WO2009111340A2 - Flash lamp annealing crystallization for large area thin films - Google Patents
Flash lamp annealing crystallization for large area thin films Download PDFInfo
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- WO2009111340A2 WO2009111340A2 PCT/US2009/035566 US2009035566W WO2009111340A2 WO 2009111340 A2 WO2009111340 A2 WO 2009111340A2 US 2009035566 W US2009035566 W US 2009035566W WO 2009111340 A2 WO2009111340 A2 WO 2009111340A2
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- 238000002425 crystallisation Methods 0.000 title claims abstract description 53
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Classifications
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02104—Forming layers
- H01L21/02365—Forming inorganic semiconducting materials on a substrate
- H01L21/02367—Substrates
- H01L21/0237—Materials
- H01L21/02422—Non-crystalline insulating materials, e.g. glass, polymers
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02104—Forming layers
- H01L21/02365—Forming inorganic semiconducting materials on a substrate
- H01L21/02518—Deposited layers
- H01L21/02521—Materials
- H01L21/02524—Group 14 semiconducting materials
- H01L21/02532—Silicon, silicon germanium, germanium
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02104—Forming layers
- H01L21/02365—Forming inorganic semiconducting materials on a substrate
- H01L21/02656—Special treatments
- H01L21/02664—Aftertreatments
- H01L21/02667—Crystallisation or recrystallisation of non-monocrystalline semiconductor materials, e.g. regrowth
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/04—Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer
- H01L21/18—Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer the devices having semiconductor bodies comprising elements of Group IV of the Periodic Table or AIIIBV compounds with or without impurities, e.g. doping materials
- H01L21/26—Bombardment with radiation
- H01L21/263—Bombardment with radiation with high-energy radiation
- H01L21/268—Bombardment with radiation with high-energy radiation using electromagnetic radiation, e.g. laser radiation
- H01L21/2686—Bombardment with radiation with high-energy radiation using electromagnetic radiation, e.g. laser radiation using incoherent radiation
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/67—Apparatus specially adapted for handling semiconductor or electric solid state devices during manufacture or treatment thereof; Apparatus specially adapted for handling wafers during manufacture or treatment of semiconductor or electric solid state devices or components ; Apparatus not specifically provided for elsewhere
- H01L21/67005—Apparatus not specifically provided for elsewhere
- H01L21/67011—Apparatus for manufacture or treatment
- H01L21/67098—Apparatus for thermal treatment
- H01L21/67115—Apparatus for thermal treatment mainly by radiation
Definitions
- the disclosed subject matter generally relates to crystallization of large area thin films and particularly relates to utilizing flash lamp annealing in combination with patterning techniques in making thin film devices.
- Flash lamp annealing (FLA) of thin silicon films can be used as a low-cost alternative to laser crystallization.
- Such films for example, may be used in producing different devices, including thin film transistors (TFTs).
- TFTs thin film transistors
- the flash lamp pulse durations may be as short as 10 ⁇ s or as long as 10 ms.
- FLA provides limited control over the nature and the location of the grain boundaries in the crystallized thin film. This limitation can pose problems for creating uniform transistors. FLA also may result in a material with a high volume of defects resulting from long lateral explosive crystallization. Therefore, materials produced by FLA may have lower performance levels than materials produced from other methods, including Sequential Lateral Solidification (SLS) and Excimer Laser Annealing (ELA). ELA crystallized thin films with an excimer laser. However, such laser source is not only expensive to purchase but also expensive to use, largely because of the laser tube replacements that are required. Conversely, FLA may provide uniform materials at a low cost and high-throughput, and scalable to large area thin films.
- SLS Sequential Lateral Solidification
- ELA Excimer Laser Annealing
- SLS and ELA crystallization techniques are limited by the length of the line beam in both applications.
- the SLS or ELA line beam can not provide uniform beam properties over the entire width or length of the large area thin film.
- the SLS or ELA scan is performed in small sections of the film area, requiring panel movement in both the x and y directions to successfully process the film. Not only does scanning in both the x and y directions increase the duration of the process, but it also produces lesser quality films with beam edges and non-uniformities between crystallization scans, than scanning a smaller film would produce.
- This application describes methods and systems for utilizing flash lamp annealing (FLA) in combination with patterning techniques to crystallize large area thin films on glass substrates or other substrates that have low tolerance for high temperatures.
- FLA flash lamp annealing
- Some embodiments use a shielding layer to shield areas of the substrate from exposure to the flash lamp.
- proximity masks may be used to expose areas that exactly match the size of one or multiple devices.
- barriers are etched into the film, and even the underlying layer, to control heat transfer from one area to the next.
- the film is covered with a patterned capping layer before being irradiated. The film in the uncovered region is melted and the crystallographic lateral growth will proceed from the edges between the covered and uncovered regions.
- melt-mediated explosive crystallization is used between the covered and uncovered regions.
- a method of irradiating a large area film with a pulsed light source includes providing a large area film on a substrate, covering at least a portion of the large area film with a covering material, wherein the covering material has one or more exposure areas that expose one or more sections of the film, irradiating the film and covering material with a pulsed light source under conditions to at least partially melt a portion of the film, wherein the irradiation area has a dimension at least substantially equal to a dimension of the film and the irradiating of the film causes crystallization to proceed from the interface between the exposed sections and the non-exposed sections of the film.
- the large area film has a length of greater than 1.3 meters and a width of greater than 1.5 meters or a length of greater than 1.5 meters and a width of greater than 1.8 meters. In some embodiments, one dimension of the irradiation area is greater than about 1.3 meters.
- the covering layer comprises a capping layer.
- the capping layer is deposited on the film, is a film, is at least one of absorptive and reflective, is metallic, and/or is opaque to the pulsed light source.
- the energy density of the FLA radiation is selected to induce at least one of lateral growth and explosive crystallization in the film.
- the pulsed light source is a flash lamp.
- the method includes providing an absorber layer between the film and the substrate, wherein the absorber layer absorbs the pulsed light source irradiation and the absorber layer can be metallic.
- the substrate is glass.
- the method includes removing a portion of the film prior to covering the film and/or removing a portion of the substrate below the portion of removed film.
- the method the film comprises a plurality of single crystal island segments.
- the method the covering comprises a proximity mask, wherein the proximity mask is located at a first position and covers only a first portion of the film and/or the proximity mask is opaque to the pulsed light source.
- the method includes moving the proximity mask to a second position, said second position covering a second portion of the film.
- the second portion of the film does not overlap the first portion of the film or the first section and the second section partially overlap.
- a method of irradiating a large area film using a pulsed light source includes providing a large area film having a first dimension and a second dimension on a substrate, covering the film with a capping layer having a pattern, wherein the pattern exposes one or more sections of the film, irradiating the film with a pulsed light source under conditions to at least partially melt a first portion of the film while a second portion of the film remains solid, wherein the irradiation area has a dimension at least substantially equal to a dimension of the film, and re-solidifying the first portion of the film to form a crystalline portion thereby releasing heat to melt an adjacent portion of the film.
- FIG. 1 is a schematic illustration of a flash lamp apparatus that may be used, according to some embodiments of the disclosed subject matter.
- FIG. 2A is a schematic of a thin film crystallization system implementing utilizing FLA and patterned capping layer for lateral growth, according to some embodiments of the disclosed subject matter.
- FIG. 2B is a top view of the lateral growth in the capped film, according to some embodiments of the disclosed subject matter.
- FIG. 2C is a schematic of a thin film crystallization system implementing FLA and patterned capping layer for explosive crystallization, according to some embodiments of the disclosed subject matter.
- FIG. 2D is a top view of explosive crystallization in the capped film, according to some embodiments of the disclosed subject matter.
- FIG. 3 is a schematic of a thin film crystallization system implementing shielding layers, according to some embodiments of the disclosed subject matter.
- FIG. 4 sketches examples of the effect of lateral heat diffusion.
- FIGs. 5A and 5B are schematics of a thin film crystallization system implementing heat flow isolation, according to some embodiments of the disclosed subject matter.
- FIG. 6A is a schematic of a thin film crystallization system implementing proximity masks, according to some embodiments of the disclosed subject matter.
- FIG. 6B is a schematic of a thin film crystallization system implementing proximity masks, according to some embodiments of the disclosed subject matter.
- AMLCDs active matrix liquid crystal displays
- AMOLEDs active matrix organic light emitting diode displays
- Large area thin films refer to thin films having a length greater than 1.3 meters and a width greater than 1.5 meters.
- large area thin films can be Gen 5.5 (1.3m x 1.5m or 1.32m x 1.5m), Gen 6 (1.5m x 1.8m or 1.5m x 1.85m), Gen 7 (1.87.
- Gen 8 (2.16m x 2.46m or 2.2m x 2.5m)
- Gen 9 (2.2m x 2.6 m or 2.4m x 2.8m)
- Gen 10 (2.6m x 3.1m) thin film panels.
- C-SLG lithography- based controlled super-lateral growth
- the method is not limited to silicon thin film crystallization and may be practiced for any thin film.
- the methods may be used for any such material.
- other pulsed light sources may be used, so long as they also provide a pulsed divergent light source or a pulsed flood light and the desired control of the mixed phase partial melting process.
- flash lamp annealing or "FLA” is also meant to include diode lasers and other divergent pulsed light sources used as a "flash lamp.”
- the pulse duration for FLA pulses can range from about 10 ⁇ s to about 10 ms or even longer.
- the upper boundary of the FLA pulse duration is considerably larger than the pulse durations in the commonly used pulsed-laser approaches, for which typical pulse durations vary from about ⁇ 30 ns to about 300 ns.
- the heat diffusion length (SQRT(Dt)) is considerably larger for FLA.
- higher pulse energies are required to reach the desired degree of melting in the silicon film. This excess heat can lead to a higher degree of heating in the underlying substrate and therefore can result in melting or distortion of a glass substrate, if used. Therefore, it may be more challenging to implement FLA for films on glass or other high-temperature -intolerant substrates.
- Flash laser annealing uses a flash lamp to produce white light over a wide wavelength range, e.g., 400-800 nm.
- the flash lamp is a gas-filled discharging lamp that produces intense, incoherent full-spectrum white light for very short durations.
- a flash lamp annealing apparatus uses white light energy for surface irradiation, in which the light is focused using, for example, an elliptical reflector to direct the light energy onto a substrate, such as is shown in FIG. 1.
- FIG. 1 is a simplified side view diagram representing a flash lamp reactor 100 with a reflecting device 110, in accordance with an embodiment of the present invention.
- the flash lamp reactor may include an array of flash lamps 120 located above a support 130, with a target area 150 situated between the two.
- the reflecting device 110 may be positioned above the flash lamps to reflect varying amount of radiation 160 from the flash lamps back towards different portions of a facing side of the target area.
- the target area may be adapted to receive a substrate (wafer).
- the lamp power is supplied by a series of capacitors and inductors (not shown) that allow the formation of well defined flash pulses on a microsecond to millisecond scale.
- a typical flash lamp light energy densities in the range of up to 3-5 J/cm 2 (for a 50 ⁇ s discharge) or 50-60 J/cm 2 for a 1-20 ms discharge can be obtained.
- the light energy density can be about 2-150 J/cm 2 .
- Flash lamp annealing allows fast heating of solid surfaces with a single light flash between some tens microseconds and some tens milliseconds, e.g., 10 ⁇ s-100 ms.
- Variables of the flash lamp that affect the quality of thin film crystallization include the energy intensity of the incident light, as well as the pulse duration and shape of the light (which results in a certain dwell time, i.e., a duration of melting).
- flash lamp irradiation is a flood irradiation process
- the flash lamps can irradiate large areas of the substrate surface in a single pulse. It is possible that the entire film on a substrate, for example a glass panel, can be processed simultaneously. Thus, multi-pulse operations in a scanned fashion to cover a large substrate area, for example, as used in laser- based recrystallization, are not required.
- a patterned capping layer 200 that is reflective, absorptive, or both, is provided on top of a thin film 210.
- the capping layer 200 can be a continuous film with a plurality of openings.
- the capping layer 210 can be substantially opaque to the irradiated light or reflective.
