TW201005977A - Method and apparatus for manufacturing solar battery - Google Patents

Method and apparatus for manufacturing solar battery Download PDF

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Publication number
TW201005977A
TW201005977A TW098110464A TW98110464A TW201005977A TW 201005977 A TW201005977 A TW 201005977A TW 098110464 A TW098110464 A TW 098110464A TW 98110464 A TW98110464 A TW 98110464A TW 201005977 A TW201005977 A TW 201005977A
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Taiwan
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structural defect
defect
solar cell
resistance value
structural
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TW098110464A
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Chinese (zh)
Inventor
Kazuhiro Yamamuro
Seiichi Sato
Mitsuru Yahagi
Junpei Yuyama
Kyuzo Nakamura
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Ulvac Inc
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    • 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
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E10/00Energy generation through renewable energy sources
    • Y02E10/50Photovoltaic [PV] energy
    • 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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Abstract

A method for manufacturing a solar battery, includes: forming a photoelectric converter which includes a plurality of compartment elements, and in which the compartment elements adjacent to each other are electrically connected; specifying the compartment element having a structural defect in the photoelectric converter; restricting a portion in which the structural defect exists in the compartment element so as to focus an area in which the structural defect exists in the compartment element based on a resistance value distribution that is obtained by measuring resistance values of portions between the compartment elements adjacent to each other, capture the focused area in which the structural defect exists using an image capturing section, and accurately specify a position of the structural defect from an obtained image; and removing the structural defect so as to irradiate a portion in which the structural defect exists with a laser beam.

Description

201005977 六、發明說明: 【發明所屬之技術領域】 本發明係關於太陽電池之製造方法及太陽電池之製造裝 置,更詳細而言係關於一種能以低成本檢測構造缺陷並修 復之太陽電池之製造方法及太陽電池之製造裝置。 【先前技術】 從能量有效率利用的觀點來看,近年來,太陽電池日益 廣泛地受到一般利用。特別是利用矽單結晶之太陽電池的 每單位面積之能量轉換率良好。然而,另一方面,利用矽 單結晶之太陽電池係由於使用將矽單結晶鑄錠切片之矽晶 圓’因此於鑄錠之製造上耗費大量能量,製造成本高。特 別於實現設置於屋外等之大面積的太陽電池之情況時,若 利用矽單結晶來製造太陽電池,則現狀下相當花費成本。 因此’利用可更低價地製造之非晶(非晶質)矽薄膜之太陽 電池’係作為低成本的太陽電池而普及。 非晶石夕太陽電池係使用稱為pin接合之層構造的半導體 膜,該pin接合係由p型及!!型之矽膜,夾住當受光則發生 電子及電洞之非晶矽膜(i型)。於該半導體膜之兩面分別形 成有電極。由於太陽光而發生之電子及電洞係由於P型·n 型半導體之電位差而活潑地移動,由於連續地重複此而於 兩面的電極產生電位差。 作為此類非晶矽太陽電池之具體構成係採用例如於玻璃 板將 TCO(Transparent Conductive Oxide :透明導電氧 物)等之透明電極作為下部電極而成膜,於其上形成有 139429.doc 201005977 包含非μ石夕之半導體膜、及作為上部電極之Ag薄膜等之構 成。 於包含如此含有上下電極及半導體膜之光電轉換體之非 晶矽太陽電池,若僅於基板上,以寬廣面積均勻地將各層 予以成膜,則會有電位差小、電阻值變大的問題。因此, 例如形成以特定尺寸逐一電性劃分光電轉換體而形成劃分201005977 VI. TECHNOLOGICAL FIELD OF THE INVENTION The present invention relates to a method for manufacturing a solar cell and a device for manufacturing a solar cell, and more particularly to a method for manufacturing a solar cell capable of detecting structural defects and repairing at low cost. Method and manufacturing device for solar cells. [Prior Art] From the viewpoint of efficient energy utilization, solar cells have been increasingly widely used in recent years. In particular, the energy conversion rate per unit area of a solar cell using single crystals is good. On the other hand, however, the solar cell utilizing 矽 single crystals consumes a large amount of energy in the manufacture of the ingot due to the use of a twinned circle in which a single crystal ingot is sliced, and the manufacturing cost is high. In particular, when a solar cell is installed in a large area such as a house, it is costly to manufacture a solar cell using a single crystal. Therefore, a solar cell using an amorphous (amorphous) tantalum film which can be produced at a lower cost has been widely used as a low-cost solar cell. The amorphous quartz solar cell uses a semiconductor film called a pin-bonded layer structure, which is a p-type and a p-type film, which sandwiches an amorphous film which generates electrons and holes when light is received ( Type i). Electrodes are formed on both sides of the semiconductor film. The electrons and holes generated by the sunlight are actively moved by the potential difference of the P-type and n-type semiconductors, and the potential difference is generated between the electrodes on both sides by continuously repeating this. As a specific configuration of such an amorphous germanium solar cell, for example, a transparent electrode such as TCO (Transparent Conductive Oxide) is used as a lower electrode in a glass plate to form a film, and 139429.doc 201005977 is formed thereon. A semiconductor film of non-μ Shi Xi, and an Ag film as an upper electrode. In a non-crystalline solar cell including a photoelectric conversion body including the upper and lower electrodes and the semiconductor film, if the layers are formed uniformly over a wide area on the substrate, there is a problem that the potential difference is small and the resistance value is increased. Therefore, for example, forming a division by electrically dividing the photoelectric conversion body one by one with a specific size

元件’電性連接相i鄰接之劃分元件彼此,#&構成非晶 矽太陽電池。 具體而言’採用一種於基板上以寬廣面積均勻地形成之 光電轉換體’使用雷射光等’形成稱為切割線㈣如㈣ 之溝槽而獲得許多長條狀之劃分元件,並將該劃分元件彼 此電性串聯連接之構造。 然而’於此類構造之非晶碎太陽電池,據知在製造階段 會產生數種構造缺陷。例如於非晶⑦膜之歧時混入粒子 或產生針孔’從而於上部電極與下部電極可能局部地短 路。而且,於基板上形成光電轉換體後,藉由切割線分割 為許多劃分元件時,沿著該㈣線,構成上部電極之金属 膜熔融而到達下部電極,上部電極與下部電極亦可能局部 地短路。 如此’於錢轉換體,若產生夾著半導體媒而於上部電 極與下部電極之間局部地短路之構造缺陷,會引起發電電 1之降低或光電轉換效率降低該類故障。因此,於以往的 :晶石夕太陽電池之製造步驟中’藉由檢測此類短路等構造 缺陷’去除產生構造缺陷處而修復故障。 139429.doc 201005977The element 'electrically connected phase i adjacent to the dividing elements are mutually, #& constitutes an amorphous germanium solar cell. Specifically, 'a photoelectric conversion body formed uniformly on a wide area on a substrate is formed using laser light or the like to form a groove called a cutting line (4) such as (4), and a plurality of strip-shaped dividing elements are obtained, and the division is performed. The configuration in which the elements are electrically connected in series to each other. However, in such a structured amorphous solar cell, it is known that several structural defects occur during the manufacturing stage. For example, in the case of the amorphous 7 film, particles are mixed or pinholes are generated so that the upper electrode and the lower electrode may be partially short-circuited. Further, after the photoelectric conversion body is formed on the substrate and divided into a plurality of division elements by the dicing line, the metal film constituting the upper electrode is melted along the (4) line to reach the lower electrode, and the upper electrode and the lower electrode may be partially short-circuited. . In the case of the money conversion body, if a structural defect is locally short-circuited between the upper electrode and the lower electrode with the semiconductor medium interposed therebetween, the power generation electric power 1 is lowered or the photoelectric conversion efficiency is lowered. Therefore, in the conventional manufacturing process of the spar solar cell, the structural defect is removed by detecting a structural defect such as such a short circuit, and the failure is repaired. 139429.doc 201005977

