JP2000036606A - Thin film insulated gate semiconductor device - Google Patents

Abstract

PROBLEM TO BE SOLVED: To simplify a process by forming one silicon film, and reforming it in such a manner that a certain part is of a source/drain region and another certain part is of a channel forming region. SOLUTION: A substrate is cleaned, and a tantalum film is formed. With a mask used the film is patterned, and etched, and then an anodized film 103 is formed. A resist is removed, and a silicon nitride film 104 is formed. After the substrate is cleaned, an amorphous silicon film is formed, and patterned with a mask. Then, the amorphous silicon film is etched to form a semiconductor region 105. The retained resist is removed. The substrate is cleaned, a silicon nitride film is formed. Then, a silicon nitride mask 106 is patterned with a mask, then etched, phosphorus ion is implanted to form an impurity region 108. Then the substrate is cleaned, and the resist is removed. The mask 106 is etched by laser annealing, then cleaned to form an aluminum film, and etched to form aluminum wiring 110. Then, an NTFT can be manufactured.

Description

DETAILED DESCRIPTION OF THE INVENTION

[0001]

BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a MIS (Metal-Insu
The present invention relates to a metal-insulator-semiconductor type semiconductor device, particularly to a MIS transistor. In particular, the present invention relates to a MIS type semiconductor device and a thin film transistor (TFT) on a thin film formed on an insulating substrate, and particularly has a so-called inverted stagger type structure in which a channel formation region is located above a gate electrode. The present invention relates to a MIS type semiconductor device. The fields where the present invention can be used include:
It is a semiconductor integrated circuit formed on an insulating substrate, for example, an active matrix circuit used for a liquid crystal display device, a driving circuit of an image sensor, and the like.

[0002]

2. Description of the Related Art In recent years, a device in which a thin-film MIS type semiconductor device is formed on an insulating substrate is sometimes used. For example, it is an active matrix type liquid crystal display device. Currently, commercially available active matrix type circuits include T
There are ones using FT and ones using diodes such as MIM. In particular, the former has been actively manufactured in recent years because high-quality images can be obtained.

An active matrix circuit using a TFT is a TF using a polycrystalline semiconductor such as polycrystalline silicon.
A TFT utilizing T and an amorphous semiconductor such as amorphous silicon is known. The latter is difficult to produce on a large screen due to problems in the production process. For the large screen, the latter which can be produced at a process temperature of 350 ° C. or less is mainly used.

FIG. 2 shows a conventional amorphous silicon TF.
The production process of T (inverted stagger type) is shown. As the substrate 201, heat-resistant non-alkali glass such as Corning 7059 is used. Since the maximum temperature of the amorphous silicon TFT process is about 350 ° C., a material that can withstand this temperature is required. In particular, when used as a liquid crystal display panel, heat resistance and high glass transition temperature that do not cause distortion due to heat treatment are required. In the case of Corning 7059, this condition is satisfied because the glass transition temperature is slightly less than 600 ° C.

Further, in order to stabilize the operation of the TFT, it is not desirable that mobile ions such as sodium are contained in the substrate. Corning 7059 has no problem because the alkali concentration is sufficiently low. However, if the substrate contains a large amount of sodium or the like, silicon nitride, oxidized silicon oxide, etc. are used to prevent mobile ions in the substrate from entering the TFT. It is necessary to form a passivation film of aluminum or the like.

Next, a film is formed with a material such as aluminum or tantalum, and is patterned by using a mask.
A gate electrode 202 is formed. In particular, in order to prevent a short circuit between the gate electrode / wiring and the upper wiring, an oxide film 203 may be formed on the surface of the gate electrode. An anodic oxidation method is mainly used as a method for forming an oxide film.

Then, a gate insulating film 204 is formed. As the gate insulating film, silicon nitride is generally used, but it may be silicon oxide or silicide in which nitrogen and oxygen are mixed at an arbitrary ratio. Further, it may be a single-layer film or a multilayer film. When a silicon nitride film is used as a gate insulating film, when a plasma CVD method is used, the process temperature is about 350 ° C., which is the highest in this step. This state is shown in FIG.

Further, an amorphous silicon film is formed. If the plasma CVD method is used, the substrate temperature needs to be 250 to 300 ° C. The thickness of this film is desirably thin, and is usually 10 to 100 nm, preferably 10 to 30 nm. Then, the amorphous silicon region 205 is formed by patterning with a mask. This amorphous silicon region will later become a channel forming region of the TFT. The state up to this point is shown in FIG.

Further, a silicon nitride film is formed on the whole, and is patterned by using a mask to form an etching stopper 206. This etching stopper is provided so as not to erroneously etch the amorphous silicon region 205 in the channel formation region in a later step. Because the amorphous silicon region 2
This is because 05 is as thin as 10 to 100 nm.
Further, since the amorphous silicon region below the etching stopper functions as a channel forming region, the etching stopper is designed to overlap as much as possible with the gate electrode. However, some misalignment occurs in normal mask alignment, so that patterning is performed so as to sufficiently overlap the gate electrode.

