EP3114712A2 - RÜCKSEITENKONTAKTIERTE Si-DÜNNSCHICHT-SOLARZELLE - Google Patents
RÜCKSEITENKONTAKTIERTE Si-DÜNNSCHICHT-SOLARZELLEInfo
- Publication number
- EP3114712A2 EP3114712A2 EP15719595.9A EP15719595A EP3114712A2 EP 3114712 A2 EP3114712 A2 EP 3114712A2 EP 15719595 A EP15719595 A EP 15719595A EP 3114712 A2 EP3114712 A2 EP 3114712A2
- Authority
- EP
- European Patent Office
- Prior art keywords
- layer
- thickness
- absorber
- thin
- solar cell
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Withdrawn
Links
- 239000010409 thin film Substances 0.000 title claims abstract description 24
- 239000006096 absorbing agent Substances 0.000 claims abstract description 69
- 230000004888 barrier function Effects 0.000 claims abstract description 21
- 229910021419 crystalline silicon Inorganic materials 0.000 claims abstract description 21
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 claims abstract description 18
- 239000007791 liquid phase Substances 0.000 claims abstract description 17
- 238000002161 passivation Methods 0.000 claims abstract description 17
- 238000002425 crystallisation Methods 0.000 claims abstract description 16
- 230000008025 crystallization Effects 0.000 claims abstract description 16
- 239000000758 substrate Substances 0.000 claims abstract description 14
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 claims abstract description 13
- 229910052760 oxygen Inorganic materials 0.000 claims abstract description 13
- 239000001301 oxygen Substances 0.000 claims abstract description 13
- 229910052710 silicon Inorganic materials 0.000 claims abstract description 13
- 239000010703 silicon Substances 0.000 claims abstract description 13
- 239000011521 glass Substances 0.000 claims abstract description 12
- 239000000463 material Substances 0.000 claims abstract description 12
- 230000003287 optical effect Effects 0.000 claims abstract description 10
- 229910021421 monocrystalline silicon Inorganic materials 0.000 claims abstract description 8
- 239000004065 semiconductor Substances 0.000 claims abstract description 7
- 239000010410 layer Substances 0.000 claims description 181
- 238000000034 method Methods 0.000 claims description 17
- 229910004298 SiO 2 Inorganic materials 0.000 claims description 12
- 229910045601 alloy Inorganic materials 0.000 claims description 12
- 239000000956 alloy Substances 0.000 claims description 12
- 229910021417 amorphous silicon Inorganic materials 0.000 claims description 12
- 229910052814 silicon oxide Inorganic materials 0.000 claims description 12
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 claims description 11
- 229910021423 nanocrystalline silicon Inorganic materials 0.000 claims description 11
- 229910017107 AlOx Inorganic materials 0.000 claims description 10
- 229910004012 SiCx Inorganic materials 0.000 claims description 10
- 229910004205 SiNX Inorganic materials 0.000 claims description 9
- -1 T1O2 Inorganic materials 0.000 claims description 9
- 238000000151 deposition Methods 0.000 claims description 8
- 239000002800 charge carrier Substances 0.000 claims description 6
- 239000002243 precursor Substances 0.000 claims description 6
- 230000015572 biosynthetic process Effects 0.000 claims description 5
- 230000008021 deposition Effects 0.000 claims description 5
- 238000004519 manufacturing process Methods 0.000 claims description 5
- 239000002356 single layer Substances 0.000 claims description 5
- 238000000137 annealing Methods 0.000 claims description 4
- 239000011248 coating agent Substances 0.000 claims description 4
- 238000000576 coating method Methods 0.000 claims description 4
- OAICVXFJPJFONN-UHFFFAOYSA-N Phosphorus Chemical compound [P] OAICVXFJPJFONN-UHFFFAOYSA-N 0.000 claims description 3
- 229910052698 phosphorus Inorganic materials 0.000 claims description 3
- 239000011574 phosphorus Substances 0.000 claims description 3
- 229910010413 TiO 2 Inorganic materials 0.000 claims description 2
- 229910052787 antimony Inorganic materials 0.000 claims description 2
- WATWJIUSRGPENY-UHFFFAOYSA-N antimony atom Chemical compound [Sb] WATWJIUSRGPENY-UHFFFAOYSA-N 0.000 claims description 2