構造缺陷之劃分元件的方法。 而如上述於劃分元件全體施加偏壓電壓而檢測缺陷 的方法, 雖可特定出劃分元件内大概的缺陷位置 ,但難以 特疋出詳細位置,而且亦需要紅外線感測器之掃描等,會 有檢測精度或檢測用之裝置成本大的問題。 而且,由於施加偏壓電壓至缺陷處發熱的程度,因此亦 有對半導體膜造成損傷之虞。 以CCD相機等放大觀察而檢測缺陷之方法,係必須使相 機遍及太陽電池之全區進行掃描,特別於太陽電池為大面 積之情況下,會有構造缺陷的檢測花費人力及時間的問 題。而且,亦有未檢測到未出現於表層的缺陷之虞。 照射光而測定各劃分元件之FF的方法雖可檢測存在有缺 陷之劃分元件本身,但難以特定出劃分元件内之何處存在 有缺陷。 然後’於該專上述之缺陷檢測方法中,由於僅可特定出 大概的缺陷位置,因此以雷射光等修復缺陷處時係大範圍 地去除半導體膜,會有不僅作為太陽電池的特性不適宜, 139429.doc 201005977 外觀上亦不適宜的問題。 而且’僅特定出大概的缺陷位置而施加偏壓電壓以去除 缺陷之情況下,必須升高偏壓電壓。然而,若施加高過必 要以上之偏壓電壓,會有對未產生缺陷之正常部分造成損 傷的問題。 【發明内容】 本發明係有鑑於上述事情而完成,其目的在於提供一種A method of constructing a component that divides a defect. On the other hand, as described above, a method of detecting a defect by applying a bias voltage to the entire division element can specify the approximate defect position in the division element, but it is difficult to specifically display the detailed position, and it is also necessary to scan the infrared sensor. The problem of detection accuracy or cost of the device for detection is large. Further, since the bias voltage is applied to the extent of heat generation at the defect, there is also a fear of damage to the semiconductor film. The method of detecting defects by magnifying observation by a CCD camera or the like is necessary to scan the camera over the entire area of the solar cell. Especially in the case where the solar cell has a large area, the detection of structural defects requires labor and time. Moreover, there are also defects in which no defects appearing on the surface layer are detected. The method of measuring the FF of each divided element by irradiating light can detect the defective component itself, but it is difficult to specify where the defective element is defective. Then, in the defect detection method described above, since only the approximate defect position can be specified, when the defect is repaired by laser light or the like, the semiconductor film is largely removed, and the characteristics of the solar cell are not suitable. 139429.doc 201005977 An unsuitable problem in appearance. Further, in the case where a bias voltage is applied only to specify a defect position to remove a defect, the bias voltage must be raised. However, if a bias voltage higher than necessary is applied, there is a problem that damage is caused to a normal portion where no defect occurs. SUMMARY OF THE INVENTION The present invention has been made in view of the above, and an object thereof is to provide a

不對太陽電池之光電轉換體造成大損傷,能以短時間正確 地特定出構造缺陷之發生處,確實地去除、修復所特定出 的構造缺陷之太陽電池之製造方法及太陽電池之製造裝 置。 ' 為了解決上述問題,本發明提供如下之太陽電池之製造 方法。亦即,本發明之第丨態樣之太陽電池之製造方法係 形成光電轉換體,該光電轉換體包含複數個劃分元件,且 相互鄰接之前述劃分元件彼此電性連接;特定出前述光電 轉換體中含有構造缺陷之前述劃分元件(缺陷劃分特定步 驟根據則目互鄰接之前㈣分元件彼此之間測定複數 處之電阻值所獲得之電阻值分布’縮限前述劃分元件内存 在前述構造缺陷之區域,藉由圖像攝像部拍攝該經縮限之 存在前述構造缺陷之前述區域内,從所獲得之圖像正確地 特定出前述構造缺陷之位置,藉此於前述劃分元件内限定 存在前述構造缺陷之部位(缺陷部位特定步驟);於存在前 述構造缺陷之部位,昭射雪蘇本砼 (修復步驟)。’、,、㈣射光“切料構造缺陷 139429.doc 201005977 於本發明之第】態樣之太陽電池之製造方法,限定存在 别述構以缺陷之部位時(缺陷部位特定步驟),宜至少2階段 以上地改變電阻值之測定密度而進行測定。而且,電阻值 之測足且使用4探針式之電阻測定裝置。 而且’本發明提供如下之太陽電池之製造裝置。 亦即,本發明之第2態樣之太陽電池之製造裝置係該太 陽電池具有包含複數個劃分元件之光電轉換體;且包含: 電P測疋》卩,其係為了於前述光電轉換體中含有構造缺陷 之劃刀元件内,—限存在構造缺陷之區域,而於相互鄰接 之劃分元件彼此間測定複數處之電阻值;圖像攝像部,其 係拍攝前述經縮限之存在有構造缺陷之區域内,正確地特 定出構造缺陷之位置;及修復部,其係向前述構造缺陷照 射雷射光線而去除前述構造缺陷。 若依據本發明之第1態樣之太陽電池之製造方法,最初 於缺陷劃分特定步驟中,篩選包含具有構造缺陷之劃分元 件之太陽電池。然後,僅將經_選之具有缺陷之太陽電池 送至缺陷部位特定步驟。於缺陷部位特定步驟,正確地特 定出缺陷之存在部位。藉此,可有效率地製造無構造缺陷 之太陽電池。 而且,於缺陷部位特定步驟,測定鄰接之劃分元件彼此 間之電阻值之分布’於劃分元件之長度方向料出存在構 造缺陷之區域。其後,進-步以圖像攝像部拍攝該經縮限 之區域,能以針點正確地特定出劃分元件内存在有構造缺 陷之位置。 139429.doc 201005977 产兄時舍-缺陷特疋方法申’在拍攝大面積之被檢查物之 =::極多時間。相對於此,於本發明中,作為缺 夕 去,將藉由被檢查物為大面積之情況下花費極 :間之攝像所進行之方法,僅限定於藉由以短時間可測 值之刀布所預先縮限之小面積區域的攝像。因 此’此以極短時間迅速地正確特定出構造缺陷之位置。藉 此’於修復步驟,可僅去除包含缺陷之最小限度的區域,The manufacturing method of the solar cell and the manufacturing apparatus of the solar cell, which are capable of accurately identifying the occurrence of structural defects in a short period of time, and reliably removing and repairing the specific structural defects, can be performed. In order to solve the above problems, the present invention provides a method of manufacturing a solar cell as follows. That is, the manufacturing method of the solar cell according to the first aspect of the present invention forms a photoelectric conversion body including a plurality of dividing elements, and the dividing elements adjacent to each other are electrically connected to each other; the photoelectric conversion body is specified The above-mentioned dividing element including the structural defect (the defect-dividing step is based on the resistance value obtained by measuring the resistance value of the plurality of elements before the mutual adjacent to each other) And capturing, by the image capturing unit, the narrowed-down region in which the structural defect exists, and correctly identifying the position of the structural defect from the obtained image, thereby defining the structural defect in the dividing element The part (defective part specific step); in the part where the above-mentioned structural defect exists, Zhaoshe Xuesuben (remediation step). ',, (4) the light "cutting structure defect 139429.doc 201005977 in the invention" The manufacturing method of the solar cell, when there is a part where the defect is specified (the defect site is specified) The measurement of the resistance value is preferably carried out at least two stages or more, and the resistance value is measured and a four-probe type resistance measuring device is used. Further, the present invention provides the following solar cell manufacturing apparatus. That is, the solar cell manufacturing apparatus according to the second aspect of the present invention is characterized in that the solar cell has a photoelectric conversion body including a plurality of division elements; and includes: an electric P test, which is used in the photoelectric conversion body In the dicing element including the structural defect, there is a region where the structural defect exists, and the resistance values at the complex portion are measured between the mutually adjacent dividing members; the image capturing portion is configured to detect the existence of the above-mentioned contracted limit and has a structural defect In the region, the position of the structural defect is correctly specified; and the repairing portion is configured to irradiate the structural defect with the laser beam to remove the structural defect. According to the method of manufacturing the solar cell according to the first aspect of the present invention, initially In a specific step of defect division, a solar cell including a dividing element having a structural defect is screened. Then, only the selected one is defective. The solar cell is sent to the defect site for a specific step. In the specific step of the defect portion, the location where the defect exists is correctly specified. Thereby, the solar cell without structural defects can be efficiently manufactured. Moreover, in the specific step of the defect portion, the adjacent portion is determined. The distribution of the resistance values between the divided elements is a region where the structural defects are present in the longitudinal direction of the dividing element. Thereafter, the narrowed region is imaged by the image capturing portion, and can be accurately specified with the stitch point. There is a structural defect in the dividing element. 139429.doc 201005977 The method of producing a brother-defective method is to take a large area of the object to be inspected =:: a lot of time. In contrast, in the present invention As a eve of the eve, the method of performing the camera in the case of a large area is limited to a small area that is pre-shrinked by a knife with a short time measurable value. The camera of the area. Therefore, this quickly and accurately identifies the location of the structural defect in a very short time. By this, in the repair step, only the minimum area containing the defect can be removed.