Thereafter, a film of N-type or P-type silicon is formed. Normal amorphous silicon T
The FT is an N-channel type. Since this silicon film has too low conductivity in amorphous silicon,
The silicon film is in a microcrystalline state. The N-type microcrystalline silicon film can be formed at a temperature of 350 ° C. or lower by a plasma CVD method. However, the resistance is still not sufficiently low, so that the thickness has to be 200 nm or more. In addition, a P-type microcrystalline silicon film cannot be used because it has a remarkably large resistance.
Was difficult to fabricate with amorphous silicon.

The silicon film thus formed is patterned using a mask to form an N-type microcrystalline silicon region 20.
7 is formed. The state up to this point is shown in FIG.

In the state shown in FIG. 2C, the TFT does not function because the (N-type) microcrystalline silicon film is bonded on the etching stopper. Therefore, it is necessary to divide it. Therefore, the groove 208 is divided using a mask to form a groove 208. If there is no etching stopper, the amorphous silicon region 2
There is a possibility that the etching is performed up to 05. . This is because the thickness of the microcrystalline silicon region 207 is several times to ten and several times larger than the amorphous silicon region thereunder, or more.

Thereafter, the wiring 209 is formed by a known method.
The pixel electrode 210 is manufactured using a mask. This state is shown in FIG.

In the above method, since the number of masks is as large as seven, the yield may be reduced. Therefore, a method of reducing the number of masks as described below has been proposed. First, a gate electrode portion is patterned on a substrate using a first mask. After that, a gate insulating film is formed, and further, an amorphous silicon film and a silicon nitride film (which will later become an etching stopper) are continuously formed. Then, exposure is performed from the back surface, and only the silicon nitride film is etched in a self-aligned manner using the gate electrode portion as a mask to form an etching stopper. Then, a microcrystalline silicon film is formed thereon, and a TFT region including a groove (corresponding to 208 in FIG. 2) above the channel is formed using a second mask. Then, using the third and fourth masks,
Form wiring and electrodes. Eventually, one equivalent to that shown in FIG. 2 (D) is obtained. By making full use of the self-alignment process, the number of masks can be reduced by three.

[0015]

The TFT formed in this way has a very severe unevenness, as can be seen from the figure. This is mainly due to the gate electrode portion (including the oxide 203 of the gate electrode), the etching stopper, and the microcrystalline silicon region. The thickness of the gate electrode portion is 300 nm, the thickness of the etching stopper is 200 nm, The thickness of the microcrystalline silicon region 206 is 30
If it is set to 0 nm, unevenness as much as 800 nm will be generated on the substrate.

For example, when the cell is used as an active matrix circuit of a liquid crystal display panel, the thickness of the cell is 5 to 5.
It is controlled with a thickness of 6 μm and an accuracy of 0.1 μm or less. Under such conditions, if there is unevenness as large as 1 μm, a significant defect is given to the uniformity of the cell thickness.

However, none of these factors mentioned above as the cause of the unevenness of the TFT can be easily reduced. That is, in order to reduce the thickness of the gate electrode portion, the resistance of the gate electrode / wiring is increased. On the other hand, if the width of the gate electrode (that is, the channel length) is widened in order to keep the resistance constant, not only the operation speed of the TFT is reduced, but also the area of the TFT portion is increased, so that the TFT is used in a liquid crystal display device. Leads to a decrease in aperture ratio.

If the etching stopper is thin, there is a possibility that while the microcrystalline silicon region is being etched, the amorphous silicon region thereunder may be erroneously etched, thereby lowering the yield. Further, when the thickness of the microcrystalline silicon region is small, the resistance of the source / drain region of the TFT is large, and the ON / OFF ratio of the TFT is reduced.

Further, the etching stopper remains as it is when the TFT is completed. However, the silicon nitride film used for this has a property of trapping electric charge. An undesired channel is formed in the amorphous silicon region 205, which causes a drain current leak. In order to avoid this problem, the etching stopper needs to have a two-layer structure of silicon oxide and silicon nitride. In this case, the thickness of the silicon oxide film needs to be sufficiently large. Needs to be 100 nm or more.

The present invention has been made in view of such conventional problems, and one of the objects of the present invention is to simplify the process. For example, the yield is improved by reducing the number of masks compared to the conventional method. Alternatively, an object is to improve throughput and reduce cost by reducing the number of film formation steps.

Another object of the present invention is to make the TFT flatter. This not only solves the problem of using it for a liquid crystal display panel, but also flattening is an important technical issue in other applications, and it is difficult to apply it to conventional TFTs. It can be applied.

[0022]

SUMMARY OF THE INVENTION In order to solve the above problems, the present invention proposes a completely new method of manufacturing a TFT without using an etching stopper and a TFT manufactured by the method. Further, in order to reduce the thickness of the microcrystalline silicon region (source / drain), its resistance is made sufficiently low. Further, in the present invention, a two-stage process is conventionally performed, such as formation of an amorphous silicon region (film) serving as a channel formation region and formation of a microcrystalline silicon region (film) serving as source / drain regions. To form one silicon film,
This has a structure in which a part is formed in the source / drain region and a part is formed in the channel formation region.

In order to improve the throughput, the most important issue is to reduce the number of coatings. In the film forming process, not only the time required for film formation but also the time required for cleaning the inside of the chamber is about the same, and in a modern semiconductor process that requires an extremely clean environment, the time between cleaning the chamber is increased. The fact is that a film is formed. Therefore, it is necessary to form a thinner film than to form a thick film and to form a single-layer film rather than to form a multilayer film in order to increase the throughput. In that sense, it is desirable to reduce the number of film formation steps.

