KR20100021539A - High efficiency solar cells - Google Patents
High efficiency solar cells Download PDFInfo
- Publication number
- KR20100021539A KR20100021539A KR1020080080214A KR20080080214A KR20100021539A KR 20100021539 A KR20100021539 A KR 20100021539A KR 1020080080214 A KR1020080080214 A KR 1020080080214A KR 20080080214 A KR20080080214 A KR 20080080214A KR 20100021539 A KR20100021539 A KR 20100021539A
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- solar cell
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- electric field
- high efficiency
- photovoltaic
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- 230000005684 electric field Effects 0.000 claims abstract description 30
- 238000006243 chemical reaction Methods 0.000 claims abstract description 9
- 230000031700 light absorption Effects 0.000 claims abstract description 6
- 239000004065 semiconductor Substances 0.000 claims description 65
- 238000010248 power generation Methods 0.000 claims description 9
- 238000000034 method Methods 0.000 claims description 7
- 238000005215 recombination Methods 0.000 abstract description 9
- 230000006798 recombination Effects 0.000 abstract description 9
- 239000010408 film Substances 0.000 description 110
- 239000000758 substrate Substances 0.000 description 47
- 229910021417 amorphous silicon Inorganic materials 0.000 description 24
- 239000010409 thin film Substances 0.000 description 24
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 11
- 229910052710 silicon Inorganic materials 0.000 description 11
- 239000010703 silicon Substances 0.000 description 11
- 229910021419 crystalline silicon Inorganic materials 0.000 description 6
- 239000000463 material Substances 0.000 description 6
- 229910021421 monocrystalline silicon Inorganic materials 0.000 description 5
- 229910021423 nanocrystalline silicon Inorganic materials 0.000 description 5
- 229910004613 CdTe Inorganic materials 0.000 description 4
- 239000013078 crystal Substances 0.000 description 4
- 230000005611 electricity Effects 0.000 description 4
- 239000002184 metal Substances 0.000 description 4
- 229910052751 metal Inorganic materials 0.000 description 4
- 150000001875 compounds Chemical class 0.000 description 3
- 230000006866 deterioration Effects 0.000 description 3
- 238000010586 diagram Methods 0.000 description 3
- 238000009792 diffusion process Methods 0.000 description 3
- 239000011521 glass Substances 0.000 description 3
- 238000004519 manufacturing process Methods 0.000 description 3
- 230000004044 response Effects 0.000 description 3
- 230000008901 benefit Effects 0.000 description 2
- 239000000969 carrier Substances 0.000 description 2
- 238000000151 deposition Methods 0.000 description 2
- 229910021424 microcrystalline silicon Inorganic materials 0.000 description 2
- 230000004048 modification Effects 0.000 description 2
- 238000012986 modification Methods 0.000 description 2
- 230000002093 peripheral effect Effects 0.000 description 2
- 229910021420 polycrystalline silicon Inorganic materials 0.000 description 2
- 230000008569 process Effects 0.000 description 2
- 229910052709 silver Inorganic materials 0.000 description 2
- 238000000427 thin-film deposition Methods 0.000 description 2
- 229910006404 SnO 2 Inorganic materials 0.000 description 1
- 238000005452 bending Methods 0.000 description 1
- 239000000919 ceramic Substances 0.000 description 1
- 230000007547 defect Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000010292 electrical insulation Methods 0.000 description 1
- 238000004049 embossing Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- -1 for example Substances 0.000 description 1
- 239000012535 impurity Substances 0.000 description 1
- 238000009434 installation Methods 0.000 description 1
- 238000013082 photovoltaic technology Methods 0.000 description 1
- 230000000704 physical effect Effects 0.000 description 1
- 229910021426 porous silicon Inorganic materials 0.000 description 1
- 238000002791 soaking Methods 0.000 description 1
- 238000003860 storage Methods 0.000 description 1
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Classifications
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L31/00—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
- H01L31/02—Details
- H01L31/0224—Electrodes
- H01L31/022408—Electrodes for devices characterised by at least one potential jump barrier or surface barrier
- H01L31/022425—Electrodes for devices characterised by at least one potential jump barrier or surface barrier for solar cells
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L31/00—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
- H01L31/04—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof adapted as photovoltaic [PV] conversion devices
- H01L31/06—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof adapted as photovoltaic [PV] conversion devices characterised by potential barriers
- H01L31/072—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof adapted as photovoltaic [PV] conversion devices characterised by potential barriers the potential barriers being only of the PN heterojunction type
- H01L31/0745—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof adapted as photovoltaic [PV] conversion devices characterised by potential barriers the potential barriers being only of the PN heterojunction type comprising a AIVBIV heterojunction, e.g. Si/Ge, SiGe/Si or Si/SiC solar cells
- H01L31/0747—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof adapted as photovoltaic [PV] conversion devices characterised by potential barriers the potential barriers being only of the PN heterojunction type comprising a AIVBIV heterojunction, e.g. Si/Ge, SiGe/Si or Si/SiC solar cells comprising a heterojunction of crystalline and amorphous materials, e.g. heterojunction with intrinsic thin layer
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- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E10/00—Energy generation through renewable energy sources
- Y02E10/50—Photovoltaic [PV] energy
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- Engineering & Computer Science (AREA)
- Life Sciences & Earth Sciences (AREA)
- Sustainable Energy (AREA)
- Physics & Mathematics (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- Electromagnetism (AREA)
- General Physics & Mathematics (AREA)
- Computer Hardware Design (AREA)
- Microelectronics & Electronic Packaging (AREA)
- Power Engineering (AREA)
- Sustainable Development (AREA)
- Photovoltaic Devices (AREA)
Abstract
Description
The present invention relates to a solar cell, and in particular, by applying a bias voltage to the solar cell so that the charge generated by the light is rapidly flowed and collected, the high energy conversion efficiency can be obtained by preventing the recombination of the electron-hole pair as much as possible. An improved high efficiency solar cell is provided.