可使作為太陽電池之特性不會大幅降低,且亦不損及外觀 而修復缺陷處。 而且,依據本發明之第2態樣之太陽電池之製造裝置, 由於包含·為了特定出構造缺陷之位置,而於劃分元件彼 此間測定複數處之電阻值之電阻測定部,及拍攝藉由该電 阻測定部所縮限之小面積區域之圖像攝像部因此可正確 且以短時間特定出劃分元件内存在缺陷之位置。進一步於 修復步驟,可僅去除包含缺陷之最小限度的區域,可使作 為太陽電池之特性不會大幅降低,且亦不損及外觀而修復 缺陷處。 【實施方式】 以下,根據圖式詳細說明關於本發明之太陽電池之製造 方法、及使用於其之本發明之太陽電池之製造裝置。此 外,本實施型態係為了更加理解發明旨趣而具體地說明, 只要未特別指定,均不限定本發明。 圖1係表示藉由本發明之太陽電池之製造方法所製造的 非晶矽型之太陽電池之要部的一例之放大立體圖。而JL, 139429.doc 201005977 圖2(a)係表示圖】之太陽電池之層構成之剖面圖。圖2(b)係 放大圖2(a)之符號B所示之部分之剖面放大圖。太陽電池 1 〇具有光電轉換體12,其形成於透明的絕緣性之基板〗丨之 第1面11a(—面)。基板u若以例如玻璃或透明樹脂等,太 陽光之穿透性良好、且具有耐久性之絕緣材料形成即可。 於該基板11之第2面lib(另一面)射入太陽光。 於光電轉換體12,從基板11依序疊層有第一電極層(下 口 P電極)13、半導體層14及第二電極層(上部電極)i5 ^第一 電極層(下部電極)13若包含透明之導電材料,例如TC〇、 ITO(IndiUm Tin Oxide:氧化銦錫)等光穿透性之金屬氧化 物即可。而且,第二電極層(上部電極)15若藉由Ag、Cu等 導電性之金屬膜形成即可。 半導體層14係例如圖2(b)所示具有pin接合構造,其係於 P型非晶石夕膜17與n型非晶矽膜18之間,夾有丨型非晶矽膜 16而構成。然後,當太陽光射入於該半導體層14,產生電 子及電洞,由於P型非晶矽膜1 7與η型非晶石夕膜18之電位 差,電子及電洞活潑地移動,由於連續地重複此而於第一 電極層13與第二電極層15之間產生電位差(光電轉換)。 光電轉換體12係由切割線(scribe line) 19分割成外形為長 條狀的許多劃分元件21,21…。該劃分元件21,21·..係相互 電性劃分,並且於相互鄰接之劃分元件2丨彼此之間電性串 聯連接。藉此,光電轉換體12具有劃分元件21, 21…全部 電性串聯連結之構造。於該構造中,可取出高電位差的電 流。切割線19係藉由例如於基板丨丨之第1面na均勻地形成 139429.doc •10- 201005977 光電轉換體12後,利用雷射光線等,於光電轉換體12以特 定間隔形成溝槽而形成。 此外’於構成此類光電轉換體12之第二電極層(上部電 極)15上’宜進—步形成包含絕緣性的樹脂等之保護層(未 . 圖示)。 說明用以製造如玛上構成之太陽電池之製造方法。圖3 係階段性地表示本發明之太陽電池之第1實施型態之製造 φ 方法之流程圖。其中,特別詳述關於從構造缺陷的檢測到 修復之步驟。 首先’如圖1所示,於透明之基板^之第1面Ua上形成 光電轉換體12(光電轉換體之形成步驟:P1)。作為光電轉 換體12之構造,若為例如從基板π之第丨面11&依序疊層有 第一電極層(下部電極)13、半導體層14及第二電極層(上部 電極)15之構造即可。 於此類光電轉換體12之形成步驟中,如圖4(a)所示,會 • 有發生雜質等混入於(污染)半導體層14而產生之構造缺陷 A1、或於半導體層14產生微細針孔之構造缺陷A2等故障 的情況。此類構造缺陷Al,A2係使第一電極層13與第二電 • 極層15之間局部地短路(漏電)而使發電效率降低。 接著,向光電轉換體12照射例如雷射光線等,形成切割 線(scribe line)19,分割成長條狀的許多劃分元件21, (劃分元件之形成步驟:P2)。 於此類切割線19之形成步驟中,會有發生如圖4(a)所 示,由於雷射照射位置之偏離等,構成第二電極層15之金 139429.doc 201005977 屬熔融而流下至切割線19之溝槽内,因其所產生之構造缺 陷A3等故障之情況。此類構造缺陷A3係使第一電極層13 與第二電極層15之間局部地短路(漏電)而使發電效率降 低。 於以上步驟所形成之太陽電池10,特定出存在上述A1至 A3所代表之構造缺陷之劃分元件幻,21 .(缺陷區域特定步 驟:P3)。於該缺陷劃分特定步驟中,作為特定出存在構 造缺陷之劃分元件21,21…之具體方法,可舉出例如電阻 值之測定、FF(fill factor :曲線因子)之測定等。 藉由電阻值之測定特定出存在構造缺陷之劃分元件以之 情況時,如圖5所示,沿著長條狀的劃分元件21之長度方 向L,設定數個測定點,於相互鄰接之劃分元件2ι,2ι彼此 之間測定電阻值,從該測定值之分布特定出存在構造缺陷 之劃分元件21 s(缺陷劃分元件)。 於圖6表示在例如包含12〇個劃分元件之太陽電池中,測 定相互鄰接之劃分元件彼此之電阻值之一例。若依據該圖 6所示之測定結果,當比較第35個劃分元件與第^個割分 元件之電阻值時’第35個劃分元件之電阻值顯然降低。亦 即,預測於第35個劃分元件存在有短路原因之構造缺陷。 同樣地’預測於第1G9個劃分元件亦存在有構造缺陷。 於此類缺_分特定步射,藉由電阻值之敎而特定 存在構造缺陷之劃分元件的情況時’可舉出數種方法作為 測定方法。若為例如使用沿著劃分元件2ι之長度方向乙, 以特定間隔排列有許多探針之測定裝置,以〖次的探針上 139429.doc 12 201005977 下移動完成劃分元件彼此之電卩且彳自> + i 割八m 錄值之方法’或使探針沿著 劃分7G件21之長度方向L掃描, 於特疋測定點重複探針之 上下移動而測定之方法等即可。 此類缺陷劃分特定步驟中之電 沮〈判疋亦可利用下述 ::方法:施加特定值之偏壓電壓的方法;以兼作電流值 /、疋之1組2支探針所進行之2探針式的方法;或由使用於 施加衫值之偏壓電流之探針、及用於㈣值之測定之探It can be used as a solar cell without significantly reducing the characteristics and repairing defects without damaging the appearance. Further, in the solar cell manufacturing apparatus according to the second aspect of the present invention, the electric resistance measuring unit that measures the resistance value of the plurality of elements between the dividing elements in order to specify the position of the structural defect, and the photographing by the The image capturing unit in the small-area region in which the resistance measuring unit is limited can specify the position of the defect in the dividing element correctly and in a short time. Further, in the repairing step, only the region containing the minimum defect can be removed, so that the characteristics of the solar cell can be not greatly reduced, and the defect can be repaired without damaging the appearance. [Embodiment] Hereinafter, a method for manufacturing a solar cell according to the present invention and a manufacturing apparatus for a solar cell of the present invention used in the present invention will be described in detail based on the drawings. Further, the present embodiment is specifically described in order to better understand the object of the invention, and the present invention is not limited unless otherwise specified. Fig. 1 is an enlarged perspective view showing an example of a main part of an amorphous germanium type solar cell manufactured by the method for producing a solar cell of the present invention. JL, 139429.doc 201005977 Fig. 2(a) is a cross-sectional view showing the layer structure of the solar cell. Fig. 2(b) is an enlarged cross-sectional view showing a portion enlarged by the symbol B of Fig. 2(a). The solar cell 1 has a photoelectric conversion body 12 formed on a first surface 11a (-surface) of a transparent insulating substrate. The substrate u may be formed of an insulating material which is excellent in penetration of sunlight and has durability, such as glass or a transparent resin. Sunlight is incident on the second surface lib (the other surface) of the substrate 11. In the photoelectric conversion body 12, a first electrode layer (lower P electrode) 13, a semiconductor layer 14, and a second electrode layer (upper electrode) i5 ^first electrode layer (lower electrode) 13 are laminated in this order from the substrate 11. A transparent conductive material such as a light-transmitting metal oxide such as TC 〇 or ITO (IndiUm Tin Oxide) may be used. Further, the second electrode layer (upper electrode) 15 may be formed of a conductive metal film such as Ag or Cu. The semiconductor layer 14 has a pin bonding structure, for example, as shown in FIG. 2(b), and is formed between the P-type amorphous lithium film 17 and the n-type amorphous germanium film 18, and is formed by sandwiching the bismuth-type amorphous germanium film 16. . Then, when sunlight is incident on the semiconductor layer 14, electrons and holes are generated. Due to the potential difference between the P-type amorphous germanium film 17 and the n-type amorphous stone film 18, the electrons and the holes move actively, due to continuous This is repeated to generate a potential difference (photoelectric conversion) between the first electrode layer 13 and the second electrode layer 15. The photoelectric conversion body 12 is divided into a plurality of division elements 21, 21, ... which are elongated in shape by a scribe line 19. The dividing elements 21, 21·. are electrically divided from each other, and are electrically connected in series to each other in the mutually adjacent dividing elements 2丨. Thereby, the photoelectric conversion body 12 has a structure in which the division elements 21, 21, ... are electrically connected in series. In this configuration, a high potential difference current can be taken out. The dicing line 19 is formed by, for example, forming a 139429.doc •10-201005977 photoelectric conversion body 12 uniformly on the first surface na of the substrate ,, and forming a groove at a specific interval in the photoelectric conversion body 12 by using a laser beam or the like. form. Further, a protective layer (not shown) containing an insulating resin or the like is formed on the second electrode layer (upper electrode) 15 constituting the photoelectric conversion body 12. A method of manufacturing a solar cell configured to be used in the manufacture of a solar cell. Fig. 3 is a flow chart showing the method of manufacturing the φ of the first embodiment of the solar cell of the present invention in stages. Among them, the steps from the detection of the structural defect to the repair are specifically described in detail. First, as shown in Fig. 1, a photoelectric conversion body 12 is formed on the first surface Ua of the transparent substrate (step of forming a photoelectric conversion body: P1). The structure of the photoelectric conversion body 12 is, for example, a structure in which a first electrode layer (lower electrode) 13, a semiconductor layer 14, and a second electrode layer (upper electrode) 15 are laminated in this order from the first surface 11 & Just fine. In the step of forming such a photoelectric conversion body 12, as shown in FIG. 4(a), there is a structural defect A1 generated by mixing impurities (contamination) of the semiconductor layer 14 or the like, or a fine needle is generated in the semiconductor layer 14. The case where the hole is structurally defective A2 or the like. Such structural defects Al, A2 partially short-circuit (leakage) between the first electrode layer 13 and the second electrode layer 15 to lower the power generation efficiency. Then, the photoelectric conversion body 12 is irradiated with, for example, a laser beam or the like to form a scribe line 19, and a plurality of division elements 21 of a strip shape are divided, (step of forming the division element: P2). In the step of forming such a cutting line 19, as shown in FIG. 4(a), the gold 139429.doc 201005977 constituting the second electrode layer 15 is melted and flows down to the cutting due to the deviation of the laser irradiation position and the like. In the groove of the line 19, a failure such as a structural defect A3 is generated. Such a structural defect A3 causes a local short circuit (leakage) between the first electrode layer 13 and the second electrode layer 15 to lower the power generation efficiency. The solar cell 10 formed in the above steps specifies the divisional element of the structural defect represented by the above A1 to A3, 21 (defective area specific step: P3). In the specific step of the defect division, specific methods for specifying the division elements 21, 21, etc. in which the construction defects are present include, for example, measurement of resistance value, measurement of FF (fill factor), and the like. When the division element having the structural defect is specified by the measurement of the resistance value, as shown in FIG. 5, a plurality of measurement points are set along the longitudinal direction L of the elongated division element 21, and are adjacent to each other. The elements 2, 2 and 1 are each measured for a resistance value, and a division element 21 s (defect division element) having a structural defect is specified from the distribution of the measured values. Fig. 6 shows an example of measuring the resistance values of the mutually adjacent division elements in, for example, a solar cell including 12 division elements. According to the measurement results shown in Fig. 6, when the resistance values of the 35th dividing element and the second dividing element are compared, the resistance value of the 35th dividing element is remarkably lowered. That is, it is predicted that there is a structural defect in the 35th division element that causes a short circuit. Similarly, it is predicted that there are structural defects in the 1G9 division elements. In the case where such a missing step is a specific step, when a component having a structural defect is specified by a resistance value, several methods are used as the measuring method. For example, if the measuring device is arranged with a plurality of probes arranged at a specific interval along the length direction B of the dividing member 2, the movement of the dividing elements is completed by moving under the 138429.doc 12 201005977 of the secondary probe. > + i Method of cutting eight m records' or scanning the probe along the longitudinal direction L of the divided 7G member 21, and repeating the method of measuring the probe up and down at the characteristic measurement point. The defect in the specific step of the defect is also determined by the following method: Method: applying a bias voltage of a specific value; performing 2 sets of 2 probes which double as the current value /, 疋Probe-based method; or probe for bias current applied to the value of the shirt, and for the determination of (iv) values

