Santu Mazumder, Supriya Borgohain, Senthilkumar Kasilingam
{"title":"Simulation Study for Nb-Doped MoS2 Layer in CZTS-Based Solar Cells: Assessment of Challenges","authors":"Santu Mazumder, Supriya Borgohain, Senthilkumar Kasilingam","doi":"10.1002/adts.202400396","DOIUrl":null,"url":null,"abstract":"The unintentional formation of a <span data-altimg=\"/cms/asset/d4c0d7ae-095a-4b03-b08e-aaeafd92cb58/adts202400396-math-0002.png\"></span><mjx-container ctxtmenu_counter=\"19\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" data-semantic- data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\"></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math data-semantic-=\"\" data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\" xmlns=\"http://www.w3.org/1998/Math/MathML\"></math></mjx-assistive-mml></mjx-container> layer as a reaction product between the copper zinc tin sulfide (CZTS) thin film and the Mo back contact reduces cell efficiency due to high sheet resistance and carrier recombination. To limit the formation of <span data-altimg=\"/cms/asset/ff67218d-9f31-4fd0-9977-2b682bec2f73/adts202400396-math-0003.png\"></span><mjx-container ctxtmenu_counter=\"20\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" data-semantic- data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\"></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math data-semantic-=\"\" data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\" xmlns=\"http://www.w3.org/1998/Math/MathML\"></math></mjx-assistive-mml></mjx-container>, an intentionally grown p-type Nb-doped <span data-altimg=\"/cms/asset/291dfbdb-c247-41df-92fa-9c2d5140226c/adts202400396-math-0004.png\"></span><mjx-container ctxtmenu_counter=\"21\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" data-semantic- data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\"></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math data-semantic-=\"\" data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\" xmlns=\"http://www.w3.org/1998/Math/MathML\"></math></mjx-assistive-mml></mjx-container> layer can serve as an effective hole transport layer. This study presents a detailed study and calculations for CZTS/Mo-based solar cells, providing guidelines for calibration. Optimizing cell efficiency is influenced by various interconnected factors in Nb-doped <span data-altimg=\"/cms/asset/3d55f8dc-8318-42d1-81fe-da79ba6aade8/adts202400396-math-0005.png\"></span><mjx-container ctxtmenu_counter=\"22\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" data-semantic- data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\"></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math data-semantic-=\"\" data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\" xmlns=\"http://www.w3.org/1998/Math/MathML\"></math></mjx-assistive-mml></mjx-container>. While a high carrier concentration in Nb-doped <span data-altimg=\"/cms/asset/8b1fba9c-cb00-474a-888c-8a4ecd6d47ea/adts202400396-math-0006.png\"></span><mjx-container ctxtmenu_counter=\"23\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" data-semantic- data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\"></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math data-semantic-=\"\" data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\" xmlns=\"http://www.w3.org/1998/Math/MathML\"></math></mjx-assistive-mml></mjx-container> is assumed to enhance efficiency, other parameters such as band state, optical absorption, and carrier mobility also play crucial roles and can limit cell performance. This simulation study evaluated the effect of Nb-doped <span data-altimg=\"/cms/asset/a6565481-0910-4a5c-bfb3-bb8dfc127368/adts202400396-math-0007.png\"></span><mjx-container ctxtmenu_counter=\"24\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" data-semantic- data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\"></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math data-semantic-=\"\" data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\" xmlns=\"http://www.w3.org/1998/Math/MathML\"></math></mjx-assistive-mml></mjx-container> layers with different carrier concentrations to determine the optimal conditions for this p-type layer. This work reveals that a very thin layer (13 nm) of Nb-doped p-type <span data-altimg=\"/cms/asset/4f75109e-dedb-4447-9fcb-aae6dbae4960/adts202400396-math-0008.png\"></span><mjx-container ctxtmenu_counter=\"25\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" data-semantic- data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\"></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math data-semantic-=\"\" data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\" xmlns=\"http://www.w3.org/1998/Math/MathML\"></math></mjx-assistive-mml></mjx-container> can achieve a maximum efficiency of 11.34% (with <span data-altimg=\"/cms/asset/14b60358-22b1-4acb-8f86-7ae21557b365/adts202400396-math-0009.png\"></span><mjx-container ctxtmenu_counter=\"26\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" data-semantic- data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\"></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math data-semantic-=\"\" data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\" xmlns=\"http://www.w3.org/1998/Math/MathML\"></math></mjx-assistive-mml></mjx-container> = 1.5<span data-altimg=\"/cms/asset/e0ae198f-be97-4049-8924-418fe739db85/adts202400396-math-0010.png\"></span><mjx-container