Photovoltaic power generation is an infinite clean power generation technology that produces electricity from sunlight. The photovoltaic power generation system is a solar cell (module) that generates electricity by receiving sunlight, and a peripheral device such as a power regulator for converting the generated direct current electricity into alternating current and a storage battery for storing the generated electricity. It consists of. Solar cells are basically diodes composed of pn junctions, and are classified into various types according to materials used as light absorbing layers. Solar cells using silicon as a light absorption layer are classified into crystalline substrate type solar cells and thin film type solar cells. In addition, CdTe or CIS (CuInSe2) compound thin film solar cell, group III-V solar cell, dye-sensitized solar cell and organic solar cell are the representative solar cells.
Thin film solar cells may be silicon based, CuInSe 2 based or CdTe thin film solar cells depending on the light absorbing layer material used. The advantage of such thin film solar cells is that they can be used on low-cost substrates such as glass or metal plates instead of expensive silicon substrates. It is possible to manufacture solar cells at low cost by minimizing material consumption through thin film deposition inside and outside the micron. Another advantage is that large-area modules can be manufactured using an in-line process to improve productivity and reduce manufacturing costs. Types of silicon thin film solar cells are classified into various types according to the thin film deposition temperature, the type of substrate used (glass, metal plate, ceramic, silicon substrate, etc.) and the deposition method. Depending on the crystal characteristics of the light absorbing layer, it is classified into amorphous and crystalline silicon thin film solar cells, and the crystalline silicon thin film solar cells are again classified according to the crystal size and the thickness of the light absorbing layer.
Amorphous silicon (a-Si: H) thin-film solar cells have a very low diffusion length of carriers due to the properties of the material itself compared to monocrystalline (or polycrystalline) silicon substrates. The collection efficiency of electron-hole pairs is very low. Therefore, in general, an amorphous silicon thin film solar cell has a pin structure in which a light absorbing layer composed of an intrinsic semiconductor layer to which impurities are not added is inserted between a p-type semiconductor layer having a high doping concentration and an n-type semiconductor layer. In this structure, the light absorbing layer is depleted by the p and n layers having high doping concentrations above and below, and an electric field is generated therein. Therefore, the electron-hole pairs generated from the light absorbing layer by the incident light are collected into the n-layer and p-layer by the drift by the internal electric field rather than by diffusion, and generate current.
In an ideal device, an electric field is generated uniformly inside, so that an electron-hole pair flows smoothly. In real devices, however, defects present in the light absorbing layer increase the space charge density at the pi and ni interfaces and decrease the electric field in the light absorbing layer. In general, when the solar cell is exposed to light, a deterioration characteristic (Staebler-Wronski Effect) appears, and the solar cell characteristics decrease by up to 30% depending on the thickness and physical properties of the light absorbing layer. Light-soaking also increases the density of dangling bonds in the light absorbing layer and reduces the internal electric field, further accelerating the recombination of electron-hole pairs generated by light, which is why the characteristics of solar cells Deterioration occurs.
Meanwhile, nanocrystalline (nc-Si: H) silicon thin film solar cells use nanocrystalline silicon, commonly called microcrystalline silicon (μc-Si: H), as a light absorbing layer as a boundary material between amorphous and single crystal silicon. do. Nanocrystalline silicon has a crystal size of several tens of nm to hundreds of nm depending on the deposition method, the amorphous boundary is often present in the grain boundary and most carrier recombination occurs in the crystal boundary due to the high bonding density. However, there is no deterioration phenomenon that occurs in amorphous silicon thin film solar cell. The nanocrystalline silicon thin film solar cell is also manufactured in the same pin structure as the amorphous silicon thin film solar cell, which has a small grain size of nanocrystalline silicon and contains a large number of amorphous matrices. Although larger than silicon, the np structure alone is not enough to collect carriers by diffusion.