針互異而進行包含2組4支探針之4探針式的方法。從該等 電壓值及電流值算出電阻值。 料,於此類缺_分特定㈣,除藉由電阻值之測定 所進订的方法以外,例如於太陽電池照射特定光量之照明 光,於各個劃分元件逐一進行汀⑴丨丨fact〇r :曲線因子)之 測定,比較相互鄰接之劃分元件彼此之FF之值的方法亦 可。該情況下’㈣之值特職落之劃分元件敎為存在 構造缺陷之劃分元件。 經過如以上之缺陷劃分特定步驟,發現存在有構造缺陷 之劃分7C件之太陽電池係送至其次說明之缺陷部位特定步 驟另方面,未找到存在有構造缺陷之劃分元件之太陽 電池係直接作為良品,經過保護層之形成步驟P6等而製品 化。 於上述缺陷劃分特定步驟中發現存在有構造缺陷之太陽 電池,係進一步送至限定劃分元件内存在有構造缺陷之部 位之步驟(缺陷部位特定步驟:P4)。於該缺陷部位特定步 驟,首先限於在前步驟之缺陷劃分特定步驟中被視為存在 139429.doc •13- 201005977 有構造缺陷之劃分元件’沿著劃分元件之長度方向匕測定A 4-probe method comprising two sets of four probes was carried out with different needles. The resistance value is calculated from the voltage value and the current value. In addition to the method specified by the measurement of the resistance value, for example, the solar cell illuminates the illumination light of a specific amount of light, and the T1(1)丨丨fact〇r is performed one by one for each of the divided components: The measurement of the curve factor) may be a method of comparing the values of FFs of mutually adjacent divided elements. In this case, the component of the value of (4) is divided into components with structural defects. After the specific steps are divided as described above, it is found that the solar cell system of the 7C piece having the structural defect is sent to the defect step specific step of the second description, and the solar cell system in which the component having the structural defect is not found is directly used as the good product. The product is formed by the formation of the protective layer P6 or the like. The solar cell in which the structural defect is found in the specific step of the above-described defect division is further sent to the step of defining the portion having the structural defect in the dividing element (defect site specific step: P4). The specific step at the defect site is first limited to the presence of the defect step in the previous step. 139429.doc •13- 201005977 The component with structural defects is measured along the length of the dividing element.

