TWI503999B - Solar cell and manufacturing method thereof - Google Patents

Solar cell and manufacturing method thereof Download PDF

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TWI503999B
TWI503999B TW102121551A TW102121551A TWI503999B TW I503999 B TWI503999 B TW I503999B TW 102121551 A TW102121551 A TW 102121551A TW 102121551 A TW102121551 A TW 102121551A TW I503999 B TWI503999 B TW I503999B
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emitter layer
substrate
solar battery
solar cell
nano
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TW201415649A (en
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Keiji Watanabe
Mieko Matsumura
Takashi Hattori
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Hitachi Ltd
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00Semiconductor 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
    • H01L31/0248Semiconductor 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
    • H01L31/0352Semiconductor 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 shape or by the shapes, relative sizes or disposition of the semiconductor regions
    • H01L31/035272Semiconductor 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 shape or by the shapes, relative sizes or disposition of the semiconductor regions characterised by at least one potential jump barrier or surface barrier
    • H01L31/03529Shape of the potential jump barrier or surface barrier
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00Semiconductor 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
    • H01L31/04Semiconductor 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
    • H01L31/06Semiconductor 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
    • H01L31/068Semiconductor 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 homojunction type, e.g. bulk silicon PN homojunction solar cells or thin film polycrystalline silicon PN homojunction solar cells
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00Semiconductor 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
    • H01L31/18Processes or apparatus specially adapted for the manufacture or treatment of these devices or of parts thereof
    • H01L31/1804Processes or apparatus specially adapted for the manufacture or treatment of these devices or of parts thereof comprising only elements of Group IV of the Periodic Table
    • YGENERAL 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
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    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E10/00Energy generation through renewable energy sources
    • Y02E10/50Photovoltaic [PV] energy
    • Y02E10/547Monocrystalline silicon PV cells
    • YGENERAL 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
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02PCLIMATE CHANGE MITIGATION TECHNOLOGIES IN THE PRODUCTION OR PROCESSING OF GOODS
    • Y02P70/00Climate change mitigation technologies in the production process for final industrial or consumer products
    • Y02P70/50Manufacturing or production processes characterised by the final manufactured product

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Description

太陽能電池單元及其製造方法Solar battery unit and method of manufacturing same

本發明係有關太陽能電池單元及其製造方法。The present invention relates to a solar cell unit and a method of manufacturing the same.

目前,作為太陽能電池單元之表面反射防止構造,係一般而言最為採用以經由鹼性溶液或氧溶液之濕蝕刻所形成之紋理構造。對此,知道有由將周期性地形成有與太陽光的波長同等或更細微尺寸之凹凸的構造(所謂次波長構造)使用於表面反射防止構造者,實現更低的反射率。因此,由將次波長構造作為太陽能電池單元之表面反射防止構造而使用者,可期待較以往降低反射率,而增大輸出電流者。例如,在非專利文獻1中,即使為次波長構造之中,由將後述之奈米柱陣列構造作為表面反射防止構造而使用者,與以往構造之太陽能電池單元做比較,可經由反射防止效果之輸出電流增大者則經由模擬加以顯示。At present, as a surface reflection preventing structure of a solar battery cell, a texture structure formed by wet etching through an alkaline solution or an oxygen solution is generally used. On the other hand, it is known that a structure (so-called sub-wavelength structure) in which irregularities of the same or finer wavelength as the wavelength of sunlight are periodically formed is used for the surface reflection preventing structure, and a lower reflectance is achieved. Therefore, the user who uses the sub-wavelength structure as the surface reflection preventing structure of the solar battery cell can be expected to lower the reflectance than in the related art and increase the output current. For example, in the case of the sub-wavelength structure, the user can use the nano-column array structure, which will be described later, as the surface reflection preventing structure, and the user can compare the solar cell with the conventional structure. The increase in output current is displayed by simulation.

至目前為止所提案及研究之後述的奈米柱太陽能電池單元之構造係分類成3種類。此等3種類係指顯 示於非專利文獻1之表2的Nanowire Solar Cell(subsurface-junction)、Nanowire Solar Cell(planar-junction)、及Nanowire SolarCell(radial-junction)。在此之Nanowire係與本說明書之奈米柱同義。以下,在本說明書中,各將Nanowire Solar Cell(subsurface-junction)記述為planar深接合型奈米柱太陽能電池單元,而將Nanowire Solar Cell(planar-junction)記述為planar淺接合型奈米柱太陽能電池單元,將Nanowire Solar Cell(radial-junction)記述為radial接合型奈米柱太陽能電池單元。The structure of the nanocolumn solar cell units described and studied later has been classified into three types. These 3 types are indicated Nanowire Solar Cell (subsurface-junction), Nanowire Solar Cell (planar-junction), and Nanowire Solar Cell (radial-junction) shown in Table 2 of Non-Patent Document 1. The Nanowire system here is synonymous with the nano column of this specification. Hereinafter, in the present specification, a Nanowire Solar Cell (subsurface-junction) is described as a planar deep junction type nano column solar battery cell, and a Nanowire Solar Cell (planar-junction) is described as a planar shallow junction type nano column solar energy. In the battery unit, the Nanowire Solar Cell (radial-junction) is described as a radial junction type nano column solar battery unit.

在此,對於上述3種類之太陽能電池單元,係經由形成有高濃度地摻雜不純物於p型基板表面之n+層之時,而形成有pn接合(p與n係亦可為相反)。以下,將「高濃度地摻雜不純物的層」者記述為「射極層」。射極層之作用係主要為形成pn接合的位能差而使電子與電洞分離之作用,作為收集於射極層的載體到達至電極為止的傳導路徑之作用,及降低與電極之接觸阻抗的作用之3點。在planar深接合型奈米柱太陽能電池單元,和planar淺接合型奈米柱太陽能電池單元中,pn接合面係平行之平面狀地形成於基板表面。另一方面,在radial接合型奈米柱太陽能電池單元中,pn接合面係與奈米柱表面平行地加以形成。Here, in the above-described three types of solar battery cells, a pn junction is formed by forming an n+ layer in which a high concentration of impurities is doped on the surface of the p-type substrate (p and n may be reversed). Hereinafter, a "layer in which a high concentration is doped with an impurity" is described as an "emitter layer". The role of the emitter layer is mainly to form the potential difference of the pn junction and separate the electrons from the hole, function as a conduction path for the carrier collected in the emitter layer to reach the electrode, and reduce the contact impedance with the electrode. The role of 3 points. In the planar deep junction type nano column solar cell and the planar shallow junction type nano column solar cell, the pn junction surface is formed in a planar shape parallel to the substrate surface. On the other hand, in the radial junction type nano column solar cell, the pn junction surface is formed in parallel with the surface of the nano column.

在此,上述3種類之太陽能電池單元之不同係位於在奈米柱內之射極層的位置。在planar深接合型奈 米柱太陽能電池單元中,射極層係存在於奈米柱之全範圍。對此,在planar淺接合型奈米柱太陽能電池單元中,射極層係存在於奈米柱之頂部。另外,在radial接合型奈米柱太陽能電池單元中,射極層係存在於奈米柱之側壁部分。如以上,雖在奈米柱內之射極層的位置係為不同,但均在以往的奈米柱太陽能電池單元構造中,於奈米柱之至少一部分的範圍存在有射極層的點係為共通。Here, the difference between the above three types of solar cells is located at the position of the emitter layer in the nano column. Deep joint type nai in planar In the rice column solar cell unit, the emitter layer exists in the entire range of the nano column. In this regard, in the planar shallow junction type nano column solar cell, the emitter layer is present on the top of the column. Further, in the radial junction type nano column solar cell, the emitter layer is present in the side wall portion of the column. As described above, although the positions of the emitter layers in the nano-pillar are different, in the conventional nano-pillar solar cell structure, the point system of the emitter layer exists in at least a part of the column of the nano column. For common.

另外,對於非專利文獻2係記載有經由模擬而調查在奈米柱太陽能電池單元的載體產生率分布的結果,而在奈米柱內部之載體產生率則顯示有相較於在其正下方的基板之載體產生率高出2位數至3位數程度者。Further, Non-Patent Document 2 discloses that the carrier generation rate distribution in the nano-column solar cell is investigated by simulation, and the carrier generation rate inside the nano-column is shown to be directly below The carrier yield of the substrate is higher by two to three digits.

然而,對於專利文獻1係揭示有設置具有光封閉於基板表面效果之複數的開口部之太陽能電池。此係乍看時會認為有如與本申請發明之實施例3相關的構造,但作為其開口部之開口寬度而可舉出1~15μm程度的大小,此係與上述次波長構造不同程度的大小。隨之,記載於專利文獻1之技術係期待與本申請發明之實施例3不同的光學效果之構成。詳細係在實施例3後述之。However, Patent Document 1 discloses a solar cell in which a plurality of openings having light effect on the surface of the substrate are provided. In view of the structure related to the third embodiment of the present invention, the opening width of the opening portion is approximately 1 to 15 μm, which is different from the sub-wavelength structure. . Accordingly, the technique described in Patent Document 1 is expected to have a configuration different from that of Embodiment 3 of the present invention. The details are described later in the third embodiment.

〔先前技術文獻〕[Previous Technical Literature] 〔專利文獻〕[Patent Document]

專利文獻1:日本特開2011-77370號公報Patent Document 1: Japanese Laid-Open Patent Publication No. 2011-77370

〔非專利文獻〕[Non-patent literature]

非專利文獻1:IEEE IEDM Technical Digest,pp. 856 - 859 (2011).Non-Patent Document 1: IEEE IEDM Technical Digest, pp. 856 - 859 (2011).

非專利文獻2:IEEE IEDM Technical Digest,pp. 704 - 707 (2010).Non-Patent Document 2: IEEE IEDM Technical Digest, pp. 704 - 707 (2010).

<對於再結合損失><For recombination loss>

如上述,對於射極層係有著對於太陽能電池單元而言有用的作用之故,設置射極層之情況本身係為必要。但在以往的3種類太陽能電池單元中,於奈米柱內存在有射極層之故,而存在有再結合損失大的課題。以下,以奈米柱太陽能電池單元為例,對於此課題加以敘述。As described above, the emitter layer has a useful function for the solar cell, and the case of providing the emitter layer itself is necessary. However, in the conventional three types of solar battery cells, there is an emitter layer in the nano column, and there is a problem that the recombination loss is large. Hereinafter, a nano column solar battery cell will be taken as an example, and this problem will be described.

圖9係於本發明之前,經由發明者所進行之檢討的結果,對於以40nm間隔配列直徑40nm,高度200nm之奈米柱2於基板1上之奈米柱陣列構造而言,經由FDTD法(Finite Differential Time Domain method)而計算入射波長460nm的光時之載體產生率分布的結果。在圖9中,黑色越濃的範圍,載體產生率越高,反之,白色的範圍係載體產生率為低。與非專利文獻2的結果同樣地,在圖9中,在奈米柱2內部之載體產生率係比在基板的載體產生率高。不僅如此,從圖9亦了解到在奈米柱2內部之中,在側壁部的載體產生率特別高。9 is a result of a review conducted by the inventors before the present invention, and a nanocolumn array structure in which a nanocolumn 2 having a diameter of 40 nm and a height of 200 nm is arranged on the substrate 1 at intervals of 40 nm is subjected to an FDTD method ( The result of the carrier generation rate distribution when light having an incident wavelength of 460 nm is calculated by Finite Differential Time Domain method). In Fig. 9, the darker the range of black, the higher the carrier generation rate, and conversely, the white range is that the carrier generation rate is low. Similarly to the result of Non-Patent Document 2, in FIG. 9, the carrier generation rate in the inside of the column 2 is higher than that in the substrate. Moreover, it is also understood from Fig. 9 that in the inside of the nanocolumn 2, the carrier generation rate in the side wall portion is particularly high.

