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On the Question of the Need for a Built‐In Potential in Perovskite Solar Cells
Advanced Materials Interfaces, Volume: 7, Issue: 10, Start page: 2000041
Swansea University Authors: Oskar Sandberg , Paul Meredith , Ardalan Armin
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DOI (Published version): 10.1002/admi.202000041
Abstract
Perovskite semiconductors as the active materials in efficient solar cells exhibit free carrier diffusion lengths on the order of microns at low illumination fluxes and many hundreds of nanometers under 1 sun conditions. These lengthscales are significantly larger than typical junction thicknesses,...
Published in: | Advanced Materials Interfaces |
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ISSN: | 2196-7350 2196-7350 |
Published: |
Wiley
2020
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URI: | https://cronfa.swan.ac.uk/Record/cronfa53844 |
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2022-12-05T12:38:16.1122315 v2 53844 2020-03-21 On the Question of the Need for a Built‐In Potential in Perovskite Solar Cells 9e91512a54d5aee66cd77851a96ba747 0000-0003-3778-8746 Oskar Sandberg Oskar Sandberg true false 31e8fe57fa180d418afd48c3af280c2e 0000-0002-9049-7414 Paul Meredith Paul Meredith true false 22b270622d739d81e131bec7a819e2fd Ardalan Armin Ardalan Armin true false 2020-03-21 BGPS Perovskite semiconductors as the active materials in efficient solar cells exhibit free carrier diffusion lengths on the order of microns at low illumination fluxes and many hundreds of nanometers under 1 sun conditions. These lengthscales are significantly larger than typical junction thicknesses, and thus the carrier transport and charge collection should be expected to be diffusion controlled. A consensus along these lines is emerging in the field. However, the question as to whether the built-in potential plays any role is still of matter of some conjecture. This important question using phase-sensitive photocurrent measurements and theoretical device simulations based upon the drift-diffusion framework is addressed. In particular, the role of the built-in electric field and charge-selective transport layers in state-of-the-art p–i–n perovskite solar cells comparing experimental findings and simulation predictions is probed. It is found that while charge collection in the junction does not require a drift field per se, a built-in potential is still needed to avoid the formation of reverse electric fields inside the active layer, and to ensure efficient extraction through the charge transport layers. Journal Article Advanced Materials Interfaces 7 10 2000041 Wiley 2196-7350 2196-7350 20 5 2020 2020-05-20 10.1002/admi.202000041 COLLEGE NANME Biosciences Geography and Physics School COLLEGE CODE BGPS Swansea University European Regional Development Fund Welsh European Funding Office Swansea University strategic initiative in Sustainable Advanced Materials 2022-12-05T12:38:16.1122315 2020-03-21T13:34:44.7801557 Faculty of Science and Engineering School of Biosciences, Geography and Physics - Physics Oskar Sandberg 0000-0003-3778-8746 1 Jona Kurpiers 2 Martin Stolterfoht 3 Dieter Neher 4 Paul Meredith 0000-0002-9049-7414 5 Safa Shoaee 6 Ardalan Armin 7 53844__16882__2cd424fc8ab0466da6b8866254206c47.pdf 2020 ACDC.pdf 2020-03-21T13:43:10.0439538 Output 1504118 application/pdf Version of Record true Released under the terms of a Creative Commons Attribution License (CC-BY). true eng http://creativecommons.org/licenses/by/4.0/ |
title |
On the Question of the Need for a Built‐In Potential in Perovskite Solar Cells |
spellingShingle |
On the Question of the Need for a Built‐In Potential in Perovskite Solar Cells Oskar Sandberg Paul Meredith Ardalan Armin |
title_short |
On the Question of the Need for a Built‐In Potential in Perovskite Solar Cells |
title_full |
On the Question of the Need for a Built‐In Potential in Perovskite Solar Cells |
title_fullStr |
On the Question of the Need for a Built‐In Potential in Perovskite Solar Cells |
title_full_unstemmed |
On the Question of the Need for a Built‐In Potential in Perovskite Solar Cells |
title_sort |
On the Question of the Need for a Built‐In Potential in Perovskite Solar Cells |
author_id_str_mv |
9e91512a54d5aee66cd77851a96ba747 31e8fe57fa180d418afd48c3af280c2e 22b270622d739d81e131bec7a819e2fd |
author_id_fullname_str_mv |
9e91512a54d5aee66cd77851a96ba747_***_Oskar Sandberg 31e8fe57fa180d418afd48c3af280c2e_***_Paul Meredith 22b270622d739d81e131bec7a819e2fd_***_Ardalan Armin |
author |
Oskar Sandberg Paul Meredith Ardalan Armin |
author2 |
Oskar Sandberg Jona Kurpiers Martin Stolterfoht Dieter Neher Paul Meredith Safa Shoaee Ardalan Armin |
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Advanced Materials Interfaces |
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10.1002/admi.202000041 |
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Wiley |
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description |
Perovskite semiconductors as the active materials in efficient solar cells exhibit free carrier diffusion lengths on the order of microns at low illumination fluxes and many hundreds of nanometers under 1 sun conditions. These lengthscales are significantly larger than typical junction thicknesses, and thus the carrier transport and charge collection should be expected to be diffusion controlled. A consensus along these lines is emerging in the field. However, the question as to whether the built-in potential plays any role is still of matter of some conjecture. This important question using phase-sensitive photocurrent measurements and theoretical device simulations based upon the drift-diffusion framework is addressed. In particular, the role of the built-in electric field and charge-selective transport layers in state-of-the-art p–i–n perovskite solar cells comparing experimental findings and simulation predictions is probed. It is found that while charge collection in the junction does not require a drift field per se, a built-in potential is still needed to avoid the formation of reverse electric fields inside the active layer, and to ensure efficient extraction through the charge transport layers. |
published_date |
2020-05-20T13:52:18Z |
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11.048149 |