- 229910052785 arsenic Inorganic materials 0.000 claims description 2
- RQNWIZPPADIBDY-UHFFFAOYSA-N arsenic atom Chemical compound [As] RQNWIZPPADIBDY-UHFFFAOYSA-N 0.000 claims description 2
- 239000002019 doping agent Substances 0.000 claims description 2
- 238000011065 in-situ storage Methods 0.000 claims description 2
- 229910018072 Al 2 O 3 Inorganic materials 0.000 claims 1
- 229910004286 SiNxOy Inorganic materials 0.000 claims 1
- 229910052681 coesite Inorganic materials 0.000 abstract description 4
- 229910052906 cristobalite Inorganic materials 0.000 abstract description 4
- 229910052682 stishovite Inorganic materials 0.000 abstract description 4
- 229910052905 tridymite Inorganic materials 0.000 abstract description 4
- 239000000377 silicon dioxide Substances 0.000 abstract description 2
- 238000005546 reactive sputtering Methods 0.000 description 3
- GWEVSGVZZGPLCZ-UHFFFAOYSA-N Titan oxide Chemical compound O=[Ti]=O GWEVSGVZZGPLCZ-UHFFFAOYSA-N 0.000 description 2
- 238000009792 diffusion process Methods 0.000 description 2
- 239000012535 impurity Substances 0.000 description 2
- 238000005259 measurement Methods 0.000 description 2
- PNEYBMLMFCGWSK-UHFFFAOYSA-N aluminium oxide Inorganic materials [O-2].[O-2].[O-2].[Al+3].[Al+3] PNEYBMLMFCGWSK-UHFFFAOYSA-N 0.000 description 1
- 238000004364 calculation method Methods 0.000 description 1
- 238000005229 chemical vapour deposition Methods 0.000 description 1
- 238000004140 cleaning Methods 0.000 description 1
- 150000001875 compounds Chemical class 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000002346 layers by function Substances 0.000 description 1
- 230000008018 melting Effects 0.000 description 1
- 238000002844 melting Methods 0.000 description 1
- 230000008092 positive effect Effects 0.000 description 1
- 238000002360 preparation method Methods 0.000 description 1
- 238000000746 purification Methods 0.000 description 1
- 238000005215 recombination Methods 0.000 description 1
- 230000006798 recombination Effects 0.000 description 1
- 238000001953 recrystallisation Methods 0.000 description 1
- 238000002310 reflectometry Methods 0.000 description 1
- 235000012239 silicon dioxide Nutrition 0.000 description 1
- 238000004088 simulation Methods 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
- 238000005496 tempering Methods 0.000 description 1
Classifications
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- H01L31/0392—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 characterised by their semiconductor bodies characterised by their crystalline structure or particular orientation of the crystalline planes including thin films deposited on metallic or insulating substrates ; characterised by specific substrate materials or substrate features or by the presence of intermediate layers, e.g. barrier layers, on the substrate
- H01L31/03921—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 characterised by their semiconductor bodies characterised by their crystalline structure or particular orientation of the crystalline planes including thin films deposited on metallic or insulating substrates ; characterised by specific substrate materials or substrate features or by the presence of intermediate layers, e.g. barrier layers, on the substrate including only elements of Group IV of the Periodic System
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Definitions
- the invention relates to a back-contacted Si thin-film solar cell, at least comprising a crystalline Si absorber layer and arranged on the crystalline Si absorber layer emitter layer
- Semiconductor materials of different conductivity (absorber and emitter) generated charge carriers arranged on one side.
- the charge carriers are separated at the pn junction between emitter and absorber layer and fed to the corresponding contact system.
- Shading losses due to a contact system are avoided during back contact, which increases the efficiency of the solar cell.
- the possibility can be used to provide further functional layers on the side of the solar cell facing the light incidence.