ctxtmenu_counter=\"27\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" data-semantic- data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\"></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math data-semantic-=\"\" data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\" xmlns=\"http://www.w3.org/1998/Math/MathML\"></math></mjx-assistive-mml></mjx-container> <span data-altimg=\"/cms/asset/b7130127-164a-4f53-b754-970e94fe8808/adts202400396-math-0011.png\"></span><mjx-container ctxtmenu_counter=\"28\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" data-semantic- data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\"></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math data-semantic-=\"\" data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\" xmlns=\"http://www.w3.org/1998/Math/MathML\"></math></mjx-assistive-mml></mjx-container>) and that for an Nb-doped p-type 62 nm <span data-altimg=\"/cms/asset/82a6a111-3f87-4aeb-8718-f69f6a4a161c/adts202400396-math-0012.png\"></span><mjx-container ctxtmenu_counter=\"29\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" data-semantic- data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\"></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math data-semantic-=\"\" data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\" xmlns=\"http://www.w3.org/1998/Math/MathML\"></math></mjx-assistive-mml></mjx-container> is 15.82 % (with <span data-altimg=\"/cms/asset/411671b3-db78-43c4-ab50-a10b1640253c/adts202400396-math-0013.png\"></span><mjx-container ctxtmenu_counter=\"30\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" data-semantic- data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\"></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math data-semantic-=\"\" data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\" xmlns=\"http://www.w3.org/1998/Math/MathML\"></math></mjx-assistive-mml></mjx-container> = 4.03<span data-altimg=\"/cms/asset/269a155e-077b-4b26-9f30-67a0e7c83122/adts202400396-math-0014.png\"></span><mjx-container ctxtmenu_counter=\"31\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" data-semantic- data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\"></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math data-semantic-=\"\" data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\" xmlns=\"http://www.w3.org/1998/Math/MathML\"></math></mjx-assistive-mml></mjx-container> <span data-altimg=\"/cms/asset/d1bcd413-9819-467e-8d0c-79a01c551a70/adts202400396-math-0015.png\"></span><mjx-container ctxtmenu_counter=\"32\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" data-semantic- data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\"></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math data-semantic-=\"\" data-semantic-role=\"unknown\" data-semantic-speech=\"\" data-semantic-type=\"empty\" xmlns=\"http://www.w3.org/1998/Math/MathML\"></math></mjx-assistive-mml></mjx-container>).","PeriodicalId":7219,"journal":{"name":"Advanced Theory and Simulations","volume":"3 1","pages":""},"PeriodicalIF":2.9000,"publicationDate":"2024-08-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Advanced Theory and Simulations","FirstCategoryId":"5","ListUrlMain":"https://doi.org/10.1002/adts.202400396","RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"MULTIDISCIPLINARY SCIENCES","Score":null,"Total":0}
引用次数: 0
Abstract
The unintentional formation of a layer as a reaction product between the copper zinc tin sulfide (CZTS) thin film and the Mo back contact reduces cell efficiency due to high sheet resistance and carrier recombination. To limit the formation of , an intentionally grown p-type Nb-doped layer can serve as an effective hole transport layer. This study presents a detailed study and calculations for CZTS/Mo-based solar cells, providing guidelines for calibration. Optimizing cell efficiency is influenced by various interconnected factors in Nb-doped . While a high carrier concentration in Nb-doped is assumed to enhance efficiency, other parameters such as band state, optical absorption, and carrier mobility also play crucial roles and can limit cell performance. This simulation study evaluated the effect of Nb-doped layers with different carrier concentrations to determine the optimal conditions for this p-type layer. This work reveals that a very thin layer (13 nm) of Nb-doped p-type can achieve a maximum efficiency of 11.34% (with = 1.5) and that for an Nb-doped p-type 62 nm is 15.82 % (with = 4.03).
在铜锌锡硫化物(CZTS)薄膜和钼背触点之间无意形成的反应产物层,会因高片电阻和载流子重组而降低电池效率。为了限制掺杂 p 型铌层的形成,有意生长的 p 型铌层可以作为有效的空穴传输层。本研究对基于 CZTS/Mo 的太阳能电池进行了详细的研究和计算,为校准提供了指导。优化电池效率受到掺铌太阳能电池中各种相互关联因素的影响。虽然掺铌中的高载流子浓度被认为能提高效率,但带态、光吸收和载流子迁移率等其他参数也起着至关重要的作用,并可能限制电池的性能。这项模拟研究评估了不同载流子浓度的掺铌层的效果,以确定这种 p 型层的最佳条件。研究结果表明,掺铌 p 型极薄层(13 纳米)的最高效率可达 11.34%(含 = 1.5),而 62 纳米掺铌 p 型层的最高效率为 15.82%(含 = 4.03)。
期刊介绍:
Advanced Theory and Simulations is an interdisciplinary, international, English-language journal that publishes high-quality scientific results focusing on the development and application of theoretical methods, modeling and simulation approaches in all natural science and medicine areas, including:
materials, chemistry, condensed matter physics
engineering, energy
life science, biology, medicine
atmospheric/environmental science, climate science
planetary science, astronomy, cosmology
method development, numerical methods, statistics