173 mJ/cm2. The laser beam having the energy is radiated on the film several times to scan the film, and similarly, an amount of hydrogen is monitored. In addition, the energy is further increased to, e.g., 240 mJ (energy density: 207 mJ/cm2), and the same process as described above is performed. In this manner, the energy is gradually increased, and the above process is repeated, thereby gradually discharging hydrogen from the a-Si:H film. A laser beam having an energy enough to poly-crystallize the a-Si:H film is radiated on the a-Si:H film, and the a-Si:H film is transformed into a polysilicon film. In this case, an aperture for the laser beam may be regulated without changing the output energy of the laser beam to change the irradiation energy (energy per unit area of a surface to be processed) of the laser beam.
FIG. 6 is a schematic view showing the state of the above laser annealing. In FIG. 6, reference symbol 81 denotes a glass substrate; 82, an a-Si:H film for forming TFTs of a pixel portion; and 83, an a-Si:H film for forming a driver unit.
According to the above method, when a laser beam having a low energy is radiated on the a-Si:H film, an amount of hydrogen proportional to the energy is discharged. When a laser beam having the same energy is radiated on the a-Si:H film several times to scan the a-Si:H film, an amount of hydrogen proportional to the energy is gradually decreased in accordance with the number of times of scanning, and almost all hydrogen is discharged. The energy of the laser beam is slightly higher than the previous irradiation energy, and the same process as described above is performed. At this time, an amount of hydrogen proportional to the high energy is gradually generated in accordance with the number of times of scanning irradiation. In this manner, when the irradiation energy of the laser beam is increased, hydrogen in the a-Si:H film is sequentially discharged in accordance with a change in energy.
Hydrogen in the a-Si:H film is discharged stepwise, and irradiation is shifted to irradiation having a high energy while an amount of hydrogen is monitored, thereby substantially preventing the film from being damaged. Almost all hydrogen which the a-Si:H film contains is discharged, and the hydrogen content of the a-Si:H film is small when a high energy is applied to the a-Si:H film to poly-crystallize the a-Si:H film. For this reason, even when the remaining hydrogen is discharged at once, the film is not damaged. In contrast to this, when a laser beam having an energy enough to poly-crystallize the a-Si:H film is radiated on the a-Si:H film from the beginning, hydrogen contained in the a-Si:H film is discharged at once to be exploded. For this reason, the abrupt hydrogen jet damages the film.
An amount of hydrogen smaller than a predetermined amount is generated even when the irradiation energy of the laser beam is increased. In this state, the step of radiating the laser beam having an energy required for poly-crystallizing the a-Si:H film is performed for the first time.
A method of setting the output energy of the laser beam and the number of times of scanning irradiation may be set on the basis of the result obtained as follows. For example, irradiation having various patterns is performed to each of various types of objects to be processed in advance, and an amount of discharged hydrogen is detected by the mass spectrograph 8. In other words, when the values of an energy of the laser beam for discharging hydrogen for the first time, an intermediate energy of the laser beam for discharging hydrogen, and an energy of the laser beam for crystallizing the film are set in advance by performing experiments such as experiments (will be described later) to a sample having a condition similar to that of an actual object to be processed, the present invention can be performed without monitoring an amount of discharged hydrogen. Note that a measuring means other than a mass spectrograph may be used to detect an amount of hydrogen gas.
The polysilicon film is formed as described above, and the pressure in the vacuum chamber 4 is returned to an atmospheric pressure. The gate valve G is opened, and the substrate 5 is unloaded from the vacuum chamber 4 by a convey mechanism (not shown). A film formation process is performed to the substrate in a semiconductor processing station including a film form processing station or a lithographic station. In this film formation process, masks having different predetermined patterns are independently used in a pixel portion area and a driver unit area of an LCD substrate on the same substrate, and TFTs each constituting a part of a pixel unit and switching elements of the driver unit are simultaneously formed. At the same time, in this process, an electrode wiring layer for connecting the pixel portion to the driver unit is formed.
In the apparatus shown in FIG. 3, the reflecting member 10 is arranged outside the vacuum chamber 4 below the vacuum chamber 4, and the surface to be processed of the substrate faces downward such that a laser beam is radiated upward on the surface. For this reason, the moving mechanism may be fixed on the support plate 2 without being suspended, and the moving mechanism can be stably moved, so that the accuracy of the movement path of the reflecting member 10 can be kept high.