- Thin-film solar cells require compared to wafer-based ones
- a Si absorber layer is applied, which is p-type (see, for example Amkreutz et al. in Solar Energy Materials & Solar Cells 123 (2014) 13-16; Haschke et al. in Solar Energy Materials & Solar Cells 1 15 (2013) 7-10; Dore et al. in EPJ Photovoltaics 4, 40301 (2013)), since this type of conductivity is supported by the impurities diffusing out of the glass substrate in the further process steps, in particular also by the liquid-phase recrystallization of an amorphous or nanocrystalline silicon layer.
- Both DE 2005 025 125 B4 and DE 10 2010 007 695 A1 describe different contacting systems for back-contacted Si thin-film solar cells. These solar cells have at least one absorber layer and a rear-side emitter layer of semiconductor materials of opposite p- and n-type doping.
- a passivation / cover / antireflection layer on the side of light incidence is furthermore described for the thin-film solar cell.
- a buffer layer (a-Si: H) covering the back contact structure is provided for better passivation of the emitter-absorber interface.
- the thin-film solar cell described there has an intrinsically conductive passivation layer (a-Si: H, intrinsic) between the absorber layer and the emitter layer arranged on the rear side.
- a-Si: H intrinsically conductive passivation layer
- the object of the invention is now to provide a further back-contacted Si thin-film solar cell of the type mentioned, which has improved parameters compared to the cited prior art, in particular an increased open circuit voltage, and a method for producing such a back-contacted Si thin film - solar cell.
- a barrier layer is arranged on a glass substrate to prevent the diffusion of impurities from the substrate into the following layers.
- the barrier layer is formed of SiOx, SiNx, SiCx, TiO2, AlOx or their mixed alloys (for example: SixOyN, SixOyC) individually or in multilayers which have a
- At least one layer for optical compensation is arranged on the barrier layer.
- This layer is made of SiNx, SiOx, SiCx, T1O2, AlOx or their
- Mixed alloys e.g., SixOyN, SixOyC having a total layer thickness of 20 nm to 250 nm formed, and has one from the substrate, of the
- Barrier layer and differs from the semiconductor material refractive index. On top of this is a 0.5 nm to 20 nm thin silicon and / or oxygen-containing layer on the side facing away from the light
- the crystalline Si absorber layer can be produced by a liquid phase crystallization process, it is n-type and has a layer thickness between 200 nm and 40 ⁇ m with a homogeneous one
- the solution according to the invention is based on an n-type crystalline Si absorber layer.
- the formation of a very thin S1O2 layer during the liquid-phase crystallization process of the Si layer during the melting of the amorphous or nanocrystalline Si layer and an underlying at least oxygen-containing layer is utilized.
- the formation of this thin SiO 2 layer renders the application of an n + doped front drift field superfluous, as known in the art.
- the doping concentration in the specified range causes a higher transverse conductivity in the absorber layer, whereby the horizontal current transport in the solar cell according to the invention is improved. This has a positive effect on the fill factor and the achievable open circuit voltages of the solar cell. Furthermore, with the arrangement according to the invention, a good passivation of the absorptive layer side facing the glass substrate is ensured, whereby recombination losses are reduced.
- the homogeneous doping of the n-type crystalline Si absorber layer is over its entire thickness
- ND Co ⁇ 1 / d, where d denotes the thickness of the absorber layer in microns, which is between 200 nm and 40 ⁇ , and Co a
- an a-Si: H (i) buffer layer and an a-Si: H (p) emitter layer are deposited.
- a barrier layer having a layer thickness in the range from 50 nm to 1 ⁇ m onto a cleaned glass substrate.
- the material for the barrier layer is
- SiO x selected from SiO x , SiN x , SiC x , TiO 2, AlO x or their mixed alloys (eg: SixOyN, SixOyC), wherein the barrier layer as a single layer or in
- At least one layer which improves the optical properties and has a layer thickness of 20 nm to 250 nm is applied to this barrier layer.
- the material for the temper layer SiNx, SiOx, SiCx, T1O2, AlOx or the like
- SiOx, Si Nx, Si x O y N or AI2O3 - is an amorphous or nano-crystalline Si layer and thereon a further layer as a doping source for the n- conductivity of the absorber layer, for example, containing phosphorus or Arsenic or antimony, deposited.