在此,在加以高濃度地摻雜之半導體中,了解到在各種再結合過程中,歐格再結合的機率變高者。另外,歐格再結合的壽命亦伴隨著不純物濃度之增大而變短。因此,即時由高濃度地加以摻雜之半導體引起有光吸收,而電子電洞對所產生,此等載體係於短時間之中,經由歐格再結合而消滅的機率亦高。隨之,在於奈米柱內存在有射極層之太陽能電池單元中,係因歐格再結合引起的損失則成為課題。Here, in a semiconductor doped with a high concentration, it is understood that the probability of recombination of the Auger becomes high in various recombination processes. In addition, the life of the Auger recombination is also shortened as the concentration of impurities increases. Therefore, the semiconductor which is doped at a high concentration causes light absorption, and the electron hole pair is generated. These carriers are in a short period of time, and the probability of elimination by the Auger recombination is also high. Along with the fact that there is a solar cell having an emitter layer in the nanocolumn, the loss due to the recombination of the Auger is a problem.

以往3種類的奈米柱太陽能電池單元構造之中,在planar深接合型奈米柱太陽能電池單元中,從射極層之佔有體積較其他2種類之構造為大之情況,再結合損失則最大。如對於此做比較時,在planar淺接合型奈米柱太陽能電池單元,和radial接合型奈米柱太陽能電池單元中,將射極層作為薄膜化之故,而再結合損失係比較小,但此等係亦無法避免於奈米柱之至少一部分的範圍,經由存在有高濃度地加以摻雜之射極層之再結合損失。另外,如上述,圖9所示,如根據奈米柱2內部之載體產生率分布,在奈米柱2之側壁部的載體產生率則特別高。從此情況,在radial接合型奈米柱太陽能電池單元中,雖說將射極層作為薄膜化,但所有的側壁部則經由高濃度地加以摻雜之時,有再結合損失變大之情況疑慮。In the conventional three-column solar cell structure, in the planar deep junction type nano column solar cell, the volume occupied by the emitter layer is larger than that of the other two types, and the recombination loss is the largest. . For comparison, in the planar shallow junction type nano column solar cell unit and the radial junction type nano column solar cell unit, the emitter layer is thinned, and the recombination loss is relatively small, but These systems are also incapable of avoiding the recombination loss of the emitter layer doped with a high concentration in the range of at least a portion of the nanopillar. Further, as described above, as shown in Fig. 9, the carrier generation rate in the side wall portion of the nanocolumn 2 is particularly high as the carrier generation rate distribution in the inside of the nanocolumn 2. In this case, in the radial junction type nano column solar battery cell, although the emitter layer is formed into a thin film, when all the side wall portions are doped with a high concentration, there is a fear that the recombination loss becomes large.

<對於表面電極><For surface electrode>

作為以往的太陽能電池單元之其他的課題,對於有關 表面電極之課題加以敘述。在planar深接合型奈米柱太陽能電池單元中,係由射極層作為連續的層所成之故,即使將表面電極設置於射極層之任一的範圍,亦可使自射極層全體的載體到達至表面電極者。因此,可將表面電極設置於與奈米柱不同的範圍者。隨之,表面電極係一般而言使用在結晶Si太陽能電池單元,而亦可為Ag或Al之非透明之金屬所成之指狀.匯流排圖案之電極,而使用在薄膜太陽能電池單元,將ITO(In-Sn-O)等之透明導電性氧化物形成於全面之電極亦可。As another problem of the conventional solar battery unit, The subject of the surface electrode is described. In the planar deep junction type nano column solar cell, the emitter layer is formed as a continuous layer, and even if the surface electrode is provided in any of the emitter layers, the entire emitter layer can be made. The carrier reaches the surface electrode. Therefore, the surface electrode can be placed in a different range from the nano column. Subsequently, the surface electrode is generally used in a crystalline Si solar cell, but may also be a finger made of a non-transparent metal of Ag or Al. The electrode of the bus bar pattern may be used in a thin film solar cell, and a transparent conductive oxide such as ITO (In-Sn-O) may be formed on the entire electrode.

另一方面,在planar淺接合型奈米柱太陽能電池單元與radial接合型奈米柱太陽能電池單元中,作為表面電極,無法使用指狀.匯流排圖案之電極,而必須使用形成於全面的電極,其結果,電極材料則限定為ITO等之透明導電性氧化物。該理由係如以下。首先,對於planar淺接合型奈米柱太陽能電池單元之情況,係僅於奈米柱之頂部形成有射極層之故,而不同的奈米柱內之射極層係相互孤立而存在。隨之,對於為了從此等射極層收集載體,係成為必需為與孤立的複數之射極層加以電性連接之電極之故,而必須使用並非圖案電極而形成於全面之電極。另外,對於radial接合型奈米柱太陽能電池單元之情況係如上述,為了將射極層作為薄膜化而射極層之薄片阻抗變高,其結果,當使用圖案電極時,串聯阻抗損失則變大之故,作為表面電極係有必要使用形成於全面之電極。On the other hand, in the planar shallow junction type nano column solar cell and the radial junction type nano column solar cell, as the surface electrode, the finger shape cannot be used. The electrodes of the bus bar pattern must be formed using a full-surface electrode, and as a result, the electrode material is limited to a transparent conductive oxide such as ITO. The reason is as follows. First, in the case of a planar shallow junction type nano column solar battery cell, an emitter layer is formed only on the top of the nano column, and the emitter layers in different nano columns are isolated from each other. Accordingly, in order to collect the carrier from the emitter layers, it is necessary to electrically connect the electrodes to the isolated plurality of emitter layers, and it is necessary to form the electrodes in a comprehensive manner without using the pattern electrodes. Further, in the case of the radial junction type nano column solar battery cell, as described above, the sheet resistance of the emitter layer is increased in order to thin the emitter layer, and as a result, when the pattern electrode is used, the series impedance loss becomes For the sake of the big reason, it is necessary to use a full-surface electrode as a surface electrode system.

如以上2個單元,對於必需形成電極於全面 之單元構造之情況,係奈米柱上部亦成為由電極加以被覆之故,而無法將反射太陽光之Ag,Al等之金屬作為表面電極而使用者。因而,表面電極之材料係限定為透明導電性氧化物。Such as the above two units, for the necessary formation of electrodes in a comprehensive In the case of the unit structure, the upper portion of the nano column is also covered by the electrode, and the metal such as Ag or Al which reflects sunlight is not used as the surface electrode. Thus, the material of the surface electrode is defined as a transparent conductive oxide.

作為表面電極而使用ITO等之透明導電性氧化物時,產生有因射極層與透明導電性氧化物之接觸阻抗,及透明導電性氧化物之光吸收引起的損失。When a transparent conductive oxide such as ITO is used as the surface electrode, contact resistance between the emitter layer and the transparent conductive oxide and loss due to light absorption of the transparent conductive oxide occur.

首先,對於接觸阻抗加以敘述。與作為圖案電極的材料而一般而言所使用之Ag或Al之金屬做比較時,ITO等之透明導電性氧化物係與將Si為首之半導體材料的接觸阻抗為高。一般而言,接觸阻抗係可由提高半導體之表面不純物濃度者而降低,但如上述,在太陽能電池單元中,提高表面不純物濃度之情況係帶來再結合損失的增大之故,而無法為了接觸阻抗降低而任意地提高表面不純物濃度者。隨之,將透明導電性氧化物作為表面電極而使用時,同時迴避經由高接觸阻抗之損失,和再結合損失雙方情況則為困難。First, the contact impedance is described. When compared with the metal of Ag or Al which is generally used as the material of the pattern electrode, the transparent conductive oxide of ITO or the like has a high contact resistance with a semiconductor material such as Si. In general, the contact resistance can be lowered by increasing the surface impurity concentration of the semiconductor. However, as described above, in the solar cell unit, the increase in the surface impurity concentration causes an increase in the recombination loss, and cannot be contacted. Those whose impedance is lowered to arbitrarily increase the surface impurity concentration. Accordingly, when the transparent conductive oxide is used as the surface electrode, it is difficult to avoid both the loss through the high contact resistance and the recombination loss.

另外,透明導電性氧化物係一般而言知道有吸收紫外線光或紅外線光者,而將此作為表面電極而使用時,產生有到達至太陽能電池單元之光吸收層的光量降低之損失。從以上情況,作為表面電極而使用ITO等之透明導電性氧化物時,成為招致太陽能電池單元之特性下降之要因。Further, in general, a transparent conductive oxide is known to absorb ultraviolet light or infrared light, and when it is used as a surface electrode, a loss of light amount reaching the light absorbing layer of the solar battery cell is reduced. In the above case, when a transparent conductive oxide such as ITO is used as the surface electrode, the characteristics of the solar cell are degraded.

當匯整以上時,將次波長構造,特別是奈米 柱陣列構造,作為表面反射防止構造而使用,以往的太陽能電池單元的課題係如以下。第一,在存在有高濃度地加以摻雜於奈米柱內部之射極層的太陽能電池單元中,存在有再結合損失大之課題。第二,在射極層相互作為孤立之太陽能電池單元,或將射極層作為薄膜化之太陽能電池單元中,作為表面電極,無法使用圖案電極,而必須使用形成ITO等之透明導電性氧化物於全面之電極,其結果,產生有因射極層與透明導電性氧化物之接觸阻抗,及透明導電性氧化物之光吸收引起之損失。在具有次波長構造之太陽能電池單元中,解決上述2個課題之手法係在以往未有過。When merging above, the subwavelength structure, especially the nanometer The column array structure is used as a surface reflection preventing structure, and the problems of the conventional solar cell are as follows. First, in a solar battery cell in which an emitter layer doped at a high concentration in a nano column is present, there is a problem that the recombination loss is large. Secondly, in the case where the emitter layers are used as isolated solar cells or the emitter layer is used as a thinned solar cell, as the surface electrode, the pattern electrode cannot be used, and it is necessary to use a transparent conductive oxide which forms ITO or the like. As a result of the overall electrode, there is a loss due to the contact resistance between the emitter layer and the transparent conductive oxide and the light absorption by the transparent conductive oxide. In the solar battery cell having the sub-wavelength structure, the method for solving the above two problems has not been conventionally used.

本發明係有鑑於上述情形所研發,其目的為實現可並存在次波長構造內部之再結合損失降低,與作為表面電極而使用圖案電極情況之太陽能電池單元者。本發明之前述及其他目的與新的特徵,係可從本說明書的記述及附加圖面了解。The present invention has been made in view of the above circumstances, and an object thereof is to realize a solar cell unit in which a re-bonding loss in a sub-wavelength structure can be reduced and a pattern electrode is used as a surface electrode. The above and other objects and novel features of the present invention will become apparent from the description and appended claims.

如將在本申請所揭示之發明之中所代表之構成,簡單地進行說明時,如以下。The configuration represented by the invention disclosed in the present application will be briefly described as follows.

第1,一種太陽能電池單元,其特徵為具有:具備延伸於特定方向之複數的柱體,且為第1導電型之基板,和與基板接合加以設置,不同於第1導電型之第2導電型之射極層,複數的柱體係由第1導電型的半導體所 成,各複數的柱體係在其側面中與前述射極層接合者。First, a solar battery cell comprising: a plurality of pillars extending in a specific direction; and a substrate of a first conductivity type and a substrate bonded to the substrate, different from the second conductivity of the first conductivity type Type of emitter layer, plural column system by first conductivity type semiconductor In this case, each of the plurality of column systems is joined to the aforementioned emitter layer in its side.