In terms of the price of each component of the photovoltaic system, modules (60%), peripheral devices (25%) and installation costs (15%) are known to account for the largest share of the total system price. The module price, which accounts for 60% of the total system price, consists of the substrate (40%, silicon), the solar cell manufacturing process (25%), and module assembly (35%). Given that the market share of silicon substrate solar cells is very high, the current high price of the photovoltaic system is due to the high price of the solar module, that is, the high price share of the silicon substrate constituting the solar cell. The biggest problem that PV technology currently sits on is the high cost of power generation due to the high price of the system, which is the biggest obstacle to the widespread deployment of PV power. Therefore, energy conversion efficiency is very important for solar cells.
SUMMARY OF THE INVENTION An object of the present invention is to provide an improved high efficiency solar cell that can obtain high energy conversion efficiency by preventing the recombination of electron-hole pairs as much as possible by applying a bias voltage to the solar cell so that the charge generated by the light is flowed and collected quickly. have.
One aspect of the present invention for achieving the above technical problem relates to a high efficiency solar cell. A high efficiency solar cell of the present invention includes: a photovoltaic power generation unit generating charges by light absorption; First and second electrodes having different polarities for outputting photovoltaic power generated by the photovoltaic generator to an external load; And a bias electrode for applying an electric field added to the photovoltaic generator, wherein charges generated in the photovoltaic generator are caused by an added electric field due to an internal electric field and a bias voltage applied to the bias electrode. By being flowed and collected more quickly toward the second electrode, high energy conversion efficiency can be obtained by preventing recombination of the electron-hole pair.
In one embodiment, an insulating film for electrically insulating the bias electrode.
In example embodiments, the photovoltaic generator may include a light absorbing layer having a multi-layer structure in which an intrinsic amorphous semiconductor film and an intrinsic microcrystalline semiconductor film are alternately repeated.
In one embodiment, the photovoltaic generator comprises a heterojunction with Intrinsic Thin-layer (HIT) structure.
In one embodiment, the first and second electrodes have an integrated backside contact (IBC) structure.
In one embodiment, the photovoltaic generation unit includes an antireflection film of a multi-layered structure in which one porous antireflection film or two or more porous antireflection films overlap.
According to the high-efficiency solar cell of the present invention, the charge generated by the bias voltage applied to the bias electrode is rapidly flowed and collected to prevent the recombination of the electron-hole pair as much as possible to obtain high energy conversion efficiency. The high efficiency solar cell of the present invention can be applied to all kinds of amorphous or crystalline silicon thin film solar cells, or substrate type solar cells using a single crystalline or polycrystalline silicon substrate. In addition, high efficiency solar cells can be realized by adding bias electrodes to CdTe or CIS (CuInSe2) compound thin film solar cells, III-V solar cells, dye-sensitized solar cells, and organic solar cells.
In order to fully understand the present invention, preferred embodiments of the present invention will be described with reference to the accompanying drawings. Embodiment of the present invention may be modified in various forms, the scope of the invention should not be construed as limited to the embodiments described in detail below. This embodiment is provided to more completely explain the present invention to those skilled in the art. Therefore, the shape of the elements in the drawings and the like may be exaggerated to emphasize a more clear description. It should be noted that the same members in each drawing are sometimes shown with the same reference numerals. Detailed descriptions of well-known functions and configurations that are determined to unnecessarily obscure the subject matter of the present invention are omitted.
The general
However, electron-electron pairs that are flowed by the internal electric field are recombined for various reasons in the flow process. The higher the recombination rate, the lower the energy conversion efficiency. In order to overcome this problem, the high-efficiency solar cell of the present invention applies the added electric field by the bias voltage to the solar cell so that the charge generated by the light flows rapidly and collects the high energy by preventing the recombination of the electron-hole pair as much as possible. Conversion efficiency can be obtained.
2 is a schematic configuration diagram of a high efficiency solar cell having a bias electrode of the present invention.
Referring to FIG. 2, the high-efficiency
3 to 6 show various embodiments of a high efficiency solar cell.
