TWI909771B - Photoelectric device module and operation method thereof - Google Patents
Photoelectric device module and operation method thereofInfo
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- TWI909771B TWI909771B TW113140420A TW113140420A TWI909771B TW I909771 B TWI909771 B TW I909771B TW 113140420 A TW113140420 A TW 113140420A TW 113140420 A TW113140420 A TW 113140420A TW I909771 B TWI909771 B TW I909771B
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Abstract
Description
本揭示內容是關於一種光電元件模組及其操作方法。This disclosure pertains to an optoelectronic component module and its operation method.
為了提升光感測器或影像感測器的性能(例如高光電轉換效率、高亮度、高靈敏度、寬發光波長範圍及/或寬感光波長範圍)及降低其成本,目前已開發出許多可應用的新材料,例如有機半導體。To improve the performance of photosensors or image sensors (e.g., high photoelectric conversion efficiency, high brightness, high sensitivity, wide emission wavelength range and/or wide sensing wavelength range) and reduce their cost, many new materials, such as organic semiconductors, have been developed for application.
以有機半導體作為光電轉換材料的優勢在於其光譜響應範圍(spectral response range)比傳統材料矽來的更寬。並且,一部分的有機半導體具有較小的光學能隙,可對於波長大於等於1000 nm的短波紅外(short-wave infrared, SWIR)光產生響應。然而,有機半導體的吸收係數較低,因此,由有機半導體作為光電轉換層的光感測器或影像感測器的外部量子效率(external quantum efficiency, EQE)通常較低。The advantage of using organic semiconductors as photoelectric conversion materials lies in their wider spectral response range compared to traditional silicon. Furthermore, some organic semiconductors possess smaller optical band gaps, enabling them to respond to short-wave infrared (SWIR) light with wavelengths greater than or equal to 1000 nm. However, organic semiconductors have lower absorption coefficients; therefore, the external quantum efficiency (EQE) of photosensors or image sensors using organic semiconductors as the photoelectric conversion layer is typically lower.
本揭示內容提供一種光電元件模組,其包括基板、第一反射層、光電轉換層及第二反射層。第一反射層設置於基板上,其中第一反射層具有第一反射率。光電轉換層設置於第一反射層上,且具有大於等於135 nm的厚度。第二反射層設置於光電轉換層上,其中第二反射層具有第二反射率,第一反射率大於第二反射率。This disclosure provides an optoelectronic component module, comprising a substrate, a first reflective layer, a photoelectric conversion layer, and a second reflective layer. The first reflective layer is disposed on the substrate, wherein the first reflective layer has a first reflectivity. The photoelectric conversion layer is disposed on the first reflective layer and has a thickness greater than or equal to 135 nm. The second reflective layer is disposed on the photoelectric conversion layer, wherein the second reflective layer has a second reflectivity, and the first reflectivity is greater than the second reflectivity.
在一些實施方式中,光電轉換層的厚度為135 nm至500 nm。In some embodiments, the thickness of the photoelectric conversion layer is 135 nm to 500 nm.
在一些實施方式中,第一反射層具有大於等於50%的第一反射率,第二反射層具有大於等於5%的第二反射率。In some embodiments, the first reflective layer has a first reflectivity of ≥50%, and the second reflective layer has a second reflectivity of ≥5%.
在一些實施方式中,光電元件模組更包括載子傳輸層設置於第一反射層與光電轉換層之間或光電轉換層與第二反射層之間。In some embodiments, the optoelectronic module further includes a carrier transport layer disposed between the first reflective layer and the photoelectric conversion layer or between the photoelectric conversion layer and the second reflective layer.
在一些實施方式中,載子傳輸層的厚度為10 nm至100 nm。In some implementations, the thickness of the carrier transport layer is 10 nm to 100 nm.
在一些實施方式中,第一反射層的厚度大於等於50 nm。In some embodiments, the thickness of the first reflective layer is greater than or equal to 50 nm.
在一些實施方式中,第一反射層包括銀(Ag)、鋁(Al)、銅(Cu)、金(Au)、鈦(Ti)、鎢(W)、鉬(Mo)、氮化鈦(TiN)或其組合。In some embodiments, the first reflective layer includes silver (Ag), aluminum (Al), copper (Cu), gold (Au), titanium (Ti), tungsten (W), molybdenum (Mo), titanium nitride (TiN), or combinations thereof.
在一些實施方式中,第二反射層的厚度為50 nm至300 nm。In some embodiments, the thickness of the second reflective layer is 50 nm to 300 nm.
在一些實施方式中,第二反射層包括透明導電氧化物(transparent conductive oxide, TCO)、透明導電高分子、奈米銀線、厚度小於或等於15 nm的含金屬層或其組合。In some embodiments, the second reflective layer includes a transparent conductive oxide (TCO), a transparent conductive polymer, silver nanowires, a metal-containing layer with a thickness of less than or equal to 15 nm, or a combination thereof.
在一些實施方式中,光電轉換層具有小於等於1.24 eV的光學能隙。In some embodiments, the photoelectric conversion layer has an optical bandgap of less than or equal to 1.24 eV.
本揭示內容提供一種操作光電元件模組的方法,其包括藉由前述任一實施方式的光電元件模組接收光線,其中第二反射層的上表面為受光面。This disclosure provides a method for operating an optoelectronic element module, which includes receiving light through the optoelectronic element module of any of the foregoing embodiments, wherein the upper surface of the second reflective layer is the light-receiving surface.
以附圖詳細描述及揭露以下的複數個實施方式。為明確說明,許多實務上的細節將在以下敘述中一併說明。然而,應當理解,這些實務上的細節並非旨在限制本揭示內容。也就是說,在本揭示內容部分實施方式中,這些實務上的細節是非必要的。此外,為簡化圖式,一些習知結構與元件在圖式中將以示意方式示出。The following embodiments are described and disclosed in detail with reference to the accompanying drawings. For clarity, many practical details will be explained in the following description. However, it should be understood that these practical details are not intended to limit the scope of this disclosure. That is, these practical details are not essential in the embodiments described herein. Furthermore, for the sake of simplicity, some known structures and elements will be shown schematically in the drawings.