第2,一種太陽能電池單元,其特徵為具有:於其表面具有複數的柱狀凹部而且為第1導電型之基板,和設置於基板的表面且未設置有柱狀凹部之部分,與第1導電型不同之第2導電型的射極層,柱狀凹部的寬度為1μm以下者。According to a second aspect of the invention, there is provided a solar battery cell comprising: a first conductive type substrate having a plurality of columnar recesses on a surface thereof; and a portion provided on a surface of the substrate and not provided with a columnar recess, and the first The second conductivity type emitter layer having different conductivity types has a columnar recess having a width of 1 μm or less.

第3,一種太陽能電池單元的製造方法,其特徵為具有將金屬圖案作為光罩,而於第1導電型之基板表面形成與第1導電型不同之第2導電型的射極層之第1工程,和使用金屬圖案而於基板表面形成第1導電型之複數的柱體之第2工程者。According to a third aspect of the invention, in a method of manufacturing a solar cell, the first pattern of the second conductivity type emitter layer different from the first conductivity type is formed on the surface of the first conductivity type substrate by using a metal pattern as a mask. Engineering, and a second engineer who uses a metal pattern to form a plurality of columns of the first conductivity type on the surface of the substrate.

根據本發明時,在具有次波長構造的太陽能電池單元中,可並存在次波長構造內部之再結合損失降低,與作為表面電極而使用圖案電極者。According to the present invention, in the solar battery cell having the sub-wavelength structure, the recombination loss inside the sub-wavelength structure can be reduced, and the pattern electrode can be used as the surface electrode.

1‧‧‧基板1‧‧‧Substrate

2‧‧‧奈米柱2‧‧‧Neizhu

3‧‧‧凸部3‧‧‧ convex

4‧‧‧奈米孔4‧‧‧Nemicon

11‧‧‧射極層11‧‧ ‧ emitter layer

12‧‧‧鈍化膜12‧‧‧ Passivation film

13‧‧‧表面電極13‧‧‧ surface electrode

21‧‧‧BSF層21‧‧‧BSF layer

22‧‧‧背面電極22‧‧‧Back electrode

31‧‧‧光阻劑31‧‧‧ photoresist

32‧‧‧觸媒金屬32‧‧‧catalyst metal

33‧‧‧蝕刻光罩33‧‧‧ etching mask

圖1(a)係有關本發明之實施例1之奈米柱太陽能電池單元的上面圖。Fig. 1(a) is a top view of a nanocolumn solar cell unit according to Embodiment 1 of the present invention.

圖1(b)係有關本發明之實施例1之奈米柱太陽能電池單元的剖面圖。Fig. 1(b) is a cross-sectional view showing a nanocolumn solar cell unit according to Embodiment 1 of the present invention.

圖2(a)係僅從有關本發明之實施例1之奈米柱太 陽能電池單元去除鈍化膜構造的上面圖。Figure 2 (a) is only from the nano column of the embodiment 1 of the present invention. The top view of the passive cell structure is removed from the solar cell.

圖2(b)係僅從有關本發明之實施例1之奈米柱太陽能電池單元去除鈍化膜構造的剖面圖。Fig. 2 (b) is a cross-sectional view showing only the structure of the passivation film removed from the column solar cell of Example 1 of the present invention.

圖3(a)係顯示有關本發明之實施例1之奈米柱太陽能電池單元之第1製造方法的第1上面圖。Fig. 3 (a) is a first top view showing a first manufacturing method of the nanocolumn solar battery cell of the first embodiment of the present invention.

圖3(b)係顯示有關本發明之實施例1之奈米柱太陽能電池單元之第1製造方法的第1剖面圖。Fig. 3 (b) is a first cross-sectional view showing a first manufacturing method of the nanocolumn solar battery cell of the first embodiment of the present invention.

圖3(c)係顯示有關本發明之實施例1之奈米柱太陽能電池單元之第1製造方法的第2上面圖。Fig. 3 (c) is a second top view showing a first manufacturing method of the nanocolumn solar battery cell of the first embodiment of the present invention.

圖3(d)係顯示有關本發明之實施例1之奈米柱太陽能電池單元之第1製造方法的第2剖面圖。Fig. 3 (d) is a second cross-sectional view showing a first manufacturing method of the nanocolumn solar battery cell according to the first embodiment of the present invention.

圖3(e)係顯示有關本發明之實施例1之奈米柱太陽能電池單元之第1製造方法的第3上面圖。Fig. 3 (e) is a third top view showing a first manufacturing method of the column solar cell of the first embodiment of the present invention.

圖3(f)係顯示有關本發明之實施例1之奈米柱太陽能電池單元之第1製造方法的第3剖面圖。Fig. 3 (f) is a third cross-sectional view showing a first manufacturing method of the nanocolumn solar battery cell according to the first embodiment of the present invention.

圖3(g)係顯示有關本發明之實施例1之奈米柱太陽能電池單元之第1製造方法的第4上面圖。Fig. 3 (g) is a fourth top view showing a first manufacturing method of the nanocolumn solar battery cell according to the first embodiment of the present invention.

圖3(h)係顯示有關本發明之實施例1之奈米柱太陽能電池單元之第1製造方法的第4剖面圖。Fig. 3 (h) is a fourth cross-sectional view showing a first method of manufacturing the nanocolumn solar cell of the first embodiment of the present invention.

圖3(i)係顯示有關本發明之實施例1之奈米柱太陽能電池單元之第1製造方法的第5上面圖。Fig. 3 (i) is a fifth top view showing a first manufacturing method of the nanocolumn solar battery cell of the first embodiment of the present invention.

圖3(j)係顯示有關本發明之實施例1之奈米柱太陽能電池單元之第1製造方法的第5剖面圖。Fig. 3 (j) is a fifth sectional view showing a first manufacturing method of the nanocolumn solar battery cell according to the first embodiment of the present invention.

圖3(k)係顯示有關本發明之實施例1之奈米柱太 陽能電池單元之第1製造方法的第6上面圖。Figure 3 (k) shows the nanocolumn of the embodiment 1 of the present invention. The sixth top view of the first manufacturing method of the solar battery unit.

圖3(l)係顯示有關本發明之實施例1之奈米柱太陽能電池單元之第1製造方法的第6剖面圖。Fig. 3 (l) is a sixth sectional view showing a first manufacturing method of the nanocolumn solar battery cell of the first embodiment of the present invention.

圖3(m)係顯示有關本發明之實施例1之奈米柱太陽能電池單元之第1製造方法的第7上面圖。Fig. 3 (m) is a seventh top view showing a first manufacturing method of the nanocolumn solar battery cell of the first embodiment of the present invention.

圖3(n)係顯示有關本發明之實施例1之奈米柱太陽能電池單元之第1製造方法的第7剖面圖。Fig. 3 (n) is a seventh sectional view showing a first manufacturing method of the nanocolumn solar battery cell of the first embodiment of the present invention.

圖3(o)係顯示有關本發明之實施例1之奈米柱太陽能電池單元之第1製造方法的第8上面圖。Fig. 3 (o) is an eighth top view showing a first manufacturing method of the nanocolumn solar battery cell of the first embodiment of the present invention.

圖3(p)係顯示有關本發明之實施例1之奈米柱太陽能電池單元之第1製造方法的第8剖面圖。Fig. 3 (p) is a cross-sectional view showing the eighth manufacturing method of the first column solar cell of the first embodiment of the present invention.

圖4(a)係顯示有關本發明之實施例1之奈米柱太陽能電池單元之第1製造方法的第1上面圖。Fig. 4 (a) is a first top view showing a first manufacturing method of the nanocolumn solar battery cell of the first embodiment of the present invention.

圖4(b)係顯示有關本發明之實施例1之奈米柱太陽能電池單元之第1製造方法的第1剖面圖。Fig. 4 (b) is a first cross-sectional view showing a first method of manufacturing the nanocolumn solar cell of the first embodiment of the present invention.

圖4(c)係顯示有關本發明之實施例1之奈米柱太陽能電池單元之第1製造方法的第2上面圖。Fig. 4 (c) is a second top view showing a first manufacturing method of the nanocolumn solar battery cell of the first embodiment of the present invention.

圖4(d)係顯示有關本發明之實施例1之奈米柱太陽能電池單元之第1製造方法的第2剖面圖。Fig. 4 (d) is a second cross-sectional view showing a first manufacturing method of the nanocolumn solar battery cell of the first embodiment of the present invention.

圖4(e)係顯示有關本發明之實施例1之奈米柱太陽能電池單元之第1製造方法的第3上面圖。Fig. 4 (e) is a third top view showing a first manufacturing method of the nanocolumn solar battery cell of the first embodiment of the present invention.

圖4(f)係顯示有關本發明之實施例1之奈米柱太陽能電池單元之第1製造方法的第3剖面圖。Fig. 4 (f) is a third cross-sectional view showing a first method of manufacturing the nanocolumn solar cell of the first embodiment of the present invention.

圖5(a)係有關本發明之實施例2之奈米溝槽太陽 能電池單元的上面圖。Figure 5 (a) is a nano-groove sun relating to Embodiment 2 of the present invention. The above figure of the battery unit.

圖5(b)係有關本發明之實施例2之奈米溝槽太陽能電池單元的剖面圖。Figure 5 (b) is a cross-sectional view showing a nanochannel solar cell of Embodiment 2 of the present invention.

圖6(a)係僅從有關本發明之實施例2之奈米溝槽太陽能電池單元去除鈍化膜構造的上面圖。Fig. 6(a) is a top view showing only the structure of the passivation film removed from the nanochannel solar cell of Example 2 of the present invention.

圖6(b)係僅從有關本發明之實施例2之奈米溝槽太陽能電池單元去除鈍化膜構造的剖面圖。Fig. 6 (b) is a cross-sectional view showing only the structure of the passivation film removed from the nanochannel solar cell of Example 2 of the present invention.

圖7(a)係有關本發明之實施例3之奈米孔太陽能電池單元的上面圖。Fig. 7 (a) is a top view of a nanoporous solar cell unit according to Example 3 of the present invention.

圖7(b)係有關本發明之實施例3之奈米孔太陽能電池單元的剖面圖。Fig. 7 (b) is a cross-sectional view showing a nanopore solar battery cell of Example 3 of the present invention.

圖8(a)係僅從有關本發明之實施例3之奈米孔太陽能電池單元去除鈍化膜構造的上面圖。Fig. 8(a) is a top view showing only the structure of the passivation film removed from the nanopore solar cell unit of Example 3 of the present invention.

圖8(b)係僅從有關本發明之實施例3之奈米孔太陽能電池單元去除鈍化膜構造的剖面圖。Fig. 8 (b) is a cross-sectional view showing only the structure of the passivation film removed from the nanoporous solar cell unit of Example 3 of the present invention.

圖9係對於以40nm間隔配列直徑40nm,高度200nm之奈米柱之奈米柱陣列構造而言,經由FDTD法而計算入射波長460nm的光時之載體產生率分布的結果。9 is a result of a carrier generation rate distribution when light having an incident wavelength of 460 nm is calculated by an FDTD method for a nanocolumn array structure in which a nanometer column having a diameter of 40 nm and a height of 200 nm is arranged at intervals of 40 nm.