The support plate 2 can be horizontally maintained under the pneumatic control, and the vacuum chamber 4 is supported on the support plate 2. For this reason, both the movement path and the LCD substrate 5 can be horizontally maintained at high accuracy. Therefore, scanning irradiation of a laser beam can be performed at high accuracy. As the support plate 2, any support plate having a structure which does not transmit external vibrations even when the support plate is not horizontally controlled by an air pressure or the like may be used.
In laser annealing to an a-Si:H film, various irradiation modes of the laser beam were used, and experiments of detecting an amount of hydrogen discharged from the a-Si:H film and of observing the state of the a-Si:H film were performed. A sample obtained by formed an a-Si:H film having a thickness of 1,000 Å on a glass substrate by plasma CVD was prepared. This sample was placed in the vacuum chamber 4 of the apparatus shown in FIG. 3. The pressure in the vacuum chamber 4 was set to be 2.5×10-7 Torr. The temperature of the susceptor 18 was set such that the temperature of the sample was set at 300°C The distance between the sample and the biprism lens 25 was set to be 340 mm when a laser beam had a beam size of 0.9 cm×0.9 cm, and the distance was set to be 230 mm when the laser beam had a beam size of 0.65 cm×0.65 cm.
As described above, an excimer laser beam was oscillated like a pulse, and the period of the beam was 10 Hz. Scanning was performed such that the laser beam was shifted by an interval of 1.25 mm every pulse. Therefore, when the laser beam having a beam size of 0.9 cm×0.9 cm was used, the a-Si:H film was irradiated with the laser beam corresponding to about 7.2 pulses per scanning operation. When a laser beam having a beam size of 0.65 cm×0.65 cm was used, the a-Si:H film was irradiated with the laser beam corresponding to about 5.2 pulses per scanning operation. In addition, the transmittance of the entire optical system through which the laser beam passes was 70%.
As shown in FIG. 7, the a-Si:H film was divided into five areas A to E. A laser beam having a beam size of 0.9 cm×0.9 cm and an output energy of 120 mJ was repeatedly radiated on all the areas predetermined times. At this time, the energy density of the laser beam per pulse on the film surface was about 104 mJ/cm2. A relationship between an output energy, a repetition count, and an amount of discharged hydrogen is shown in FIG. 8. In FIG. 8, output values corresponding to amounts of discharged hydrogen (H2) in the mass spectrometer are plotted along the ordinate. Each of the areas was divided into three regions of each area, and the same processing as described above was performed to the three regions, and an average of output values obtained by performing the processing three times was calculated. Assuming that a process of performing scanning irradiation from one end of each area to the other end is called one scanning operation, the repetition count means the number of times of scanning in the same area. In this experiment, any damage was not detected in the a-Si:H film. It was understood that a variation in output value of the areas was caused by experimental errors.
After Experiment 1, a laser beam having a beam size Of 0.9 cm×0.9 cm was repeatedly radiated on the areas A to E with output energies of 160 mJ, 200 mJ, 240 mJ, 280 mJ, and 340 mJ predetermined times, respectively. At this time, energy densities of the laser beam per pulse on the film surface were about 138 mJ/cm2, 173 mJ/cm2, 207 mJ/cm2, 242 mJ/cm2, and 294 mJ/cm2, respectively. Relationships between the output energies, repetition counts, and amounts of discharged hydrogen are shown in FIG. 9. In this experiment, any damage was not detected in the a-Si:H film.
A laser beam having a beam size of 0.9 cm×0.9 cm was repeatedly radiated on all the areas with an output energy being increased in an order of 120 mJ, 160 mJ, 220 mJ, 280 mJ, 340 mJ, and 450 mJ four times without distinguishing the areas from each other. At this time, energy densities per pulse of the laser beam having the output energies on the film surface were about 104 mJ/cm2, 138 mJ/cm2, 190 mJ/cm2, 242 mJ/cm2, 294 mJ/cm2, and 389 mJ/cm2, respectively. The result is shown in FIG. 10. In this experiment, any damage was not detected in the a-Si:H film.