應理解的是,雖然第一、第二與第三等等之詞彙可在本文中用於描述各種元件、組件、區域、層和/或區塊,但是這些元件、組件、區域、層和/或區塊不應該被這些詞彙所限制。這些詞彙僅用於將單一元件、組件、區域、層或區塊與另一元件、組件、區域、層或區塊區分開來。因此,在下文中的第一元件、組件、區域、層或區塊也可被稱為第二元件、組件、區域、層或區塊,而不脫離本揭示內容的教示。It should be understood that while the terms first, second, third, etc., may be used herein to describe various elements, components, regions, layers, and/or blocks, these elements, components, regions, layers, and/or blocks should not be limited by these terms. These terms are used only to distinguish a single element, component, region, layer, or block from another element, component, region, layer, or block. Therefore, the first element, component, region, layer, or block referred to below may also be referred to as the second element, component, region, layer, or block without departing from the teachings of this disclosure.
本揭示內容提供一種光電元件模組。第1圖是根據本揭示內容各種實施方式的光電元件模組100的剖面示意圖。如第1圖所示,光電元件模組100包括基板110、第一反射層120、第一載子傳輸層130、光電轉換層140、第二載子傳輸層150及第二反射層160。第一反射層120設置於基板110上,其中第一反射層120具有第一反射率。第一載子傳輸層130設置於第一反射層120上。光電轉換層140設置於第一載子傳輸層130上,且具有大於等於135 nm的厚度T4。第二載子傳輸層150設置於光電轉換層140上。第二反射層160設置於第二載子傳輸層150上,其中第二反射層160具有第二反射率,第一反射率大於第二反射率。在一些實施方式中,第一反射層120具有大於等於50%的第一反射率,例如50、55、60、65、70、75、80、85、90或95%。在一些實施方式中,第一反射層120對於波長為600至2600 nm的光線,具有大於等於50%的第一反射率。當第一反射率越高,能夠被第一反射層120反射進入光電轉換層140內的光線越多。在一些實施方式中,第二反射層160具有大於等於5%的第二反射率,例如,第二反射率可大於等於5、10、15、20、25或30%。此外,第二反射率可小於等於50%,以使光電元件模組100仍能夠接收足夠的光線用於光電轉換。在一些實施方式中,光電元件模組100更包括讀取或收集光電轉換層140產生的訊號及電流的外接導線或電路結構(未示出)。舉例來說,外接導線及/或電路結構設置於基板110中。光電元件模組100可做為感光元件或是影像感測元件。This disclosure provides an optoelectronic device module. Figure 1 is a schematic cross-sectional view of an optoelectronic device module 100 according to various embodiments of this disclosure. As shown in Figure 1, the optoelectronic device module 100 includes a substrate 110, a first reflective layer 120, a first carrier transport layer 130, a photoelectric conversion layer 140, a second carrier transport layer 150, and a second reflective layer 160. The first reflective layer 120 is disposed on the substrate 110, wherein the first reflective layer 120 has a first reflectivity. The first carrier transport layer 130 is disposed on the first reflective layer 120. The photoelectric conversion layer 140 is disposed on the first carrier transport layer 130 and has a thickness T4 greater than or equal to 135 nm. The second carrier transport layer 150 is disposed on the photoelectric conversion layer 140. A second reflective layer 160 is disposed on the second carrier transport layer 150, wherein the second reflective layer 160 has a second reflectivity, and the first reflectivity is greater than the second reflectivity. In some embodiments, the first reflective layer 120 has a first reflectivity greater than or equal to 50%, such as 50, 55, 60, 65, 70, 75, 80, 85, 90, or 95%. In some embodiments, the first reflective layer 120 has a first reflectivity greater than or equal to 50% for light with wavelengths from 600 to 2600 nm. The higher the first reflectivity, the more light can be reflected by the first reflective layer 120 into the photoelectric conversion layer 140. In some embodiments, the second reflective layer 160 has a second reflectivity greater than or equal to 5%, for example, the second reflectivity may be greater than or equal to 5%, 10, 15, 20, 25, or 30%. Furthermore, the second reflectivity can be less than or equal to 50% to ensure that the optoelectronic module 100 can still receive sufficient light for photoelectric conversion. In some embodiments, the optoelectronic module 100 further includes external conductors or circuit structures (not shown) for reading or collecting signals and currents generated by the photoelectric conversion layer 140. For example, the external conductors and/or circuit structures are disposed in the substrate 110. The optoelectronic module 100 can serve as a photosensitive element or an image sensing element.
本揭示內容提供一種操作光電元件模組100的方法,其包括藉由光電元件模組100接收光線L1,其中第二反射層160的上表面為受光面。由於光電元件模組100可接收來自上方的光線L1,以作為頂部照光式的裝置。在光線L1自上方進入光電元件模組100後,由於第一反射層120的第一反射率大於第二反射層160的第二反射率,光線L1容易被第一反射層120反射再次進入光電轉換層140內,從而有利於光電轉換層140再次吸收光線L1以提升光電元件模組100的外部量子效率(EQE)。更詳細來說,光電元件模組100具有共振腔(micro-cavity),亦即第一反射層120的上表面與第二反射層160的下表面之間的空間,因此,光線L1會在如同兩面鏡子一般的第一反射層120與第二反射層160之間反射,藉由共振腔效應(micro-cavity effect)提升光電轉換層140的吸光量,從而提升光電元件模組100的EQE及光電流。值得注意的是,共振腔效應會被第一反射層120與第二反射層160之間的膜層的厚度影響。藉由調整光電轉換層140的厚度T4、第一載子傳輸層130的厚度T2及第二載子傳輸層150的厚度T3可進一步優化共振腔效應,從而提升光電轉換層140的吸光能力。第一載子傳輸層130可作為光學間隙子(optical spacer),適當調整光場並有效地分配光子至光電轉換層140內,使反射光能夠被光電轉換層140再次吸收利用,從而提升光電元件模組100的EQE及光電流。可藉由調整光電場分佈(optical-electrical field distribution)調控光電響應的波長範圍,以符合不同產品需求及應用需求。當光電轉換層140含有可對於短波紅外(short-wave infrared, SWIR)光產生響應的材料時,光電元件模組100可應用於SWIR感測器領域,雖然這些材料的吸收係數通常較低,光電元件模組100仍可藉由共振腔效應來提升光電轉換層140的吸光率。當光電轉換層140的厚度T4較小時,可以藉由第一反射層120提供共振腔效應來提升光電轉換層140的吸光率。