實施例1Example 1 <用語的定義><Definition of terms>

在本說明書中,係在次波長構造之中,亦採納奈米柱 陣列構造,奈米孔陣列構造,及奈米溝槽陣列構造之3種類的構造。以下,敘述此等3種類之構造的定義。奈米柱陣列構造係指與太陽光的波長同等,或具有更細微寬度之柱狀構造(以下,記述為「奈米柱」或單為「柱體」),則周期性地配列於基板表面之構造。該柱狀構造之柱軸方向係與基板面垂直。在以下的實施例中,作為奈米柱的例而舉出圓柱,但亦可為角柱等不同之剖面形狀。奈米孔陣列構造係指與太陽光的波長同等,或構成更細微寬度之柱狀構造的空隙,則周期性地開孔於基板表面之構造。該柱狀構造之柱軸方向係與基板面垂直。同樣地,柱狀構造之形狀係並非圓柱,而亦可為角柱等不同之剖面形狀。奈米溝槽陣列構造係指與太陽光的波長同等,或具有更細微寬度之凸部則周期性地配列於基板表面上,其結果,於凸部之間具有周期性的溝(溝槽)之構造。作為凸部之剖面形狀係一般為四角形,三角形,或者扇形等。從基板的上面觀察之情況,奈米柱陣列構造與奈米孔陣列構造則對於具有2次元之周期性之構造而言,奈米溝槽陣列構造係具有1次元之周期性之構造。然而,將柱狀構造,及凸部的「寬度」,作為平行於基板面之方向之長度。In this specification, in the sub-wavelength structure, the nano column is also adopted. Array structure, nanopore array structure, and three types of structures of nano-groove array structure. Hereinafter, the definitions of the three types of structures will be described. The nano-column array structure is a columnar structure (hereinafter referred to as "nano column" or "column") which is equivalent to the wavelength of sunlight or has a finer width, and is periodically arranged on the surface of the substrate. Construction. The column axis direction of the columnar structure is perpendicular to the substrate surface. In the following examples, a column is exemplified as the column of the nano column, but a different cross-sectional shape such as a corner column may be used. The nanopore array structure refers to a structure in which a columnar structure having a finer width is formed in the same manner as the wavelength of sunlight, and the structure is periodically opened on the surface of the substrate. The column axis direction of the columnar structure is perpendicular to the substrate surface. Similarly, the shape of the columnar structure is not a cylinder, but may be a different sectional shape such as a corner post. The nano-groove array structure means that the convex portions having the same wavelength as the sunlight or having a finer width are periodically arranged on the surface of the substrate, and as a result, there are periodic grooves (grooves) between the convex portions. Construction. The cross-sectional shape of the convex portion is generally a quadrangle, a triangle, or a fan shape. When viewed from the upper surface of the substrate, the nano-pillar array structure and the nanopore array structure have a one-dimensional periodic structure for a structure having a periodicity of two dimensions. However, the columnar structure and the "width" of the convex portion are taken as the length parallel to the direction of the substrate surface.

對於此等3種類之次波長構造之反射防止效果加以敘述時,奈米柱陣列構造與奈米孔陣列構造之反射率係一般而言略相同程度,而奈米溝槽陣列構造係與前述2種類的構造做比較時,一般而言反射率為高。另外,奈米柱陣列構造與奈米孔陣列構造係即使在入射光則並非從 垂直方向而是從斜方向進入至基板面之情況,亦顯示比較低之反射率,但奈米溝槽陣列構造係對於傾斜進入於垂直方向至溝的光而言,係了解到反射率成為比較高者。如此,前述3種類的次波長構造係雖在反射防止效果的點為不同,但如以下所述地,均成為本發明之對象。在本說明書中,將奈米柱陣列構造,奈米孔陣列構造,奈米溝槽陣列構造作為表面反射防止構造而具有之太陽能電池單元,各記述為奈米柱太陽能電池單元,奈米孔太陽能電池單元,奈米溝槽太陽能電池單元。When the reflection preventing effect of these three types of sub-wavelength structures is described, the reflectance of the nano-pillar array structure and the nanopore array structure is generally the same, and the nano-groove array structure is the same as the above 2 When the types of structures are compared, the reflectance is generally high. In addition, the nano-column array structure and the nanopore array structure are not from the incident light. The vertical direction enters the substrate surface from the oblique direction, and also shows a relatively low reflectance. However, the nano-groove array structure is known to reflect the reflectance when the light enters the vertical direction to the groove. The taller. As described above, the three types of sub-wavelength structures are different in point of the anti-reflection effect, but they are all objects of the present invention as described below. In the present specification, a nano-column array structure, a nanopore array structure, and a nano-groove array structure are provided as solar cell units having a surface reflection preventing structure, and each is described as a nano column solar cell unit, and a nanopore solar cell Battery unit, nano-groove solar cell unit.

然而,在以下的實施例中,將基板等作為p型,而將射極層作為n型而加以說明,但對於將此等導電型作為相反的構成亦可作為相同的討論,而屬於本申請發明之技術範圍的範疇。However, in the following embodiments, the substrate or the like is referred to as a p-type, and the emitter layer is described as an n-type. However, the same configuration may be considered as the opposite configuration, and the present application is hereby incorporated by reference. The scope of the technical scope of the invention.

<單元構造><unit construction>

圖1(a)及(b)係有關本發明之實施例1之奈米柱太陽能電池單元的上面圖及剖面圖。實施例1之奈米柱太陽能電池單元係於基板1上,形成有奈米柱2之奈米柱太陽能電池單元。對於圖1係顯示有奈米柱2為圓柱情況的構造,但如上述,奈米柱2係亦可為角柱等,具有不同剖面形狀之柱狀構造。對於奈米柱2及射極層11的最表面係形成有鈍化膜12,但對於表面電極13的正下方係未存在有鈍化膜12,而相互接觸有射極層11與表面電極13。圖1(b)的剖面圖係描繪有是否相互孤立而存在有複數 之射極層11,但實際上,射極層11係遍佈連續於基板1上全面的層。為了顯示此,將從實施例1之奈米柱太陽能電池單元構造,僅除去鈍化層12之構造的上面圖及剖面圖,各示於圖2(a)及(b)。如圖2(a)之上面圖所示,射極層11係網羅奈米柱2之間的範圍,隨之,並無相互孤立而遍佈連續於基板1上全面。1(a) and 1(b) are a top view and a cross-sectional view of a nanocolumn solar cell unit according to Embodiment 1 of the present invention. The nanocolumn solar cell of Example 1 was attached to a substrate 1, and a nanocolumn solar cell of a nanocolumn 2 was formed. Fig. 1 shows a structure in which the column 2 is cylindrical. However, as described above, the column 2 can also be a column or the like having a columnar structure having different cross-sectional shapes. The passivation film 12 is formed on the outermost surface of the nanopillar 2 and the emitter layer 11, but the passivation film 12 is not present directly under the surface electrode 13, and the emitter layer 11 and the surface electrode 13 are in contact with each other. Figure 1 (b) is a cross-sectional view of whether there are isolated or not The emitter layer 11 is actually, but the emitter layer 11 is spread over a layer that is continuous over the substrate 1. To show this, the top view and the cross-sectional view of the structure in which only the passivation layer 12 is removed from the nanocolumn solar cell structure of the first embodiment are shown in Figs. 2(a) and 2(b). As shown in the upper diagram of Fig. 2(a), the range of the emitter layer 11 between the nano-columns 2 is, without being isolated from each other, continuous throughout the substrate 1.

一般而言,太陽能電池單元係經由半導體pn接合或pin接合,或者半導體與金屬之肖特基接合而加以構成。在以下中,設想經由pn接合而加以構成之太陽能電池單元而敘述。在實施例1之奈米柱太陽能電池單元中,基板1與奈米柱2係同樣由導電型(第1導電型)之半導體材料所成。以下,對於基板1與奈米柱2均為p型半導體之情況加以敘述,但本發明係對於p型與n型為相反之情況亦可適用。基板1與奈米柱2為p層之情況,射極層11係高濃度地加以摻雜,且與第1導電型不同之導電型(第2導電型)的層,而將基板1及奈米柱2作為p型之情況係n+ 層。隨之,基板1及奈米柱2,和射極層11則形成pn接合。特別是對於奈米柱2係在其側面,形成與射極層11加以pn接合,而在其前端部係未與射極層11形成pn接合。另外,在太陽能電池單元中係為與基板相同導電型,一般進行將高濃度地加以摻雜之BSF(Back Surface Field)層形成於基板與背面電極之間之情況。在實施例1之奈米柱太陽能電池單元中,係於基板1與背面電極22之間,形成有p+ 層所成之BSF層21。然而,在圖 1中,係顯示有BSF層21與背面電極22則遍佈全面而接觸之構造,但例如,於BSF層21與背面電極22之間形成有鈍化膜,僅在局部的範圍,除去鈍化膜,接觸有BSF層21與背面電極22,使用所謂點接觸構造亦可。In general, a solar cell is configured by semiconductor pn bonding or pin bonding, or Schottky bonding of a semiconductor and a metal. Hereinafter, a solar battery cell configured by pn bonding will be described. In the nanocolumn solar cell of the first embodiment, the substrate 1 and the nanopillar 2 are made of a conductive (first conductivity type) semiconductor material. Hereinafter, the case where the substrate 1 and the nano-pillar 2 are both p-type semiconductors will be described, but the present invention is also applicable to the case where the p-type and the n-type are opposite. When the substrate 1 and the nano-pillar 2 are p-layers, the emitter layer 11 is doped at a high concentration, and a conductive type (second conductivity type) layer different from the first conductivity type is used, and the substrate 1 and the substrate are provided. When the rice column 2 is a p-type, it is an n + layer. Accordingly, the substrate 1 and the nano-pillar 2 and the emitter layer 11 form a pn junction. In particular, the nanopillar 2 is formed with a pn junction with the emitter layer 11 on its side surface, and does not form a pn junction with the emitter layer 11 at its front end portion. Further, in the solar battery cell, the same conductivity type as the substrate is used, and a BSF (Back Surface Field) layer doped with a high concentration is generally formed between the substrate and the back surface electrode. In the nanocolumn solar cell of the first embodiment, a BSF layer 21 made of a p + layer is formed between the substrate 1 and the back surface electrode 22. However, in FIG. 1, a structure in which the BSF layer 21 and the back surface electrode 22 are spread over the entire surface is shown, but for example, a passivation film is formed between the BSF layer 21 and the back surface electrode 22, and is removed only in a partial range. The passivation film is in contact with the BSF layer 21 and the back surface electrode 22, and a so-called point contact structure may be used.

對於構成實施例1之奈米柱太陽能電池單元之材料加以敘述。光吸收層之基板1,奈米柱2,射極層11,及BSF層21之材料係Si、CdTe、CuInGaSe、InP、GaAs、Ge等之半導體,此等係可採取單結晶,多結晶,微結晶,非晶質等之各種構造。鈍化膜12的材料係SiO2 、SiN(氮化矽)、非晶質Si、SiC(碳化矽)、CdS等之絕緣體、或者此等絕緣體的層積構造。表面電極13及背面電極22的材料係Ag、Al、Ti、Pd、Ni、Cu等之金屬,或此等之層積構造。The material constituting the nanocolumn solar cell of Example 1 will be described. The substrate 1 of the light absorbing layer, the material of the nano-pillar 2, the emitter layer 11, and the BSF layer 21 are semiconductors of Si, CdTe, CuInGaSe, InP, GaAs, Ge, etc., which may adopt single crystal, polycrystalline, Various structures such as microcrystals, amorphous, and the like. The material of the passivation film 12 is an insulator such as SiO 2 , SiN (tantalum nitride), amorphous Si, SiC (cerium carbide), CdS, or the like, or a laminated structure of these insulators. The material of the surface electrode 13 and the back surface electrode 22 is a metal such as Ag, Al, Ti, Pd, Ni, Cu, or the like, or a laminated structure thereof.

如此,有關實施例1之太陽能電池單元,其特徵為具有:具備延伸於特定方向之複數的柱體2,且為第1導電型(p型)之基板1,和與基板1接合加以設置之不同於第1導電型的第2導電型(n型)之射極層11,複數的柱體2係由第1導電型的半導體所成,複數的柱體2係在其側面中與射極層11接合者。在此,射極層11之不純物濃度係較複數之柱體2之不純物濃度為高。As described above, the solar battery cell of the first embodiment is characterized in that the substrate 1 having the plurality of columns 2 extending in a specific direction and being the first conductivity type (p type) is bonded to the substrate 1 and provided. Unlike the second conductivity type (n-type) emitter layer 11 of the first conductivity type, the plurality of pillars 2 are formed of a first conductivity type semiconductor, and the plurality of pillars 2 are formed on the side surface thereof and the emitter. Layer 11 joiner. Here, the impurity concentration of the emitter layer 11 is higher than the impurity concentration of the plurality of columns 2.