A laser beam having a beam size of 0.9 cm×0.9 cm was repeatedly radiated on the areas A to E with outputs energies of 110 mJ, 160 mJ, 200 mJ, 240 mJ, and 280 mJ predetermined times, respectively. At this time, energy densities of the laser beam per one pulse on the film surface were about 95 mJ/cm2, 138 mJ/cm2, 173 mJ/cm2, 207 mJ/cm2, and 242 mJ/cm2, respectively. The result is shown in FIG. 11. In this experiment, damage to the film was detected in an area on which the laser beam having an output energy of 200 mJ (energy density: 173 mJ/cm2) or more was radiated.
A laser beam having a beam size of 0.9 cm×0.9 cm was repeatedly radiated on all the areas with an output energy being increased in an order of 120 mJ, 160 mJ, 340 mJ, and 450 mJ predetermined times without distinguishing the areas from each other. At this time, energy densities per pulse of the laser beam having the output energies on the film surface were about 104 mJ/cm2, 138 mJ/cm2, 294 mJ/cm2, and 389 mJ/cm2, respectively. The result is shown in FIG. 12. In this experiment, when a laser beam having an output energy of 340 mJ (energy density: 294 mJ/cm2) or less was radiated on the film, any damage was not detected in the film. However, when a laser beam having an output energy of 450 mJ (energy density: 389 mJ/cm2) was radiated on the film, damage to the film was detected.
A laser beam a beam size of 0.9 cm×0.9 cm was repeatedly radiated on all the areas with an output energy being gradually increased in an order of 120 mJ and 450 mJ predetermined times without distinguishing the areas from each other. At this time, energy densities per pulse of the laser beam having the output energies on the film surface were about 104 mJ/cm2 and 389 mJ/cm2, respectively. The result is shown in FIG. 13. In this experiment, when the laser beam having the output energy of 450 mJ (energy density: 389 mJ/cm2) was radiated on the film, damage to the film was detected.
A laser beam having a beam size of 0.65 cm×0.65 cm was radiated on all the areas once with an output energy being gradually increased from 120 mJ to 480 mJ, as shown in FIG. 14, without distinguishing the areas from each other. The result is shown in FIG. 14. In this experiment, any damage was not detected in the a-Si:H film. The a-Si:H film was poly-crystallized by radiating the laser beam having the output energy of 480 mJ on the a-Si:H film. This was confirmed by an X-ray analyzer.
When the output energies of 120 mJ and 480 mJ were used, energy densities per pulse of the laser beam on the film surface were about 199 mJ/cm2 and 795 mJ/cm2, respectively. In addition, since the light absorbance of the a-Si:H film at a wavelength of 248 nm was 30%, the absorption energy densities of the a-Si:H film at the output energies of 120 mJ and 480 mJ were 60 mJ/cm2 and 239 mJ/cm2, respectively.
An a-Si:H film was divided into two areas. A laser beam having a beam size of 0.65 cm×0.65 cm was radiated on one area with an output energy being gradually increased in an order of 120 mJ, 220 mJ, 300 mJ, 400 mJ, and 480 mJ once. A laser beam having a beam size of 0.65 cm×0.65 cm was radiated on the other area with an output energy being gradually increased in an order of 160 mJ, 280 mJ, 380 mJ, and 480 mJ once. The result is shown in FIG. 15. In this experiment, damage to all the films was detected. At each hatched point in FIG. 15, an output value of hydrogen exceeded 25.
Under the same conditions as those in Experiment the temperature of the substrate 5 was set to be 25°C and 300°C through the susceptor 18 to poly-crystallize the a-Si:H film. When the temperature of the substrate 5 was 25°C, an average crystal grain size was about 100 nm. When the temperature of the substrate 5 was 300°C, an average crystal grain size was six times of the above average crystal grain size, i.e., about 600 nm.
According to the above results, when a laser beam having a high energy is radiated on the a-Si:H film from the beginning, hydrogen in the a-Si:H film is discharged at once to damage the film. Although a laser beam having a low energy is radiated on the a-Si:H film from the beginning, when a laser beam having a high energy is then radiated on the a-Si:H film at once, the film is damaged as described above. However, the following fact will be understood. That is, a laser beam having a low energy is radiated on the a-Si:H film from the beginning, and the energy is gradually increased, thereby preventing the film from being damaged. This leads to the following analysis result surmised by the following reason. When the irradiation energy of a laser beam is gradually increased, hydrogen in the film is gradually discharged, and a shock caused by the discharge is small, such that the film is not damaged. Although a method of forming a polysilicon film while an amount of hydrogen is monitored had been described in the above embodiment, when required data are obtained in advance, the polysilicon film can be formed without monitoring the amount of hydrogen. For example, when a relationship between a laser beam intensity, an irradiation count, and an amount of discharged hydrogen for each of substrates having the same thin film and the same size is obtained in advance, the relationship can be used as data in place of data obtained by monitoring an amount of discharged hydrogen.