TFT based on one technical idea of the present invention
Has the following configuration. First, the inverted stagger type T
FT. A gate insulating film is formed to cover the gate electrode, and a semiconductor film is further formed. A portion above the gate electrode is substantially intrinsic so as to function as a channel forming region. Other portions are N-type or P-type, and function as a source / drain. Also,
The portion functioning as a channel formation region can be in any of amorphous, semi-amorphous, microcrystalline, polycrystalline, and intermediate states thereof. To suppress the off-state current, amorphous is desirable. On the other hand, a region functioning as a source / drain is polycrystalline, semi-amorphous, or microcrystalline having sufficiently small resistance. Moreover, the present invention is characterized in that this region is formed by laser annealing.

In such a configuration, the film needs to be formed by only one semiconductor film, and mass productivity is improved. Further, if conventional microcrystalline silicon is not formed, TF
T unevenness can be reduced. Of course, the present invention
It is not required that the channel formation region and the impurity region such as the source / drain are formed by a single semiconductor film. It goes without saying that it is good.

Further, T based on another technical idea of the present invention.
The FT has no etching stopper above the channel formation region. At least silicon nitride or a material having similar charge trapping properties does not adhere to the channel formation region or exist through a thin (100 nm or less) insulating film.

The presence of the etching stopper
This is an important factor of the unevenness of the TFT, and when the etching stopper is made of a material such as silicon nitride,
Drain current leakage also occurs. Such a problem is solved by the above technical idea of the present invention.

Of course, this technical idea of the present invention does not require that no object is present on the channel forming region, but it is not a problem that there is an object that does not reveal the above-mentioned problem. is not.

[0029]

DESCRIPTION OF THE PREFERRED EMBODIMENTS The fabrication of the TFT of the present invention is carried out by the method shown in FIG. 1, but it is needless to say that necessary changes can be made to this process chart. As shown in the figure, a heat-resistant alkali-free glass (for example, Corning 7)
059) On the substrate 101, the gate electrode 102 is patterned by using a mask. If necessary, an oxide film 103 may be formed on the surface of the gate electrode as shown in FIG. 1 to enhance the insulation. Further, the gate insulating film 10
4 is formed. Thus, FIG. 1A is obtained.

Next, amorphous, semi-amorphous,
A semiconductor film 105 is formed by forming a thin film of microcrystal, polycrystal, or silicon in an intermediate state between them, and performing patterning with a mask. Actually, in many cases, an amorphous silicon film is formed in consideration of the film formation temperature and off-state current. However, polycrystalline or semi-amorphous silicon may be formed by using a low-temperature crystallization technique such as laser annealing. However, when polycrystalline silicon or semi-amorphous silicon is used, the electric field mobility increases, but the off-state current also increases, which is not suitable for an active matrix circuit of a liquid crystal display panel.

Next, a film serving as a mask material for a laser beam, for example, a silicon-rich silicon nitride film (thickness 50)
nm or more is preferably formed, and is patterned using a mask. At this time, a photoresist may be left on the silicon nitride film. That is, FIG.
In the figure, 106 is a silicon nitride film, and 107 is a photoresist. Assuming a later ion implantation step, the thickness of the photoresist is 100 nm or more, preferably 50 nm or more.
0 nm or more.

In this state, first, impurities are selectively implanted into the semiconductor region 105 by a method such as ion implantation or ion doping. Thus, impurity regions 108 are formed. However, a very large defect occurs in the semiconductor film due to the impurity implantation, and the semiconductor film no longer functions as a semiconductor. Therefore, crystallization is performed by irradiating a laser beam from above. In this laser annealing step, by appropriately controlling the pulse width and energy density of the laser light, silicon in various states from a polycrystalline state, which is extremely close to a single crystal state, to a semi-amorphous state can be formed.

If the silicon nitride film 106 does not exist, the laser beam reaches a region functioning as a channel forming region where impurities are not doped, and the portion is crystallized. When a silicon nitride film is present, a large amount of light is absorbed by the silicon nitride film and crystallization does not occur, and the initial state is maintained.

It seems that crystallization of the channel region by laser light is preferable from the viewpoint of increasing the mobility. However, in the current laser technology, the crystallization of the crystallization is caused by the variation in the energy of the laser shot. The degree of variation is extremely large, and TFTs having various mobilities are formed.

There is no problem when only a TFT having a constant mobility is required. However, if the mobility satisfies a certain lower limit and the off-current also satisfies a certain upper limit, the condition is extremely high. It becomes severe. This is because a TFT having a high mobility generally has a large off-state current. For example, in an active matrix circuit of a liquid crystal display panel, not only mobility but also off-state current is an important factor, and therefore, a TFT having uniform grains is required. Therefore, in such a case, a TFT made of amorphous silicon having a low off-current but a low mobility or a material close thereto is desired. Therefore, also in the present invention, in such a case, it is necessary to prevent laser light from accidentally entering the channel formation region.

This doping step may be performed by laser doping. What is laser doping?
A method of placing a sample in an atmosphere containing impurities and irradiating it with laser light or an equivalent strong light to heat and activate the sample surface, further decompose the impurity gas and diffuse it to the sample surface It is. As the impurity gas, PH ₃ (phosphine) is generally used when N-type is provided, and B ₂ H ₆ (diborane) is generally used when P-type is provided.