- This further layer serving as a doping source can also be applied before the application of an amorphous or nanocrystalline Si layer.
- the Si layer is subsequently crystallized by means of a line energy source by liquid-phase crystallization. In liquid phase crystallization, a very thin SiO 2 passivation layer is formed between precursor layer and silicon absorber.
- the process parameters are chosen so that the resulting in the absorber layer monocrystalline Si grains in their extension are at least as large as the thickness of the absorber layer.
- the homogeneous doping for the n-type conductivity of the absorber layer can also be produced by in-situ doping during the deposition of the silicon layer, as provided in a further independent method claim. This can be done for example by a constant doping during the deposition of an amorphous or nanocrystalline Si layer or by local doping, i. by briefly adding mentioned dopants at a certain location.
- the doping concentration of the absorber layer in a range of 1.5-10 16 cm 3 to 2-10 18 cm 3 or the doping concentration ND of the absorber layer in FIG
- ND Co ⁇ 1 / d set, where d denotes the thickness of the absorber layer in microns, which is between 200 nm and 40 ⁇ , and Co denotes a surface-related doping whose value is in a range between 6-10 17 ⁇ "3 to 8-10 18 ⁇ " 3 is located.
- the surface of the n-type crystalline absorber layer thus prepared is then cleaned, on which an a-Si: H (i) buffer layer and an a-Si: H (p) emitter layer are deposited.
- the back contact is made - as already mentioned - with the prior art by known means.
- Line power source are known and described for example in DE 2012 004 314 A1 or in Solar Energy Materials & Solar Cells 123 (2014) 13-16 of Amkreutz et al. described.
- a 250 nm thick SiO x barrier layer is deposited on a glass substrate by means of reactive sputtering.
- a SiNx tempering layer with a thickness of 70 nm is applied by means of reactive sputtering.
- the application of the layers can also take place by means of chemical vapor deposition.
- a 20 nm thin SiOx layer is applied by means of reactive sputtering.
- a 10 ⁇ thick nanocrystalline Si layer is deposited, on this a phosphorus-containing layer of thickness of 2.5 nm as a doping source.
- the Si layer is crystallized by means of a line energy source by liquid phase crystallization. This will be on this
- Layer stack produces a crystalline n-type absorber layer having a thickness of 10 ⁇ , a doping concentration of 1-10 17 cm 3 and monocrystalline Si grains having a vertical extent of> 10 ⁇ .
- absorber layer / annealing layer is formed during the
- d denotes the thickness of the absorber layer, which lies between 200 nm and 40 ⁇ m
- Co denotes a surface-related doping whose value lies in a range between 6-10 17 ⁇ 3 to 8-10 18 ⁇ "3.
- the corresponding parameter ranges are shown in the figure 1.