A method of laser-annealing the amorphous area of an object to be processed and evaluating the crystallized state of the area by using the apparatus shown in FIGS. 3 and 5 will be described below. In this case, as in the above embodiment, a polysilicon film is formed on the surface of a glass substrate using a hydrogenated amorphous silicon (a-Si:H) film manufactured by plasma CVD. However, when the problem of the heat resistance of the substrate 5 is solved, a polysilicon film can be formed by using an amorphous silicon film manufactured by LPCVD. Laser annealing in which a polysilicon film is formed while the crystallized state is evaluated can be applied to a case of using the above LPCVD silicon film and a case of using a semiconductor film consisting of a material other than silicon.
The method of this embodiment will be described below with reference to a flow chart shown in FIG. 16.
In step S1, the laser power source 21 is turned on according to a command from the CPU 20 in which a control program on the basis of the present invention is incorporated. A laser beam is transmitted from the excimer laser source 22 to the reflecting member 10 through the homogenizer 23. The laser beam is directed toward a desired area on a surface to be processed of the substrate 5. When the moving mechanism 11 is appropriately driven, the laser is radiated to scan the amorphous silicon film in the desired area.
In step S2, the substrate 5 is irradiated with a beam from the light source 17 (FIG. 5) having a light intensity which is uniform within the range of 200 nm to 500 nm. A reflected beam from the desired amorphous silicon area is focused on the spectroscope 16 by the optical system (not shown) to be spectroscopically detected.
In step S3, a band gap spectroscopic reflectance distribution obtained by the reflected beam in the above area is compared with a prestored band gap spectroscopic reflectance distribution concerning a reference semiconductor crystal material. As will be described later, is known that a sample having a desired semiconductor crystal state represents a spectroscopic reflectance distribution which is almost fixed. Therefore, a reference spectroscopic reflectance distribution is compared with the detected spectroscopic reflectance distribution of the observed portion. By using a degree of approximation of the distributions, the crystallized state of the observed portion, i.e., the progress of the laser annealing can be determined.
As the result of the comparison, when it is determined that the crystallized state of the observed portion does not reach a reference level, the CPU 20 transmits a command signal for increasing a laser irradiation energy to the system, and the laser irradiation energy is adjusted in step S4. Note that it is preferable that the laser irradiation energy is gradually increased in a normal state because of the following reasons. That is, as described above, when an excessive laser irradiation energy is applied to the film at once, hydrogen in an amorphous silicon film containing an excessive amount of hydrogen and manufactured by plasma CVD is sprayed at once, so that the silicon film may be damaged.
As a method of adjusting a laser irradiation energy, a method of changing an output from the excimer laser source 22, a method of changing a laser irradiation interval in spot irradiation, or a method of adjusting the moving speed of the moving mechanism 11 for driving the reflecting member 10 on the X-Y plane is known. When each of these methods is independently used, or these methods are combined and used, the laser irradiation energy can be adjusted to a desired value.
A sequence of laser irradiation (S1), spectroscopic detection (S2), and crystallized state evaluation (S3) is continuously repeated in accordance with a command from step S4 until the crystallized state of the observed portion, i.e., a portion to be processed reaches a reference level. When it is determined in step S3 that the crystallized state of the portion to be processed reaches the reference level, the flow advances to step S5. The moving mechanism 11 is driven, and the laser beam is radiated to scan the next irradiation area. In this manner, the sequence from steps S1 to S5 is repeated until it is determined in step S6 that laser annealing to all the areas to be processed is finished.
As described above, according to a method of forming a polysilicon thin film using a method of evaluating a semiconductor crystal state according to the present invention, a crystallized state is determined by a spectroscopic reflectance distribution typically conspicuously representing the characteristics crystallized state of the semiconductor without using an expensive apparatus such as a Raman spectroscope, for a special purpose. On the basis of this determination, a laser irradiation energy can be feedback-controlled in real time. For this reason, laser annealing can easily be performed at a low cost. In addition, TFT liquid crystal displays can be manufactured at a high yield and throughput.