According to the knowledge of the present inventors, at the time of laser irradiation, if the sample is heated to about 250 to 500 ° C., the diffusion of impurities proceeds to the inside of the sample, and the impurity concentration can be sufficiently increased. . In order to keep the channel formation region in amorphous silicon, it is not desirable to place the sample at a very high temperature, and it is desirable to limit the heating to about 250 to 350 ° C. because the glass substrate is also restricted. When laser doping is performed, the photoresist mask 107 is not always necessary. Doping methods such as ion implantation require a mask such as a photoresist of sufficient thickness to sufficiently attenuate the ion energy so that the implanted high-energy ions do not accidentally enter the channel formation region. However, since laser doping is a kind of thermal diffusion method, only a mask made of a material having a sufficient masking action against thermal diffusion, such as the silicon nitride mask 106, is sufficient. Details of the laser doping technique are described in Japanese Patent Application No. 3-283981 filed by the present inventors.

After doping in this manner, the silicon nitride film 106 and the photoresist 107 (mostly evaporated by laser light irradiation) 107 are removed.
The wiring 110 and the pixel electrode 1 of ITO are formed by a known method.
11 is formed by the mask and. Although a total of five masks are required by the above steps, the number of masks can be reduced to four by making full use of the self-alignment method as in the related art. That is, one sheet is required for forming the gate electrode, one sheet is required for forming the semiconductor region, and two sheets are required for forming the pixel electrode and the wiring. The patterning of the silicon nitride film 106 and the like is dealt with by performing backside exposure using a gate electrode as a mask.

As is clear from FIG. 1D, the TFT according to the present invention has smaller irregularities than the conventional TFT. This is because the main factor of the unevenness is only the unevenness of the gate electrode portion. Since the thickness of the semiconductor region 105 is extremely thin and is 10 to 100 nm similarly to the conventional TFT, it does not contribute much.

As described above, the semiconductor region, that is, the source /
The reason why the drain may be thin is that the impurity concentration of the region is sufficiently high and the crystallinity thereof is good. In other words, the feature of the present invention is brought about by laser annealing or laser doping. Further, in the present invention, there is no etching stopper unlike the prior art, and the mask material used in the present invention does not need to remain after the TFT is completed, so that the unevenness of the TFT is significantly reduced.

According to the present invention, an N-channel TFT (N
In addition to TFTs, practical P-channel TFTs (PTFTs), which have been difficult with conventional techniques, can now be manufactured. That is, in the prior art, the mobility of holes in the amorphous silicon in the channel region was smaller than the mobility of electrons, and in addition, P-type silicon having sufficiently low source / drain resistance could not be obtained. Although it was not a target, the present invention made it possible to reduce the resistance of P-type silicon to a level comparable to that of N-type silicon, so that a PTFT that actually functioned as an element could be manufactured. is there.

Therefore, a complementary MOS circuit (CMOS
Circuit) can be constituted by an amorphous silicon TFT or a low-temperature fabrication TFT. Conventionally, T
A CMOS circuit using an FT can be a high-temperature TFT formed on a quartz substrate at a temperature of 1000 ° C. or higher, or a TFT manufactured at 600 ° C.
It has been limited to medium-temperature TFTs formed on a non-alkali glass substrate at about the same temperature. Maximum process temperature is 350
Conventionally, it has been considered impossible to form a CMOS circuit composed of TFTs of about ° C.

FIG. 3 shows an example. In the same manner as the method shown in FIG.
02 and the gate electrode 303 of the PTFT are formed using the first mask, and then, if necessary, the surface of the gate electrode is oxidized by anodic oxidation to form a gate insulating film 304.
To form Further, using a second mask, NTFT
And a PTFT semiconductor region 306 are formed.

The better the crystallinity of the semiconductor region, the higher the P
A TFT having high mobility can be obtained. In order to function as a CMOS, the mobility of the NTFT and the mobility of the PTFT should not be too different. Large mobility P
In order to obtain a TFT, it is preferable to increase the film forming temperature. However, the film forming temperature cannot be raised unnecessarily due to conditions such as restrictions on the substrate. However, when a film is formed using polysilane such as disilane or trisilane even at a substrate temperature of about 350 ° C., an apparently amorphous film having a mobility of about a fraction of NTFT is obtained. After a film is formed by plasma CVD, the film is formed in a hydrogen atmosphere.
Annealing may be performed at about 00 to 350 ° C. for 24 hours or more.

Thereafter, silicon nitride masks 307 and 308
Are patterned using a third mask. Of course, as described above, the silicon nitride mask may be formed in a self-aligned manner by the back surface exposure method using the gate electrode as a mask. In that case, the third mask is unnecessary. FIG. 3 is a sectional view of the element thus obtained.
It is shown in (A).

Thereafter, first, a photoresist mask 309 is formed in the PTFT region using a fourth mask, and as shown in FIG. 3B, laser irradiation is performed in an atmosphere of phosphor PH ₃ . Thus NTFT (left)
Is formed. Furthermore, this time NTF
A photoresist mask 311 is formed in the region T using a fifth mask, and as shown in FIG. 3C, laser is irradiated in an atmosphere of diborane B ₂ H ₆ to form a PTFT.
(Right) impurity region 312 is formed. In any of the laser doping steps, the laser light is absorbed by the silicon nitride mask.
13, 314 do not crystallize.

