Effect of Low-Concentration Rb<sup>+</sup> Mixing on Semiconductor Majority Charge Carriers Type of Perovskite Light-Absorption Layer by Using Two-Step Spin-Coating Method
In recent years, perovskite materials have been the subject of great progress in optoelectronic devices. The perovskite layer is the light absorption layer of perovskite solar cells (PSCs), and the majority charge carriers type play a crucial role in the formation of a P–N junction. In this paper, t...
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MDPI AG
2020-06-01
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Online Access: | https://www.mdpi.com/2079-6412/10/7/627 |
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Article |
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DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Baoyu Liu Xiaoping Zou Jin Cheng Tao Ling Yujun Yao Dan Chen Chuangchuang Chang Xing Yu Junqi Wang Zixiao Zhou Guangdong Li |
spellingShingle |
Baoyu Liu Xiaoping Zou Jin Cheng Tao Ling Yujun Yao Dan Chen Chuangchuang Chang Xing Yu Junqi Wang Zixiao Zhou Guangdong Li Effect of Low-Concentration Rb<sup>+</sup> Mixing on Semiconductor Majority Charge Carriers Type of Perovskite Light-Absorption Layer by Using Two-Step Spin-Coating Method Coatings low concentrations Rb mixing majority charge carriers type two-step |
author_facet |
Baoyu Liu Xiaoping Zou Jin Cheng Tao Ling Yujun Yao Dan Chen Chuangchuang Chang Xing Yu Junqi Wang Zixiao Zhou Guangdong Li |
author_sort |
Baoyu Liu |
title |
Effect of Low-Concentration Rb<sup>+</sup> Mixing on Semiconductor Majority Charge Carriers Type of Perovskite Light-Absorption Layer by Using Two-Step Spin-Coating Method |
title_short |
Effect of Low-Concentration Rb<sup>+</sup> Mixing on Semiconductor Majority Charge Carriers Type of Perovskite Light-Absorption Layer by Using Two-Step Spin-Coating Method |
title_full |
Effect of Low-Concentration Rb<sup>+</sup> Mixing on Semiconductor Majority Charge Carriers Type of Perovskite Light-Absorption Layer by Using Two-Step Spin-Coating Method |
title_fullStr |
Effect of Low-Concentration Rb<sup>+</sup> Mixing on Semiconductor Majority Charge Carriers Type of Perovskite Light-Absorption Layer by Using Two-Step Spin-Coating Method |
title_full_unstemmed |
Effect of Low-Concentration Rb<sup>+</sup> Mixing on Semiconductor Majority Charge Carriers Type of Perovskite Light-Absorption Layer by Using Two-Step Spin-Coating Method |
title_sort |
effect of low-concentration rb<sup>+</sup> mixing on semiconductor majority charge carriers type of perovskite light-absorption layer by using two-step spin-coating method |
publisher |
MDPI AG |
series |
Coatings |
issn |
2079-6412 |
publishDate |
2020-06-01 |
description |
In recent years, perovskite materials have been the subject of great progress in optoelectronic devices. The perovskite layer is the light absorption layer of perovskite solar cells (PSCs), and the majority charge carriers type play a crucial role in the formation of a P–N junction. In this paper, the light absorption layer of PSCs was Rb-mixed at a low concentrations by using a two-step spin-coating method, which could adjust the majority charge carriers type in perovskite films from N-type to P-type, and it has little influence on the crystal structure and light absorption capacity of perovskite. In addition, low concentration Rb-mixing is different from high concentration Rb-mixing. With increasing Rb-mixing concentration, the perovskite grains does not change shape. Although the quality of perovskite films deteriorated and the PL peaks exhibit a slight blue shift after mixing, the efficiency only slightly decreased, indicating that the new P-N hetero-junction was still formed after mixing, which provided a new idea for the future research of homo-junction PSCs. |
topic |
low concentrations Rb mixing majority charge carriers type two-step |
url |
https://www.mdpi.com/2079-6412/10/7/627 |
work_keys_str_mv |
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spelling |
doaj-0a1329ad95704a4795ed3c01aa86e2e62020-11-25T03:53:24ZengMDPI AGCoatings2079-64122020-06-011062762710.3390/coatings10070627Effect of Low-Concentration Rb<sup>+</sup> Mixing on Semiconductor Majority Charge Carriers Type of Perovskite Light-Absorption Layer by Using Two-Step Spin-Coating MethodBaoyu Liu0Xiaoping Zou1Jin Cheng2Tao Ling3Yujun Yao4Dan Chen5Chuangchuang Chang6Xing Yu7Junqi Wang8Zixiao Zhou9Guangdong Li10Beijing Advanced Innovation Center for Materials Genome Engineering, Research Center for Sensor Technology, Beijing Key Laboratory for Sensor, MOE Key Laboratory for Modern Measurement and Control Technology, School of Applied Sciences, School of Instrument Science and Optoelectronics