This disclosure provides a method for operating an optoelectronic module 100, which includes receiving light L1 through the optoelectronic module 100, wherein the upper surface of the second reflective layer 160 is a light-receiving surface. Since the optoelectronic module 100 can receive light L1 from above, it serves as a top-illuminated device. After light L1 enters the optoelectronic module 100 from above, because the first reflectivity of the first reflective layer 120 is greater than the second reflectivity of the second reflective layer 160, light L1 is easily reflected by the first reflective layer 120 and re-enters the photoelectric conversion layer 140. This facilitates the photoelectric conversion layer 140 in re-absorbing light L1, thereby improving the external quantum efficiency (EQE) of the optoelectronic module 100. More specifically, the optoelectronic module 100 has a micro-cavity, which is the space between the upper surface of the first reflective layer 120 and the lower surface of the second reflective layer 160. Therefore, light L1 is reflected between the first reflective layer 120 and the second reflective layer 160, which act like two mirrors. The micro-cavity effect increases the light absorption of the photoelectric conversion layer 140, thereby improving the EQE and photocurrent of the optoelectronic module 100. It is worth noting that the micro-cavity effect is affected by the thickness of the film layer between the first reflective layer 120 and the second reflective layer 160. By adjusting the thickness T4 of the photoelectric conversion layer 140, the thickness T2 of the first carrier transport layer 130, and the thickness T3 of the second carrier transport layer 150, the resonant cavity effect can be further optimized, thereby improving the light absorption capability of the photoelectric conversion layer 140. The first carrier transport layer 130 can act as an optical spacer, appropriately adjusting the light field and effectively distributing photons into the photoelectric conversion layer 140, so that the reflected light energy can be absorbed and utilized again by the photoelectric conversion layer 140, thereby improving the EQE and photocurrent of the optoelectronic device module 100. The wavelength range of the photoelectric response can be controlled by adjusting the optical-electrical field distribution to meet the needs of different products and applications. When the photoelectric conversion layer 140 contains materials that respond to short-wave infrared (SWIR) light, the photoelectric element module 100 can be applied in the field of SWIR sensors. Although the absorption coefficient of these materials is usually low, the photoelectric element module 100 can still improve the light absorption of the photoelectric conversion layer 140 through the resonant cavity effect. When the thickness T4 of the photoelectric conversion layer 140 is small, the light absorption of the photoelectric conversion layer 140 can be improved by providing a resonant cavity effect through the first reflective layer 120.
在一些實施方式中,基板110包括玻璃、陶瓷、矽、塑膠、高分子或其組合。在一些實施方式中,基板110為不透光的。在一些實施方式中,第一反射層120的厚度T1大於等於50 nm。舉例來說,厚度T1為50 nm至500 nm,例如50、100、150、200、250、300、350、400、450或500 nm。第一反射層120的厚度T1不會影響光電轉換效率,故可根據設計需求調整。在一些實施方式中,第一反射層120為導電層,例如包括銀、鋁、銅、金、鈦、鎢、鉬、氮化鈦或其組合。若以銀層作為第一反射層120,當波長大於600 nm的光線L1從第一載子傳輸層130進入銀層時,會產生趨近全反射的現象,從而能夠提升光電轉換層140的吸光率。光線L1的波長例如為600 nm至2600 nm。In some embodiments, the substrate 110 comprises glass, ceramic, silicon, plastic, polymer, or combinations thereof. In some embodiments, the substrate 110 is opaque. In some embodiments, the thickness T1 of the first reflective layer 120 is greater than or equal to 50 nm. For example, the thickness T1 is from 50 nm to 500 nm, such as 50, 100, 150, 200, 250, 300, 350, 400, 450, or 500 nm. The thickness T1 of the first reflective layer 120 does not affect the photoelectric conversion efficiency and can therefore be adjusted according to design requirements. In some embodiments, the first reflective layer 120 is a conductive layer, such as comprising silver, aluminum, copper, gold, titanium, tungsten, molybdenum, titanium nitride, or combinations thereof. If a silver layer is used as the first reflective layer 120, when light L1 with a wavelength greater than 600 nm enters the silver layer from the first carrier transport layer 130, near total internal reflection will occur, thereby increasing the absorbance of the photoelectric conversion layer 140. The wavelength of light L1 is, for example, 600 nm to 2600 nm.
請繼續參照第1圖。在一些實施方式中,第一載子傳輸層130的厚度T2及第二載子傳輸層150的厚度T3各自為10 nm至100 nm,例如10、20、30、40、50、60、70、80、90或100 nm。第一載子傳輸層130具備載子傳輸能力並可作為光學間隙子,以適當調整光場並有效地分配光子至光電轉換層140內,使反射光能夠被光電轉換層140再次吸收利用,從而提升光電元件模組100的EQE及光電流。當第一載子傳輸層130的厚度T2增加,光電元件模組100的EQE也會隨之上升。Please continue referring to Figure 1. In some embodiments, the thickness T2 of the first carrier transport layer 130 and the thickness T3 of the second carrier transport layer 150 are each from 10 nm to 100 nm, for example, 10, 20, 30, 40, 50, 60, 70, 80, 90, or 100 nm. The first carrier transport layer 130 has carrier transport capability and can act as an optical gapper to appropriately adjust the optical field and effectively distribute photons into the photoelectric conversion layer 140, so that the reflected light energy can be absorbed and utilized again by the photoelectric conversion layer 140, thereby improving the EQE and photocurrent of the optoelectronic device module 100. As the thickness T2 of the first carrier transport layer 130 increases, the EQE of the optoelectronic device module 100 also increases accordingly.