- the capping layer 210 can be a proximity mask or a deposited layer, for example, by using a lithography technique. Lithography techniques in FLA processing of thin films is disclosed in co-pending, PCT Serial No.
- the capping layer is reflective, it can be composed of any reflective material, for example, a metallic material, such as, e.g., aluminum. It may be desired to place a thin barrier layer such as, e.g., SiO 2 between the metallic cap layer and the film to prevent metal diffusion.
- the film 210 is irradiated by using a flash lamp 220 at an energy density sufficient to melt the uncovered film but insufficient to completely melt the covered portion of the film.
- lateral growth 230 of the crystalline structure will initiate at the edges between the covered and uncovered regions and propagate along arrow 230 to produce a crystalline material.
- Si grains tend to grow laterally from or perpendicular to interfaces between the liquid phase and solid phase silicon.
- the crystalline growth starts from the solid/liquid interface of the film 210 along arrow 230 and proceeds laterally along the film 210. This form of crystalline growth is called lateral growth.
- Lateral crystalline growth can produce large Si grains that can be used for device manufacture.
- devices can be made in the laterally grown regions of the thin film 210, i.e., the regions of the crystalline material in which the crystalline structure was formed as a result of lateral growth.
- the system can have one or more underlying absorber layers that can absorb the longer wavelength radiation, for example, longer than 600 nm, from the flash lamps.
- These absorber layers can be positioned between the thin film and the substrate or below the substrate. Because they preferentially absorb the longer wavelength radiation, the absorber layer will heat up first and can transfer the thermal energy from the radiation to the film to induce melting, while other regions in the film are heated by shorter wavelength light only and may remain solid. Because the flash lamps provide broad spectrum light, this arrangement provides the most efficient capture of the full energy spectrum of the flash lamp radiation and also can permit the capture of radiation that is transparent to the Si.
- These absorbing layers can be composed of any heat absorbing material, for example a metallic substance, such as molybdenum.
- the silicon film can be irradiated from the top portion of the film.
- the flash lamp radiation irradiates the top portion of the film and penetrates through the thickness of the film to the absorber layer.
- the majority of the light is absorbed by the absorber layer. This absorption heats the absorber layer, thus providing heat to the silicon film from the bottom and thus melting the thin film.
- the above embodiment offers ways of accurately defining the location of regions of lateral growth using a non-patterned light source.
- FIG. 2C a similar configuration of thin film 210 and cap layer 200 is used.
- the energy density of the flash lamp 220 is selected such that the covered portion film remains amorphous, while the uncovered portion of the film is at least partially molten.
- This situation triggers melt-mediated explosive crystallization 250.
- the first section melted portion reforms as crystalline silicon, an exotherm is created by the energy being dissipated as heat from the silicon as the silicon forms a more thermodynamically stable crystalline form.
- the amorphous material melts in the presence of the crystalline material, but the temperature of the liquid is still below the melting point of the crystalline material, the crystallizing materials will grow epitaxially.
- That exotherm is sufficient to melt adjacent amorphous silicon which itself then re-crystallizes as crystalline silicon and releases an additional amount of energy.
- An exotherm therefore, propagates as a wave through the material from the region closest to amorphous/front and propagates throughout the amorphous section of the thin film, in the direction of the arrow 250.
- the explosive crystallization process will continue until quenched or until all the amorphous material is transformed into crystalline material. Quenching is known to result in lowering of the temperature at the growth front and formation of defects and ultimately of halting of the process. Quenching is often the result of nearby conductive materials and/or nearby substrates.
- the flash lamp annealing conditions are selected such that the explosive crystallization can continue laterally for a sufficient distance through the thin film.
- the heat generated at the crystallization front by explosive crystallization can result in (1) further melting of the amorphous Si in region 215, (2) diffusive heat loss into the a-Si in region 225 (which will can be used for heating of the a-Si towards the melting point), and (3) diffusive heat loss into the substrate.
- the further melting of the amorphous Si is what drives the explosive nature of the process, because it requires less heat than what is generated by the explosive crystallization process. If heat absorption to the substrate or a-Si region 225 becomes too large, then insufficient heat will be available to drive further melting of the a-Si, leading to quenching of the process.
- pre-heating the a-Si and/or pre-heating the substrate can increase the explosive crystallization distance by reducing diffusive heat loss.
- Pre-heating mechanisms include use of a heated substrate, such as a hot plate and co- irradiation, in which one radiation is used for heating and a second irradiation is used for preheating.
- the flash lamp energy can be such that the amorphous region is substantially heated by the beam, but not to the point that crystallization occurs.
- the heat deposited in the amorphous film permits the explosive crystallization process to proceed over a longer distance.
- the absorber layer used in the lateral growth embodiments also can be used to induce explosive crystallization by heating the sections of a-Si and extending the explosive crystallization growth length.
- the irradiation used for triggered explosive crystallization may have a lower energy density. This is because lateral growth requires complete melting of the thin film, while explosive crystallization only requires at a minimum some partial melting. Conversely, for explosive crystallization only some melting needs to be triggered before the crystallization process proceeds. Therefore, because explosive crystallization can be triggered with only partial melting of the silicon, explosive crystallization can occur at lower temperature than lateral growth crystallization. Thus, because of the lower temperature, explosive crystallization techniques may be better suited to thin films on glass substrates.
- the pattern of the capping layer on the film can be different from the capping layer pattern used for lateral growth.
- rectangular areas of the capping layer should cover the film where lateral explosive crystallization is desired.
- the remainder of the film need not be entirely uncovered. In principle, it is enough to have just a narrow trench in the capping layer adjacent to the region where explosive crystallization is sought.
- the above approaches also can be combined with the patterning of the silicon islands.
- the patterning of silicon islands is disclosed in co-pending PCT Application Serial No. PCT/US08/077199, filed on September 22, 2008, entitled “Collections of Laterally Crystallized Semiconductor Islands for Use in Thin Film Transistors and Systems and Methods for Making Same," the entire disclosure of which is incorporated by reference.
- the patterning of silicon islands can be used to create high quality TFTs by reducing the length of similarly oriented domains in a long laterally grown material, which can reduce intragrain defects.
- oriented domains in the crystalline structure may lead to device non- uniformity when they are of a size comparable or larger than the size of the devices, and when there are different types of oriented domains that can co-exist, as may result from SLS or even a single-pulse process.
- oriented domains can be created as a result of occlusion in lateral growth.
- FIGs. 2B and 2D show lateral growth 230 and explosive crystallization 250, respectively, in a plurality of striped patterned crystal islands 240 contained within a substrate 260. With the very long lateral growth distances, even in a single pulse, oriented domains may form that are too large for device manufacturing.
- the present application pertains to increasing the compatibility of the FLA process with films on glass substrates.
- a shielding layer 300 e.g., a layer that is reflective or absorptive or both reflective and absorptive
- a shielding layer 300 is deposited on the film 310, which rests on a substrate 315, and openings 320 are etched in the shielding layer 300 corresponding to regions in the film 320 where TFT channel regions will be fabricated.
- This method can be used for pixel TFTs where the density of the devices is relatively low.
- the substrate 315, and the thin film 310 which may be patterned and/or composed of silicon, will be largely shielded from the beam.
- the small pockets of heating may lead to local "over-heating" of the substrate 315, but the resultant stresses will be localized and therefore less harmful to the substrate 315.
- some smearing also may result from fluence gradients, which are non-sharp transitions between light and dark regions that may exist at the edges of radiation beams, as shown in the beam profile 406 in FIG. 4, as a result of poor projection properties of the light or even the absence of such optics.
- fluence gradients which are non-sharp transitions between light and dark regions that may exist at the edges of radiation beams, as shown in the beam profile 406 in FIG. 4, as a result of poor projection properties of the light or even the absence of such optics.
- wide edge regions may exist in which non-uniform microstructures can be created. These regions will have different optical properties from the surrounding amorphous regions and will likely have a different melting threshold, making subsequent processing more difficult.
- closely- spaced radiations of the film in order to fully crystallize with minimized edge regions may not be possible. Therefore, a full irradiation of the film would be preferred.
- the unwanted lateral crystallization can be reduced by providing barriers for lateral heat flow at the edges of the radiated region of a thin film 500 on a substrate 505.
- the barriers or isolation of the film can be provided by etching the thin film 500 or by also etching the underlying layers, for example, a buffer layer 510 (as shown in FIG. 5A).
- the etching of the thin film can reduce irradiation heat transfer between a first section 501, a second section 502 and a third section 503.
- some heat may be transferred through the substrate. Therefore, as shown in FIG. 5B, the substrate 505 can have one or more trenches 515.
- trenches 515 can further reduce heat flow between the first section 501, the second section 502 and the third sections 503, thereby further limiting unwanted lateral crystallization.
- Such trenches 515 can be made using conventional etching techniques or even laser scribing techniques.
- This embodiment can prevent non-sharp/smeared crystallized domains, as shown in FIG. 4.
- wide edges that are non-uniformly crystallized can form, which may prevent close tiling.
- PCT Application Serial No. PCT/US09/xxx filed on even date herewith, titled "Flash Light Annealing for Thin Films," has shifted and a next radiation may thus not lead to MPS in those explosive crystallization regions.
- the process shown in FIG. 5 allows for more sharply defined crystallized regions and can alleviate these problems.
- this approach can be combined with the other embodiments disclosed herein, including the use of capping layers, underlying absorbing films, and/or proximity masks.
- the effect of the edge regions as shown in FIG. 4 in subsequently made devices can be reduced by using proximity masks 600.
- a proximity mask 600 may be used to expose areas 620 of the thin film 605 to the FLA radiation produced by the flash lamps 615 that exactly match the size of one or multiple display(s) or other device(s) or are relatively close in size to such displays or devices.
- One or multiple radiations may be performed with the proximity mask.
- the proximity mask 600 should be composed of a material that is substantially opaque to the incident light. Exemplary mask materials include, but are not limited to, metallic substrates.
- the proximity mask may be moved or replaced by second proximity mask 610 to irradiate other regions 625 corresponding to one or more displays or devices. This process may be repeated several times until the location of all devices on the panel have been irradiated. In typical embodiments, as few as two iterations may be sufficient. In some embodiments, the mask can be different from the capping layer discussed above.
- the flash lamp uses divergent light, therefore, it does not lend itself well for overlapped radiation that leads to extended lateral growth. Rather, the entire film is radiated (or large regions thereof).
- the proximity mask divides the film into sections to limit the heating of the substrate on any given pulse. Thus, the surface of the film is being tiled. However, some overlapping radiations can result in continuous microstructure, but more likely that is not the case, and, for example, some lateral growth may occur on the edges. In that case, care must be taken to not make devices from those edge regions. This can be possible using alignment techniques.
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Abstract
The disclosed subject matter generally relates a method of irradiating a large area thin film with a pulsed light source. In some embodiments, the disclosed subject matter particularly relates to utilizing flash lamp annealing in combination with patterning techniques for making thin film devices. The flash lamp annealing can trigger lateral growth crystallization or explosive crystallization in large area thin films. In some embodiments, capping layers or proximity masks can be used in conjunction with the flash lamp annealing.
Description
FLASH LAMP ANNEALING CRYSTALLIZATION FOR LARGE AREA THIN
FILMS
Cross-Reference to Related Application
[0001] This application claims the benefit under 35 U. S. C. § 119(e) of U.S. Provisional Application No. 61/032,737, filed February 29, 2008, entitled "Flash Lamp Annealing Lateral Growth," and U.S. Provisional Application No. 61/032,784, filed February 29, 2008, entitled Flash Lamp Annealing on Glass," the entirety of each of the disclosures of which are explicitly incorporated by references herein.
Field
[0002] The disclosed subject matter generally relates to crystallization of large area thin films and particularly relates to utilizing flash lamp annealing in combination with patterning techniques in making thin film devices.
Background
[0003] Flash lamp annealing (FLA) of thin silicon films can be used as a low-cost alternative to laser crystallization. Such films, for example, may be used in producing different devices, including thin film transistors (TFTs). The flash lamp pulse durations may be as short as 10 μs or as long as 10 ms.