經由有關的構造,有關實施例1之太陽能電池係具有以下的效果。第1,可將射極層11作為未設置於奈米柱2內部之構造者。經由此,成為可享受經由射極層11之優點同時,且可降低在奈米柱內部之再結合損失 的機率者。The solar cell system according to Example 1 has the following effects via the related configuration. First, the emitter layer 11 can be used as a structure that is not provided inside the nano-pillar 2. Thereby, the advantage of passing through the emitter layer 11 can be enjoyed at the same time, and the recombination loss inside the nanocolumn can be reduced. Probability.

第2,可將射極層11作為在奈米柱2之間連續的層者。經由此,與射極層之孤立之planar淺接合型奈米柱太陽能電池單元不同,表面電極13係如與射極層11之一部分電性連接時,可收集自射極層11之全範圍的載體者。隨之,有關實施例1之太陽能電池單元係作為與射極層11加以電性連接之表面電極13,成為可使用Ag、Al、Ti、Pd、Ni、Cu、或此等之層積構造所成之圖案電極者。Second, the emitter layer 11 can be used as a continuous layer between the nanopillars 2. Thus, unlike the isolated planar shallow junction type nano column solar cell of the emitter layer, the surface electrode 13 can be collected from the entire range of the emitter layer 11 when electrically connected to a portion of the emitter layer 11. Carrier. Accordingly, the solar cell of the first embodiment is a surface electrode 13 electrically connected to the emitter layer 11, and a laminated structure of Ag, Al, Ti, Pd, Ni, Cu, or the like can be used. The pattern electrode is formed.

另外,如上述,奈米柱2係由p型的半導體所成,而未含有n型之射極層之故,而成為可將鈍化膜12,與奈米柱2及射極層11接合而設置者。Further, as described above, the nano-pillar 2 is formed of a p-type semiconductor and does not include an n-type emitter layer, so that the passivation film 12 can be bonded to the nano-pillar 2 and the emitter layer 11 . Setter.

另外,與必須將射極層作為薄膜化之radial接合型奈米柱太陽能電池單元不同,無需將射極層11作為薄膜化。隨之,將射極層11作為厚膜化,可相對地降低薄片阻抗者。具體而言,射極層11之膜厚,例如可作為500nm以上者。Further, unlike the radial junction type nano column solar cell in which the emitter layer is required to be thinned, it is not necessary to form the emitter layer 11 as a thin film. Accordingly, the emitter layer 11 is made thicker, and the sheet resistance can be relatively reduced. Specifically, the film thickness of the emitter layer 11 can be, for example, 500 nm or more.

如以上,如根據有關實施例1之太陽能電池單元,與以往的太陽能電池單元作比較,成為可並存在次波長構造內部之再結合損失降低,和作為表面電極而使用圖案電極之情況者。As described above, according to the solar battery cell of the first embodiment, compared with the conventional solar battery cell, the recombination loss inside the sub-wavelength structure can be reduced, and the pattern electrode can be used as the surface electrode.

<第1製造方法><First Manufacturing Method>

圖3係顯示實施例1之奈米柱太陽能電池單元之第1 製造方法的圖。對於實施例1之奈米柱太陽能電池單元之製造方法係有不同奈米柱之形成方法的2種方法。在第1製造方法中,係經由成長法而形成奈米柱,而在第2製造方法中,係經由加工法而形成奈米柱。以下,依據圖3而說明實施例1之奈米柱太陽能電池單元之第1製造方法。然而,在圖3所示之製造方法中,係省略背面側之構造,即BSF層21與背面電極22之形成工程。此等2種工程係可與一般的太陽能電池單元之製造方法同樣地進行。3 is a view showing the first of the nano column solar battery cells of Example 1. Diagram of the manufacturing method. The method for producing a nanocolumn solar cell of the first embodiment is two methods for forming a different column. In the first production method, a nano column is formed by a growth method, and in the second production method, a nano column is formed by a processing method. Hereinafter, a first manufacturing method of the nanocolumn solar battery cell of the first embodiment will be described with reference to Fig. 3 . However, in the manufacturing method shown in FIG. 3, the structure of the back side, that is, the formation of the BSF layer 21 and the back surface electrode 22 is omitted. These two types of engineering can be performed in the same manner as the general solar cell manufacturing method.

首先,於基板1的表面形成光阻劑31。將形成後之構造的上面圖示於圖3(a),將剖面圖示於圖3(b)。光阻劑31係首先偏佈基板1上之全面加以塗佈之後,經由光微影而加以圖案化。圖案化後,未存在有光阻劑31之範圍則成為最終的太陽能電池單元構造之奈米柱2的範圍。然而,如圖3(a)及(b)所示,對於最終形成有表面電極13之範圍,係未進行圖案化而作為呈未形成有奈米柱2者為佳。First, a photoresist 31 is formed on the surface of the substrate 1. The upper view of the structure after formation is shown in Fig. 3(a), and the cross-sectional view is shown in Fig. 3(b). The photoresist 31 is first patterned on the substrate 1 and then patterned by photolithography. After the patterning, the range in which the photoresist 31 is not present becomes the range of the nano column 2 of the final solar cell structure. However, as shown in FIGS. 3(a) and 3(b), the range in which the surface electrode 13 is finally formed is not patterned, and it is preferable that the nanopillar 2 is not formed.

接著,將觸媒金屬32形成於光阻劑31上。將形成後之構造的上面圖示於圖3(c),將剖面圖示於圖3(d)。觸媒金屬32係如後述,在奈米柱2成長時成為必要之構成,一般使用Cu、Au、Pt等。觸媒金屬32之形成係經由蒸鍍法,濺鍍法,CVD法等而進行。Next, the catalyst metal 32 is formed on the photoresist 31. The upper view of the structure after formation is shown in Fig. 3(c), and the cross-sectional view is shown in Fig. 3(d). The catalyst metal 32 is a structure which is necessary when the nano column 2 is grown as described later, and generally Cu, Au, Pt or the like is used. The formation of the catalyst metal 32 is performed by a vapor deposition method, a sputtering method, a CVD method, or the like.

之後,經由舉離法而除去光阻劑31,及形成於光阻劑31之正上方之觸媒金屬32。將除去後之構造的上面圖示於圖3(e),將剖面圖示於圖3(f)。舉離法 的結果,於基板1上,形成存在有加以圖案化之觸媒金屬32之構造。作為形成此構造之方法,在實施例1中,敘述過使用光阻劑31之舉離法的方法,但亦有如以下之另外的方法。即,於基板1的表面,並非形成光阻劑31而從最初形成加以圖案化之觸媒金屬32之方法。對於形成加以圖案化之觸媒金屬32,係使用採用金屬光罩之蒸鍍法,或使觸媒金屬的奈米粒子分散之方法。對於此等方法係與在實施例1所述,使用舉離法之方法作比較,有著可縮短工程數與成本的優點,但另一方面,存在有對於觸媒金屬32之圖案尺寸容易產生有不均之課題。觸媒金屬32之圖案尺寸的不均係最終係成為奈米柱2之圖案尺寸的不均。採用舉離法,或還是從最初形成加以圖案化之觸媒金屬32的選擇係應考慮可將奈米柱2之圖案尺寸的不均容許至何種程度的點。Thereafter, the photoresist 31 and the catalyst metal 32 formed directly above the photoresist 31 are removed by the lift-off method. The upper view of the structure after removal is shown in Fig. 3(e), and the cross-sectional view is shown in Fig. 3(f). Lifting method As a result, a structure in which the patterned catalyst metal 32 is present is formed on the substrate 1. As a method of forming this structure, in the first embodiment, a method of removing the photoresist 31 is described, but there are also other methods as follows. That is, on the surface of the substrate 1, a method of forming the patterned catalyst metal 32 from the beginning is not formed without forming the photoresist 31. For forming the patterned catalyst metal 32, a vapor deposition method using a metal mask or a method of dispersing nano particles of a catalyst metal is used. For these methods, compared with the method described in Embodiment 1, the method of using the lift-off method has the advantage of shortening the number of projects and cost, but on the other hand, there is a possibility that the pattern size of the catalyst metal 32 is likely to occur. The problem of unevenness. The unevenness of the pattern size of the catalyst metal 32 is ultimately the unevenness of the pattern size of the nano-pillars 2. The selection by the lift-off method, or the formation of the patterned catalyst metal 32 from the beginning, should be considered to the extent that the unevenness of the pattern size of the nano-pillars 2 can be tolerated.

另外,對於進行經由使觸媒金屬的奈米粒子分散的方法,僅於如上述之最終形成有表面電極13之範圍,未進行圖案化而作為呈未形成有奈米柱2之情況,係必須施加如以下之手段。即,必須另外要有除去在使奈米粒子分散於基板1上之全面之後未進行圖案化之範圍的奈米粒子,或者由調整在分散奈米粒子之前未進行圖案化之範圍的基板1表面之化學性質者,所分散之奈米粒子產生排斥,作為呈於未進行圖案化之範圍未存在有奈米粒子之工程。隨之,對於使用奈米粒子之分散的方法,作為如上述之方法的結果,亦存在有工程數或成本增大的課題。In addition, in the method of dispersing the nanoparticles of the catalyst metal, only in the range where the surface electrode 13 is finally formed as described above, the patterning is not performed, and the nanopillar 2 is not formed. Apply the following means. That is, it is necessary to additionally have a surface in which the nanoparticle which has not been patterned after dispersing the nanoparticles on the substrate 1 is removed, or the surface of the substrate 1 which is not subjected to patterning before the dispersion of the nanoparticles is adjusted. In the case of chemical properties, the dispersed nanoparticles are repelled as a process in which nanoparticles are not present in the range where they are not patterned. Accordingly, as a result of the method described above, there is a problem that the number of projects or the cost increases as a result of the method of dispersing the nanoparticles.

接著,形成射極層11。伴隨此,在圖3(j)之工程中成為奈米柱2之範圍之中,亦合併接合於射極層11之部分(pn接合部)而加以形成者。將形成後之構造的上面圖示於圖3(g),將剖面圖示於圖3(h)。射極層11之形成係經由氣相擴散法,固相擴散法,離子注入法等之不純物注入法而進行。隨之,觸媒金屬32係成為使用於奈米柱2之成長的觸媒之同時,亦達成作為不純物擴散之光罩的作用者。因此,將奈米柱2與射極層11之相對位置,自我整合地調整。然而,在經由不純物注入法而形成射極層11時,如上述,雖觸媒金屬32達成光罩的作用,但一旦注入於基板1之內部之不純物的擴散係一般而言成為同向性。隨之,實際上,射極層11係對於觸媒金屬32之下部,也就是奈米柱2之下部,亦一部分加以形成。如果,射極層11的橫方向擴散長度變為較奈米柱2的直徑為大時,成為奈米柱2與基板1則經由射極層11而隔開之構造。如上述,對於基板1與奈米柱2為p層,射極層11為n+ 層之情況,奈米柱2,射極層11,基板1之順序的構造係成為pn+ p構造之故,在奈米柱2內部產生的電洞則在到達基板1之前,產生有在射極層11再結合之損失。如此,基板1與奈米柱2則必須呈未由射極層11加以隔開地,抑制射極層11之橫方向擴散。Next, the emitter layer 11 is formed. Along with this, in the range of the nano-pillar 2 in the process of FIG. 3(j), the portion joined to the emitter layer 11 (pn junction portion) is also formed and formed. The upper view of the structure after formation is shown in Fig. 3(g), and the cross-sectional view is shown in Fig. 3(h). The formation of the emitter layer 11 is performed by an impurity injection method such as a vapor phase diffusion method, a solid phase diffusion method, or an ion implantation method. Accordingly, the catalyst metal 32 serves as a catalyst for the growth of the nanocolumn 2, and also serves as a mask for the diffusion of impurities. Therefore, the relative positions of the nanopillar 2 and the emitter layer 11 are self-integratedly adjusted. However, when the emitter layer 11 is formed by the impurity implantation method, as described above, the catalyst metal 32 functions as a photomask, but the diffusion of the impurity injected into the substrate 1 is generally the same. Accordingly, in fact, the emitter layer 11 is formed partially on the lower portion of the catalytic metal 32, that is, the lower portion of the nanocolumn 2. When the lateral diffusion length of the emitter layer 11 is larger than the diameter of the nano-pillar 2, the structure in which the nano-pillar 2 and the substrate 1 are separated by the emitter layer 11 is formed. As described above, when the substrate 1 and the nano-pillar 2 are p-layers and the emitter layer 11 is an n + layer, the structure of the nano-pillar 2, the emitter layer 11, and the substrate 1 is a pn + p structure. The holes generated inside the nanopillar 2 are caused to be recombined in the emitter layer 11 before reaching the substrate 1. Thus, the substrate 1 and the nano-pillar 2 must be separated from each other by the emitter layer 11, and the lateral diffusion of the emitter layer 11 can be suppressed.