請繼續參照第1圖。第一載子傳輸層130與第二載子傳輸層150的材料不同。在一些實施方式中,在第一載子傳輸層130及第二載子傳輸層150中,一者為電子傳輸層,另一者為電洞傳輸層。舉例來說,第一載子傳輸層130為電子傳輸層,第二載子傳輸層150為電洞傳輸層。舉例來說,第一載子傳輸層130為電洞傳輸層,第二載子傳輸層150為電子傳輸層。在一些實施方式中,第一載子傳輸層130及第二載子傳輸層150各自包括金屬氧化物或有機材料(例如有機小分子、高分子或可交聯分子)。在一些實施方式中,電子傳輸層包括氧化鋁鋅、氧化鋅(ZnO)、氧化鈦(如二氧化鈦)、氧化錫(如二氧化錫)、聚電解質(polyelectrolyte)、4,7-二苯基-1,10-菲咯啉(4,7-diphenyl-1,10-phenanthroline, BPhen)或其組合。在一些實施方式中,電洞傳輸層包括三氧化鉬(MoO 3)、一氧化鎳(NiO)、三氧化鎢(WO 3)、PEDOT:PSS、 、 、 、 、 、浴銅靈(bathocuproine, BCP)、巴克明斯特富勒烯(C60)、聚乙烯亞胺(polyethylenimine, PEI)、乙氧基聚乙烯亞胺(ethoxylated polyethylenimine, PEIE)或其組合。PEI可具有以下結構 。PEIE可具有以下結構 ,其中x、y及z為莫耳分率,x、y及z的總合為1。在其他實施方式中,省略設置於第一反射層120與光電轉換層140之間的第一載子傳輸層130,從而使光電轉換層140設置於第一反射層120上且直接接觸第一反射層120。在其他實施方式中,省略設置於光電轉換層140與第二反射層160之間的第二載子傳輸層150,從而使第二反射層160設置於光電轉換層140上且直接接觸光電轉換層140。 Please continue referring to Figure 1. The first carrier transport layer 130 and the second carrier transport layer 150 are made of different materials. In some embodiments, one of the first carrier transport layer 130 and the second carrier transport layer 150 is an electron transport layer and the other is a hole transport layer. For example, the first carrier transport layer 130 is an electron transport layer and the second carrier transport layer 150 is a hole transport layer. For example, the first carrier transport layer 130 is a hole transport layer and the second carrier transport layer 150 is an electron transport layer. In some embodiments, the first carrier transport layer 130 and the second carrier transport layer 150 each comprise a metal oxide or an organic material (e.g., small organic molecules, polymers, or crosslinkable molecules). In some embodiments, the electron transport layer includes alumina (e.g., zinc oxide, ZnO), titanium oxide (e.g., titanium dioxide), tin oxide (e.g., tin dioxide), polyelectrolyte, 4,7-diphenyl-1,10-phenanthroline (BPhen), or combinations thereof. In some embodiments, the hole transport layer includes molybdenum trioxide ( MoO₃ ), nickel monoxide (NiO), tungsten trioxide ( WO₃ ), PEDOT:PSS, etc. , , , , Bath copper alloy (BCP), barkminster fullerene (C60), polyethylenimine (PEI), ethoxylated polyethylenimine (PEIE), or combinations thereof. PEI may have the following structure. PEIE can have the following structure Where x, y, and z are molar fractions, and the sum of x, y, and z is 1. In other embodiments, the first carrier transport layer 130 disposed between the first reflective layer 120 and the photoelectric conversion layer 140 is omitted, so that the photoelectric conversion layer 140 is disposed on the first reflective layer 120 and directly contacts the first reflective layer 120. In other embodiments, the second carrier transport layer 150 disposed between the photoelectric conversion layer 140 and the second reflective layer 160 is omitted, so that the second reflective layer 160 is disposed on the photoelectric conversion layer 140 and directly contacts the photoelectric conversion layer 140.
在一些實施方式中,光電轉換層140含有可對於短波紅外(SWIR)光產生響應的材料,更具體來說,光電轉換層140可對於波長大於等於1000 nm的光線產生響應。舉例來說,光電轉換層140可偵測波長介於1000 nm至5500 nm的光線,例如1000、1050、1500、2000、2500、3000、3500、4000、4500、5000 或5500 nm。在一些實施方式中,光電轉換層140具有小於等於1.24 eV的光學能隙,例如0.84、0.94、1.04、1.14或1.24 eV。在一些實施方式中,光電轉換層140的厚度T4為135 nm至500 nm,例如135、140、160、180、200、220、240、260、280、300、320、340、360、380、400、420、440、460、480或500 nm。當厚度T4小於135 nm,第一反射層120與第二反射層160之間的共振腔效應可能較弱。當厚度T4超過500 nm,受限於光電轉換層140的載子傳遞能力,光電元件模組100的EQE可能會下降。在一些實施方式中,光電轉換層140是由旋轉塗佈來形成。In some embodiments, the photoelectric conversion layer 140 contains a material responsive to short-wavelength infrared (SWIR) light; more specifically, the photoelectric conversion layer 140 is responsive to light with wavelengths greater than or equal to 1000 nm. For example, the photoelectric conversion layer 140 can detect light with wavelengths between 1000 nm and 5500 nm, such as 1000, 1050, 1500, 2000, 2500, 3000, 3500, 4000, 4500, 5000, or 5500 nm. In some embodiments, the photoelectric conversion layer 140 has an optical bandgap of less than or equal to 1.24 eV, such as 0.84, 0.94, 1.04, 1.14, or 1.24 eV. In some embodiments, the thickness T4 of the photoelectric conversion layer 140 is between 135 nm and 500 nm, for example, 135, 140, 160, 180, 200, 220, 240, 260, 280, 300, 320, 340, 360, 380, 400, 420, 440, 460, 480, or 500 nm. When the thickness T4 is less than 135 nm, the resonant cavity effect between the first reflective layer 120 and the second reflective layer 160 may be weak. When the thickness T4 exceeds 500 nm, the EQE of the optoelectronic element module 100 may decrease due to the limited carrier transport capability of the photoelectric conversion layer 140. In some embodiments, the photoelectric conversion layer 140 is formed by rotational coating.