Thereafter, as shown in FIG. 3 (C), if metal wirings (aluminum or the like) 315, 316, 317 are formed by a known metal wiring technique (using a sixth mask), NTFT 318 and PTFT 319 are formed. CMOS
A circuit is formed.

In the above process, six masks are used. However, if the backside exposure technique is used in manufacturing the silicon nitride masks 307 and 308, one mask can be reduced. Further, the laser doping step can also be performed by a known ion implantation method or ion doping method. In addition, in the case where the impurity region is formed by an ion implantation method or an ion doping method in which the impurity concentration can be finely controlled, the impurity region of the NTFT and the impurity region of the PTFT are not separately manufactured. First, the impurity region of any conductivity type is
It is also possible to form at T and then reverse the conductivity type only to a particular TFT. In that case, the number of masks is further reduced by one. However, this method is difficult with laser doping where it is difficult to control the impurity concentration.

If such a method is to be performed by laser doping, first, the substrate temperature is set slightly lower, and a certain conductivity type impurity region is formed for all TFTs. This can be dealt with by raising the substrate temperature and performing doping of the opposite conductivity type only on a specific TFT. This is because the higher the substrate temperature, the higher the impurity concentration to be doped.

In the present invention, particularly with respect to laser doping, a method as shown in FIG. 4 is also possible. In this method, laser light is irradiated from the back surface to perform doping in a self-aligned manner using the gate electrode portion as a mask.

First, as in the case of FIG. 1, a gate electrode 402 is formed using a mask on a substrate 401 that transmits laser light. An oxide 403 is formed as needed, and a gate insulating film 404 is further formed. Then, the semiconductor region 405 is patterned using a mask. (FIGS. 4A and 4B)

Next, a laser beam is irradiated from the back surface of the substrate. At this time, the laser beam travels in parallel in the substrate as shown in FIG. 4 (C), but the laser beam is refracted because of the unevenness of the gate electrode, and also diffracted by the gate electrode and the like, and the parallelism is increased. Is impaired. In addition, in such an uneven portion, a laser beam is more absorbed in a portion where the laser is transmitted (the oxide layer 403 and the gate insulating film 404) than in other portions. As a result, not only is the mask masked by the gate electrode, but also due to the above-described complex phenomena, the intensity of the laser light is significantly reduced in the convex portions above the gate electrode portion, and the laser doping is no longer performed. Absent. Therefore, the initial state is maintained, and the channel formation region 406 is formed.

On the other hand, laser doping is performed in other portions, and impurity regions 407 are formed. After that, the metal wiring 409 and the pixel electrode 4 are masked.
10 or the like may be formed.

In this method, the steps are extremely simple as compared with other methods. That is, the number of masks is four as in the case of employing the self-alignment process of backside exposure in the method of FIG. Also, unlike the method of FIG. 1, the number of exposure steps for forming a mask (for example, 106 in FIG. 1) is reduced by one. As a matter of course, a step of forming a silicon nitride film or the like used as a mask is unnecessary. Also, this is the most significant feature of the present method. However, the overlap between the source / drain and the gate electrode is small, and the parasitic capacitance can be suppressed.

However, in this method, the substrate must be transparent to the laser beam. Corning 7059 glass substrate is an ideal alkali-free glass, but is not suitable for laser doping with an excimer laser due to poor transparency of ultraviolet light. If the Corning 7059 glass is not used, it is necessary to increase the wavelength of the laser (for example, an argon ion laser or an Nd: YAG laser). Furthermore, the wavelength of the excimer laser beam can be doubled or longer by the nonlinear optical effect.

[0056]

Example 1 Example 1 was formed according to the manufacturing process shown in FIG. The manufacturing process cross-sectional view corresponds to FIG. However, the step of forming the ITO pixel electrode 111 is not included until the step of forming the metal wiring / electrode 110 in FIG. The gate electrode was tantalum, and an anodized film having a thickness of about 200 nm was formed on the surface of the gate electrode in step 5 to improve the insulating property. As an impurity doping means, an ion doping method was used. The number of masks used in this step is four. All steps consist of 26 steps.

In FIG. 5 to FIG. 10, “sputter” is a sputtering film forming method, and “PCVD” is a plasma CVD method.
The method "RIE" means a reactive ion etching method. After these methods, what is written after: is the film thickness, the used gas, and the like.

FIG. 2 is a cross-sectional view of a conventional manufacturing process corresponding to this embodiment, and FIG. 9 is a process diagram. Here, the number of masks used is six, and the total number of processes is 29. Process.

Hereinafter, this embodiment will be described in detail with reference to the flowcharts. Corning 7059 glass (101 in FIG. 1) was used as the substrate. This was washed (step 1), and a tantalum film having a thickness of 200 n was formed thereon by sputtering.
m (Step 2). Then, this is patterned with a mask (step 3), and mixed acid (phosphoric acid containing 5% nitric acid)
(Step 4). Thereafter, a current is supplied to the tantalum gate electrode (102 in FIG. 1) to perform anodic oxidation.
The voltage was increased to a maximum of 250 V, and an anodic oxide film (103 in FIG. 1) was formed to a thickness of 200 nm (step 5). The anodic oxidation method is described in Japanese Patent Application Nos. 3-237100 or 3-238713, and will not be described in detail here.