與鄰接之劃分元件21之間的電阻值。使此時之長度方向L =電阻值的測定間隔(測定密度),較前步驟之缺陷劃分特 定步驟之電阻值的測定間隔更細密而進行電阻值之測定。 例如圖7(a)所示,於被視為存在有構造缺陷尺之劃分元 = 21s之長度方向L之全區,於每特定之測定間隔τι(測定 密度),在鄰接之劃分元件21之間進行電阻值之測定。藉 由該電阻值之測定,於劃分元件21s之長度方向L,特定出 構造缺陷R之大概位置。測定間隔T1若為例如2〇 mm程度春 即可。 例如於圖8表示在長度方向L之長度為14〇〇 mm之長條狀 之劃分元件(存在有1處缺陷),測定與鄰接之劃分元件之間 之電阻值之一例。若依據該圖8所示之測定結果,從劃分 兀件之一端部之距離逼近250 mm附近時,電阻值降低。 存在有引起短路之構造缺陷之情況下,如此越接近缺陷之 存在位置’越會觀察到電阻值漸減的趨勢。因此,於劃分 元件21 s之長度方向l,以特定間隔測定電阻值,若觀察該 粵 電阻值之變化,可於劃分元件21s内得知構造缺陷尺之大概 位置。 如上述’於劃分元件21s之長度方向L,特定出構造缺陷 R之大概位置後,宜進一步縮限存在有構造缺陷R之區 · 域亦即’如上述於劃分元件21s之長度方向L,特定出構 泣缺陷尺之大概位置後’宜於該位置前後100 mm程度之 間以較則述測定間隔T1進一步更細密之測定間隔T2,測 139429.doc -14- 201005977 定與鄰接之劃分元件之間之電阻值(參考圖7⑽1 隔T2係設定為例如2 mm程度,以較上述特定出大概的^ 陷位置之步驟更細密10倍程度之精度,縮限存在有構造缺 陷R之區域Ζ» 、 此類缺陷部位特定步驟中之電阻值之敎亦可利用下述 任一方法:施加特定值之偏壓電壓的方法;以兼作電法值 測定之m2支探針所進行之2探針式的方法;或由^於 施加特定值之偏壓電流之探針、及用於電麼值之測定之探 針互異而進行包含2組4支探針之4探針式的方法 電壓值及電流值算出電阻值。 < 此外’於本實施型態之缺陷部位料步驟雖使阻抗值之 測定間隔呈2階段地變化,以特定出含有缺陷之位置,作 進-步呈3階段以上地改變測定間隔,更細密地縮限割分 元件内存在有構造缺陷R之區域Ζ亦可。 另一方面,於上述缺陷部位特定步驟(ρ4)中,亦可採用 如圖10(a)所示之探針單元U,纟沿著劃分元件A之長度 方向L’以間隔T2形成有許多探針。首先,最初於料定 之寬廣測定間_ ’間歇地僅於探針χι施加偏壓電峨 廢)’特定出構造缺陷R之大概位置。 接著,如圖10(b)所示,於被視為存在有構造缺陷r之區 間,亦即給予偏麼電流(電壓)之探針間,在電阻值最低之 區間之探針X2,施加偏磨電流(電壓)。此時,由於以校最 初之寬廣敎間隔η更狹窄的探針之形成間隔τ2進行測 定,因此更正確地特定出劃分元件内之構造缺陷r之位 139429.doc 15 201005977 如此 1史用、/α者劃分元件21S之長度方向L,卩間隔72緊 密地排财探針之賴單元U,適线變更絲偏壓電流 (電麼)之探針,藉此不使探針往 卞4長度方向L移動,僅選擇 供給偏壓電流之彳笑 彳木針即可迅迷地檢測構造缺陷R之位 置。 而且’作為其他檢測方法亦可採用於測定中,變更進行 測定之端子之間隔的方法。例如使用圖Μ⑷及⑼所示之 裝置之情況下’最初較大地設定端子間隔而測定電阻值,❹ 於檢㈣低於臨限值之電阻值的情況下’或電阻值較一定 $例更降低之情況下’縮窄端子間隔,於每個端子進行測 定於每個端子之測定中,電阻值高於臨限值之情況下, 或回到正常值之情況下,回到原本㈣隔進行測定。 步作為其他檢測方法,亦可採用決定複數臨限值, 於每個臨限值變更端子之測定間隔之方法。例如預先決定 電阻值之臨限值A,B,C(A>B>C)。電阻值為臨限值A以上 之It况時’空出1〇端子間隔而進行測定,當成為臨限值A _ =下時,空出5端子而進行測定,當成為臨限值B以下時, 空出2端子而進行敎,當成為臨限值C以下時,於各端子 •、於電阻值變大之情況下,相反地每當超過臨限 - 值時擴大測定間隔而進行測定。有缺陷的情況時,由於 . 值逐漸變化(參考圖8),因此藉由如此就每個臨限值變 更測疋間隔,可迅速且正確地檢測缺陷位置。 又,於該等檢出方法中,已說明使用關於如圖1〇排有許 139429.doc •16- 201005977 多端子,讓使用於測定之端子的間隔變化之裝置之情況。 於一面移動端子一面測定之情況下,亦可實現以就每個臨 限值變更測定間隔或移動速度之方法。 於此類鄰接之劃分元件彼此之電阻值之測定方法中,可 於劃分元件21s之長度方向L限定存在有構造缺陷r之範 . 圍’但難以於劃分元件21s之寬度方向霤特定出存在有構 造缺陷R之位置。因此,藉由圖像攝像部,拍攝藉由電阻 φ 值之測定而於劃分元件内縮限至狹窄範圍之存在有構造缺 陷R之區域Z(參考圖9⑷)。作為圖像攝像部係採用例如於 CCD相機24,組合有高倍率之鏡頭之装置。 然後,根據藉由CCD相機24所拍攝之存在有構造缺陷r 之區域z的圖像,正確地特定出區域z内之劃分元件⑴在 寬度方向W之存在有構造缺陷R的位置。此外,作為從如 2拍攝之圖像判斷構造缺陷R之位置之方法,採用由人進 行目視判斷$藉由使用電腦來比較被檢查對象之劃分元 參件之圖像資料、與預先拍攝之無缺陷之劃分元件的圖像資 料而進行之判斷。 _及#接之劃分%件彼此間之電阻值的分有, ;11刀凡件21S之長度方向L特定出存在構造缺陷R之區域Ζ =進:步藉由圖像攝像部(ccd相綱拍攝該經縮瑕之 此’能以針點正確地特◎劃分元件⑴内存在 有構k缺陷R之位置。 於以在之缺陷特定方法中,在 情況時會花費極㈣π 4 卸積之破檢查物之 ' 相對於此,於本實施型態中,作 139429.doc 201005977 為缺陷特定之方法’僅限定於藉由以短時間可敎之電阻 值之分布所預先縮限之小面積之區域2的攝像。因此,能 以極短時間迅速地特定出構造缺陷R正確之位置。 b 當於劃分元件21s,以針點正確地特定出構造缺陷汉之位 置時,接著修復太陽電池之構造缺陷R(修復步驟:Μ)。 於該修復步驟’向藉由電阻值之測定及圖像之攝像並以針 點特定出之構造缺陷R,於最小限度之範圍内,從雷射裝 置25照射雷射光線Q(參考圖9(b))。然後,僅蒸發而除掉存 在有構造缺陷R之部分之半導體層或電極(參考圖9(c)及圖 4(b))。 如此,藉由向以針點所特定出之構造缺陷汉,於最小限 度之範圍内照射雷射光線Q,可僅去除包含構造缺陷尺之 最小限度之範圍E1至E3。可將由於修復所造成之光電轉換 特性的劣化抑制在最小限度,並且於外觀上,修復痕跡幾 乎不醒目而可去除構造缺陷R。亦即,從圖4(勾所示之構 w缺陷Ai至A3之各者係如圖4(b)之符號E1至^所示而去 除。 如上述,經過缺陷劃分特定步驟(p3)、缺陷部位特定步 驟(P4)及修復步驟(P5),特定、去除存在於太陽電池之劃 分兀件之構造缺陷。經去除構造缺陷之太陽電池係送至保 濩層之形成步驟(P6),並進行後步驟之處理。 右依據此類之本發明之太陽電池之製造方法,最初於缺 陷劃分特定步驟’篩選包含含有構造缺陷之劃分元件之太 陽電池。然後’僅將經篩選之含有構造缺陷之太陽電池送 139429.doc -18· 201005977 至缺陷部位特定步驟。於缺陷部位特定步驟,藉由電阻值 之測定及藉其所縮限之區域之攝像,正確地特定出構造缺 陷之存在部位。藉此,可有效率地製造無構造缺陷之太陽 電池。 本發月之太%電池之製造裝置若包含下述即可:電阻測 疋部,其係為了於圖7(a)、(b)及圖叫至⑷所示之缺陷部 位特定步驟中,縮限構造缺之位置,而於劃分元件21The resistance value between the adjacent dividing element 21 and the adjacent element. The measurement interval (measurement density) of the longitudinal direction L = resistance value at this time is measured more finely than the measurement interval of the resistance value of the specific step of the defect division in the previous step, and the resistance value is measured. For example, as shown in Fig. 7(a), in the entire length direction L of the division element = 21s in which the structural defect rule is present, the measurement interval τι (measurement density) is specified for each of the adjacent division elements 21 The resistance value is measured between. By the measurement of the resistance value, the approximate position of the structural defect R is specified in the longitudinal direction L of the dividing element 21s. The measurement interval T1 is, for example, about 2 mm in spring. For example, Fig. 8 shows a long strip-shaped dividing element having a length of 14 mm in the longitudinal direction L (there is one defect), and an example of the resistance value between the adjacent dividing elements is measured. According to the measurement result shown in Fig. 8, the resistance value is lowered when the distance from one end of the divided member approaches 250 mm. In the case where there is a structural defect causing a short circuit, the closer to the existence position of the defect, the more the resistance value gradually decreases. Therefore, the resistance value is measured at a specific interval in the longitudinal direction l of the dividing element 21s, and if the change in the resistance value is observed, the approximate position of the structural defect ruler can be known in the dividing element 21s. As described above, after the approximate position of the structural defect R is specified in the longitudinal direction L of the dividing element 21s, it is preferable to further narrow the region/domain in which the structural defect R exists, that is, as described above in the longitudinal direction L of the dividing element 21s, After the approximate position of the weeping defect ruler, it is preferable to further measure the interval T2 between the distances of 100 mm before and after the position, and to measure the interval T1, and measure 139429.doc -14-201005977 The resistance value between the two (refer to Fig. 7 (10) 1 is set to, for example, about 2 mm, and the precision is 10 times more precise than the step of specifying the above-mentioned specific position, and there is a region where the structural defect R exists. The resistance value in a specific step of such a defect portion may also be any one of the following methods: a method of applying a bias voltage of a specific value; and a 2-probe type using a m2 probe which also serves as an electrical value measurement Method; or a method of applying a bias current of a specific value and a probe for measuring the value of the voltage to perform a 4-probe method comprising two sets of four probes, voltage value and current The value is calculated as the resistance value. In addition, in the defect portion step of the present embodiment, the measurement interval of the impedance value is changed in two stages, and the position including the defect is specified, and the measurement interval is changed in three steps or more, more finely. In the narrowing-cutting component, there is a region where the structural defect R exists. On the other hand, in the specific step (ρ4) of the defect portion, the probe unit U as shown in FIG. 10(a) may be used. A plurality of probes are formed at intervals T2 along the longitudinal direction L' of the dividing element A. First, initially, a wide measurement is made _ 'intermittently, only a bias voltage is applied to the probe )1' to specify a structural defect R The approximate location. Next, as shown in FIG. 10(b), in the section where the structural defect r is considered to exist, that is, between the probes that give the bias current (voltage), the probe X2 in the region where the resistance value is the lowest is applied. Grinding current (voltage). In this case, since the measurement interval τ2 of the probe which is narrower at the beginning of the first wide interval is measured, the position of the structural defect r in the division element is more accurately specified. 