Engineering, Beijing Information Science and Technology University, Beijing 100101, ChinaBeijing Advanced Innovation Center for Materials Genome Engineering, Research Center for Sensor Technology, Beijing Key Laboratory for Sensor, MOE Key Laboratory for Modern Measurement and Control Technology, School of Applied Sciences, School of Instrument Science and Optoelectronics Engineering, Beijing Information Science and Technology University, Beijing 100101, ChinaBeijing Advanced Innovation Center for Materials Genome Engineering, Research Center for Sensor Technology, Beijing Key Laboratory for Sensor, MOE Key Laboratory for Modern Measurement and Control Technology, School of Applied Sciences, School of Instrument Science and Optoelectronics Engineering, Beijing Information Science and Technology University, Beijing 100101, ChinaBeijing Advanced Innovation Center for Materials Genome Engineering, Research Center for Sensor Technology, Beijing Key Laboratory for Sensor, MOE Key Laboratory for Modern Measurement and Control Technology, School of Applied Sciences, School of Instrument Science and Optoelectronics Engineering, Beijing Information Science and Technology University, Beijing 100101, ChinaBeijing Advanced Innovation Center for Materials Genome Engineering, Research Center for Sensor Technology, Beijing Key Laboratory for Sensor, MOE Key Laboratory for Modern Measurement and Control Technology, School of Applied Sciences, School of Instrument Science and Optoelectronics Engineering, Beijing Information Science and Technology University, Beijing 100101, ChinaState Key Laboratory on Integrated Optoelectronics, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, ChinaBeijing Advanced Innovation Center for Materials Genome Engineering, Research Center for Sensor Technology, Beijing Key Laboratory for Sensor, MOE Key Laboratory for Modern Measurement and Control Technology, School of Applied Sciences, School of Instrument Science and Optoelectronics Engineering, Beijing Information Science and Technology University, Beijing 100101, ChinaBeijing Advanced Innovation Center for Materials Genome Engineering, Research Center for Sensor Technology, Beijing Key Laboratory for Sensor, MOE Key Laboratory for Modern Measurement and Control Technology, School of Applied Sciences, School of Instrument Science and Optoelectronics Engineering, Beijing Information Science and Technology University, Beijing 100101, ChinaBeijing Advanced Innovation Center for Materials Genome Engineering, Research Center for Sensor Technology, Beijing Key Laboratory for Sensor, MOE Key Laboratory for Modern Measurement and Control Technology, School of Applied Sciences, School of Instrument Science and Optoelectronics Engineering, Beijing Information Science and Technology University, Beijing 100101, ChinaBeijing Advanced Innovation Center for Materials Genome Engineering, Research Center for Sensor Technology, Beijing Key Laboratory for Sensor, MOE Key Laboratory for Modern Measurement and Control Technology, School of Applied Sciences, School of Instrument Science and Optoelectronics Engineering, Beijing Information Science and Technology University, Beijing 100101, ChinaBeijing Advanced Innovation Center for Materials Genome Engineering, Research Center for Sensor Technology, Beijing Key Laboratory for Sensor, MOE Key Laboratory for Modern Measurement and Control Technology, School of Applied Sciences, School of Instrument Science and Optoelectronics Engineering, Beijing Information Science and Technology University, Beijing 100101, ChinaIn recent years, perovskite materials have been the subject of great progress in optoelectronic devices. The perovskite layer is the light absorption layer of perovskite solar cells (PSCs), and the majority charge carriers type play a crucial role in the formation of a P–N junction. In this paper, the light absorption layer of PSCs was Rb-mixed at a low concentrations by using a two-step spin-coating method, which could adjust the majority charge carriers type in perovskite films from N-type to P-type, and it has little influence on the crystal structure and light absorption capacity of perovskite. In addition, low concentration Rb-mixing is different from high concentration Rb-mixing. With increasing Rb-mixing concentration, the perovskite grains does not change shape. Although the quality of perovskite films deteriorated and the PL peaks exhibit a slight blue shift after mixing, the efficiency only slightly decreased, indicating that the new P-N hetero-junction was still formed after mixing, which provided a new idea for the future research of homo-junction PSCs.https://www.mdpi.com/2079-6412/10/7/627low concentrationsRb mixingmajority charge carriers typetwo-step |