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Abstract
Description
Claims
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Application Number | Priority Date | Filing Date | Title |
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DE102014102864.3A DE102014102864A1 (de) | 2014-03-04 | 2014-03-04 | Rückseitenkontaktierte Si-Dünnschicht-Solarzelle |
PCT/DE2015/100085 WO2015131881A2 (de) | 2014-03-04 | 2015-03-04 | RÜCKSEITENKONTAKTIERTE Si-DÜNNSCHICHT-SOLARZELLE |
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EP3114712A2 true EP3114712A2 (de) | 2017-01-11 |
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EP15719595.9A Withdrawn EP3114712A2 (de) | 2014-03-04 | 2015-03-04 | RÜCKSEITENKONTAKTIERTE Si-DÜNNSCHICHT-SOLARZELLE |
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US (1) | US10074758B2 (de) |
EP (1) | EP3114712A2 (de) |
JP (1) | JP6635934B2 (de) |
DE (2) | DE102014102864A1 (de) |
WO (1) | WO2015131881A2 (de) |
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DE102014102864A1 (de) | 2014-03-04 | 2015-09-10 | Helmholtz-Zentrum Berlin Für Materialien Und Energie Gmbh | Rückseitenkontaktierte Si-Dünnschicht-Solarzelle |
CN110098269A (zh) * | 2019-04-29 | 2019-08-06 | 北京铂阳顶荣光伏科技有限公司 | 薄膜太阳能电池及其制备方法 |
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JP2740284B2 (ja) | 1989-08-09 | 1998-04-15 | 三洋電機株式会社 | 光起電力素子 |
DE102005025125B4 (de) | 2005-05-29 | 2008-05-08 | Hahn-Meitner-Institut Berlin Gmbh | Verfahren zur Herstellung einer einseitig kontaktierten Solarzelle und einseitig kontaktierte Solarzelle |
DE202005019799U1 (de) | 2005-12-13 | 2006-03-02 | Hahn-Meitner-Institut Berlin Gmbh | Amorph/kristalline Silizium-Heterosolarzelle |
US20080072953A1 (en) * | 2006-09-27 | 2008-03-27 | Thinsilicon Corp. | Back contact device for photovoltaic cells and method of manufacturing a back contact device |
DE102007009924A1 (de) * | 2007-02-27 | 2008-08-28 | Carl Zeiss Laser Optics Gmbh | Durchlaufbeschichtungsanlage, Verfahren zur Herstellung kristalliner Dünnschichten und Solarzellen sowie Solarzelle |
DE102010007695A1 (de) | 2010-02-09 | 2011-08-11 | Helmholtz-Zentrum Berlin für Materialien und Energie GmbH, 14109 | Rückseitenkontaktierte Solarzelle mit unstrukturierter Absorberschicht |
US20120018733A1 (en) * | 2010-07-23 | 2012-01-26 | Venkatraman Prabhakar | Thin Film Solar Cells And Other Devices, Systems And Methods Of Fabricating Same, And Products Produced By Processes Thereof |
DE102012004314A1 (de) | 2012-02-29 | 2013-08-29 | Helmholtz-Zentrum Berlin Für Materialien Und Energie Gmbh | Verfahren zur Herstellung einer dünnen Si-Absorberschicht, Dünnschicht-Silizium-Absorber und seine Verwendung |
DE102014102864A1 (de) | 2014-03-04 | 2015-09-10 | Helmholtz-Zentrum Berlin Für Materialien Und Energie Gmbh | Rückseitenkontaktierte Si-Dünnschicht-Solarzelle |
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2014
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- 2015-03-04 US US15/121,777 patent/US10074758B2/en not_active Expired - Fee Related
- 2015-03-04 DE DE202015009864.9U patent/DE202015009864U1/de not_active Expired - Lifetime
- 2015-03-04 WO PCT/DE2015/100085 patent/WO2015131881A2/de active Application Filing
Non-Patent Citations (3)
Title |
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ANDRA GUDRUN ET AL: "Multicrystalline silicon thin film solar cells based on a two-step liquid phase laser crystallization process", 2013 IEEE 39TH PHOTOVOLTAIC SPECIALISTS CONFERENCE (PVSC), IEEE, 16 June 2013 (2013-06-16), pages 1330 - 1333, XP032568650, DOI: 10.1109/PVSC.2013.6744388 * |
S. VARLAMOV ET AL: "Polycrystalline silicon on glass thin-film solar cells: A transition from solid-phase to liquid-phase crystallised silicon", SOLAR ENERGY MATERIALS AND SOLAR CELLS., vol. 119, 1 December 2013 (2013-12-01), NL, pages 246 - 255, XP055565813, ISSN: 0927-0248, DOI: 10.1016/j.solmat.2013.08.001 * |
See also references of WO2015131881A2 * |
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JP2017507496A (ja) | 2017-03-16 |
US20170018668A1 (en) | 2017-01-19 |
JP6635934B2 (ja) | 2020-01-29 |
WO2015131881A2 (de) | 2015-09-11 |
WO2015131881A3 (de) | 2015-10-29 |
DE102014102864A1 (de) | 2015-09-10 |
DE202015009864U1 (de) | 2020-10-26 |
US10074758B2 (en) | 2018-09-11 |
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