139429.doc 15 201005977 Thus, 1 history, / The α is divided into the length direction L of the element 21S, and the 卩 interval 72 closely aligns the probe unit U, and the probe of the wire bias current (electricity) is adapted to the length of the probe. L moves, and only selects the giggling eucalyptus needle that supplies the bias current to quickly detect the position of the structural defect R. Further, as another detection method, a method of changing the interval between the terminals to be measured may be employed in the measurement. For example, in the case of using the devices shown in Figures (4) and (9), the resistance value is measured by setting the terminal interval to a large extent, and the resistance value is lower than the value of the resistance value when the detection (4) is lower than the threshold value. In the case of 'narrowing the terminal spacing, measuring each terminal in the measurement of each terminal, if the resistance value is higher than the threshold value, or returning to the normal value, return to the original (four) interval to measure . As another detection method, the method of determining the complex threshold and changing the measurement interval of the terminal at each threshold may be employed. For example, the threshold value A, B, C (A > B > C) of the resistance value is determined in advance. When the resistance value is in the case of the A value of the threshold value A or more, the measurement is performed by vacating the terminal spacing of 1 〇. When the threshold value A _ = is obtained, the measurement is performed by vacating 5 terminals, and when the threshold value B or lower is reached. When the terminal is vacant, the measurement is performed when the threshold value is equal to or less than C. When the resistance value is increased, the measurement interval is increased every time the threshold value is exceeded. In the case of a defect, since the value gradually changes (refer to Fig. 8), the defect position can be detected quickly and correctly by changing the detection interval for each threshold. Further, in the above-described detection methods, it has been described that a device having a plurality of terminals of 139429.doc • 16-201005977 as shown in Fig. 1 is used to change the interval of the terminals used for measurement. In the case where one side of the mobile terminal is measured, it is also possible to change the measurement interval or the moving speed for each threshold. In the method of measuring the resistance values of the adjacent divided elements, the longitudinal direction L of the dividing element 21s can be limited to the existence of the structural defect r. However, it is difficult to diverge in the width direction of the dividing element 21s. Construct the location of the defect R. Therefore, the image capturing unit captures a region Z having a structural defect R in the narrowing range by the measurement of the resistance φ value (refer to Fig. 9 (4)). As the image pickup unit, for example, a CCD camera 24 is used, and a high-magnification lens is combined. Then, based on the image of the region z in which the structural defect r is photographed by the CCD camera 24, the position of the dividing element (1) in the region z in the width direction W where the structural defect R exists is correctly specified. Further, as a method of judging the position of the structural defect R from an image taken as in 2, a visual judgment by a person is made by comparing the image data of the divided meta-parameter of the object to be inspected by using a computer, and the pre-photographing is not performed. The defect is determined by dividing the image data of the component. _ and #接分分% of the resistance values of each other,; 11 knives 21S length direction L specifies the existence of structural defects R Ζ = advance: step by image camera (ccd phase This can be used to capture the position of the component (1) with the k-defect R. In the specific method of the defect, in the case of the case, it will cost the pole (4) π 4 to be broken. In contrast to this, in the present embodiment, 139429.doc 201005977 is a defect-specific method' limited to a small area that is pre-shrinked by a distribution of resistance values that can be shortened in a short time. Therefore, it is possible to quickly specify the position of the structural defect R in a very short time. b When the component 21s is divided, the position of the structural defect is correctly specified by the pin point, and then the structural defect of the solar cell is repaired. R (repair step: Μ). In the repair step, the laser is irradiated from the laser device 25 within a minimum range by measuring the resistance value and imaging the image and specifying the defect R specified by the pin point. Ray ray Q (refer to Figure 9(b)). Then, only The semiconductor layer or electrode in which the portion having the structural defect R exists is removed (refer to FIGS. 9(c) and 4(b)). Thus, by minimizing the defect to the structure specified by the pin point Irradiation of the laser beam Q within the range can remove only the minimum range E1 to E3 including the structural defect rule. The deterioration of the photoelectric conversion characteristics due to the repair can be minimized, and the appearance of the repair mark is almost The structural defect R can be removed without being conspicuous. That is, from FIG. 4 (each of the w-deficiencies Ai to A3 shown in the figure is removed as shown by the symbols E1 to ^ in FIG. 4(b). The defect-specific step (p3), the defect-specific step (P4), and the repairing step (P5), specifically, remove the structural defects existing in the dividing element of the solar cell. The solar cell system with the structural defect removed is sent to the protective layer Forming step (P6) and performing the subsequent step processing. Right according to the manufacturing method of the solar cell of the present invention, the solar cell of the dividing element containing the structural defect is initially screened in the specific step of defect division. Then ' The selected solar cell containing the structural defect is sent to 139429.doc -18·201005977 to the defect site specific step. In the specific step of the defect site, the specific value of the defect is determined by the measurement of the resistance value and the image of the region of the defect The existence of the structural defect is obtained. Thereby, the solar cell without structural defects can be efficiently manufactured. The manufacturing device of the solar cell of the present month is as follows: the electric resistance measuring portion is used for FIG. 7 In (a), (b), and the specific step of the defect portion shown in (4), the position of the narrowing structure is missing, and the dividing element 21