[0004] However, FLA provides limited control over the nature and the location of the grain boundaries in the crystallized thin film. This limitation can pose problems for creating uniform transistors. FLA also may result in a material with a high volume of defects resulting from long lateral explosive crystallization. Therefore, materials produced by FLA may have lower performance levels than materials produced from other methods, including Sequential Lateral Solidification (SLS) and Excimer Laser Annealing (ELA). ELA crystallized thin films with an excimer laser. However, such laser source is not only expensive to purchase but also expensive to use, largely because of the laser tube replacements that are required. Conversely, FLA may provide uniform materials at a low cost and high-throughput, and scalable to large area thin films.
[0005] SLS and ELA crystallization techniques are limited by the length of the line beam in both applications. For example, for large area thin films, e.g., thin films having a length greater than 1.3 meters and a width greater than 1.5 (for example, Gen-5 (1.3m x 1.5m), Gen-
6 (1.5m x 1.8m) or Gen-8 (2.2m x 2.5m) thin film panels) the SLS or ELA line beam can not provide uniform beam properties over the entire width or length of the large area thin film. Thus, the SLS or ELA scan is performed in small sections of the film area, requiring panel movement in both the x and y directions to successfully process the film. Not only does scanning in both the x and y directions increase the duration of the process, but it also produces lesser quality films with beam edges and non-uniformities between crystallization scans, than scanning a smaller film would produce.
Summary
[0006] This application describes methods and systems for utilizing flash lamp annealing (FLA) in combination with patterning techniques to crystallize large area thin films on glass substrates or other substrates that have low tolerance for high temperatures. Some embodiments use a shielding layer to shield areas of the substrate from exposure to the flash lamp. In other embodiments, proximity masks may be used to expose areas that exactly match the size of one or multiple devices. In yet other embodiments, barriers are etched into the film, and even the underlying layer, to control heat transfer from one area to the next. In certain embodiments, the film is covered with a patterned capping layer before being irradiated. The film in the uncovered region is melted and the crystallographic lateral growth will proceed from the edges between the covered and uncovered regions. In another approach, melt-mediated explosive crystallization is used between the covered and uncovered regions.
[0007] In one embodiment, a method of irradiating a large area film with a pulsed light source includes providing a large area film on a substrate, covering at least a portion of the large area film with a covering material, wherein the covering material has one or more exposure areas that expose one or more sections of the film, irradiating the film and covering material with a pulsed light source under conditions to at least partially melt a portion of the film, wherein the irradiation area has a dimension at least substantially equal to a dimension of the film and the irradiating of the film causes crystallization to proceed from the interface between the exposed sections and the non-exposed sections of the film.
[0008] In one or more embodiments, the large area film has a length of greater than 1.3 meters and a width of greater than 1.5 meters or a length of greater than 1.5 meters and a width of greater than 1.8 meters. In some embodiments, one dimension of the irradiation area is greater than about 1.3 meters.
[0009] In one or more embodiments, the covering layer comprises a capping layer.
[0010] In one or more embodiment, the capping layer is deposited on the film, is a film, is at least one of absorptive and reflective, is metallic, and/or is opaque to the pulsed light source.
[0011] In one or more embodiments, the energy density of the FLA radiation is selected to induce at least one of lateral growth and explosive crystallization in the film.
[0012] In one or more embodiments, the pulsed light source is a flash lamp.
[0013] In one or more embodiments, the method includes providing an absorber layer between the film and the substrate, wherein the absorber layer absorbs the pulsed light source irradiation and the absorber layer can be metallic.
[0014] In one or more embodiments, the substrate is glass.
[0015] In one or more embodiments, the method includes removing a portion of the film prior to covering the film and/or removing a portion of the substrate below the portion of removed film.
[0016] In one or more embodiments, the method the film comprises a plurality of single crystal island segments.
[0017] In one or more embodiments, the method the covering comprises a proximity mask, wherein the proximity mask is located at a first position and covers only a first portion of the film and/or the proximity mask is opaque to the pulsed light source.
[0018] In one or more embodiments, the method includes moving the proximity mask to a second position, said second position covering a second portion of the film.
[0019] In one or more embodiments, the second portion of the film does not overlap the first portion of the film or the first section and the second section partially overlap.
[0020] In one or more embodiments, the method includes moving the mask comprises placing a second mask having a different configuration of openings over the film.
[0021] In one embodiment, a method of irradiating a large area film using a pulsed light source includes providing a large area film having a first dimension and a second dimension on a substrate, covering the film with a capping layer having a pattern, wherein the pattern exposes one or more sections of the film, irradiating the film with a pulsed light source under conditions to at least partially melt a first portion of the film while a second portion of the film remains solid, wherein the irradiation area has a dimension at least substantially equal to a dimension of the film, and re-solidifying the first portion of the film to form a crystalline portion thereby releasing heat to melt an adjacent portion of the film.
Brief Description of Drawings
[0022] FIG. 1 is a schematic illustration of a flash lamp apparatus that may be used, according to some embodiments of the disclosed subject matter.
[0023] FIG. 2A is a schematic of a thin film crystallization system implementing utilizing FLA and patterned capping layer for lateral growth, according to some embodiments of the disclosed subject matter.
[0024] FIG. 2B is a top view of the lateral growth in the capped film, according to some embodiments of the disclosed subject matter.
[0025] FIG. 2C is a schematic of a thin film crystallization system implementing FLA and patterned capping layer for explosive crystallization, according to some embodiments of the disclosed subject matter.
[0026] FIG. 2D is a top view of explosive crystallization in the capped film, according to some embodiments of the disclosed subject matter.
[0027] FIG. 3 is a schematic of a thin film crystallization system implementing shielding layers, according to some embodiments of the disclosed subject matter.
[0028] FIG. 4 sketches examples of the effect of lateral heat diffusion.
[0029] FIGs. 5A and 5B are schematics of a thin film crystallization system implementing heat flow isolation, according to some embodiments of the disclosed subject matter.
[0030] FIG. 6A is a schematic of a thin film crystallization system implementing proximity masks, according to some embodiments of the disclosed subject matter.
[0031] FIG. 6B is a schematic of a thin film crystallization system implementing proximity masks, according to some embodiments of the disclosed subject matter.
Detailed Description
[0032] The present application describes a general approach for applying the FLA process to obtain an ordered microstructure on large area thin films useful for device applications, such as active matrix liquid crystal displays (AMLCDs) or active matrix organic light emitting diode displays (AMOLEDs). Large area thin films, as discussed herein, refer to thin films having a length greater than 1.3 meters and a width greater than 1.5 meters. For example, large area thin films can be Gen 5.5 (1.3m x 1.5m or 1.32m x 1.5m), Gen 6 (1.5m x 1.8m or 1.5m x 1.85m), Gen 7 (1.87. x 2.2m or 1.95m x 2.25m), Gen 8 (2.16m x 2.46m or 2.2m x 2.5m), Gen 9 (2.2m x 2.6 m or 2.4m x 2.8m), or Gen 10 (2.6m x 3.1m) thin film panels. Several techniques of pulsed-radiation crystallization of thin films and lithography- based controlled super-lateral growth (C-SLG) are explained and utilized. Masking layers, lithography or other patterning techniques are used to create patterns, such as patterned cap layers, patterned silicon films, patterned underlayers, heat sinks, surface morphology, and thickness variations. These layers and structures are used to locally adjust the melting thresholds of the thin film. It will be apparent from the description that follows that the method is not limited to silicon thin film crystallization and may be practiced for any thin film. For the purposes of discussion that follows, unless specifically noted the methods may be used for any such material. It also will be apparent from the description that follows that other pulsed light sources may be used, so long as they also provide a pulsed divergent light source or a pulsed flood light and the desired control of the mixed phase partial melting process. Unless explicitly stated, flash lamp annealing or "FLA" is also meant to include diode lasers and other divergent pulsed light sources used as a "flash lamp."
[0033] However, the use of FLA techniques on glass substrates may introduce new challenges compared to the previous techniques. The pulse duration for FLA pulses can range from about 10 μs to about 10 ms or even longer. The upper boundary of the FLA pulse duration is considerably larger than the pulse durations in the commonly used pulsed-laser approaches, for which typical pulse durations vary from about ~30 ns to about 300 ns. As a
result, the heat diffusion length (SQRT(Dt)) is considerably larger for FLA. Thus, higher pulse energies are required to reach the desired degree of melting in the silicon film. This excess heat can lead to a higher degree of heating in the underlying substrate and therefore can result in melting or distortion of a glass substrate, if used. Therefore, it may be more challenging to implement FLA for films on glass or other high-temperature -intolerant substrates.
[0034] Flash laser annealing uses a flash lamp to produce white light over a wide wavelength range, e.g., 400-800 nm. The flash lamp is a gas-filled discharging lamp that produces intense, incoherent full-spectrum white light for very short durations. A flash lamp annealing apparatus uses white light energy for surface irradiation, in which the light is focused using, for example, an elliptical reflector to direct the light energy onto a substrate, such as is shown in FIG. 1. FIG. 1 is a simplified side view diagram representing a flash lamp reactor 100 with a reflecting device 110, in accordance with an embodiment of the present invention. The flash lamp reactor may include an array of flash lamps 120 located above a support 130, with a target area 150 situated between the two. The reflecting device 110 may be positioned above the flash lamps to reflect varying amount of radiation 160 from the flash lamps back towards different portions of a facing side of the target area. The target area may be adapted to receive a substrate (wafer).
[0035] The lamp power is supplied by a series of capacitors and inductors (not shown) that allow the formation of well defined flash pulses on a microsecond to millisecond scale. In a typical flash lamp, light energy densities in the range of up to 3-5 J/cm2 (for a 50 μs discharge) or 50-60 J/cm2 for a 1-20 ms discharge can be obtained. In exemplary embodiments, the light energy density can be about 2-150 J/cm2. Flash lamp annealing allows fast heating of solid surfaces with a single light flash between some tens microseconds and some tens milliseconds, e.g., 10 μs-100 ms. Variables of the flash lamp that affect the quality of thin film crystallization include the energy intensity of the incident light, as well as the pulse duration and shape of the light (which results in a certain dwell time, i.e., a duration of melting).
[0036] Because flash lamp irradiation is a flood irradiation process, the flash lamps can irradiate large areas of the substrate surface in a single pulse. It is possible that the entire film on a substrate, for example a glass panel, can be processed simultaneously. Thus, multi-pulse
operations in a scanned fashion to cover a large substrate area, for example, as used in laser- based recrystallization, are not required.
[0037] In one approach for processing large area thin films, shown in FIGs. 2A, a patterned capping layer 200 that is reflective, absorptive, or both, is provided on top of a thin film 210. The capping layer 200 can be a continuous film with a plurality of openings. The capping layer 210 can be substantially opaque to the irradiated light or reflective. The capping layer 210 can be a proximity mask or a deposited layer, for example, by using a lithography technique. Lithography techniques in FLA processing of thin films is disclosed in co-pending, PCT Serial No. PCT/US09/XXXX, entitled "Lithographic Method of Making Uniform Crystalline Si-Films," which is hereby incorporated by reference in its entirety. If the capping layer is reflective, it can be composed of any reflective material, for example, a metallic material, such as, e.g., aluminum. It may be desired to place a thin barrier layer such as, e.g., SiO2 between the metallic cap layer and the film to prevent metal diffusion.
[0038] In one embodiment, the film 210 is irradiated by using a flash lamp 220 at an energy density sufficient to melt the uncovered film but insufficient to completely melt the covered portion of the film. In this embodiment, lateral growth 230 of the crystalline structure will initiate at the edges between the covered and uncovered regions and propagate along arrow 230 to produce a crystalline material. Generally, Si grains tend to grow laterally from or perpendicular to interfaces between the liquid phase and solid phase silicon. Thus, when sections of the film 210 are irradiated and melted while other sections of the film 210 remain solid, the crystalline growth starts from the solid/liquid interface of the film 210 along arrow 230 and proceeds laterally along the film 210. This form of crystalline growth is called lateral growth. Lateral crystalline growth can produce large Si grains that can be used for device manufacture. Thus, devices can be made in the laterally grown regions of the thin film 210, i.e., the regions of the crystalline material in which the crystalline structure was formed as a result of lateral growth.