Thereafter, the resist was removed (Step 6), and a silicon nitride film (104 in FIG. 1) as a gate insulating film was formed to a thickness of 200 nm by a plasma CVD method (Step 7). At this time, the substrate temperature was 300 ° C. And
After the substrate was washed (Step 8), an amorphous silicon film having a thickness of 30 nm was formed by a plasma CVD method (Step 9).

Then, the semiconductor region is patterned by using a mask (Step 10), and the amorphous silicon film is etched by a reactive ion etching method using CF ₄ as a reaction gas (Step 11) to form a semiconductor region (FIG. 1). 105) was formed. The remaining resist was removed (Step 12), and the substrate was washed (Step 13).

Thereafter, a silicon nitride film having a thickness of 200 nm was formed by a plasma CVD method (step 14). At this time, the substrate temperature was 300 ° C. Then, the silicon nitride mask was patterned using a mask (step 15), and the silicon nitride film was etched with buffer hydrofluoric acid (step 16) to form a silicon nitride mask (106 in FIG. 1). A resist having a thickness of about 500 nm (107 in FIG. 1) was left on the silicon nitride mask.

Then, 1
Phosphorus ions at a dose of × 10 ¹⁴ cm ^-2 were implanted at an acceleration energy of 10 keV (step 17) to form an impurity region (108 in FIG. 1). Thereafter, the substrate was washed (Step 18), and the remaining resist was removed (Step 1).
9).

Thereafter, laser annealing was performed with a XeCl excimer laser (step 20), and the silicon nitride mask (106 in FIG. 1) was removed by etching with buffered hydrofluoric acid (step 21). Thereafter, the substrate was washed (Step 22).

Then, an aluminum film is formed to a thickness of 400 nm by a sputtering method (step 23), and the aluminum wiring is patterned using a mask (step 2).
4) Further, the aluminum film is etched with a mixed acid (step 25), and the aluminum wiring (11 in FIG. 1) is formed.
0). The remaining resist was removed (Step 2
6). The NTFT was manufactured through the above steps.

Example 2 This example was formed according to the manufacturing process shown in FIG. The manufacturing process sectional view corresponds to FIG. 1 except that a backside exposure technique is used. However, FIG. 6 shows the steps up to the step of forming the metal wiring / electrode 110 in FIG. 1 as in the first embodiment. The gate electrode is made of aluminum, and the surface of the gate electrode is subjected to step 5
In Example 2, an anodic oxide film having a thickness of about 200 nm was formed to improve the insulating property. A backside exposure technique was used to form the silicon nitride mask. As an impurity doping means, an ion doping method was used. The number of masks used in this step is reduced by one by the backside exposure technique, and is three. All steps consist of 26 steps.

The conventional manufacturing process corresponding to this embodiment is shown in FIG.
Although shown as 0, here, the number of masks used is three, and all the steps are 23 steps.

Hereinafter, this embodiment will be described in detail with reference to the flowcharts. Corning 7059 glass (101 in FIG. 1) was used as the substrate. This was washed (step 1), and an aluminum film having a thickness of 40 was formed thereon by sputtering.
0 nm was formed (Step 2). Then, this was patterned with a mask (Step 3), and etched with a mixed acid (phosphoric acid containing 5% nitric acid) (Step 4). Thereafter, the aluminum gate electrode (102 in FIG. 1) was energized to perform anodic oxidation, and the voltage was increased up to 250 V to form an anodic oxide film (103 in FIG. 1) with a thickness of 200 nm (step 5).

Thereafter, the resist was removed (Step 6), and a silicon nitride film (104 in FIG. 1) as a gate insulating film was formed to a thickness of 200 nm by a plasma CVD method (Step 7). At this time, the substrate temperature was 300 ° C. And
After the substrate was washed (Step 8), an amorphous silicon film having a thickness of 30 nm was formed by a plasma CVD method (Step 9).

Then, the semiconductor region is patterned by using a mask (Step 10), and the amorphous silicon film is etched by a reactive ion etching method using CF ₄ as a reaction gas (Step 11), thereby forming a semiconductor region (FIG. 1). 105) was formed. The remaining resist was removed (Step 12), and the substrate was washed (Step 13).

Thereafter, a silicon nitride film having a thickness of 200 nm was formed by a plasma CVD method (step 14). At this time, the substrate temperature was 300 ° C. Then, exposure is performed from the back surface of the substrate in a state where the resist is applied, the silicon nitride mask is patterned in a self-aligned manner using the gate electrode as a mask (step 15), and the silicon nitride film is etched with buffered hydrofluoric acid (step 16). ), And a silicon nitride mask (106 in FIG. 1) was formed. A resist having a thickness of about 500 nm (107 in FIG. 1) was left on the silicon nitride mask.

Next, by ion doping, 1
Phosphorus ions at a dose of × 10 ¹⁴ cm ^-2 were implanted at an acceleration energy of 10 keV (step 17) to form an impurity region (108 in FIG. 1). Thereafter, the substrate was washed (Step 18), and the remaining resist was removed (Step 1).
9).