彼此m複數處之電阻值;及圖像攝像部(ccd相機 2句’其係僅拍攝藉由該電阻測定部所縮限之存在有構造 缺陷R之區域Z。 電阻測定部右由2探針式或4探針式之電阻測定裝置、及 使劃分元件21及探針沿著長度方向L相對移動之移動裝置 所構成即可。而且,作為圖像攝像部可舉出例如光學 機、CCD相機等。 然後’於圖9⑷至⑷所示之修復步射,藉由圖像攝像 部正域地特定出構造缺陷R之位置。而且,作為用 確地特U之構造缺陷R照射f射光線k修復部,使用 =雷射,置〜此類修復部進—步包含使雷射光線於特 ^ 之掃描機構’或載置被修復物之太陽電池並 使其水平移動之移動台即可。 及f晋^所'^述,本發明係對於—種製造太陽電池之方法 =置有用’該製造太陽電池之方法及裝置係抑制對於光 轉換體之損傷’正確地特定出構造缺陷之發生處,確實 地去除及修復所特定的構造缺陷。 處確實 139429.doc •19· 201005977 【圖式簡單說明】 圖1係表示非晶矽型太陽電池之要部之一例之放大立體 IS] ·圃, 圖2(a)、(b)係表示非晶石夕型太陽電池之一例之剖面圖; 圖3係表示本發明之太陽電池之製造方法之流程圖; 圖4(a)、(b)係表示構造缺陷之存在例及缺陷修復後之狀 況之剖面圖; 圖5係表示缺陷劃分特定步驟之狀況之說明圖; 圖6係表示缺陷劃分特宗 . 刀符疋步驟中之電阻值之測定例之 參 圖7(a)、(b)係表示缺陷部位 ^ |位特定步驟之狀況之說明 圖8係表示缺陷部位特 . &步驟中之電阻值之測定 圖;例之 圖9(a)〜(c)係表示缺陷部位特* 之說明圖;及 心 步驟及修復步驟之—例 圖圖係表示缺陷部位特定步驟之-例之說明 【主要元件符號說明】The resistance value of the complex part of each other; and the image capturing unit (the ccd camera has two sentences): only the region Z in which the structural defect R exists by the resistance measuring unit is captured. The resistance measuring unit is composed of 2 probes right. A four-probe type resistance measuring device and a moving device that relatively move the dividing element 21 and the probe in the longitudinal direction L. Further, as the image capturing unit, for example, an optical machine or a CCD camera Then, in the repairing step shown in Fig. 9 (4) to (4), the position of the structural defect R is specified by the image capturing unit in the positive direction. Moreover, the f-ray ray is irradiated as the structural defect R of the specific U. In the repairing section, use the laser, and set the repairing section to include a laser that allows the laser to be irradiated to the scanning mechanism or a mobile station that mounts the solar cell of the object to be repaired and moves it horizontally. The present invention relates to a method for manufacturing a solar cell. The method and apparatus for manufacturing a solar cell suppress damage to a light conversion body to correctly identify the occurrence of a structural defect. Definitely remove and repair specific Structural defects 139429.doc •19· 201005977 [Simple description of the diagram] Figure 1 shows an enlarged stereoscopic example of an essential part of an amorphous germanium solar cell. ·圃, Figure 2(a), (b) FIG. 3 is a flow chart showing an example of a method for manufacturing a solar cell of the present invention; FIG. 4 is a flow chart showing a method for manufacturing a solar cell of the present invention; and FIG. 4(a) and FIG. FIG. 5 is an explanatory view showing the state of the specific step of the defect division; FIG. 6 is a diagram showing the defect classification. The measurement example of the resistance value in the tool step is shown in Fig. 7(a), ( b) indicates the location of the defective portion. The description of the condition of the specific step is shown in Fig. 8. The measurement of the resistance value in the step of the defect portion is shown in Fig. 9 (a) to (c) * Description of the figure; and the steps of the heart and the steps of the repair - the illustration of the figure shows the specific steps of the defect - the description of the example [the main component symbol description]