[0039] In yet another embodiment, the system can have one or more underlying absorber layers that can absorb the longer wavelength radiation, for example, longer than 600 nm, from the flash lamps. These absorber layers can be positioned between the thin film and the substrate or below the substrate. Because they preferentially absorb the longer wavelength radiation, the absorber layer will heat up first and can transfer the thermal energy from the radiation to the film to induce melting, while other regions in the film are heated by shorter
wavelength light only and may remain solid. Because the flash lamps provide broad spectrum light, this arrangement provides the most efficient capture of the full energy spectrum of the flash lamp radiation and also can permit the capture of radiation that is transparent to the Si. These absorbing layers can be composed of any heat absorbing material, for example a metallic substance, such as molybdenum.
[0040] In embodiments having the absorber layer, the silicon film can be irradiated from the top portion of the film. The flash lamp radiation irradiates the top portion of the film and penetrates through the thickness of the film to the absorber layer. In some instances, the majority of the light is absorbed by the absorber layer. This absorption heats the absorber layer, thus providing heat to the silicon film from the bottom and thus melting the thin film. Thus, the above embodiment offers ways of accurately defining the location of regions of lateral growth using a non-patterned light source.
[0041] In another approach, shown in FIG. 2C, a similar configuration of thin film 210 and cap layer 200 is used. However, the energy density of the flash lamp 220 is selected such that the covered portion film remains amorphous, while the uncovered portion of the film is at least partially molten. This situation triggers melt-mediated explosive crystallization 250. As the first section melted portion reforms as crystalline silicon, an exotherm is created by the energy being dissipated as heat from the silicon as the silicon forms a more thermodynamically stable crystalline form. As the amorphous material melts in the presence of the crystalline material, but the temperature of the liquid is still below the melting point of the crystalline material, the crystallizing materials will grow epitaxially. That exotherm is sufficient to melt adjacent amorphous silicon which itself then re-crystallizes as crystalline silicon and releases an additional amount of energy. An exotherm, therefore, propagates as a wave through the material from the region closest to amorphous/front and propagates throughout the amorphous section of the thin film, in the direction of the arrow 250.
[0042] Generally, the explosive crystallization process will continue until quenched or until all the amorphous material is transformed into crystalline material. Quenching is known to result in lowering of the temperature at the growth front and formation of defects and ultimately of halting of the process. Quenching is often the result of nearby conductive materials and/or nearby substrates.
[0043] The flash lamp annealing conditions are selected such that the explosive crystallization can continue laterally for a sufficient distance through the thin film. The heat generated at the crystallization front by explosive crystallization can result in (1) further melting of the amorphous Si in region 215, (2) diffusive heat loss into the a-Si in region 225 (which will can be used for heating of the a-Si towards the melting point), and (3) diffusive heat loss into the substrate. The further melting of the amorphous Si is what drives the explosive nature of the process, because it requires less heat than what is generated by the explosive crystallization process. If heat absorption to the substrate or a-Si region 225 becomes too large, then insufficient heat will be available to drive further melting of the a-Si, leading to quenching of the process. Therefore, pre-heating the a-Si and/or pre-heating the substrate can increase the explosive crystallization distance by reducing diffusive heat loss. Pre-heating mechanisms include use of a heated substrate, such as a hot plate and co- irradiation, in which one radiation is used for heating and a second irradiation is used for preheating. For example, the flash lamp energy can be such that the amorphous region is substantially heated by the beam, but not to the point that crystallization occurs. The heat deposited in the amorphous film permits the explosive crystallization process to proceed over a longer distance. Further, the absorber layer used in the lateral growth embodiments also can be used to induce explosive crystallization by heating the sections of a-Si and extending the explosive crystallization growth length.
[0044] Compared with lateral growth from the melt as shown in FIG. 2A, the irradiation used for triggered explosive crystallization may have a lower energy density. This is because lateral growth requires complete melting of the thin film, while explosive crystallization only requires at a minimum some partial melting. Conversely, for explosive crystallization only some melting needs to be triggered before the crystallization process proceeds. Therefore, because explosive crystallization can be triggered with only partial melting of the silicon, explosive crystallization can occur at lower temperature than lateral growth crystallization. Thus, because of the lower temperature, explosive crystallization techniques may be better suited to thin films on glass substrates.
[0045] However, in the explosive crystallization embodiment, the pattern of the capping layer on the film can be different from the capping layer pattern used for lateral growth. For example, when using reflective capping layers to prevent the thin film from melting, rectangular areas of the capping layer should cover the film where lateral explosive
crystallization is desired. However, the remainder of the film need not be entirely uncovered. In principle, it is enough to have just a narrow trench in the capping layer adjacent to the region where explosive crystallization is sought.
[0046] The above approaches also can be combined with the patterning of the silicon islands. The patterning of silicon islands is disclosed in co-pending PCT Application Serial No. PCT/US08/077199, filed on September 22, 2008, entitled "Collections of Laterally Crystallized Semiconductor Islands for Use in Thin Film Transistors and Systems and Methods for Making Same," the entire disclosure of which is incorporated by reference. The patterning of silicon islands can be used to create high quality TFTs by reducing the length of similarly oriented domains in a long laterally grown material, which can reduce intragrain defects. These oriented domains in the crystalline structure may lead to device non- uniformity when they are of a size comparable or larger than the size of the devices, and when there are different types of oriented domains that can co-exist, as may result from SLS or even a single-pulse process. In general, oriented domains can be created as a result of occlusion in lateral growth. FIGs. 2B and 2D show lateral growth 230 and explosive crystallization 250, respectively, in a plurality of striped patterned crystal islands 240 contained within a substrate 260. With the very long lateral growth distances, even in a single pulse, oriented domains may form that are too large for device manufacturing.
[0047] In another aspect, the present application pertains to increasing the compatibility of the FLA process with films on glass substrates. In some embodiments, as shown in FIG. 3, a shielding layer 300 (e.g., a layer that is reflective or absorptive or both reflective and absorptive) is deposited on the film 310, which rests on a substrate 315, and openings 320 are etched in the shielding layer 300 corresponding to regions in the film 320 where TFT channel regions will be fabricated. This method can be used for pixel TFTs where the density of the devices is relatively low. As a result, the substrate 315, and the thin film 310 which may be patterned and/or composed of silicon, will be largely shielded from the beam. The small pockets of heating may lead to local "over-heating" of the substrate 315, but the resultant stresses will be localized and therefore less harmful to the substrate 315.
[0048] Furthermore, as shown in FIG. 4, because of the increased heat diffusion in the lateral direction, it may also be more challenging to crystallize well-defined regions in the film without considerable "smearing" of the crystallized region by lateral crystallization away from the irradiated region, which includes a large grain region 404 and a narrow small grain
region 402 at the edge of the irradiated region. The cut-off or transition between crystallized and amorphous Si is "smeared" because of the formation of an extended region crystallized via explosive crystallization 400, as brought about by the long heat diffusion length effects addressed above. In addition, some smearing also may result from fluence gradients, which are non-sharp transitions between light and dark regions that may exist at the edges of radiation beams, as shown in the beam profile 406 in FIG. 4, as a result of poor projection properties of the light or even the absence of such optics. This leads to an increased degree of smearing. In sum, wide edge regions may exist in which non-uniform microstructures can be created. These regions will have different optical properties from the surrounding amorphous regions and will likely have a different melting threshold, making subsequent processing more difficult. As a result, closely- spaced radiations of the film in order to fully crystallize with minimized edge regions may not be possible. Therefore, a full irradiation of the film would be preferred.
[0049] Therefore, in some embodiments, for example, shown in FIGs. 5A and 5B, the unwanted lateral crystallization can be reduced by providing barriers for lateral heat flow at the edges of the radiated region of a thin film 500 on a substrate 505. The barriers or isolation of the film can be provided by etching the thin film 500 or by also etching the underlying layers, for example, a buffer layer 510 (as shown in FIG. 5A). The etching of the thin film can reduce irradiation heat transfer between a first section 501, a second section 502 and a third section 503. However, some heat may be transferred through the substrate. Therefore, as shown in FIG. 5B, the substrate 505 can have one or more trenches 515. These trenches 515 can further reduce heat flow between the first section 501, the second section 502 and the third sections 503, thereby further limiting unwanted lateral crystallization. Such trenches 515 can be made using conventional etching techniques or even laser scribing techniques.
[0050] This embodiment can prevent non-sharp/smeared crystallized domains, as shown in FIG. 4. In other embodiments, because of long heat diffusion length, wide edges that are non-uniformly crystallized can form, which may prevent close tiling. For example, once a region is crystallized via explosive crystallization, the optimum energy to induce mixed phase solidification, as described in co-pending, PCT Application Serial No. PCT/US09/xxx, filed on even date herewith, titled "Flash Light Annealing for Thin Films," has shifted and a next radiation may thus not lead to MPS in those explosive crystallization regions. The process
shown in FIG. 5 allows for more sharply defined crystallized regions and can alleviate these problems. In some embodiments, this approach can be combined with the other embodiments disclosed herein, including the use of capping layers, underlying absorbing films, and/or proximity masks.
[0051] In other embodiments, for example shown in FIGs. 6A and 6B, the effect of the edge regions as shown in FIG. 4 in subsequently made devices, e.g., displays, can be reduced by using proximity masks 600. As shown in FIG. 6 A a proximity mask 600 may be used to expose areas 620 of the thin film 605 to the FLA radiation produced by the flash lamps 615 that exactly match the size of one or multiple display(s) or other device(s) or are relatively close in size to such displays or devices. One or multiple radiations may be performed with the proximity mask. The proximity mask 600 should be composed of a material that is substantially opaque to the incident light. Exemplary mask materials include, but are not limited to, metallic substrates. Subsequently, as shown in FIG. 6B, the proximity mask may be moved or replaced by second proximity mask 610 to irradiate other regions 625 corresponding to one or more displays or devices. This process may be repeated several times until the location of all devices on the panel have been irradiated. In typical embodiments, as few as two iterations may be sufficient. In some embodiments, the mask can be different from the capping layer discussed above. The flash lamp uses divergent light, therefore, it does not lend itself well for overlapped radiation that leads to extended lateral growth. Rather, the entire film is radiated (or large regions thereof). The proximity mask divides the film into sections to limit the heating of the substrate on any given pulse. Thus, the surface of the film is being tiled. However, some overlapping radiations can result in continuous microstructure, but more likely that is not the case, and, for example, some lateral growth may occur on the edges. In that case, care must be taken to not make devices from those edge regions. This can be possible using alignment techniques.
[0052] Upon review of the description and embodiments of the present invention, those skilled in the art will understand that modifications and equivalent substitutions may be performed in carrying out the invention without departing from the essence of the invention. Thus, the invention is not meant to be limiting by the embodiments described explicitly above, and is limited only by the claims which follow. Further, the features of the disclosed embodiments can be combined, rearranged, etc. within the scope of the invention to produce additional embodiments.
Claims
1. A method of irradiating a large area film with a pulsed light source comprising:
providing a large area film, having a first dimension and a second dimension, on a substrate;
covering at least a portion of the film with a covering material, wherein the covering material has one or more exposure areas that expose one or more sections of the film; and
irradiating the film and covering material with a pulsed light source under conditions to at least partially melt a portion of the film, wherein the irradiation area has a dimension at least substantially equal to a dimension of the film and the irradiating of the film causes crystallization to proceed from the interface between the exposed sections and the non- exposed sections of the film.
2. The method of claim 1 , wherein the large area film has a length of greater than 1.3 meters and a width of greater than 1.5 meters.
3. The method of claim 1 , wherein the large area film has a length of greater than 1.5 meters and a width of greater than 1.8 meters.
4. The method of claim 1 , wherein one dimension of the irradiation area is greater than 1.3 meters.
5. The method of claim 1, wherein the covering layer comprises a capping layer.
6. The method of claim 4, wherein the capping layer is deposited on the film.
7. The method of claim 4, wherein the capping layer comprises a film.
8. The method of claim 4, wherein the capping layer is at least one of absorptive, reflective, and opaque to the pulsed light source.