之後,將觸媒金屬32作為種,經由使奈米柱2之中突出於射極層11上部的部分(突出部)成長之時,形成奈米柱2。將成長後之構造的上面圖示於圖3 (i),將剖面圖示於圖3(j)。奈米柱2之成長係經由VLS(Vapor Liquid Solid)成長法等而進行。知道有作為觸媒金屬32而使用Cu,藉由在1000℃程度之高溫下進行VLS成長,實現缺陷密度少之奈米柱2者。然而,對於在射極層11之形成方法之中,使用離子注入法之情況,係經由在VLS成長之間加上於試料的熱,而可進行離子的活性化,但此時,如上述,必須注意盡可能不進行有射極層11之橫方向擴散。Thereafter, the catalyst metal 32 is used as a species, and the nanopillar 2 is formed by growing a portion (protrusion portion) of the nanopillar 2 that protrudes from the upper portion of the emitter layer 11. The above diagram of the structure after growth is shown in Figure 3. (i) The cross-sectional view is shown in Fig. 3(j). The growth of the nanocolumn 2 is carried out by a VLS (Vapor Liquid Solid) growth method or the like. It is known that Cu is used as the catalyst metal 32, and the nanocolumn having a small defect density is realized by performing VLS growth at a high temperature of about 1000 °C. However, in the case where the ion implantation method is used in the method of forming the emitter layer 11, the activation of ions can be performed by adding heat to the sample between the growth of the VLS, but at this time, as described above, Care must be taken not to carry out the lateral diffusion of the emitter layer 11 as much as possible.

接著,除去觸媒金屬32。將除去後之構造的上面圖示於圖3(k),剖面圖示於圖3(l)。觸媒金屬32之除去係經由根據溶液之濕蝕刻而進行。此時,對於基板1,奈米柱2,及射極層11而言之蝕刻速率慢,也就是使用蝕刻選擇比高的溶液為佳。Next, the catalyst metal 32 is removed. The upper view of the structure after removal is shown in Fig. 3(k), and the cross-sectional view is shown in Fig. 3(l). The removal of the catalyst metal 32 is carried out by wet etching according to the solution. At this time, the etching rate for the substrate 1, the column 2, and the emitter layer 11 is slow, that is, a solution having a high etching selectivity is preferably used.

之後,形成鈍化膜12。將形成後之構造的上面圖示於圖3(m),將剖面圖示於圖3(n)。鈍化膜12之形成係經由CVD法,濺鍍法,磊晶成長法,蒸鍍法等之成膜法而進行亦可,或者對於鈍化膜12之材料為奈米柱2及射極層11之材料的氧化物或氮化物之情況,係經由表面氧化或表面氮化而形成鈍化膜12亦可。Thereafter, the passivation film 12 is formed. The upper view of the structure after formation is shown in Fig. 3(m), and the cross-sectional view is shown in Fig. 3(n). The formation of the passivation film 12 may be performed by a film formation method such as a CVD method, a sputtering method, an epitaxial growth method, or a vapor deposition method, or the material of the passivation film 12 is a nano-pillar 2 and an emitter layer 11 In the case of an oxide or a nitride of a material, the passivation film 12 may be formed by surface oxidation or surface nitridation.

最後,形成表面電極13。將形成後之構造的上面圖示於圖3(o),將剖面圖示於圖3(p)。表面電極13之形成係經由印刷法,蒸鍍法,電鍍法,濺鍍法,CVD法等之成膜法而進行。表面電極13與射極層11則相互接合之故,而有必要除去存在於其間之鈍化膜12。 鈍化膜12之除去方法係可從經由光微影法與蝕刻之方法,使用蝕刻電糊之方法,將表面電極13印刷後進行燒成而電性導通的所謂燒成貫通之方法等之中選擇。在圖3(p)的剖面圖中,表面電極13之正下方的鈍化膜12係遍布於與表面電極13相同寬度加以除去,但由將所除去鈍化膜12的寬度作為較表面電極13的寬度為窄者,降低射極層11與表面電極13的接觸面積亦可。射極層11與表面電極13之接觸面積降低係知道有再結合抑制的效果,但另一方面,帶來接觸阻抗的增大之故,考慮再結合與接觸阻抗的2點,有必要將接觸面積作為最佳化。Finally, the surface electrode 13 is formed. The upper view of the structure after formation is shown in Fig. 3(o), and the cross-sectional view is shown in Fig. 3(p). The formation of the surface electrode 13 is performed by a film formation method such as a printing method, a vapor deposition method, a plating method, a sputtering method, or a CVD method. The surface electrode 13 and the emitter layer 11 are bonded to each other, and it is necessary to remove the passivation film 12 existing therebetween. The method of removing the passivation film 12 can be selected from a method of performing a method of photolithography and etching, using a method of etching an electric paste, and printing the surface electrode 13 and then firing it to electrically conduct it. . In the cross-sectional view of Fig. 3(p), the passivation film 12 directly under the surface electrode 13 is removed over the same width as the surface electrode 13, but the width of the removed passivation film 12 is taken as the width of the surface electrode 13. In the narrower case, the contact area of the emitter layer 11 and the surface electrode 13 may be reduced. The contact area between the emitter layer 11 and the surface electrode 13 is reduced, and the effect of recombination suppression is known. On the other hand, the contact resistance is increased, and it is necessary to consider the re-bonding and the contact resistance at two points. Area is optimized.

以上為實施例1之太陽能電池單元之第1製造方法。此製造方法係其特徵為具有將金屬圖案(觸媒金屬32)作為光罩,於第1導電型(p型)的基板1表面,形成與第1導電型不同之第2導電型(n型)之射極層的工程(圖3(g)(h)),和使用同一金屬圖案(觸媒金屬32),於基板1表面形成複數之奈米柱2的工程(圖3(i)(j))。The above is the first manufacturing method of the solar battery cell of Example 1. This manufacturing method is characterized in that a metal pattern (catalyst metal 32) is used as a mask, and a second conductivity type (n-type) different from the first conductivity type is formed on the surface of the first conductivity type (p-type) substrate 1. The project of the emitter layer (Fig. 3(g)(h)), and the process of forming a plurality of nanopillars 2 on the surface of the substrate 1 using the same metal pattern (catalytic metal 32) (Fig. 3(i) ( j)).

經由有關之特徵,第1製造方法係可將同一觸媒金屬32,作為形成射極層時之光罩,亦可作為使奈米柱成長時的種而使用,不但而可降低處理成本,還亦可將奈米柱2與射極層11之相對位置自我整合地調整。另外,與後述之第2製造方法作比較,在第1製造方法中,亦有在形成射極層11時可使用同向性注入法與異向性注入法之任一的優點。然而,於上述工程之外,適宜追加用 以改善各個膜之結晶性或膜質,或者用以提昇與鄰接膜之界面的質之熱處理,電漿處理等亦可。According to the related feature, the first catalyst method can use the same catalyst metal 32 as a mask for forming the emitter layer, or can be used as a species for growing the nano column, thereby reducing the processing cost and reducing the processing cost. The relative positions of the nanopillar 2 and the emitter layer 11 can also be self-aligned. Further, in comparison with the second manufacturing method described later, in the first manufacturing method, any of the isotropic injection method and the anisotropic injection method may be used in forming the emitter layer 11. However, in addition to the above works, it is suitable for additional use. It is also possible to improve the crystallinity or film quality of each film, or heat treatment for improving the quality of the interface with the adjacent film, plasma treatment, and the like.

<第2製造方法><Second Manufacturing Method>

圖4係顯示實施例1之奈米柱太陽能電池單元之第2製造方法的圖。如上述,在第1製造方法中,係經由成長法而形成奈米柱2,但在第2製造方法中,係經由加工法而形成奈米柱2。以下,依據圖4而說明實施例1之奈米柱太陽能電池單元之第2製造方法。然而,與第1製造方法同樣地,對於背面側之構造的形成工程係省略之。4 is a view showing a second method of manufacturing the nanocolumn solar cell of Example 1. As described above, in the first production method, the nanocolumn 2 is formed by a growth method, but in the second production method, the nanocolumn 2 is formed by a processing method. Hereinafter, a second method of manufacturing the nanocolumn solar cell of the first embodiment will be described with reference to FIG. However, similarly to the first manufacturing method, the forming process of the structure on the back side is omitted.

首先,於基板1的表面形成蝕刻光罩33。將形成後之構造的上面圖示於圖4(a),將剖面圖示於圖4(b)。蝕刻光罩33係成為接下來的工程之為了形成奈米柱2之蝕刻加工的光罩者,作為其材料係一般使用金屬奈米粒子或SiO2 、光阻劑等。使用金屬奈米粒子之情況係由使奈米粒子分散者,經由本身組織化而可形成蝕刻光罩33。另外,經由以舉離法或蝕刻之方法加工金屬,形成蝕刻光罩33亦可。對於使用SiO2 或光阻劑之情況,係經由使用光微影法之圖案化而可形成蝕刻光罩33。First, an etching mask 33 is formed on the surface of the substrate 1. The upper view of the structure after formation is shown in Fig. 4 (a), and the cross-sectional view is shown in Fig. 4 (b). The etching mask 33 is a photomask for forming an etching process of the nanocolumn 2 in the next process, and metal nanoparticle, SiO 2 , a photoresist, or the like is generally used as the material. In the case where metal nanoparticles are used, the etching mask 33 can be formed by dispersing the nanoparticles. Further, the etching of the metal may be performed by a lift-off method or an etching method to form the etching mask 33. For the case of using SiO 2 or a photoresist, the etching mask 33 can be formed by patterning using photolithography.

接著,藉由將基板1的表面進行加工,形成奈米柱2之中,之後突出於射極層11上部之部分(突出部)。將形成後之構造的上面圖示於圖4(c),將剖面圖示於圖4(d)。突出部的形成係經由乾蝕刻,濕蝕刻,雷射蒸鍍等之方法而進行。從反射防止效果之觀點係 奈米柱2之縱橫比,也就是「高度/直徑」的值為大者為佳,對於為此係使用加工之異向性高之乾蝕刻,形成突出部為佳。另外,對於為了提高縱橫比,係將蝕刻光罩33作為二層以上的層積構造亦為有效的方法。Next, the surface of the substrate 1 is processed to form a portion (protrusion portion) which protrudes into the upper portion of the emitter layer 11 and then protrudes from the upper portion of the emitter layer 11. The upper view of the structure after formation is shown in Fig. 4(c), and the cross-sectional view is shown in Fig. 4(d). The formation of the protruding portion is performed by a method such as dry etching, wet etching, or laser evaporation. From the viewpoint of reflection prevention effect It is preferable that the aspect ratio of the nano-pillar 2, that is, the value of "height/diameter" is large, and it is preferable to form a protruding portion by dry etching using high processing anisotropy. Further, in order to increase the aspect ratio, it is also effective to use the etching mask 33 as a laminated structure of two or more layers.