在一些實施方式中,光電轉換層140包括有機半導體、無機半導體、量子點、鈣鈦礦或其組合。在一些實施方式中,量子點包括CdSe、CdZnS、CdSeS、CdS、ZnSe、InP、InS、CdTe、CuInS 2、CuInZnS、ZnS、PbS、PbSe、AgInS 2、Ag 2Te、InAs、Cd 3As 2、AgBiS 2、 InAs/InP、InGaP或其組合。在一些實施方式中,鈣鈦礦具有以下通式:ABX 3,其中A為有機陽離子,B為金屬陽離子,X為鹵素陰離子。在一些實施方式中,鈣鈦礦包括CH 3NH 3PbI 3、CH 3NH 3PbBr 3、(MeNH 3)PbBr 3、Cs 2Sn 3I 6、 Ag 3BiI 6、(CH 3NH 3) 3Bi 2Cl 9、Cs 2SnI 5Br、Cs 2TiBr 6或其組合。在一些實施方式中,有機半導體包括一或多個P型有機半導體及一或多個N型有機半導體。P型有機半導體可為共軛高分子,N型有機半導體可為非富勒烯材料或富勒烯材料。舉例來說,P型有機半導體包括: 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 或其組合。在上述的P型有機半導體中,n1至n41各自獨立為1~1000的正整數。a5至a20、a22、a23、a25、a28至a34、b5至b20、b22、b23、b25、b28至b34、c35至c37、d35至d37及e35至d37各自代表莫耳分率,且各自大於0且小於1。在各個P型有機半導體中,所有的莫耳分率的總合為1。舉例來說,N型有機半導體包括: (R為 )、 、 、 、 、 、 、 、 、 、 、 (R為乙基己基)、 (R為乙基己基)、 、 、 (R為己基癸基)、 ( R為己基癸基)、 (R為癸基四癸基)、 、 、 (R為 )、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 (R為 )、 、 、 、 或其組合。 In some embodiments, the photoelectric conversion layer 140 includes organic semiconductors, inorganic semiconductors, quantum dots, perovskite, or combinations thereof . In some embodiments, the quantum dots include CdSe, CdZnS, CdSeS, CdS, ZnSe, InP, InS, CdTe , CuInS₂, CuInZnS, ZnS, PbS, PbSe, AgInS₂ , Ag₂Te , InAs, Cd₃As₂ , AgBiS₂ , InAs/InP, InGaP, or combinations thereof. In some embodiments, perovskite has the following general formula: ABX₃ , where A is an organic cation, B is a metallic cation, and X is a halogen anion. In some embodiments, the perovskite includes CH3NH3PbI3 , CH3NH3PbBr3 , ( MeNH3 ) PbBr3 , Cs2Sn3I6 , Ag3BiI6 , ( CH3NH3 ) 3Bi2Cl9 , Cs2SnI5Br , Cs2TiBr6 , or combinations thereof . In some embodiments, the organic semiconductor includes one or more p-type organic semiconductors and one or more n -type organic semiconductors. The p - type organic semiconductors may be conjugated polymers, and the n-type organic semiconductors may be non-fullerene materials or fullerene materials. For example, p-type organic semiconductors include: , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , Or combinations thereof. In the above-described P-type organic semiconductors, n1 to n41 are each independently a positive integer from 1 to 1000. a5 to a20, a22, a23, a25, a28 to a34, b5 to b20, b22, b23, b25, b28 to b34, c35 to c37, d35 to d37, and e35 to d37 each represent a mole fraction, and each is greater than 0 and less than 1. In each P-type organic semiconductor, the sum of all mole fractions is 1. For example, N-type organic semiconductors include: (R is) ), , , , , , , , , , , (R stands for ethylhexyl) (R stands for ethylhexyl) , , (R represents hexyldecyl) (R represents hexyldecyl) (R represents decyl tetradecyl) , , (R is) ), , , , , , , , , , , , , , , , , , , , (R is) ), , , , Or a combination thereof.
在一些實施方式中,第二反射層160為透光導電層。在一些實施方式中,第二反射層160的厚度T5為90 nm至200 nm,例如90、100、120、140、160、180或200 nm,當厚度T5落於上述範圍內,光電元件模組100仍能夠接收充足的光線以用於光電轉換。在一些實施方式中,第二反射層160包括透明導電氧化物、透明導電高分子、奈米銀線、厚度小於或等於15 nm的含金屬層或其組合。TCO包括氧化銦鋅(indium zinc oxide, IZO)、氧化銦鎵(indium gallium oxide, IGO)、氧化銦鎵鋅(indium gallium zinc oxide, IGZO)、氧化銦錫鋅(indium tin zinc oxide, ITZO)、氧化銦錫(indium tin oxide, ITO)、氧化鋅錫 (zinc tin oxide, ZTO)、氧化鋁鋅(aluminum zinc oxide, AZO)或其組合。透明導電高分子包括聚(3,4-乙烯二氧噻吩):聚苯乙烯磺酸(poly(3,4-ethylenedioxythiophene) polystyrene sulfonate, PEDOT:PSS)、聚苯胺、聚芴、聚吡咯、聚噻吩、聚咔唑或其組合。含金屬層可包括厚度小於或等於15 nm的金屬層,例如銀層、金層、鋁層、銅層或其組合。In some embodiments, the second reflective layer 160 is a light-transmitting conductive layer. In some embodiments, the thickness T5 of the second reflective layer 160 is 90 nm to 200 nm, for example, 90, 100, 120, 140, 160, 180, or 200 nm. When the thickness T5 falls within the above range, the optoelectronic element module 100 can still receive sufficient light for photoelectric conversion. In some embodiments, the second reflective layer 160 includes a transparent conductive oxide, a transparent conductive polymer, nano-silver wires, a metal-containing layer with a thickness of less than or equal to 15 nm, or a combination thereof. TCOs include indium zinc oxide (IZO), indium gallium oxide (IGO), indium gallium zinc oxide (IGZO), indium tin zinc oxide (ITZO), indium tin oxide (ITO), zinc tin oxide (ZTO), aluminum zinc oxide (AZO), or combinations thereof. Transparent conductive polymers include poly(3,4-ethylenedioxythiophene): poly(3,4-ethylenedioxythiophene) polystyrene sulfonate (PEDOT:PSS), polyaniline, polyfluorene, polypyrrole, polythiophene, polycarbazole, or combinations thereof. The metal layer may include a metal layer with a thickness of less than or equal to 15 nm, such as a silver layer, a gold layer, an aluminum layer, a copper layer, or a combination thereof.
下文將參照實施例,更具體地描述本揭示內容的特徵。雖然描述了以下實施例,但是在不逾越本揭示內容範疇之情況下,可適當地改變所用材料、其量及比率、處理細節以及處理流程等等。因此,不應由下文所述之實施例對本揭示內容作出限制性地解釋。The features of this disclosure will be described more specifically below with reference to embodiments. Although the following embodiments are described, the materials used, their quantities and ratios, processing details, and processing procedures may be appropriately varied without departing from the scope of this disclosure. Therefore, this disclosure should not be interpreted restrictively based on the embodiments described below.