9. The method of claim 8, wherein the capping layer is metallic.
10. The method of claim 1, wherein the energy density of the FLA radiation is selected to induce at least one of lateral growth and explosive crystallization in the film.
11. The method of claim 1 , wherein the pulsed light source is a flash lamp.
12. The method of claim 1 , further comprising providing an absorber layer between the film and the substrate, wherein the absorber layer absorbs the pulsed light source irradiation.
13. The method of claim 12, wherein the absorber layer is metallic.
14. The method of claim 1, wherein the substrate is glass.
15. The method of claim 1 , further comprising removing a portion of the film prior to covering the film.
16. The method of claim 15, further comprising removing a portion of the substrate below the portion of removed film.
17. The method of claim 1 , wherein the film comprises a plurality of single crystal island segments.
18. The method of claim 1 , wherein the covering comprises a proximity mask, wherein the proximity mask is located at a first position and covers only a first portion of the film.
19. The method of claim 18, wherein the proximity mask is opaque to the pulsed light source.
20. The method of claim 18, further comprising:
moving the proximity mask to a second position, said second position covering a second portion of the film.
21. The method of claim 18, wherein the second portion of the film does not overlap the first portion of the film
22. The method of claim 18, wherein the first section and the second section partially overlap.
23. The method of claim 18, wherein moving the mask comprises placing a second mask having a different configuration of openings over the film.
24. A method of irradiating a large area film using a pulsed light source comprising:
providing a large area film, having a first dimension and a second dimension, on a substrate; covering the film with a capping layer having a pattern, wherein the pattern exposes one or more sections of the film; irradiating the film with a pulsed light source under conditions to at least partially melt a first portion of the film while a second portion of the film remains solid, wherein the irradiation area has a dimension at least substantially equal to a dimension of the film; and re-solidifying the first portion of the film to form a crystalline portion thereby releasing heat to melt an adjacent portion of the film.
25. A large area film produced by the method of claim 1.
26. A large area film produced by the method of claim 24.
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Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2012140253A1 (en) * | 2011-04-15 | 2012-10-18 | Von Ardenne Anlagentechnik Gmbh | Method and device for thermally treating substrates |
DE102013100520A1 (en) | 2012-12-28 | 2014-07-03 | Von Ardenne Anlagentechnik Gmbh | Flashlamp arrangement for illuminating substrate, has single ignition electrode for external ignition of entire flashlamps and is arranged in lamp housing, where ignition electrode is so formed that all flash lamps ignite simultaneously |
DE102013206486A1 (en) | 2013-04-11 | 2014-10-16 | Von Ardenne Gmbh | Flash lamp assembly and method for igniting same |
WO2015127036A1 (en) * | 2014-02-19 | 2015-08-27 | The Trustees Of Columbia University In The City Of New York | Methods and systems for controlled lateral solidification |
WO2015135904A1 (en) * | 2014-03-12 | 2015-09-17 | Von Ardenne Gmbh | Processing assembly and method for operating a processing assembly |
US9466402B2 (en) | 2003-09-16 | 2016-10-11 | The Trustees Of Columbia University In The City Of New York | Processes and systems for laser crystallization processing of film regions on a substrate utilizing a line-type beam, and structures of such film regions |
Families Citing this family (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR100901343B1 (en) * | 2007-07-23 | 2009-06-05 | (주)실리콘화일 | Method of manufacturing crystalline semiconductor thin film |
FR3025936B1 (en) * | 2014-09-11 | 2016-12-02 | Saint Gobain | METHOD FOR RECLAIMING FLASH LAMPS |
CN106898540B (en) * | 2015-12-17 | 2020-01-31 | 宸鸿光电科技股份有限公司 | Semiconductor manufacturing method |
US10526242B2 (en) * | 2016-07-11 | 2020-01-07 | Guardian Glass, LLC | Coated article supporting titanium-based coating, and method of making the same |
GB2566477A (en) * | 2017-09-14 | 2019-03-20 | Nat Univ Ireland Galway | Method of processing a target material |
CN111092017A (en) * | 2018-10-23 | 2020-05-01 | 宸鸿光电科技股份有限公司 | Method for manufacturing thin film element |
CN111092124A (en) * | 2018-10-23 | 2020-05-01 | 宸鸿光电科技股份有限公司 | Semiconductor device and method for manufacturing the same |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20050112906A1 (en) * | 2003-10-28 | 2005-05-26 | Semiconductor Energy Laboratory Co., Ltd. | Methods for forming wiring and manufacturing thin film transistor and droplet discharging method |
US20060035478A1 (en) * | 2004-08-10 | 2006-02-16 | Lg Philips Lcd Co., Ltd. | Variable mask device for crystallizing silicon layer and method for crystallizing using the same |
US7183229B2 (en) * | 2000-12-08 | 2007-02-27 | Sony Corporation | Semiconductor thin film forming method, production methods for semiconductor device and electrooptical device, devices used for these methods, and semiconductor device and electrooptical device |
US7326876B2 (en) * | 2003-06-30 | 2008-02-05 | Lg.Philips Lcd Co., Ltd. | Sequential lateral solidification device |
Family Cites Families (239)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2030468A5 (en) * | 1969-01-29 | 1970-11-13 | Thomson Brandt Csf | |
US4234358A (en) | 1979-04-05 | 1980-11-18 | Western Electric Company, Inc. | Patterned epitaxial regrowth using overlapping pulsed irradiation |
US4309225A (en) * | 1979-09-13 | 1982-01-05 | Massachusetts Institute Of Technology | Method of crystallizing amorphous material with a moving energy beam |
DE3177084D1 (en) * | 1980-04-10 | 1989-09-21 | Massachusetts Inst Technology | Method of producing sheets of crystalline material |
US4382658A (en) * | 1980-11-24 | 1983-05-10 | Hughes Aircraft Company | Use of polysilicon for smoothing of liquid crystal MOS displays |
US4456371A (en) | 1982-06-30 | 1984-06-26 | International Business Machines Corporation | Optical projection printing threshold leveling arrangement |
US4691983A (en) | 1983-10-14 | 1987-09-08 | Hitachi, Ltd. | Optical waveguide and method for making the same |
US4639277A (en) * | 1984-07-02 | 1987-01-27 | Eastman Kodak Company | Semiconductor material on a substrate, said substrate comprising, in order, a layer of organic polymer, a layer of metal or metal alloy and a layer of dielectric material |
JPH084067B2 (en) | 1985-10-07 | 1996-01-17 | 工業技術院長 | Method for manufacturing semiconductor device |
JPH0732124B2 (en) | 1986-01-24 | 1995-04-10 | シャープ株式会社 | Method for manufacturing semiconductor device |
US4793694A (en) | 1986-04-23 | 1988-12-27 | Quantronix Corporation | Method and apparatus for laser beam homogenization |
JPS62293740A (en) * | 1986-06-13 | 1987-12-21 | Fujitsu Ltd | Manufacture of semiconductor device |
US4758533A (en) | 1987-09-22 | 1988-07-19 | Xmr Inc. | Laser planarization of nonrefractory metal during integrated circuit fabrication |
USRE33836E (en) * | 1987-10-22 | 1992-03-03 | Mrs Technology, Inc. | Apparatus and method for making large area electronic devices, such as flat panel displays and the like, using correlated, aligned dual optical systems |
US5204659A (en) * | 1987-11-13 | 1993-04-20 | Honeywell Inc. | Apparatus and method for providing a gray scale in liquid crystal flat panel displays |
JPH01256114A (en) | 1988-04-06 | 1989-10-12 | Hitachi Ltd | Laser annealing method |
JP2569711B2 (en) | 1988-04-07 | 1997-01-08 | 株式会社ニコン | Exposure control device and exposure method using the same |
US5523193A (en) | 1988-05-31 | 1996-06-04 | Texas Instruments Incorporated | Method and apparatus for patterning and imaging member |
JP2706469B2 (en) | 1988-06-01 | 1998-01-28 | 松下電器産業株式会社 | Method for manufacturing semiconductor device |
US4940505A (en) | 1988-12-02 | 1990-07-10 | Eaton Corporation | Method for growing single crystalline silicon with intermediate bonding agent and combined thermal and photolytic activation |
US5076667A (en) | 1990-01-29 | 1991-12-31 | David Sarnoff Research Center, Inc. | High speed signal and power supply bussing for liquid crystal displays |
JP2802449B2 (en) | 1990-02-16 | 1998-09-24 | 三菱電機株式会社 | Method for manufacturing semiconductor device |
US5247375A (en) | 1990-03-09 | 1993-09-21 | Hitachi, Ltd. | Display device, manufacturing method thereof and display panel |
US5233207A (en) | 1990-06-25 | 1993-08-03 | Nippon Steel Corporation | MOS semiconductor device formed on insulator |
JP2973492B2 (en) | 1990-08-22 | 1999-11-08 | ソニー株式会社 | Crystallization method of semiconductor thin film |
US5032233A (en) | 1990-09-05 | 1991-07-16 | Micron Technology, Inc. | Method for improving step coverage of a metallization layer on an integrated circuit by use of a high melting point metal as an anti-reflective coating during laser planarization |
KR920010885A (en) * | 1990-11-30 | 1992-06-27 | 카나이 쯔또무 | Thin film semiconductor, manufacturing method and manufacturing apparatus and image processing apparatus |
US5173441A (en) | 1991-02-08 | 1992-12-22 | Micron Technology, Inc. | Laser ablation deposition process for semiconductor manufacture |
CA2061796C (en) * | 1991-03-28 | 2002-12-24 | Kalluri R. Sarma | High mobility integrated drivers for active matrix displays |
JP3213338B2 (en) * | 1991-05-15 | 2001-10-02 | 株式会社リコー | Manufacturing method of thin film semiconductor device |
US5373803A (en) | 1991-10-04 | 1994-12-20 | Sony Corporation | Method of epitaxial growth of semiconductor |
US5485019A (en) | 1992-02-05 | 1996-01-16 | Semiconductor Energy Laboratory Co., Ltd. | Semiconductor device and method for forming the same |
US5424244A (en) * | 1992-03-26 | 1995-06-13 | Semiconductor Energy Laboratory Co., Ltd. | Process for laser processing and apparatus for use in the same |
JP2572003B2 (en) | 1992-03-30 | 1997-01-16 | 三星電子株式会社 | Method of manufacturing thin film transistor having three-dimensional multi-channel structure |
US5285236A (en) * | 1992-09-30 | 1994-02-08 | Kanti Jain | Large-area, high-throughput, high-resolution projection imaging system |
US5291240A (en) * | 1992-10-27 | 1994-03-01 | Anvik Corporation | Nonlinearity-compensated large-area patterning system |
JPH06177034A (en) | 1992-12-03 | 1994-06-24 | Sony Corp | Semiconductor single crystal growth method |
JP3587537B2 (en) | 1992-12-09 | 2004-11-10 | 株式会社半導体エネルギー研究所 | Semiconductor device |
US5444302A (en) | 1992-12-25 | 1995-08-22 | Hitachi, Ltd. | Semiconductor device including multi-layer conductive thin film of polycrystalline material |
JP3599355B2 (en) | 1993-03-04 | 2004-12-08 | セイコーエプソン株式会社 | Method for manufacturing active matrix substrate and method for manufacturing liquid crystal display |
