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Monitoring Dark-State Dynamics of a Single Nitrogen-Vacancy Center in Nanodiamond by Auto-Correlation Spectroscopy: Photonionization and Recharging

In this letter, the photon-induced charge conversion dynamics of a single Nitrogen-Vacancy (NV) center in nanodiamond between two charge states, negative (NV(−)) and neutral (NV(0)), is studied by the auto-correlation function. It is observed that the ionization of NV(−) converts to NV(0), which is...

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Autores principales: Zhang, Mengdi, Li, Bai-Yan, Liu, Jing
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8070252/
https://www.ncbi.nlm.nih.gov/pubmed/33920225
http://dx.doi.org/10.3390/nano11040979
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author Zhang, Mengdi
Li, Bai-Yan
Liu, Jing
author_facet Zhang, Mengdi
Li, Bai-Yan
Liu, Jing
author_sort Zhang, Mengdi
collection PubMed
description In this letter, the photon-induced charge conversion dynamics of a single Nitrogen-Vacancy (NV) center in nanodiamond between two charge states, negative (NV(−)) and neutral (NV(0)), is studied by the auto-correlation function. It is observed that the ionization of NV(−) converts to NV(0), which is regarded as the dark state of the NV(−), leading to fluorescence intermittency in single NV centers. A new method, based on the auto-correlation calculation of the time-course fluorescence intensity from NV centers, was developed to quantify the transition kinetics and yielded the calculation of transition rates from NV(−) to NV(0) (ionization) and from NV(0) to NV(−) (recharging). Based on our experimental investigation, we found that the NV(−)-NV(0) transition is wavelength-dependent, and more frequent transitions were observed when short-wavelength illumination was used. From the analysis of the auto-correlation curve, it is found that the transition time of NV(−) to NV(0) (ionization) is around 0.1 μs, but the transition time of NV(0) to NV(−) (recharging) is around 20 ms. Power-dependent measurements reveal that the ionization rate increases linearly with the laser power, while the recharging rate has a quadratic increase with the laser power. This difference suggests that the ionization in the NV center is a one-photon process, while the recharging of NV(0) to NV(−) is a two-photon process. This work, which offers theoretical and experimental explanations of the emission property of a single NV center, is expected to help the utilization of the NV center for quantum information science, quantum communication, and quantum bioimaging.
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spelling pubmed-80702522021-04-26 Monitoring Dark-State Dynamics of a Single Nitrogen-Vacancy Center in Nanodiamond by Auto-Correlation Spectroscopy: Photonionization and Recharging Zhang, Mengdi Li, Bai-Yan Liu, Jing Nanomaterials (Basel) Article In this letter, the photon-induced charge conversion dynamics of a single Nitrogen-Vacancy (NV) center in nanodiamond between two charge states, negative (NV(−)) and neutral (NV(0)), is studied by the auto-correlation function. It is observed that the ionization of NV(−) converts to NV(0), which is regarded as the dark state of the NV(−), leading to fluorescence intermittency in single NV centers. A new method, based on the auto-correlation calculation of the time-course fluorescence intensity from NV centers, was developed to quantify the transition kinetics and yielded the calculation of transition rates from NV(−) to NV(0) (ionization) and from NV(0) to NV(−) (recharging). Based on our experimental investigation, we found that the NV(−)-NV(0) transition is wavelength-dependent, and more frequent transitions were observed when short-wavelength illumination was used. From the analysis of the auto-correlation curve, it is found that the transition time of NV(−) to NV(0) (ionization) is around 0.1 μs, but the transition time of NV(0) to NV(−) (recharging) is around 20 ms. Power-dependent measurements reveal that the ionization rate increases linearly with the laser power, while the recharging rate has a quadratic increase with the laser power. This difference suggests that the ionization in the NV center is a one-photon process, while the recharging of NV(0) to NV(−) is a two-photon process. This work, which offers theoretical and experimental explanations of the emission property of a single NV center, is expected to help the utilization of the NV center for quantum information science, quantum communication, and quantum bioimaging. MDPI 2021-04-10 /pmc/articles/PMC8070252/ /pubmed/33920225 http://dx.doi.org/10.3390/nano11040979 Text en © 2021 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Zhang, Mengdi
Li, Bai-Yan
Liu, Jing
Monitoring Dark-State Dynamics of a Single Nitrogen-Vacancy Center in Nanodiamond by Auto-Correlation Spectroscopy: Photonionization and Recharging
title Monitoring Dark-State Dynamics of a Single Nitrogen-Vacancy Center in Nanodiamond by Auto-Correlation Spectroscopy: Photonionization and Recharging
title_full Monitoring Dark-State Dynamics of a Single Nitrogen-Vacancy Center in Nanodiamond by Auto-Correlation Spectroscopy: Photonionization and Recharging
title_fullStr Monitoring Dark-State Dynamics of a Single Nitrogen-Vacancy Center in Nanodiamond by Auto-Correlation Spectroscopy: Photonionization and Recharging
title_full_unstemmed Monitoring Dark-State Dynamics of a Single Nitrogen-Vacancy Center in Nanodiamond by Auto-Correlation Spectroscopy: Photonionization and Recharging
title_short Monitoring Dark-State Dynamics of a Single Nitrogen-Vacancy Center in Nanodiamond by Auto-Correlation Spectroscopy: Photonionization and Recharging
title_sort monitoring dark-state dynamics of a single nitrogen-vacancy center in nanodiamond by auto-correlation spectroscopy: photonionization and recharging
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8070252/
https://www.ncbi.nlm.nih.gov/pubmed/33920225
http://dx.doi.org/10.3390/nano11040979
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