第2圖是實施例1~23的光電元件模組200的剖面示意圖。如第2圖所示,光電元件模組200包括由下往上堆疊的玻璃基板210、Ag層220、ZnO層230、光電轉換層240、MoO 3層250及IZO層260。光電元件模組200為頂部照光式的(top-illuminated),故從光電元件模組200上方施加光線L2進行測量,測量結果請參第4圖至第8圖。第4圖、第5圖、第6圖、第7圖及第8圖分別是實施例1~7、實施例8~10、實施例11~16、實施例17~19及實施例20~23的光電元件模組200的外部量子效率-波長關係圖。外部量子效率是在-4V量測而得。值得注意的是,光電元件模組200具有共振腔,亦即Ag層220的上表面與IZO層260的下表面之間的空間,因此,光線L2會在Ag層220與IZO層260之間反射。更詳細來說,光線L2在進入光電元件模組200後,會被Ag層220反射,再次通過ZnO層230、光電轉換層240及MoO 3層250,且再被IZO層260反射,從而提升光電轉換層240的吸光量。 Figure 2 is a cross-sectional schematic diagram of the optoelectronic component module 200 of Embodiments 1-23. As shown in Figure 2, the optoelectronic component module 200 includes a glass substrate 210, an Ag layer 220, a ZnO layer 230, a photoelectric conversion layer 240, a MoO3 layer 250, and an IZO layer 260 stacked from bottom to top. The optoelectronic component module 200 is top-illuminated, so light L2 is applied from above the optoelectronic component module 200 for measurement. The measurement results are shown in Figures 4 to 8. Figures 4, 5, 6, 7, and 8 are the external quantum efficiency-wavelength relationship diagrams of the optoelectronic element module 200 in Examples 1-7, 8-10, 11-16, 17-19, and 20-23, respectively. The external quantum efficiency was measured at -4V. It is worth noting that the optoelectronic element module 200 has a resonant cavity, that is, the space between the upper surface of the Ag layer 220 and the lower surface of the IZO layer 260. Therefore, light L2 will be reflected between the Ag layer 220 and the IZO layer 260. More specifically, after light L2 enters the optoelectronic module 200, it is reflected by the Ag layer 220, passes through the ZnO layer 230, the photoelectric conversion layer 240 and the MoO3 layer 250 again, and is reflected by the IZO layer 260, thereby increasing the light absorption of the photoelectric conversion layer 240.
實施例1~19的光電轉換層240包括可對於SWIR光產生響應的P型有機半導體及N型有機半導體,第3圖示出P型有機半導體的吸收光譜300P及N型有機半導體的吸收光譜300N,其中P型有機半導體的最高占據分子軌域(highest occupied molecular orbital, HOMO)的能量為-4.91 eV,最低未占分子軌域(lowest unoccupied molecular orbital, LUMO)的能量為-4.16 eV,N型有機半導體的HOMO的能量為-5.73 eV,LUMO的能量為-4.42 eV。實施例1~19的光電元件模組200的製造方法包括以下操作:將莫耳比為1:2的P型有機半導體及N型有機半導體溶解於溶劑鄰二甲苯中,以得到固含量為30 mg/mL的混合液,將混合液旋轉塗佈在ZnO層230上,在100 oC下退火5分鐘,以形成光電轉換層240,接著依序沉積MoO 3層250及IZO層260。 The photoelectric conversion layer 240 in embodiments 1-19 includes a P-type organic semiconductor and an N-type organic semiconductor that can respond to SWIR light. Figure 3 shows the absorption spectrum 300P of the P-type organic semiconductor and the absorption spectrum 300N of the N-type organic semiconductor. The energy of the highest occupied molecular orbital (HOMO) of the P-type organic semiconductor is -4.91 eV, and the energy of the lowest unoccupied molecular orbital (LUMO) is -4.16 eV. The energy of the HOMO of the N-type organic semiconductor is -5.73 eV, and the energy of the LUMO is -4.42 eV. The manufacturing method of the optoelectronic component module 200 in Examples 1-19 includes the following operations: dissolving a P-type organic semiconductor and an N-type organic semiconductor with a molar ratio of 1:2 in the solvent o-xylene to obtain a mixture with a solid content of 30 mg/mL, rotating the mixture onto a ZnO layer 230, annealing it at 100 ° C for 5 minutes to form a photoelectric conversion layer 240, and then sequentially depositing a MoO3 layer 250 and an IZO layer 260.
實施例20~23的光電轉換層240包括可對於SWIR光產生響應的P型有機半導體及N型有機半導體,其分別為 及 。實施例20~23的光電元件模組200的製造方法包括以下操作:將莫耳比為1:0.75的P型有機半導體及N型有機半導體溶解於溶劑氯仿中,以得到固含量為21 mg/mL的混合液,將混合液旋轉塗佈在ZnO層230上,在100 oC下退火5分鐘,以形成光電轉換層240,接著依序沉積MoO 3層250及IZO層260。 The photoelectric conversion layer 240 in embodiments 20-23 includes a P-type organic semiconductor and an N-type organic semiconductor that can respond to SWIR light, which are respectively... and The manufacturing method of the optoelectronic component module 200 in embodiments 20-23 includes the following operations: dissolving a P-type organic semiconductor and an N-type organic semiconductor with a molar ratio of 1:0.75 in chloroform solvent to obtain a mixture with a solid content of 21 mg/mL; rotating the mixture onto a ZnO layer 230; annealing at 100 ° C for 5 minutes to form a photoelectric conversion layer 240; and then sequentially depositing a MoO3 layer 250 and an IZO layer 260.