JPH076960A (en) * | 1993-06-16 | 1995-01-10 | Fuji Electric Co Ltd | Forming method of polycrystalline semiconductor thin film |
US5453594A (en) | 1993-10-06 | 1995-09-26 | Electro Scientific Industries, Inc. | Radiation beam position and emission coordination system |
US5395481A (en) * | 1993-10-18 | 1995-03-07 | Regents Of The University Of California | Method for forming silicon on a glass substrate |
KR100299292B1 (en) | 1993-11-02 | 2001-12-01 | 이데이 노부유끼 | Polysilicon Thin Film Forming Method and Surface Treatment Apparatus |
JP2646977B2 (en) * | 1993-11-29 | 1997-08-27 | 日本電気株式会社 | Method for manufacturing forward staggered thin film transistor |
US5496768A (en) * | 1993-12-03 | 1996-03-05 | Casio Computer Co., Ltd. | Method of manufacturing polycrystalline silicon thin film |
US6130009A (en) | 1994-01-03 | 2000-10-10 | Litel Instruments | Apparatus and process for nozzle production utilizing computer generated holograms |
JPH07249591A (en) * | 1994-03-14 | 1995-09-26 | Matsushita Electric Ind Co Ltd | Laser annealing method for semiconductor thin film and thin-film semiconductor element |
US5456763A (en) | 1994-03-29 | 1995-10-10 | The Regents Of The University Of California | Solar cells utilizing pulsed-energy crystallized microcrystalline/polycrystalline silicon |
JP3072005B2 (en) * | 1994-08-25 | 2000-07-31 | シャープ株式会社 | Semiconductor device and manufacturing method thereof |
US5756364A (en) * | 1994-11-29 | 1998-05-26 | Semiconductor Energy Laboratory Co., Ltd. | Laser processing method of semiconductor device using a catalyst |
TW303526B (en) | 1994-12-27 | 1997-04-21 | Matsushita Electric Ind Co Ltd | |
US5844588A (en) | 1995-01-11 | 1998-12-01 | Texas Instruments Incorporated | DMD modulated continuous wave light source for xerographic printer |
JPH08236443A (en) | 1995-02-28 | 1996-09-13 | Fuji Xerox Co Ltd | Semiconductor crystal growing method and semiconductor manufacturing device |
WO1996033839A1 (en) | 1995-04-26 | 1996-10-31 | Minnesota Mining And Manufacturing Company | Method and apparatus for step and repeat exposures |
US5742426A (en) * | 1995-05-25 | 1998-04-21 | York; Kenneth K. | Laser beam treatment pattern smoothing device and laser beam treatment pattern modulator |
TW297138B (en) | 1995-05-31 | 1997-02-01 | Handotai Energy Kenkyusho Kk | |
US6524977B1 (en) * | 1995-07-25 | 2003-02-25 | Semiconductor Energy Laboratory Co., Ltd. | Method of laser annealing using linear beam having quasi-trapezoidal energy profile for increased depth of focus |
US5721606A (en) * | 1995-09-07 | 1998-02-24 | Jain; Kanti | Large-area, high-throughput, high-resolution, scan-and-repeat, projection patterning system employing sub-full mask |
JP3348334B2 (en) | 1995-09-19 | 2002-11-20 | ソニー株式会社 | Method for manufacturing thin film semiconductor device |
KR19990063832A (en) * | 1995-09-29 | 1999-07-26 | 세이즈 테크놀러지, 인코오포레이티드 | Optical digital media recording and playback system |
US6444506B1 (en) | 1995-10-25 | 2002-09-03 | Semiconductor Energy Laboratory Co., Ltd. | Method of manufacturing silicon thin film devices using laser annealing in a hydrogen mixture gas followed by nitride formation |
US5817548A (en) | 1995-11-10 | 1998-10-06 | Sony Corporation | Method for fabricating thin film transistor device |
US6136632A (en) | 1995-12-26 | 2000-10-24 | Seiko Epson Corporation | Active matrix substrate, method of producing an active matrix substrate, liquid crystal display device, and electronic equipment |
US5858807A (en) * | 1996-01-17 | 1999-01-12 | Kabushiki Kaisha Toshiba | Method of manufacturing liquid crystal display device |
JP3240258B2 (en) | 1996-03-21 | 2001-12-17 | シャープ株式会社 | Semiconductor device, thin film transistor and method for manufacturing the same, and liquid crystal display device and method for manufacturing the same |
JPH09270393A (en) | 1996-03-29 | 1997-10-14 | Sanyo Electric Co Ltd | Laser light irradiation device |
US5997642A (en) * | 1996-05-21 | 1999-12-07 | Symetrix Corporation | Method and apparatus for misted deposition of integrated circuit quality thin films |
US6555449B1 (en) * | 1996-05-28 | 2003-04-29 | Trustees Of Columbia University In The City Of New York | Methods for producing uniform large-grained and grain boundary location manipulated polycrystalline thin film semiconductors using sequential lateral solidfication |
CA2256699C (en) | 1996-05-28 | 2003-02-25 | The Trustees Of Columbia University In The City Of New York | Crystallization processing of semiconductor film regions on a substrate, and devices made therewith |
JPH09321310A (en) | 1996-05-31 | 1997-12-12 | Sanyo Electric Co Ltd | Manufacture of semiconductor device |
JP3306300B2 (en) | 1996-06-20 | 2002-07-24 | 三洋電機株式会社 | Laser annealing method for semiconductor film |
JP3917698B2 (en) * | 1996-12-12 | 2007-05-23 | 株式会社半導体エネルギー研究所 | Laser annealing method and laser annealing apparatus |
US5861991A (en) * | 1996-12-19 | 1999-01-19 | Xerox Corporation | Laser beam conditioner using partially reflective mirrors |
US6020244A (en) * | 1996-12-30 | 2000-02-01 | Intel Corporation | Channel dopant implantation with automatic compensation for variations in critical dimension |
US5986807A (en) | 1997-01-13 | 1999-11-16 | Xerox Corporation | Single binary optical element beam homogenizer |
US6455359B1 (en) | 1997-02-13 | 2002-09-24 | Semiconductor Energy Laboratory Co., Ltd. | Laser-irradiation method and laser-irradiation device |
JP4056577B2 (en) * | 1997-02-28 | 2008-03-05 | 株式会社半導体エネルギー研究所 | Laser irradiation method |
JPH10244390A (en) | 1997-03-04 | 1998-09-14 | Toshiba Corp | Laser machining method and its device |
JP4086932B2 (en) | 1997-04-17 | 2008-05-14 | 株式会社半導体エネルギー研究所 | Laser irradiation apparatus and laser processing method |
US6060327A (en) | 1997-05-14 | 2000-05-09 | Keensense, Inc. | Molecular wire injection sensors |
JP3642546B2 (en) | 1997-08-12 | 2005-04-27 | 株式会社東芝 | Method for producing polycrystalline semiconductor thin film |
US6014944A (en) * | 1997-09-19 | 2000-01-18 | The United States Of America As Represented By The Secretary Of The Navy | Apparatus for improving crystalline thin films with a contoured beam pulsed laser |
JP3943245B2 (en) | 1997-09-20 | 2007-07-11 | 株式会社半導体エネルギー研究所 | Semiconductor device |
JP3462053B2 (en) * | 1997-09-30 | 2003-11-05 | 株式会社半導体エネルギー研究所 | Beam homogenizer, laser irradiation apparatus, laser irradiation method, and semiconductor device |
JPH11186189A (en) * | 1997-12-17 | 1999-07-09 | Semiconductor Energy Lab Co Ltd | Laser irradiation equipment |
EP1049144A4 (en) * | 1997-12-17 | 2006-12-06 | Matsushita Electronics Corp | Semiconductor thin film, method of producing the same, apparatus for producing the same, semiconductor device and method of producing the same |
TW466772B (en) | 1997-12-26 | 2001-12-01 | Seiko Epson Corp | Method for producing silicon oxide film, method for making semiconductor device, semiconductor device, display, and infrared irradiating device |
KR100284708B1 (en) * | 1998-01-24 | 2001-04-02 | 구본준, 론 위라하디락사 | How to crystallize silicon thin film |
JP3807576B2 (en) | 1998-01-28 | 2006-08-09 | シャープ株式会社 | Polymerizable compound, polymerizable resin material composition, polymerized cured product, and liquid crystal display device |
JPH11297852A (en) | 1998-04-14 | 1999-10-29 | Sony Corp | Semiconductor device and manufacture thereof |
JP2000066133A (en) * | 1998-06-08 | 2000-03-03 | Sanyo Electric Co Ltd | Laser light irradiation device |
KR100296110B1 (en) | 1998-06-09 | 2001-08-07 | 구본준, 론 위라하디락사 | Method of manufacturing thin film transistor |
KR100292048B1 (en) | 1998-06-09 | 2001-07-12 | 구본준, 론 위라하디락사 | Manufacturing Method of Thin Film Transistor Liquid Crystal Display |
US6326286B1 (en) | 1998-06-09 | 2001-12-04 | Lg. Philips Lcd Co., Ltd. | Method for crystallizing amorphous silicon layer |
KR100296109B1 (en) | 1998-06-09 | 2001-10-26 | 구본준, 론 위라하디락사 | Thin Film Transistor Manufacturing Method |
JP2000010058A (en) * | 1998-06-18 | 2000-01-14 | Hamamatsu Photonics Kk | Spatial light modulating device |
WO2000002251A1 (en) | 1998-07-06 | 2000-01-13 | Matsushita Electric Industrial Co., Ltd. | Thin film transistor and liquid crystal display |
US6555422B1 (en) * | 1998-07-07 | 2003-04-29 | Semiconductor Energy Laboratory Co., Ltd. | Thin film transistor and method of manufacturing the same |
US6072631A (en) | 1998-07-09 | 2000-06-06 | 3M Innovative Properties Company | Diffractive homogenizer with compensation for spatial coherence |
US6246524B1 (en) | 1998-07-13 | 2001-06-12 | Semiconductor Energy Laboratory Co., Ltd. | Beam homogenizer, laser irradiation apparatus, laser irradiation method, and method of manufacturing semiconductor device |
US6346437B1 (en) | 1998-07-16 | 2002-02-12 | Sharp Laboratories Of America, Inc. | Single crystal TFT from continuous transition metal delivery method |
JP3156776B2 (en) * | 1998-08-03 | 2001-04-16 | 日本電気株式会社 | Laser irradiation method |
DE19839718A1 (en) | 1998-09-01 | 2000-03-02 | Strunk Horst P | Laser crystallization or crystal structure alteration of amorphous or polycrystalline semiconductor layers comprises paired laser pulse irradiation for extended melt time while maintaining a low substrate temperature |
GB9819338D0 (en) * | 1998-09-04 | 1998-10-28 | Philips Electronics Nv | Laser crystallisation of thin films |
EP1744349A3 (en) | 1998-10-05 | 2007-04-04 | Semiconductor Energy Laboratory Co., Ltd. | Laser irradiation apparatus, laser irradiation method, beam homogenizer, semiconductor device, and method of manufacturing the semiconductor device |
US6326186B1 (en) | 1998-10-15 | 2001-12-04 | Novozymes A/S | Method for reducing amino acid biosynthesis inhibiting effects of a sulfonyl-urea based compound |
US6081381A (en) | 1998-10-26 | 2000-06-27 | Polametrics, Inc. | Apparatus and method for reducing spatial coherence and for improving uniformity of a light beam emitted from a coherent light source |
US6313435B1 (en) | 1998-11-20 | 2001-11-06 | 3M Innovative Properties Company | Mask orbiting for laser ablated feature formation |
US6120976A (en) | 1998-11-20 | 2000-09-19 | 3M Innovative Properties Company | Laser ablated feature formation method |
KR100290787B1 (en) | 1998-12-26 | 2001-07-12 | 박종섭 | Manufacturing Method of Semiconductor Memory Device |
TW457553B (en) | 1999-01-08 | 2001-10-01 | Sony Corp | Process for producing thin film semiconductor device and laser irradiation apparatus |
JP2000208771A (en) | 1999-01-11 | 2000-07-28 | Hitachi Ltd | Semiconductor device, liquid cystal display device, and their manufacturing |
US6203952B1 (en) * | 1999-01-14 | 2001-03-20 | 3M Innovative Properties Company | Imaged article on polymeric substrate |
US6162711A (en) | 1999-01-15 | 2000-12-19 | Lucent Technologies, Inc. | In-situ boron doped polysilicon with dual layer and dual grain structure for use in integrated circuits manufacturing |