A laser reflectance distribution of a semiconductor band gap which serves as a reference used for performing the method according to the present invention will be described below. The energy band of a silicon crystal, as is known well, has the structure shown in FIG. 17. This band gad is about 3.43 eV at the Γ point and is about 4.40 eV at the X point. A laser beam having a beam size of, e.g., 0.65 (cm)×0.65 (cm)=0.43 (cm2) and an laser energy of, e.g., 400 mJ is radiated on a reference semiconductor crystal through a transparent window having an optical transmittance of 75% under the condition that the reference semiconductor crystal has the above band gap structure and a film thickness of 500 Å.
A band gap spectroscopic reflectance distribution obtained when a laser having the above conditions is radiated on the reference semiconductor crystal is shown in FIG. 18. As shown in FIG. 18, the band gap spectroscopic reflectance distribution has two peak values near 284 nm and 364 nm. These peak values correspond to the X and Γ points of particular points in the first Brillouin zone of the silicon crystal, respectively.
The band gap spectroscopic reflectance distribution of amorphous silicon is shown in FIG. 19 as a further reference. It is known that, as shown in FIG. 19, the band gap spectroscopic reflectance distribution of the amorphous silicon has a distribution having no peak and representing a characteristic curve inclined downward the right.
As described above, as is easily understood in comparing FIG. 18 with FIG. 19, the outline shape of the band gap spectroscopic reflectance distribution of the reference semiconductor crystal is a unique shape. The first information concerning the band gap spectroscopic reflectance distribution is stored as reference information in advance, and the first information is compared with the second information concerning a band gap spectroscopic reflectance distribution obtained in real time during annealing of an object to be processed, so that the crystallized state of the object can be known in real time.
For example, when a laser irradiation energy transmitted by the laser source 22 is not enough to crystallize the object, e.g., 200 mJ, the band gap spectroscopic reflectance distribution detected from a reflected beam from the object, as shown in FIG. 20, has a curve inclined downward to the right. In contrast to this, when a laser irradiation energy transmitted from the laser source 22 has a value excessively large to crystallize a semiconductor, e.g., 600 mJ, the band gap spectroscopic reflectance distribution detected from the reflected beam from the object, as shown in FIG. 21, has a characteristics curve representing that the spectroscopic reflectance distribution has an outline shifted downward due to damage to the entire film. It is understood that this phenomenon is obtained by forming a silicon oxide film on the surface of the object.
When the band gap spectroscopic reflectance distribution shown in FIG. 20 is spectroscopically detected, the system can be feedback-operated in real time so that the laser irradiation energy is gradually increased to cause the spectroscopic reflectance distribution in FIG. 20 to be close to the spectroscopic reflectance distribution in FIG. 18. In this manner, the laser irradiation energy is preferably controlled before the film damage shown in FIG. 21. In addition, if the band gap spectroscopic reflectance distribution shown in FIG. 21 is spectroscopically detected, the sample can be picked as a defective one.
As described above, a laser irradiation energy is gradually increased such that the distribution in FIG. 20 is close to the distribution in FIG. 18. As described above, when an excessive laser irradiation energy is applied from the beginning, hydrogen contained in an amorphous silicon is sprayed at once, and the silicon film may be damaged, thereby detecting the sample as a defective one.
Since the reference reflectance distribution does not completely coincide with the reflectance distribution of an object to be processed due to the characteristics of the method of analyzing these distributions, this comparison is performed by a method of finding a degree of approximation between these distributions while allowing errors to some extent. For example, when the peak values at the X point (about 284 nm) and the Γ point (about 364 nm) are compared with each other, an error of ±20 nm can be allowed. In addition, the outline shapes of the spectroscopic reflection distributions are traced and processed, and the obtained data are compared with each other with a certain allowance range, so that the crystallized state of the object to be processed can be evaluated.
Additional advantages and modifications will readily occur to those skilled in the art. Therefore, the invention in its broader aspects is not limited to the specific details, and illustrated examples shown and described herein. Accordingly, various modifications may be made without departing from the spirit or scope of the general inventive concept as defined by the appended claims and their equivalents.
Hata, Jiro, Imahashi, Issei, Hama, Kiichi
| Patent | Priority | Assignee | Title |
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