實施例1~23的光電元件模組200的結構參數及EQE測試結果請參以下表1。
表1
第9圖是比較例1~8的光電元件模組900的剖面示意圖。如第9圖所示,光電元件模組900包括由下往上堆疊的玻璃基板910、ITO層920、ZnO層930、光電轉換層940、MoO
3層950及IZO層960。光電元件模組900為頂部照光式的,不具有共振腔。比較例1~4的光電轉換層940與實施例1~19的光電轉換層240相同,故第3圖亦是比較例1~4的光電轉換層940的P型有機半導體的吸收光譜300P及N型有機半導體的吸收光譜300N。比較例5~8的光電轉換層940與實施例20~23的光電轉換層240相同。從光電元件模組900上方施加光線L3進行測量,測量結果請參第10圖及第11圖。第10圖及第11圖分別是比較例1~4及比較例5~8的光電元件模組900的外部量子效率-波長關係圖。外部量子效率是在-4V量測而得。比較例1~8的光電元件模組900的結構參數及EQE測試結果請參以下表2。
表2
請參照表1的實施例1~7、第2圖及第4圖,第4圖是實施例1~7的光電元件模組200的外部量子效率-波長關係圖。實施例1~7的光電元件模組200具有共振腔,由實施例1的曲線E1、實施例2的曲線E2、實施例3的曲線E3、實施例4的曲線E4、實施例5的曲線E5、實施例6的曲線E6及實施例7的曲線E7可知,隨著光電轉換層240的厚度增加,由於吸光量提升故EQE也隨之提升,並且,不同曲線的最大波長具紅移現象。當光電轉換層240的厚度大於303 nm,仍會發生紅移現象,這意味著共振腔效應仍會影響光電元件模組200,但EQE略為下降,顯示EQE會受到光電轉換層240的載子傳遞能力的影響。請進一步參照表2的比較例1~4、第9圖及第10圖,第10圖是比較例1~4的光電元件模組900的外部量子效率-波長關係圖。由比較例1的曲線CE1、比較例2的曲線CE2、比較例3的曲線CE3及比較例4的曲線CE4可知,比較例1~4的光電元件模組900不具有共振腔,故無法在SWIR波段展現有效EQE,並且,縱使調整光電轉換層940的厚度,也無法有效提升EQE。Please refer to Embodiments 1-7 in Table 1, Figure 2 and Figure 4. Figure 4 is a graph showing the external quantum efficiency-wavelength relationship of the photoelectric element module 200 in Embodiments 1-7. The photoelectric element module 200 in Embodiments 1-7 has a resonant cavity. As can be seen from curve E1 in Embodiment 1, curve E2 in Embodiment 2, curve E3 in Embodiment 3, curve E4 in Embodiment 4, curve E5 in Embodiment 5, curve E6 in Embodiment 6 and curve E7 in Embodiment 7, as the thickness of the photoelectric conversion layer 240 increases, the EQE also increases due to the increase in light absorption. Furthermore, the maximum wavelength of different curves exhibits a redshift phenomenon. When the thickness of the photoelectric conversion layer 240 is greater than 303 nm, a redshift still occurs, which means that the resonant cavity effect still affects the photoelectric element module 200, but the EQE decreases slightly, indicating that the EQE is affected by the carrier transport capability of the photoelectric conversion layer 240. Please refer further to Comparative Examples 1-4, Figure 9 and Figure 10 in Table 2. Figure 10 is the external quantum efficiency-wavelength relationship of the photoelectric element module 900 of Comparative Examples 1-4. As can be seen from curve CE1 of Comparative Example 1, curve CE2 of Comparative Example 2, curve CE3 of Comparative Example 3 and curve CE4 of Comparative Example 4, the optoelectronic element module 900 of Comparative Examples 1 to 4 does not have a resonant cavity, so it cannot exhibit effective EQE in the SWIR band. Furthermore, even if the thickness of the optoelectronic conversion layer 940 is adjusted, the EQE cannot be effectively improved.
請參照表1的實施例8~10、第2圖及第5圖。由實施例8的曲線E8、實施例9的曲線E9及實施例10的曲線E10可知,當ZnO層230的厚度增加時,光電元件模組200的EQE也會隨之提升。ZnO層230具備電子傳輸能力,並可作為光學間隙子,以適當調整光場並有效地分配光子至光電轉換層240內,從而提升光電元件模組200的EQE。Please refer to Examples 8-10 in Table 1, Figure 2, and Figure 5. As can be seen from curve E8 of Example 8, curve E9 of Example 9, and curve E10 of Example 10, the EQE of the optoelectronic module 200 increases as the thickness of the ZnO layer 230 increases. The ZnO layer 230 has electron transmission capability and can act as an optical gap to properly adjust the optical field and effectively distribute photons into the photoelectric conversion layer 240, thereby improving the EQE of the optoelectronic module 200.
請參照表1的實施例11~19、第2圖、第6圖及第7圖。在固定Ag層220的厚度的情況下,調整ZnO層230、光電轉換層240、MoO 3層250及IZO層260的厚度,以調整共振腔的厚度,從而優化光電元件模組200的EQE。第6圖示出實施例11的曲線E11、實施例12的曲線E12、實施例13的曲線E13、實施例14的曲線E14、實施例15的曲線E15及實施例16的曲線E16,第7圖示出實施例17的曲線E17、實施例18的曲線E18及實施例19的曲線E19。如實施例12所示,在波長為1300 nm 的光線照射下,光電元件模組200可具有高達27.6%的EQE。 Please refer to Examples 11-19 in Table 1, Figure 2, Figure 6, and Figure 7. With the Ag layer 220 thickness fixed, the thicknesses of the ZnO layer 230, photoelectric conversion layer 240, MoO3 layer 250, and IZO layer 260 are adjusted to adjust the thickness of the resonant cavity, thereby optimizing the EQE of the optoelectronic device module 200. Figure 6 shows curve E11 of Example 11, curve E12 of Example 12, curve E13 of Example 13, curve E14 of Example 14, curve E15 of Example 15, and curve E16 of Example 16. Figure 7 shows curve E17 of Example 17, curve E18 of Example 18, and curve E19 of Example 19. As shown in Example 12, under illumination with light of wavelength 1300 nm, the optoelectronic module 200 can have an EQE of up to 27.6%.
請參照表1的實施例20~23、第2圖及第8圖,第8圖是實施例20~23的光電元件模組200的外部量子效率-波長關係圖。實施例20~23的光電元件模組200具有共振腔,由實施例20的曲線E20、實施例21的曲線E21、實施例22的曲線E22及實施例23的曲線E23可知,隨著光電轉換層240的厚度增加,不同曲線的最大波長具紅移現象,並且,可藉由調整光電轉換層240的厚度,進一步優化EQE。請進一步參照表2的比較例5~8、第9圖及第11圖,第11圖是比較例5~8的光電元件模組900的外部量子效率-波長關係圖。由比較例5的曲線CE5、比較例6的曲線CE6、比較例7的曲線CE7及比較例8的曲線CE8可知,比較例5~8的光電元件模組900不具有共振腔,故無法在SWIR波段展現有效EQE,縱使調整光電轉換層940的厚度,也無法提升EQE。Please refer to Examples 20-23, Figure 2, and Figure 8 in Table 1. Figure 8 is a graph showing the external quantum efficiency-wavelength relationship of the optoelectronic module 200 in Examples 20-23. The optoelectronic module 200 in Examples 20-23 has a resonant cavity. As can be seen from curve E20 in Example 20, curve E21 in Example 21, curve E22 in Example 22, and curve E23 in Example 23, as the thickness of the photoelectric conversion layer 240 increases, the maximum wavelength of different curves exhibits a redshift phenomenon. Furthermore, the EQE can be further optimized by adjusting the thickness of the photoelectric conversion layer 240. Please further refer to Comparative Examples 5-8, Figure 9, and Figure 11 in Table 2. Figure 11 is a graph showing the external quantum efficiency-wavelength relationship of the optoelectronic module 900 in Comparative Examples 5-8. As can be seen from curve CE5 of Comparative Example 5, curve CE6 of Comparative Example 6, curve CE7 of Comparative Example 7 and curve CE8 of Comparative Example 8, the optoelectronic module 900 of Comparative Examples 5 to 8 does not have a resonant cavity, so it cannot exhibit effective EQE in the SWIR band. Even if the thickness of the optoelectronic conversion layer 940 is adjusted, the EQE cannot be improved.