10 太陽電池 11 基板 12 光電轉換體 13 第一電極 14 半導體層 15 第二電極 139429.doc "20. 201005977 19 21 25 切割線 劃分元件 雷射裝置10 solar cell 11 substrate 12 photoelectric conversion body 13 first electrode 14 semiconductor layer 15 second electrode 139429.doc "20. 201005977 19 21 25 cutting line dividing element laser device

139429.doc -21-139429.doc -21-

Claims (1)

201005977 七、申請專利範圍: 1. 一種太陽電池之製造方法,其特徵為: 形成光電轉換體,該光電轉換體包含複數個劃分元 件,且相互鄰接之前述劃分元件彼此電性連接; 特定出前述光電轉換體中含有構造缺陷之前述劃分元 件; 根據於相互鄰接之前述劃分元件彼此之間測定複數處 之電阻值所獲得之電阻值分布,縮限前述劃分元件内存 在有刖述構造缺陷之區域,藉由圖像攝像部拍攝該經縮 限之存在前述構造缺陷之前述區域内,從所獲得之圖像 正確地特定出前述構造缺陷之位置,藉此於前述劃分元 件内限定存在前述構造缺陷之部位; 於存在前述構造缺陷之部位,照射雷射光線而去除前 述構造缺陷。 2. 如凊求項1之太陽電池之製造方法,其中限定存在前述 構造缺陷之部位時,將電阻值之測定密度至少2階段以 上地改變而進行測定。 3. 如請求項1或2之太陽電池之製造方法,其中限定存在前 述構造缺陷之部位時,電阻值之測定係使用4探針式之 電阻測定裝置。 4. 一種太陽電池之製造裝置,其特徵為: 該太陽電池具有包含複數個劃分元件之光電轉換燧; 且包含:電阻測定部,其係為了於前述光電轉換體中 含有構造缺陷之劃分元件内,縮限存在構造缺陷之區 139429.doc 201005977 域,而於相互鄰接之劃分元件彼此間測定複數處之電阻 值; 圖像攝像部,其係拍攝前述經縮限之存在構造缺陷之 區域内,正確地特定出構造缺陷之位置;及 修復部,其係向前述構造缺陷照射雷射光線而去除前 述構造缺陷。 139429.doc201005977 VII. Patent application scope: 1. A method for manufacturing a solar cell, characterized in that: a photoelectric conversion body is formed, the photoelectric conversion body includes a plurality of dividing elements, and the dividing elements adjacent to each other are electrically connected to each other; The photoelectric conversion body includes the above-mentioned dividing element having a structural defect; and the resistance value distribution obtained by measuring the resistance value of the complex portion between the mutually adjacent divided element elements, and the area where the structural defect is described in the dividing element And capturing, by the image capturing unit, the narrowed-down region in which the structural defect exists, and correctly identifying the position of the structural defect from the obtained image, thereby defining the structural defect in the dividing element a portion; the portion of the structural defect is present, and the laser beam is irradiated to remove the structural defect. 2. The method for producing a solar cell according to claim 1, wherein the portion where the structural defect is present is defined, and the measured density of the resistance value is changed at least two stages to be measured. 3. The method of manufacturing a solar cell according to claim 1 or 2, wherein the portion where the structural defect is present is limited, and the resistance value is measured by using a 4-probe type resistance measuring device. A solar cell manufacturing apparatus, comprising: a photoelectric conversion device including a plurality of division elements; and a resistance measuring unit for dividing a component including a structural defect in the photoelectric conversion body a region of 139429.doc 201005977 having a structural defect, and a resistance value at a plurality of mutually adjacent dividing elements; and an image capturing portion that captures a region in which the structural defect is present in the shrinkage limit, A position where the structural defect is correctly identified; and a repairing portion that irradiates the aforementioned structural defect with the laser beam to remove the structural defect. 139429.doc
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