TW444247B (en) * | 1999-01-29 | 2001-07-01 | Toshiba Corp | Laser beam irradiating device, manufacture of non-single crystal semiconductor film, and manufacture of liquid crystal display device |
JP3161450B2 (en) | 1999-02-02 | 2001-04-25 | 日本電気株式会社 | Substrate processing apparatus, gas supply method, and laser light supply method |
US6535535B1 (en) * | 1999-02-12 | 2003-03-18 | Semiconductor Energy Laboratory Co., Ltd. | Laser irradiation method, laser irradiation apparatus, and semiconductor device |
ATE332567T1 (en) | 1999-03-01 | 2006-07-15 | Fuji Photo Film Co Ltd | PHOTOELECTROCHEMICAL CELL WITH AN ELECTROLYTE MADE OF LIQUID CRYSTAL COMPOUNDS |
US6393042B1 (en) | 1999-03-08 | 2002-05-21 | Semiconductor Energy Laboratory Co., Ltd. | Beam homogenizer and laser irradiation apparatus |
US6493042B1 (en) | 1999-03-18 | 2002-12-10 | Xerox Corporation | Feature based hierarchical video segmentation |
JP4403599B2 (en) | 1999-04-19 | 2010-01-27 | ソニー株式会社 | Semiconductor thin film crystallization method, laser irradiation apparatus, thin film transistor manufacturing method, and display apparatus manufacturing method |
JP2000315652A (en) | 1999-04-30 | 2000-11-14 | Sony Corp | Method for crystalizing semiconductor thin film and laser irradiation device |
JP2000346618A (en) | 1999-06-08 | 2000-12-15 | Sumitomo Heavy Ind Ltd | Method and apparatus for precise alignment for rectangular beam |
JP3562389B2 (en) | 1999-06-25 | 2004-09-08 | 三菱電機株式会社 | Laser heat treatment equipment |
KR100327087B1 (en) | 1999-06-28 | 2002-03-13 | 구본준, 론 위라하디락사 | Laser annealing method |
JP2001023918A (en) | 1999-07-08 | 2001-01-26 | Nec Corp | Semiconductor thin-film forming apparatus |
JP4322359B2 (en) | 1999-07-08 | 2009-08-26 | 住友重機械工業株式会社 | Laser processing equipment |
JP2001023899A (en) | 1999-07-13 | 2001-01-26 | Hitachi Ltd | Semiconductor thin film, liquid crystal display device provided with the same, and manufacture of the film |
JP3422290B2 (en) | 1999-07-22 | 2003-06-30 | 日本電気株式会社 | Manufacturing method of semiconductor thin film |
US6190985B1 (en) * | 1999-08-17 | 2001-02-20 | Advanced Micro Devices, Inc. | Practical way to remove heat from SOI devices |
US6599788B1 (en) | 1999-08-18 | 2003-07-29 | Semiconductor Energy Laboratory Co., Ltd. | Semiconductor device and method of fabricating the same |
TW457732B (en) | 1999-08-27 | 2001-10-01 | Lumileds Lighting Bv | Luminaire, optical element and method of illuminating an object |
US6573531B1 (en) | 1999-09-03 | 2003-06-03 | The Trustees Of Columbia University In The City Of New York | Systems and methods using sequential lateral solidification for producing single or polycrystalline silicon thin films at low temperatures |
JP2001144170A (en) | 1999-11-11 | 2001-05-25 | Mitsubishi Electric Corp | Semiconductor device and manufacturing method therefor |
US6368945B1 (en) | 2000-03-16 | 2002-04-09 | The Trustees Of Columbia University In The City Of New York | Method and system for providing a continuous motion sequential lateral solidification |
US6830993B1 (en) | 2000-03-21 | 2004-12-14 | The Trustees Of Columbia University In The City Of New York | Surface planarization of thin silicon films during and after processing by the sequential lateral solidification method |
US6531681B1 (en) * | 2000-03-27 | 2003-03-11 | Ultratech Stepper, Inc. | Apparatus having line source of radiant energy for exposing a substrate |
US6274488B1 (en) | 2000-04-12 | 2001-08-14 | Ultratech Stepper, Inc. | Method of forming a silicide region in a Si substrate and a device having same |
GB0009280D0 (en) | 2000-04-15 | 2000-05-31 | Koninkl Philips Electronics Nv | Method of cystallising a semiconductor film |
JP4588167B2 (en) * | 2000-05-12 | 2010-11-24 | 株式会社半導体エネルギー研究所 | Method for manufacturing semiconductor device |
US6521492B2 (en) * | 2000-06-12 | 2003-02-18 | Seiko Epson Corporation | Thin-film semiconductor device fabrication method |
US6577380B1 (en) | 2000-07-21 | 2003-06-10 | Anvik Corporation | High-throughput materials processing system |
TW452892B (en) | 2000-08-09 | 2001-09-01 | Lin Jing Wei | Re-crystallization method of polysilicon thin film of thin film transistor |
US6451631B1 (en) | 2000-08-10 | 2002-09-17 | Hitachi America, Ltd. | Thin film crystal growth by laser annealing |
US6737672B2 (en) | 2000-08-25 | 2004-05-18 | Fujitsu Limited | Semiconductor device, manufacturing method thereof, and semiconductor manufacturing apparatus |
DE10042733A1 (en) | 2000-08-31 | 2002-03-28 | Inst Physikalische Hochtech Ev | Multicrystalline laser-crystallized silicon thin-film solar cell on a transparent substrate |
US20020151115A1 (en) | 2000-09-05 | 2002-10-17 | Sony Corporation | Process for production of thin film, semiconductor thin film, semiconductor device, process for production of semiconductor thin film, and apparatus for production of semiconductor thin film |
US6445359B1 (en) | 2000-09-29 | 2002-09-03 | Hughes Electronics Corporation | Low noise block down converter adapter with built-in multi-switch for a satellite dish antenna |
JP4216068B2 (en) | 2000-10-06 | 2009-01-28 | 三菱電機株式会社 | Polycrystalline silicon film manufacturing method and manufacturing apparatus, and semiconductor device manufacturing method |
EP1259985A2 (en) * | 2000-10-10 | 2002-11-27 | The Trustees Of Columbia University In The City Of New York | Method and apparatus for processing thin metal layers |
JP4583709B2 (en) * | 2000-11-27 | 2010-11-17 | ザ・トラスティーズ・オブ・コロンビア・ユニバーシティ・イン・ザ・シティ・オブ・ニューヨーク | Method and mask projection apparatus for laser crystallization treatment of semiconductor film region on substrate |
US6582827B1 (en) | 2000-11-27 | 2003-06-24 | The Trustees Of Columbia University In The City Of New York | Specialized substrates for use in sequential lateral solidification processing |
US7217605B2 (en) | 2000-11-29 | 2007-05-15 | Semiconductor Energy Laboratory Co., Ltd. | Laser irradiation method and method of manufacturing a semiconductor device |
EP1350272A1 (en) * | 2000-12-21 | 2003-10-08 | Koninklijke Philips Electronics N.V. | Thin film transistors |
KR100400510B1 (en) | 2000-12-28 | 2003-10-08 | 엘지.필립스 엘시디 주식회사 | A machine for Si crystallization and method of crystallizing Si |
US6621044B2 (en) | 2001-01-18 | 2003-09-16 | Anvik Corporation | Dual-beam materials-processing system |
JP4732599B2 (en) | 2001-01-26 | 2011-07-27 | 株式会社日立製作所 | Thin film transistor device |
JP2002222944A (en) * | 2001-01-26 | 2002-08-09 | Kitakiyuushiyuu Techno Center:Kk | Semiconductor element |
DE10103670A1 (en) | 2001-01-27 | 2002-08-01 | Christiansen Jens I | Textured crystalline silicon layer production using laser, includes control of energy intensity to achieve textured crystallites of specific diameter |
JP4744700B2 (en) | 2001-01-29 | 2011-08-10 | 株式会社日立製作所 | Thin film semiconductor device and image display device including thin film semiconductor device |
US6573163B2 (en) | 2001-01-29 | 2003-06-03 | Sharp Laboratories Of America, Inc. | Method of optimizing channel characteristics using multiple masks to form laterally crystallized ELA poly-Si films |
US6495405B2 (en) | 2001-01-29 | 2002-12-17 | Sharp Laboratories Of America, Inc. | Method of optimizing channel characteristics using laterally-crystallized ELA poly-Si films |
JP2002231628A (en) | 2001-02-01 | 2002-08-16 | Sony Corp | Method of forming semiconductor thin film, method of manufacturing semiconductor device, device used for carrying out the same, and electro-optical device |
TW521310B (en) | 2001-02-08 | 2003-02-21 | Toshiba Corp | Laser processing method and apparatus |
JP4291539B2 (en) | 2001-03-21 | 2009-07-08 | シャープ株式会社 | Semiconductor device and manufacturing method thereof |
JP2002353159A (en) | 2001-03-23 | 2002-12-06 | Sumitomo Heavy Ind Ltd | Processing apparatus and method |
US7061959B2 (en) | 2001-04-18 | 2006-06-13 | Tcz Gmbh | Laser thin film poly-silicon annealing system |
US7167499B2 (en) | 2001-04-18 | 2007-01-23 | Tcz Pte. Ltd. | Very high energy, high stability gas discharge laser surface treatment system |
CA2412603A1 (en) * | 2001-04-19 | 2002-10-31 | The Trustee Of Columbia University In The City Of New York | Method and system for providing a single-scan, continuous motion sequential lateral solidification |
TW480735B (en) | 2001-04-24 | 2002-03-21 | United Microelectronics Corp | Structure and manufacturing method of polysilicon thin film transistor |
JP5025057B2 (en) | 2001-05-10 | 2012-09-12 | 株式会社半導体エネルギー研究所 | Method for manufacturing semiconductor device |
KR100379361B1 (en) | 2001-05-30 | 2003-04-07 | 엘지.필립스 엘시디 주식회사 | crystallization method of a silicon film |
KR100424593B1 (en) | 2001-06-07 | 2004-03-27 | 엘지.필립스 엘시디 주식회사 | A method of crystallizing Si |
SG108262A1 (en) * | 2001-07-06 | 2005-01-28 | Inst Data Storage | Method and apparatus for cutting a multi-layer substrate by dual laser irradiation |
KR100662494B1 (en) | 2001-07-10 | 2007-01-02 | 엘지.필립스 엘시디 주식회사 | Method For Crystallizing Amorphous Layer And Method For Fabricating Liquid Crystal Display Device By Using Said Method |
JP4637410B2 (en) | 2001-07-17 | 2011-02-23 | シャープ株式会社 | Semiconductor substrate manufacturing method and semiconductor device |
JP4109026B2 (en) | 2001-07-27 | 2008-06-25 | 東芝松下ディスプレイテクノロジー株式会社 | Method for manufacturing array substrate and photomask |
WO2003018882A1 (en) * | 2001-08-27 | 2003-03-06 | The Trustees Of Columbia University In The City Of New York | Improved polycrystalline tft uniformity through microstructure mis-alignment |
TWI279052B (en) | 2001-08-31 | 2007-04-11 | Semiconductor Energy Lab | Laser irradiation method, laser irradiation apparatus, and method of manufacturing a semiconductor device |
TW582062B (en) * | 2001-09-14 | 2004-04-01 | Sony Corp | Laser irradiation apparatus and method of treating semiconductor thin film |
JP3903761B2 (en) * | 2001-10-10 | 2007-04-11 | 株式会社日立製作所 | Laser annealing method and laser annealing apparatus |
US6767804B2 (en) | 2001-11-08 | 2004-07-27 | Sharp Laboratories Of America, Inc. | 2N mask design and method of sequential lateral solidification |
JP3980465B2 (en) | 2001-11-09 | 2007-09-26 | 株式会社半導体エネルギー研究所 | Method for manufacturing semiconductor device |
US6526585B1 (en) * | 2001-12-21 | 2003-03-04 | Elton E. Hill | Wet smoke mask |
US7749818B2 (en) | 2002-01-28 | 2010-07-06 | Semiconductor Energy Laboratory Co., Ltd. | Semiconductor device and method of manufacturing the same |
US7119365B2 (en) | 2002-03-26 | 2006-10-10 | Sharp Kabushiki Kaisha | Semiconductor device and manufacturing method thereof, SOI substrate and display device using the same, and manufacturing method of the SOI substrate |
US6792029B2 (en) | 2002-03-27 | 2004-09-14 | Sharp Laboratories Of America, Inc. | Method of suppressing energy spikes of a partially-coherent beam |
WO2003084688A2 (en) | 2002-04-01 | 2003-10-16 | The Trustees Of Columbia University In The City Of New York | Method and system for providing a thin film |
US7192479B2 (en) | 2002-04-17 | 2007-03-20 | Sharp Laboratories Of America, Inc. | Laser annealing mask and method for smoothing an annealed surface |