First, referring to FIG. 3, one of the embodiments of the present invention includes a
When light is incident on the
Referring to FIG. 4, according to another embodiment of the present invention, a
Referring to FIG. 5, in another embodiment of the present invention, a
The
The substrate-type
When light is incident on the
Referring to FIG. 6, in another embodiment of the present invention, the crystalline substrate type
When light enters the
The high efficiency solar cell of the present invention as described above can be applied to all kinds of amorphous or crystalline silicon thin film solar cells or substrate type solar cells using a single crystalline or polycrystalline silicon substrate in addition to the above-described embodiments. In addition, high efficiency solar cells can be realized by adding bias electrodes to CdTe or CIS (CuInSe2) compound thin film solar cells, III-V solar cells, dye-sensitized solar cells, and organic solar cells.
Embodiments of the highly efficient solar cell of the present invention described above are merely exemplary, and those skilled in the art will appreciate that various modifications and equivalent other embodiments are possible therefrom. Could be. Therefore, it will be understood that the present invention is not limited only to the form mentioned in the above detailed description. Therefore, the true technical protection scope of the present invention will be defined by the technical spirit of the appended claims. It is also to be understood that the present invention includes all modifications, equivalents, and substitutes within the spirit and scope of the invention as defined by the appended claims.
1 is a schematic configuration diagram of a general solar cell.
2 is a schematic configuration diagram of a high efficiency solar cell having a bias electrode of the present invention.
3 to 6 show various embodiments of a high efficiency solar cell.
* Description of the symbols for the main parts of the drawings *
10: solar cell 12: photovoltaic power generation unit
14: first electrode 16: second electrode
18: load 20: solar cell
22: photovoltaic power generation unit 24: first electrode
26: second electrode 30: bias power supply
32: insulating film 34: bias electrode
36: load 40: solar cell
41: photovoltaic generator 42: light absorbing layer
43: first conductive semiconductor film 44: second conductive semiconductor film
45: transparent conductive film 46: rear reflective film
47: substrate 50: solar cell
51: photovoltaic generator 52: light absorbing layer
53: first conductive semiconductor film 54: second conductive semiconductor film
55: transparent conductive film 56: back reflecting film
57: substrate 60: solar cell
61: photovoltaic generator 62: intrinsic semiconductor film
63: intrinsic semiconductor film 64: second conductive semiconductor film
65: first conductive semiconductor film 66: conductive film
67: conductive film 68: crystalline semiconductor substrate
69: intrinsic semiconductor film 70: solar cell
71: photovoltaic generator 72: intrinsic semiconductor layer
73: second conductive semiconductor film 74: first conductive semiconductor film
75: antireflection film 76: antireflection film
78: crystalline semiconductor substrate 80: antireflection film
Claims (6)
Priority Applications (1)
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KR1020080080214A KR101411996B1 (en) | 2008-08-16 | 2008-08-16 | High efficiency solar cells |
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KR1020080080214A KR101411996B1 (en) | 2008-08-16 | 2008-08-16 | High efficiency solar cells |
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KR20100021539A true KR20100021539A (en) | 2010-02-25 |
KR101411996B1 KR101411996B1 (en) | 2014-06-26 |
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Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN104882499A (en) * | 2015-05-19 | 2015-09-02 | 东南大学 | Thermovoltaic cell |
CN104964638A (en) * | 2015-06-28 | 2015-10-07 | 西安电子科技大学 | Method of measuring the forbidden band width of a strain Ge on the basis of a heterojunction capacitance-voltage method |
KR101629729B1 (en) * | 2015-09-07 | 2016-06-13 | 한국기계연구원 | Perovskite solar cell |
US11658253B2 (en) | 2016-05-06 | 2023-05-23 | Rensselaer Polytechnic Institute | High absorption photovoltaic material and methods of making the same |
Family Cites Families (3)
Publication number | Priority date | Publication date | Assignee | Title |
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KR950004594B1 (en) * | 1989-04-29 | 1995-05-02 | 삼성전자주식회사 | Thermal treatment method of amorphous silicon solar cell |
KR100303471B1 (en) * | 2000-02-15 | 2001-11-03 | 주흥로 | Avalanche photodetector device and method for manufacturing the same |
JP2003158288A (en) | 2001-11-21 | 2003-05-30 | Nippon Telegr & Teleph Corp <Ntt> | Semiconductor photo-detector and its manufacturing method |
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2008
- 2008-08-16 KR KR1020080080214A patent/KR101411996B1/en active IP Right Grant
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN104882499A (en) * | 2015-05-19 | 2015-09-02 | 东南大学 | Thermovoltaic cell |
CN104964638A (en) * | 2015-06-28 | 2015-10-07 | 西安电子科技大学 | Method of measuring the forbidden band width of a strain Ge on the basis of a heterojunction capacitance-voltage method |
KR101629729B1 (en) * | 2015-09-07 | 2016-06-13 | 한국기계연구원 | Perovskite solar cell |
US11658253B2 (en) | 2016-05-06 | 2023-05-23 | Rensselaer Polytechnic Institute | High absorption photovoltaic material and methods of making the same |
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