綜上所述,本揭示內容提供一種光電元件模組及其操作方法。光電元件模組包括依序由下往上堆疊的基板、第一反射層、光電轉換層及第二反射層,並可接收來自上方的光線。由於第一反射層的第一反射率大於第二反射層的第二反射率,光線容易被第一反射層反射而再次進入光電轉換層內,從而提升光電轉換層的吸光量,藉此提升光電元件模組的外部量子效率(EQE) 及光電流。In summary, this disclosure provides an optoelectronic device module and its operation method. The optoelectronic device module includes a substrate, a first reflective layer, a photoelectric conversion layer, and a second reflective layer stacked sequentially from bottom to top, and can receive light from above. Since the first reflectivity of the first reflective layer is greater than the second reflectivity of the second reflective layer, light is easily reflected by the first reflective layer and re-enters the photoelectric conversion layer, thereby increasing the light absorption of the photoelectric conversion layer, thereby improving the external quantum efficiency (EQE) and photocurrent of the optoelectronic device module.
儘管已經參考某些實施方式相當詳細地描述了本揭示內容,但是亦可能有其他實施方式。因此,所附申請專利範圍的精神和範圍不應限於此處包含的實施方式的描述。Although this disclosure has been described in considerable detail with reference to certain embodiments, other embodiments may also exist. Therefore, the spirit and scope of the appended patent application should not be limited to the description of the embodiments contained herein.
對於所屬技術領域具有通常知識者來說,顯而易見的是,在不脫離本揭示內容的範圍或精神的情況下,可以對本揭示內容的結構進行各種修改和變化。鑑於前述內容,本揭示內容意圖涵蓋落入所附申請專利範圍內的本揭示內容的修改和變化。It will be apparent to those skilled in the art that various modifications and changes can be made to the structure of this disclosure without departing from the scope or spirit of this disclosure. In view of the foregoing, this disclosure is intended to cover modifications and changes to this disclosure that fall within the scope of the appended patent applications.
100、200、900 : 光電元件模組 110 : 基板 120 : 第一反射層 130 : 第一載子傳輸層 140 : 光電轉換層 150 : 第二載子傳輸層 160 : 第二反射層 210、910 : 玻璃基板 220 : Ag層 230、930 : ZnO層 240、940 : 光電轉換層 250、950 : MoO 3層 260、960 : IZO層 300N、300P : 吸收光譜 920 : ITO層 CE1、CE2、CE3、CE4、CE5、CE6、CE7、CE8、E1、E2、E3、E4、E5、E6、E7、E8、E9、E10、E11、E12、E13、E14、E15、E16、E17、E18、E19、E20、E21、E22、E23 : 曲線 L1、L2、L3 : 光線 T1、T2、T3、T4、T5 : 厚度 100, 200, 900: Optoelectronic component module; 110: Substrate; 120: First reflective layer; 130: First carrier transport layer; 140: Photoelectric conversion layer; 150: Second carrier transport layer; 160: Second reflective layer; 210, 910: Glass substrate; 220: Ag layer; 230, 930: ZnO layer; 240, 940: Photoelectric conversion layer; 250, 950: MoO3 layer; 260, 960: IZO layer; 300N, 300P: Absorption spectrum; 920: ITO layer CE1, CE2, CE3, CE4, CE5, CE6, CE7, CE8, E1, E2, E3, E4, E5, E6, E7, E8, E9, E10, E11, E12, E13, E14, E15, E16, E17, E18, E19, E20, E21, E22, E23: Curves L1, L2, L3: Rays T1, T2, T3, T4, T5: Thickness
藉由閱讀以下實施方式的詳細描述,並參照附圖,可以更全面地理解本揭示內容。 第1圖是根據本揭示內容各種實施方式的光電元件模組的剖面示意圖。 第2圖是實施例1~23的光電元件模組的剖面示意圖。 第3圖示出實施例1~19及比較例1~4的光電轉換層的P型有機半導體及N型有機半導體的吸收光譜。 第4圖、第5圖、第6圖、第7圖及第8圖分別是實施例1~7、實施例8~10、實施例11~16、實施例17~19及實施例20~23的光電元件模組的外部量子效率-波長關係圖。 第9圖是比較例1~8的光電元件模組的剖面示意圖。 第10圖及第11圖分別是比較例1~4及比較例5~8的光電元件模組的外部量子效率-波長關係圖。 A more comprehensive understanding of this disclosure can be achieved by reading the detailed description of the following embodiments and referring to the accompanying figures. Figure 1 is a schematic cross-sectional view of the optoelectronic device modules according to various embodiments of this disclosure. Figure 2 is a schematic cross-sectional view of the optoelectronic device modules of Embodiments 1-23. Figure 3 shows the absorption spectra of the P-type and N-type organic semiconductors of the photoelectric conversion layers in Embodiments 1-19 and Comparative Examples 1-4. Figures 4, 5, 6, 7, and 8 are respectively external quantum efficiency-wavelength relationships for the optoelectronic device modules of Embodiments 1-7, 8-10, 11-16, 17-19, and 20-23. Figure 9 is a schematic cross-sectional view of the optoelectronic module of Comparative Examples 1-8. Figures 10 and 11 are external quantum efficiency-wavelength relationships for the optoelectronic modules of Comparative Examples 1-4 and Comparative Examples 5-8, respectively.
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100 : 光電元件模組 110 : 基板 120 : 第一反射層 130 : 第一載子傳輸層 140 : 光電轉換層 150 : 第二載子傳輸層 160 : 第二反射層 L1 : 光線 T1、T2、T3、T4、T5 : 厚度 100: Optoelectronic component module 110: Substrate 120: First reflective layer 130: First carrier transport layer 140: Optoelectronic conversion layer 150: Second carrier transport layer 160: Second reflective layer L1: Light ray T1, T2, T3, T4, T5: Thickness
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