Thereafter, laser annealing was performed with a XeCl excimer laser (step 20), and the silicon nitride mask (106 in FIG. 1) was removed by etching with buffered hydrofluoric acid (step 21). Thereafter, the substrate was washed (Step 22).

Then, an aluminum film is formed to a thickness of 400 nm by sputtering (step 23), and the aluminum wiring is patterned by using a mask (step 2).
4) Further, the aluminum film is etched with a mixed acid (step 25), and the aluminum wiring (11 in FIG. 1) is formed.
0). The remaining resist was removed (Step 2
6). The NTFT was manufactured through the above steps.

Example 3 This example was formed according to the manufacturing process shown in FIG. The manufacturing process cross-sectional view corresponds to FIG. However, FIG. 7 shows the steps up to the step of forming the metal wiring / electrode 409 in FIG. The gate electrode was aluminum, and an anodized film having a thickness of about 200 nm was formed on the surface of the gate electrode in step 5 to improve the insulating property. Impurity doping means include:
A laser doping technique using laser light irradiation from the back was used. The number of masks used in this process is 3
It is a sheet. All steps consist of 19 steps.

Hereinafter, this embodiment will be described in detail with reference to the flowcharts. Corning 7059 glass (401 in FIG. 4) was used as the substrate. This was washed (step 1), and an aluminum film having a thickness of 40 was formed thereon by sputtering.
0 nm was formed (Step 2). Then, this was patterned with a mask (Step 3), and etched with a mixed acid (phosphoric acid containing 5% nitric acid) (Step 4). Thereafter, the aluminum gate electrode (402 in FIG. 4) was energized to perform anodic oxidation, and the voltage was increased up to 250 V to form an anodic oxide film (403 in FIG. 4) with a thickness of 200 nm (step 5).

Thereafter, the resist was removed (Step 6), and a silicon nitride film (404 in FIG. 4) as a gate insulating film was formed to a thickness of 200 nm by a plasma CVD method (Step 7). At this time, the substrate temperature was 300 ° C. And
After the substrate was washed (Step 8), an amorphous silicon film having a thickness of 30 nm was formed by a plasma CVD method (Step 9).

Then, the semiconductor region is patterned using a mask (step 10), and the amorphous silicon film is etched by a reactive ion etching method using CF ₄ as a reaction gas (step 11) to form a semiconductor region (FIG. 4). 405). The remaining resist was removed (Step 12), and the substrate was washed (Step 13).

Thereafter, XeCl excimer laser light was exposed from the back surface of the substrate in a phosphine atmosphere, and laser doping of the semiconductor region was performed in a self-aligned manner using the gate electrode as a mask (step 14). Since the XeCl excimer laser has a wavelength of 308 nm, it was able to transmit even with Corning 7059. After the substrate temperature during laser doping was set to 300 ° C., the substrate was washed (step 15).

Then, an aluminum film is formed to a thickness of 400 nm by sputtering (step 16), and the aluminum wiring is patterned by using a mask (step 1).
7) Further, the aluminum film is etched with a mixed acid (step 18), and aluminum wiring (40 in FIG. 4) is formed.
9) was formed. The remaining resist was removed (Step 1).
9). The NTFT was manufactured through the above steps.

[Embodiment 4] This embodiment is for forming a CMOS circuit, and was formed according to the manufacturing process shown in FIG. The manufacturing process cross-sectional view corresponds to FIG. The gate electrode was aluminum, and an anodized film having a thickness of about 200 nm was formed on the surface of the gate electrode in step 5 to improve the insulating property. The laser doping technique was used as the impurity doping means. At the time of doping, NTFT regions and PTFT regions were separately formed on the same substrate. The number of masks used in this step is six. All steps consist of 32 steps.

Hereinafter, the present embodiment will be described in detail with reference to the process charts. Corning 7059 glass (301 in FIG. 3) was used as the substrate. This was washed (step 1), and an aluminum film having a thickness of 40 was formed thereon by sputtering.
0 nm was formed (Step 2). Then, this was patterned with a mask (Step 3), and etched with a mixed acid (phosphoric acid containing 5% nitric acid) (Step 4). Thereafter, the aluminum gate electrodes (302 and 303 in FIG. 3) were energized to perform anodic oxidation, and the voltage was increased up to 250 V to form an anodic oxide film having a thickness of 200 nm (step 5).
The anodizing technique will not be described in detail here.

Thereafter, the resist was removed (Step 6), and a silicon nitride film (304 in FIG. 3) as a gate insulating film was formed to a thickness of 200 nm by a plasma CVD method (Step 7). At this time, the substrate temperature was 300 ° C. And
After the substrate was washed (Step 8), an amorphous silicon film having a thickness of 30 nm was formed by a plasma CVD method (Step 9).

Then, the semiconductor region is patterned by using a mask (Step 10), and the amorphous silicon film is etched by a reactive ion etching method using CF ₄ as a reaction gas (Step 11) to form a semiconductor region (FIG. 3). 305 and 306). The remaining resist was removed (Step 12), and the substrate was washed (Step 1).
3).