US6984573B2 (en) * | 2002-06-14 | 2006-01-10 | Semiconductor Energy Laboratory Co., Ltd. | Laser irradiation method and apparatus |
JP2004031809A (en) | 2002-06-27 | 2004-01-29 | Toshiba Corp | Photomask and method of crystallizing semiconductor thin film |
WO2004017382A2 (en) | 2002-08-19 | 2004-02-26 | The Trustees Of Columbia University In The City Of New York | Process and system for laser crystallization processing of film regions on a substrate to provide substantial uniformity within areas in such regions and edge areas thereof, and a structure of such film regions |
TWI331803B (en) | 2002-08-19 | 2010-10-11 | Univ Columbia | A single-shot semiconductor processing system and method having various irradiation patterns |
TWI360707B (en) * | 2002-08-19 | 2012-03-21 | Univ Columbia | Process and system for laser crystallization proc |
US7259081B2 (en) | 2002-08-19 | 2007-08-21 | Im James S | Process and system for laser crystallization processing of film regions on a substrate to provide substantial uniformity, and a structure of such film regions |
JP2004087535A (en) | 2002-08-22 | 2004-03-18 | Sony Corp | Method for manufacturing crystalline semiconductor material and method for manufacturing semiconductor device |
JP4474108B2 (en) * | 2002-09-02 | 2010-06-02 | 株式会社 日立ディスプレイズ | Display device, manufacturing method thereof, and manufacturing apparatus |
JP4627961B2 (en) * | 2002-09-20 | 2011-02-09 | 株式会社半導体エネルギー研究所 | Method for manufacturing semiconductor device |
US7067867B2 (en) | 2002-09-30 | 2006-06-27 | Nanosys, Inc. | Large-area nonenabled macroelectronic substrates and uses therefor |
TW569350B (en) | 2002-10-31 | 2004-01-01 | Au Optronics Corp | Method for fabricating a polysilicon layer |
KR100646160B1 (en) | 2002-12-31 | 2006-11-14 | 엘지.필립스 엘시디 주식회사 | A mask for sequential lateral solidification and a silicon crystallizing method using the same |
US7341928B2 (en) | 2003-02-19 | 2008-03-11 | The Trustees Of Columbia University In The City Of New York | System and process for processing a plurality of semiconductor thin films which are crystallized using sequential lateral solidification techniques |
EP1468774B1 (en) * | 2003-02-28 | 2009-04-15 | Semiconductor Energy Laboratory Co., Ltd. | Laser irradiation method, laser irradiation apparatus, and method for manufacturing semiconductor device |
US20040169176A1 (en) | 2003-02-28 | 2004-09-02 | Peterson Paul E. | Methods of forming thin film transistors and related systems |
KR100618184B1 (en) | 2003-03-31 | 2006-08-31 | 비오이 하이디스 테크놀로지 주식회사 | Method of crystallization |
TWI227913B (en) | 2003-05-02 | 2005-02-11 | Au Optronics Corp | Method of fabricating polysilicon film by excimer laser crystallization process |
JP4470395B2 (en) * | 2003-05-30 | 2010-06-02 | 日本電気株式会社 | Method and apparatus for manufacturing semiconductor thin film, and thin film transistor |
JP4015068B2 (en) * | 2003-06-17 | 2007-11-28 | 株式会社東芝 | Manufacturing method of semiconductor device |
TWI294648B (en) | 2003-07-24 | 2008-03-11 | Au Optronics Corp | Method for manufacturing polysilicon film |
TWI359441B (en) * | 2003-09-16 | 2012-03-01 | Univ Columbia | Processes and systems for laser crystallization pr |
WO2005029548A2 (en) | 2003-09-16 | 2005-03-31 | The Trustees Of Columbia University In The City Of New York | System and process for providing multiple beam sequential lateral solidification |
US7318866B2 (en) | 2003-09-16 | 2008-01-15 | The Trustees Of Columbia University In The City Of New York | Systems and methods for inducing crystallization of thin films using multiple optical paths |
TWI366859B (en) * | 2003-09-16 | 2012-06-21 | Univ Columbia | System and method of enhancing the width of polycrystalline grains produced via sequential lateral solidification using a modified mask pattern |
US7164152B2 (en) * | 2003-09-16 | 2007-01-16 | The Trustees Of Columbia University In The City Of New York | Laser-irradiated thin films having variable thickness |
WO2005029550A2 (en) | 2003-09-16 | 2005-03-31 | The Trustees Of Columbia University In The City Of New York | Method and system for producing crystalline thin films with a uniform crystalline orientation |
WO2005029549A2 (en) * | 2003-09-16 | 2005-03-31 | The Trustees Of Columbia University In The City Of New York | Method and system for facilitating bi-directional growth |
WO2005029546A2 (en) | 2003-09-16 | 2005-03-31 | The Trustees Of Columbia University In The City Of New York | Method and system for providing a continuous motion sequential lateral solidification for reducing or eliminating artifacts, and a mask for facilitating such artifact reduction/elimination |
US7364952B2 (en) * | 2003-09-16 | 2008-04-29 | The Trustees Of Columbia University In The City Of New York | Systems and methods for processing thin films |
KR100971951B1 (en) * | 2003-09-17 | 2010-07-23 | 엘지디스플레이 주식회사 | Method for crystallization of amorphous silicon layer using excimer laser |
US7311778B2 (en) | 2003-09-19 | 2007-12-25 | The Trustees Of Columbia University In The City Of New York | Single scan irradiation for crystallization of thin films |
JP2005129769A (en) | 2003-10-24 | 2005-05-19 | Hitachi Ltd | Method for modifying semiconductor thin film, modified semiconductor thin film, method for evaluating the same, thin film transistor formed of semiconductor thin film, and image display device having circuit constituted by using the thin film transistor |
KR100698056B1 (en) | 2003-12-26 | 2007-03-23 | 엘지.필립스 엘시디 주식회사 | Laser Beam Pattern Mask and the Method for Crystallization with the Same |
KR100572519B1 (en) | 2003-12-26 | 2006-04-19 | 엘지.필립스 엘시디 주식회사 | Mask for laser crystallization process and laser crystallization process using the mask |
US7199397B2 (en) * | 2004-05-05 | 2007-04-03 | Au Optronics Corporation | AMOLED circuit layout |
US7645337B2 (en) | 2004-11-18 | 2010-01-12 | The Trustees Of Columbia University In The City Of New York | Systems and methods for creating crystallographic-orientation controlled poly-silicon films |
KR101212378B1 (en) | 2004-11-18 | 2012-12-13 | 더 트러스티이스 오브 콜롬비아 유니버시티 인 더 시티 오브 뉴욕 | SYSTEMS AND METHODS FOR CREATING CRYSTALLOGRAPHIC-ORIENTATION CONTROLLED poly-SILICON FILMS |
CN101111925A (en) | 2004-11-18 | 2008-01-23 | 纽约市哥伦比亚大学理事会 | System and method for generating polysilicon film controlled on crystallization direction |
JP5121118B2 (en) | 2004-12-08 | 2013-01-16 | 株式会社ジャパンディスプレイイースト | Display device |
US8221544B2 (en) | 2005-04-06 | 2012-07-17 | The Trustees Of Columbia University In The City Of New York | Line scan sequential lateral solidification of thin films |
TWI255508B (en) * | 2005-07-08 | 2006-05-21 | Univ Nat Taiwan | Manufacturing method of polysilicon thin films |
EP1922745A1 (en) | 2005-08-16 | 2008-05-21 | The Trustees of Columbia University in the City of New York | Systems and methods for uniform sequential lateral solidification of thin films using high frequency lasers |
KR101132404B1 (en) * | 2005-08-19 | 2012-04-03 | 삼성전자주식회사 | Method for fabricating thin film of poly crystalline silicon and method for fabricating thin film transistor having the same |
US7192818B1 (en) * | 2005-09-22 | 2007-03-20 | National Taiwan University | Polysilicon thin film fabrication method |
JP4680850B2 (en) | 2005-11-16 | 2011-05-11 | 三星モバイルディスプレイ株式會社 | Thin film transistor and manufacturing method thereof |
KR101191404B1 (en) | 2006-01-12 | 2012-10-16 | 삼성디스플레이 주식회사 | Mask for silicone crystallization, method for crystallizing silicone using the same and display device |
KR20070094527A (en) | 2006-03-17 | 2007-09-20 | 가부시키가이샤 에키쇼센탄 기쥬쓰 가이하쓰센타 | Crystallization method, thin film transistor manufacturing method, thin film transistor, display, and semiconductor device |
CN101622722B (en) * | 2007-02-27 | 2012-11-21 | 卡尔蔡司激光器材有限责任公司 | Continuous coating installation and methods for producing crystalline thin films and solar cells |
US8012861B2 (en) | 2007-11-21 | 2011-09-06 | The Trustees Of Columbia University In The City Of New York | Systems and methods for preparing epitaxially textured polycrystalline films |
-
2009
- 2009-02-27 US US12/919,681 patent/US8569155B2/en not_active Expired - Fee Related
- 2009-02-27 WO PCT/US2009/035566 patent/WO2009111340A2/en active Application Filing
- 2009-03-02 TW TW098106705A patent/TWI462181B/en not_active IP Right Cessation
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US7183229B2 (en) * | 2000-12-08 | 2007-02-27 | Sony Corporation | Semiconductor thin film forming method, production methods for semiconductor device and electrooptical device, devices used for these methods, and semiconductor device and electrooptical device |
US7326876B2 (en) * | 2003-06-30 | 2008-02-05 | Lg.Philips Lcd Co., Ltd. | Sequential lateral solidification device |
US20050112906A1 (en) * | 2003-10-28 | 2005-05-26 | Semiconductor Energy Laboratory Co., Ltd. | Methods for forming wiring and manufacturing thin film transistor and droplet discharging method |
US20060035478A1 (en) * | 2004-08-10 | 2006-02-16 | Lg Philips Lcd Co., Ltd. | Variable mask device for crystallizing silicon layer and method for crystallizing using the same |
Cited By (8)
Publication number | Priority date | Publication date | Assignee | Title |
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US9466402B2 (en) | 2003-09-16 | 2016-10-11 | The Trustees Of Columbia University In The City Of New York | Processes and systems for laser crystallization processing of film regions on a substrate utilizing a line-type beam, and structures of such film regions |
WO2012140253A1 (en) * | 2011-04-15 | 2012-10-18 | Von Ardenne Anlagentechnik Gmbh | Method and device for thermally treating substrates |
DE102013100520A1 (en) | 2012-12-28 | 2014-07-03 | Von Ardenne Anlagentechnik Gmbh | Flashlamp arrangement for illuminating substrate, has single ignition electrode for external ignition of entire flashlamps and is arranged in lamp housing, where ignition electrode is so formed that all flash lamps ignite simultaneously |
DE102013100520B4 (en) * | 2012-12-28 | 2017-06-01 | Von Ardenne Gmbh | Flash lamp assembly and method for igniting same |
DE102013206486A1 (en) | 2013-04-11 | 2014-10-16 | Von Ardenne Gmbh | Flash lamp assembly and method for igniting same |
DE102013206486B4 (en) * | 2013-04-11 | 2014-11-06 | Von Ardenne Gmbh | Flash lamp assembly and method for igniting same |
WO2015127036A1 (en) * | 2014-02-19 | 2015-08-27 | The Trustees Of Columbia University In The City Of New York | Methods and systems for controlled lateral solidification |
WO2015135904A1 (en) * | 2014-03-12 | 2015-09-17 | Von Ardenne Gmbh | Processing assembly and method for operating a processing assembly |
Also Published As
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TW201001556A (en) | 2010-01-01 |
US20110101368A1 (en) | 2011-05-05 |
US8569155B2 (en) | 2013-10-29 |
TWI462181B (en) | 2014-11-21 |
WO2009111340A3 (en) | 2010-01-14 |
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