之後,形成射極層11。伴隨於此,成為奈米柱2之中接合於射極層11的部分(pn接合部)亦合併加以形成者。將形成後之構造的上面圖示於圖4(e),將剖面圖示於圖4(f)。射極層11之形成係與前述第1製造方法同樣地,經由不純物注入法而進行,但與第1製造方法不同係無法使用氣相擴散法等之同向性注入法,而必須使用離子注入法等之異向性注入法者。其理由係假設在本工程中,經由同向性注入法而進行不純物注入時,對於奈米柱2之側壁部亦形成有射極層11之故。Thereafter, the emitter layer 11 is formed. Along with this, the portion (pn junction portion) bonded to the emitter layer 11 among the nano-pillars 2 is also combined and formed. The upper view of the structure after formation is shown in Fig. 4(e), and the cross-sectional view is shown in Fig. 4(f). The formation of the emitter layer 11 is performed by the impurity injection method as in the first production method. However, unlike the first production method, the isotropic implantation method such as the vapor phase diffusion method cannot be used, and ion implantation must be used. The law of anisotropic injection of law. The reason for this is assumed to be that the emitter layer 11 is also formed on the side wall portion of the nano-pillar 2 when the impurity is injected by the isotropic injection method in the present process.

作為此等之後之工程係首先,由除去蝕刻光罩33者,可得到在第1製造方法1圖3(k)及(l)所示的構造之故,之後係由歷經與第1製造方法同樣的工程,而可實現實施例1之奈米柱太陽能電池單元構造。As the engineering system after the first, the structure shown in FIGS. 3(k) and (l) of the first manufacturing method 1 can be obtained by removing the etching mask 33, and thereafter, the history and the first manufacturing method are obtained. The same engineering can realize the nano column solar cell structure construction of Embodiment 1.

以上為實施例1之太陽能電池單元之第2製造方法。此製造方法係其特徵為具有經由將蝕刻光罩33作為光罩之蝕刻之時,於基板1的表面形成複數之奈米柱2的工程(圖4(a)(b)),和經由使用異向性注入法之時,注入不純物於基板1表面且複數之奈米柱2之間的範圍之工程(圖4(c)(d))者。The above is the second manufacturing method of the solar battery cell of the first embodiment. This manufacturing method is characterized in that it has a process of forming a plurality of nano-pillars 2 on the surface of the substrate 1 by etching the etching mask 33 as a mask (Fig. 4(a)(b)), and via use. At the time of the anisotropic implantation method, a process of impregnating the surface between the substrate 1 and the plurality of columns 2 (Fig. 4(c)(d)) is injected.

經由有關的工程,亦可製造有關實施例1之 太陽能電池單元者。並且,第2製造方法係使用加工法而形成奈米柱2之故,而對於作為基板1使用單結晶之情況,係經由加工法而加以形成之奈米柱2者則與如第1製造方法經由成長法而加以形成之奈米柱2做比較,在結晶性或純度的點為優越,隨之可降低再結合損失者。The related embodiment 1 can also be manufactured through the related works. Solar battery unit. Further, in the second manufacturing method, the nano column 2 is formed by a processing method, and when a single crystal is used as the substrate 1, the nano column 2 formed by the processing method is the same as the first manufacturing method. The nano column 2 formed by the growth method is superior in terms of crystallinity or purity, and the recombination loss can be reduced.

實施例2Example 2

圖5(a)及(b)係有關本發明之實施例2之太陽能電池單元的上面圖及剖面圖。與實施例1不同的是對於實施例1之構造為奈米柱太陽能電池單元而言,實施例2之構造為奈米溝槽太陽能電池單元,於基板1表面具有延伸於平行之特定方向之複數的凸部3之單元的點。與實施例1情況同樣地,將從實施例2之奈米柱太陽能電池單元構造,僅除去鈍化層12之構造的上面圖及剖面圖,各示於圖6(a)及(b)。對於圖5及圖6係顯示有在垂直於凸部3之延伸方向及基板表面的面之剖面形狀為四角形情況之構造,但如上述,凸部3係三角形或扇形等不同之剖面形狀亦可。5(a) and 5(b) are a top view and a cross-sectional view of a solar battery cell according to a second embodiment of the present invention. The difference from Embodiment 1 is that the structure of Embodiment 1 is a nano-column solar cell, and the structure of Embodiment 2 is a nano-trench solar cell having a plurality of surfaces extending in a specific direction parallel to the surface of the substrate 1. The point of the unit of the convex portion 3. In the same manner as in the first embodiment, the top view and the cross-sectional view of the structure in which only the passivation layer 12 is removed from the nano-pillar solar cell structure of the second embodiment are shown in Figs. 6(a) and (b). 5 and 6 show a structure in which the cross-sectional shape perpendicular to the extending direction of the convex portion 3 and the surface of the substrate is a square shape. However, as described above, the convex portion 3 may have a different cross-sectional shape such as a triangle or a sector. .

如此,有關實施例2的太陽能電池單元係其特徵為具有第1導電型(p型)的基板1,和設置於基板1的表面,為第1導電型,且延伸於特定方向之複數的凸部3,和設置於基板1的表面,與第1導電型不同之第2導電型(n型)之射極層11,射極層11係設置於複數之凸部3之間者。As described above, the solar battery cell of the second embodiment is characterized in that the substrate 1 having the first conductivity type (p type) and the surface of the substrate 1 are of the first conductivity type and have a plurality of convexities extending in a specific direction. The portion 3 is provided on the surface of the substrate 1, and the second conductivity type (n-type) emitter layer 11 different from the first conductivity type, and the emitter layer 11 is provided between the plurality of convex portions 3.

經由有關之特徵,與實施例1之情況同樣地,可降低在凸部3內部之再結合損失者。另外,如圖6(a)之上面圖所示,射極層11則在複數之凸部3的外周作為連續。此係使射極層11相互作為未孤立,而遍佈於基板1上的全面作為連續之故,經由此,與實施例1同樣地,作為表面電極13而可使用圖案電極者。According to the related features, as in the case of the first embodiment, the loss of recombination inside the convex portion 3 can be reduced. Further, as shown in the upper diagram of Fig. 6(a), the emitter layer 11 is continuous on the outer circumference of the plurality of convex portions 3. In this way, the emitter layers 11 are not isolated, and the entire surface of the substrate 1 is continuous. Thus, as in the first embodiment, the pattern electrodes can be used as the surface electrodes 13.

如以上,如根據實施例2,與實施例1之奈米柱太陽能電池單元之情況同樣,在奈米溝槽太陽能電池單元,亦降低在凸部3內部之再結合損失,且作為表面電極13,而可使用圖案電極者。As described above, as in the case of the second embodiment, as in the case of the nano-column solar cell of the first embodiment, the re-bonding loss inside the convex portion 3 is also reduced in the nano-groove solar cell, and as the surface electrode 13 , and the pattern electrode can be used.

實施例2之構造的製造方法係與實施例1之情況同樣,但作為凸部3之形成方法係一般使用加工法。隨之,經由與實施例1之奈米柱太陽能電池單元之第2製造方法同樣的方法,而製作實施例2之奈米溝槽太陽能電池單元構造者為一般。上述之於基板1面內之一部分,設置未形成有凸部3之範圍的點,係可由設計在實施例1之第2製造方法的蝕刻光罩33的圖案者而實現。The manufacturing method of the structure of the second embodiment is the same as that of the first embodiment. However, as a method of forming the convex portion 3, a processing method is generally used. Subsequently, the structure of the nano-groove solar cell of Example 2 was produced by the same method as the second manufacturing method of the nano-column solar cell of Example 1. The point where the convex portion 3 is not formed in a portion of the surface of the substrate 1 described above can be realized by the pattern of the etching mask 33 designed in the second manufacturing method of the first embodiment.

實施例3Example 3

圖7(a)及(b)係有關本發明之實施例2之太陽能電池單元的上面圖及剖面圖。與實施例1不同係實施例3之構造為奈米孔太陽能電池單元的點,及在實施例3之奈米孔太陽能電池單元中,於次波長構造的內部,也就是奈米孔4的側壁範圍之頂部,形成有射極層11的點 之2個。與實施例1情況同樣地,將從實施例3之奈米柱太陽能電池單元構造,僅除去鈍化層12之構造的上面圖及剖面圖,各示於圖8(a)及(b)。對於圖7及圖8係顯示有奈米孔4為圓柱狀之凹部情況的構造,但如上述,奈米孔4係亦可為角柱等,具有不同剖面形狀之柱狀構造。實施例3之奈米孔太陽能電池單元構造係在上述planar淺接合型奈米柱太陽能電池單元中,可看做取代奈米柱而使用奈米孔情況之構造者。但對於實施例3之奈米孔太陽能電池單元與planar淺接合型奈米柱太陽能電池單元之間係有以下的不同。即在planar淺接合型奈米柱太陽能電池單元中,如上述,形成於奈米柱2頂部之射極層11則相互作為孤立之故,而作為表面電極13,並非圖案電極而有必要使用形成於全面之電極。對此,在實施例3之奈米孔太陽能電池單元中,形成於基板1表面之中未設置有奈米孔4之部分的淺射極層11係如圖8(a)之上面圖所示,遍佈於基板1上全面作為連續,隨之,作為表面電極13,可使用圖案電極者。7(a) and 7(b) are a top view and a cross-sectional view of a solar battery cell according to a second embodiment of the present invention. Different from Example 1, the structure of Example 3 is a nanopore solar cell, and in the nanopore solar cell of Example 3, inside the sub-wavelength structure, that is, the sidewall of the nanopore 4. At the top of the range, the point where the emitter layer 11 is formed 2 of them. In the same manner as in the first embodiment, the top view and the cross-sectional view of the structure in which only the passivation layer 12 is removed from the nanocolumn solar cell structure of the third embodiment are shown in Figs. 8(a) and (b). 7 and 8 show a structure in which the nanopore 4 is a cylindrical recess. However, as described above, the nanopore 4 may be a columnar structure having a different cross-sectional shape. The nanopore solar cell structure of the third embodiment can be regarded as a structure in which a nanopore is used in place of a nanocolumn in the above planar shallow junction type nano column solar cell. However, the following differences were made between the nanopore solar cell unit of Example 3 and the planar shallow junction type nano column solar cell. That is, in the planar shallow junction type nano column solar cell, as described above, the emitter layer 11 formed on the top of the column 2 is isolated from each other, and as the surface electrode 13, it is not necessary to form a pattern electrode. In the comprehensive electrode. On the other hand, in the nanopore solar battery cell of the third embodiment, the shallow electrode layer 11 formed on the surface of the substrate 1 in which the nanopore 4 is not provided is as shown in the upper view of Fig. 8(a). The entire substrate 1 is entirely continuous, and as the surface electrode 13, a pattern electrode can be used.