Thereafter, a silicon nitride film having a thickness of 200 nm was formed by a plasma CVD method (step 14). At this time, the substrate temperature was 300 ° C. Then, the silicon nitride mask is patterned using a mask (step 15), and the silicon nitride film is etched with buffered hydrofluoric acid (step 16) to form a silicon nitride mask (307 and 3 in FIG. 3).
08) was formed. The resist on the silicon nitride mask was removed (Step 17).

Next, after washing the substrate (Step 18), an NTFT pattern was formed using a mask (Step 1).
9). At this time, the PTFT is a resist (309 in FIG. 3).
Covered by In this state, phosphorus was doped by a laser doping method in a phosphine atmosphere (step 20). Thus, an N-type impurity region (310 in FIG. 3) was formed. After the completion of the laser doping, the remaining resist (309 in FIG. 3) was removed (Step 21), and the substrate was washed (Step 22).

Similarly, a PTFT pattern was formed using a mask (step 23). At this time, the NTFT is covered with the resist (311 in FIG. 3). In this state, boron was doped in a diborane atmosphere by a laser doping method (step 24). Thus, a P-type impurity region (312 in FIG. 3) was formed. After the completion of the laser doping, the remaining resist (311 in FIG. 3) was removed (Step 25), and the substrate was washed (Step 26). Further, the silicon nitride mask (307 and 308 in FIG. 3) was removed by etching with buffered hydrofluoric acid (Step 27). Thereafter, the substrate was washed (Step 2).
8).

Then, an aluminum film is formed to a thickness of 400 nm by a sputtering method (Step 29), and the aluminum wiring is patterned by using a mask (Step 3).
0), and further etching the aluminum film with a mixed acid (step 31) to form an aluminum wiring (31 in FIG. 3).
5, 316, 317). The remaining resist was removed (step 32). The NTFT was manufactured through the above steps.

[0089]

As is apparent from the above description, the effect of the present invention is characterized by the simplification of the process. As well,
It is an object of the present invention to provide a TFT having good quality (for example, excellent high-speed performance and a small threshold voltage) because the sheet resistance of the source and drain regions is small. Thus, the present invention is industrially useful.

[Brief description of the drawings]

FIG. 1 shows a sectional view of a method for manufacturing a TFT according to the present invention.

FIG. 2 shows a cross-sectional view of a conventional TFT manufacturing method.

FIG. 3 shows a sectional view of a method for manufacturing a TFT according to the present invention.

FIG. 4 shows a sectional view of a method for manufacturing a TFT according to the present invention.

FIG. 5 shows a manufacturing process diagram of a TFT according to the present invention.

FIG. 6 shows a manufacturing process diagram of a TFT according to the present invention.

FIG. 7 shows a manufacturing process diagram of a TFT according to the present invention.

FIG. 8 shows a manufacturing process diagram of a TFT according to the present invention.

FIG. 9 shows a manufacturing process diagram of a TFT according to a conventional method.

FIG. 10 shows a manufacturing process diagram of a TFT according to a conventional method.

[Explanation of symbols]

 DESCRIPTION OF SYMBOLS 101 Substrate 102 Gate electrode 103 Surface oxide of gate electrode 104 Gate insulating film 105 Semiconductor region 106 Silicon nitride mask 107 Photoresist mask 108 Impurity region 109 Channel formation region 110 Metal wiring 111 Pixel electrode (ITO)

Claims (8)

[Claims] 1. An inverted staggered thin-film insulated gate semiconductor device having a gate electrode, a gate insulating film, a channel forming region, a source region and a drain region, wherein the gate electrode is formed on a substrate having an insulating surface. The gate insulating film is formed on the gate electrode, a semiconductor film having a thickness of 10 to 100 nm is formed on the gate insulating film, and the source region is formed on the semiconductor film. Wherein the drain region and the channel forming region are formed, and the source region and the drain region contain impurities and have better crystallinity than the channel forming region. Semiconductor device. 2. The thin-film insulated gate semiconductor device according to claim 1, wherein said impurity is implanted from above a mask covering a part of said semiconductor film. 3. The thin film insulation according to claim 1, wherein the source region and the drain region are crystallized by irradiating a laser beam from above the mask. Gate type semiconductor device. 4. An inverted staggered thin-film insulated gate semiconductor device having a gate electrode, a gate insulating film, a channel forming region, a source region and a drain region, wherein the gate electrode is formed on a substrate having an insulating surface. The gate insulating film is formed on the gate electrode, a semiconductor film having a thickness of 10 to 100 nm is formed on the gate insulating film, and the source region is formed on the semiconductor film. Wherein the drain region and the channel forming region are formed, wherein the source region and the drain region have an impurity, and the impurity is implanted from above a mask covering a part of the semiconductor film. And the source region and the drain region have a higher crystallinity than the channel formation region, A thin film insulated gate semiconductor device which is characterized in that one formed by irradiating the Za light. 5. The thin-film insulated gate semiconductor device according to claim 1, wherein said semiconductor film is silicon. 6. The thin film according to claim 1, wherein the channel forming region is amorphous, semi-amorphous, microcrystalline, polycrystalline, or silicon in an intermediate state thereof. Insulated gate semiconductor device. 7. An active matrix type circuit using the thin-film insulated gate type semiconductor device according to claim 1. Description: 8. A drive circuit using the thin-film insulated gate semiconductor device according to any one of claims 1 to 6.