如此,有關實施例3之太陽能電池單元,其特徵為具有:於其表面具有複數的柱狀凹部(奈米孔4)且為第1導電型(p型)之基板1,和設置於基板1的表面且未設置有柱狀凹部之部分,與第1導電型不同之第2導電型(n型)的射極層11,前述柱狀凹部的寬度為1μm以下者。As described above, the solar battery cell of the third embodiment has a substrate 1 having a plurality of columnar recesses (nano holes 4) on its surface and being of a first conductivity type (p type), and a substrate 1 disposed on the substrate 1 The surface of the second conductivity type (n-type) of the emitter layer 11 which is different from the first conductivity type is not included in the columnar recess, and the width of the columnar recess is 1 μm or less.

如根據有關的特徵,由將射極層11較奈米孔 4的高度作為薄膜化者,可將在奈米孔之太陽能電池之再結合損失,降低為與planar淺接合型奈米柱太陽能電池單元相同程度,且與planar淺接合型奈米柱太陽能電池單元不同,作為表面電極13而可使用圖案電極者。具體而言,射極層11之膜厚,例如可作為500nm以下者。According to the relevant features, by the emitter layer 11 than the nanopore The height of 4 is used as a thin film, and the recombination loss of the solar cell in the nano hole can be reduced to the same extent as the planar shallow junction type nano column solar cell unit, and the planar shallow junction type nano column solar cell unit Unlike the surface electrode 13, a pattern electrode can be used. Specifically, the film thickness of the emitter layer 11 can be, for example, 500 nm or less.

作為實施例3之構造的製造方法係首先,遍佈於基板1上之全面形成射極層11,之後,形成奈米孔4,接著形成鈍化膜12與表面電極13即可。射極層11係亦可由不純物注入法,成膜法之任一方法形成。奈米孔4之形成係一般為經由蝕刻,或使用雷射之加工法而進行。鈍化膜12之形成係與實施例1的情況同樣,可經由表面氧化或表面氮化而進行,以及經由成膜法而進行亦可。對於經由成膜法而形成鈍化膜12之情況,從上面而視奈米孔4時,奈米孔4之側壁範圍呈未成為陰影地,即奈米孔4頂部的開口面積則作為與底部的開口面積相同程度,或較大形狀者為佳。As a manufacturing method of the structure of the third embodiment, first, the emitter layer 11 is formed over the entire substrate 1, and then the nanopore 4 is formed, and then the passivation film 12 and the surface electrode 13 are formed. The emitter layer 11 can also be formed by any method of impurity injection or film formation. The formation of the nanopore 4 is generally carried out by etching or by laser processing. The formation of the passivation film 12 can be carried out by surface oxidation or surface nitridation as in the case of Example 1, and may be carried out by a film formation method. In the case where the passivation film 12 is formed by the film formation method, when the nanopore 4 is viewed from above, the side wall of the nanopore 4 is not shaded, that is, the opening area at the top of the nanopore 4 is used as the bottom portion. It is preferred that the opening area is the same or a larger shape.

然而,於專利文獻1,揭示有作為表面反射防止構造而具有孔陣列構造,且於孔側壁部形成有淺的射極層之太陽能電池單元構造。此構造係與實施例3的構造類似,但於兩者之間係存在有如以下之不同。首先,對於在專利文獻1之構造的孔之直徑為1μm以上而言,在本發明成為對象之奈米孔的寬度係1μm以下。將奈米孔的寬度作為1μm以下的根據係奈米孔定義為具有與太陽光的波長同等,或更細微之尺寸的直徑之構成,且太陽光之 中,波長1μm以下的光則強度特別大,在太陽能電池單元中,通常加以利用之波長域的2點。另外,專利文獻1之構造係具有比較於孔的開口部而底部面積為寬的特徵。假設在奈米孔太陽能電池中,與實施例3之柱狀凹部不同,使用將底部的面積作為較奈米孔的開口部寬之形狀時,與使用如在實施例3所述之開口部與底部的面積為同等之奈米孔的場合相比則有經由鄰接之奈米孔底部間的範圍變窄而串聯阻抗增大之情況;經由奈米孔的表面積增大而表面再結合損失增大之情況;及從上面而視奈米孔時存在有成為陰影之範圍之故,而作為奈米孔之表面鈍化層,使用CVD法等之成膜法者則變為困難之情況,而上述3點則成為課題。隨之,專利文獻1之構造係將開口部的直徑作為1μm以下者則為困難。However, Patent Document 1 discloses a solar battery cell structure having a hole array structure as a surface reflection preventing structure and a shallow emitter layer formed on the side wall portion of the hole. This configuration is similar to the configuration of Embodiment 3, but there are differences between the two as follows. First, the diameter of the pores in the structure of Patent Document 1 is 1 μm or more, and the width of the nanopore to be used in the present invention is 1 μm or less. The width of the nanopore is defined as a diameter of 1 μm or less, which is defined as having the same diameter as the wavelength of sunlight or a finer diameter, and the sunlight is Among them, light having a wavelength of 1 μm or less is particularly strong, and in a solar battery cell, two points in a wavelength range generally used. Further, the structure of Patent Document 1 has a feature that the bottom portion is wider than the opening of the hole. It is assumed that in the nanopore solar cell, unlike the columnar recess of the third embodiment, when the area of the bottom portion is used as the shape of the opening portion of the nanopore, the opening portion as described in the third embodiment is used. When the area of the bottom is the same as the nanopore, the range between the bottom of the adjacent nanopore is narrowed and the series impedance is increased; the surface area of the nanopore increases and the surface recombination loss increases. In the case of the nanopore, there is a range of shadows, and as a surface passivation layer of a nanopore, it is difficult to use a film formation method such as a CVD method, and the above 3 The point becomes a topic. Accordingly, in the structure of Patent Document 1, it is difficult to make the diameter of the opening portion 1 μm or less.

當匯整以上情況時,專利文獻1之構造係所使用之孔陣列則從此尺寸,並非次波長構造。另外,假設在專利文獻1之構造中,將孔的開口部之尺寸縮小至與次波長構造同等之1μm以下程度時,串聯阻抗之增大,再結合損失之增大,及經由成膜法之鈍化膜則為困難之情況之此3點則成為課題之故,專利文獻1之構造係將開口部的口徑作為1μm以下者則為困難者。When the above is the case, the hole array used in the structure of Patent Document 1 is of such a size, not a sub-wavelength structure. Further, in the structure of Patent Document 1, when the size of the opening of the hole is reduced to about 1 μm or less which is equivalent to the sub-wavelength structure, the series resistance is increased, the recombination loss is increased, and the film formation method is used. When the passivation film is difficult, the three points are a problem. The structure of Patent Document 1 is difficult if the diameter of the opening is 1 μm or less.

以上,記載於專利文獻1之發明係與有關實施例3之發明,構成與效果均為不同。The invention described in Patent Document 1 and the invention according to the third embodiment are different in configuration and effect.

以上,將經由本發明者所成之發明,依據實施形態已具體做過說明,但本發明並不限定於前述實施 例,在不脫離其內容之範圍可做各種變更。The invention made by the inventors of the present invention has been specifically described based on the embodiments, but the present invention is not limited to the foregoing implementation. For example, various changes can be made without departing from the scope of the content.

12‧‧‧鈍化膜12‧‧‧ Passivation film

13‧‧‧表面電極13‧‧‧ surface electrode

Claims (9)

一種太陽能電池單元,其特徵為具有:具備延伸於特定方向之複數的柱體,且為第1導電型之基板,和與前述基板接合而加以設置,與前述第1導電型不同之第2導電型之射極層,前述複數之柱體係由前述第1導電型之半導體所成,前述複數之柱體係在其側面中與前述射極層接合者,前述射極層係對於前述複數之柱體內部係未加以設置者,更具有與前述射極層加以電性連接之電極,前述電極係由Ag、Al、Ti、Pd、Ni、Cu、或此等之層積構造所成者,前述射極層的膜厚係500nm以上者。 A solar battery cell comprising: a plurality of pillars extending in a specific direction; and a substrate of a first conductivity type; and a second conductive layer different from the first conductivity type and bonded to the substrate In the emitter layer of the type, the plurality of pillar systems are formed of the first conductivity type semiconductor, and the plurality of pillar systems are joined to the emitter layer on the side surface thereof, and the emitter layer is in the plurality of pillars If the portion is not provided, the electrode is electrically connected to the emitter layer, and the electrode is made of Ag, Al, Ti, Pd, Ni, Cu, or the like. The film thickness of the electrode layer is 500 nm or more. 如申請專利範圍第1項記載之太陽能電池單元,其中,更具有與前述複數之柱體及前述射極層接合而加以設置之鈍化膜者。 The solar battery unit according to claim 1, further comprising a passivation film which is provided in combination with the plurality of pillars and the emitter layer. 如申請專利範圍第1項記載之太陽能電池單元,其中,在前述射極層之不純物濃度係較在前述複數之柱體的不純物濃度為高者。 The solar battery unit according to claim 1, wherein the concentration of the impurity in the emitter layer is higher than the concentration of the impurity in the plurality of columns. 如申請專利範圍第1項記載之太陽能電池單元,其中,前述複數之柱體的寬度為1μm以下者。 The solar battery unit according to claim 1, wherein the plurality of columns have a width of 1 μm or less. 一種太陽能電池單元,其特徵為具有:於其表面具有複數之柱狀凹部,且為第1導電型之基板,和設置於前述基板表面,且未設置有前述柱狀凹部之部分,與前述第1導電型不同之第2導電型之射極層,前述柱狀凹部的寬度為1μm以下者,更具有與前述射極層加以電性連接之電極,前述電極係由Ag、Al、Ti、Pd、Ni、Cu、或此等之層積構造所成者,前述射極層的膜厚係500nm以下者。 A solar battery cell characterized by having a plurality of columnar recesses on a surface thereof, a first conductivity type substrate, and a portion provided on the surface of the substrate and not provided with the columnar recesses, and the foregoing The second conductivity type emitter layer having different conductivity types, wherein the columnar recess has a width of 1 μm or less, and further includes an electrode electrically connected to the emitter layer, wherein the electrode is made of Ag, Al, Ti, or Pd. In the case of a laminated structure of Ni, Cu, or the like, the film thickness of the emitter layer is 500 nm or less. 如申請專利範圍第5項記載之太陽能電池單元,其中,在前述射極層之不純物濃度係較在前述複數之柱體的不純物濃度為高者。 The solar battery unit according to claim 5, wherein the concentration of the impurity in the emitter layer is higher than the concentration of the impurity in the plurality of columns. 如申請專利範圍第5項記載之太陽能電池單元,其中,前述射極層之膜厚則較前述柱狀凹部的高度為小者。 The solar battery unit according to claim 5, wherein a thickness of the emitter layer is smaller than a height of the columnar recess. 一種太陽能電池單元之製造方法,其特徵為具有將金屬圖案作為光罩,於第1導電型之基板表面,形成與前述第1導電型不同之第2導電型之射極層的第1工程,和使用前述金屬圖案,於前述基板表面形成前述第1導電型之複數之柱體的第2工程者,前述射極層係對於前述複數之柱體內部係未加以設置者,更具有與前述射極層加以電性連接之電極, 前述電極係由Ag、Al、Ti、Pd、Ni、Cu、或此等之層積構造所成者。 A method for producing a solar battery cell, comprising: a first project of forming a second conductivity type emitter layer different from the first conductivity type on a surface of a first conductivity type substrate by using a metal pattern as a mask; And a second engineer who forms the plurality of pillars of the first conductivity type on the surface of the substrate by using the metal pattern, wherein the emitter layer is not provided for the plurality of pillars; Electrodes that are electrically connected to the pole layer, The electrode is made of Ag, Al, Ti, Pd, Ni, Cu, or the like. 如申請專利範圍第8項記載之太陽能電池單元之製造方法,其中,前述第2工程係將前述金屬圖案作為種而使前述複數之柱體成長之工程者。 The method of manufacturing a solar battery cell according to the eighth aspect of the invention, wherein the second engineering system is to grow the plurality of pillars by using the metal pattern as a seed.
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