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Optical and Spin Properties of NV Center Ensembles in Diamond Nano-Pillars

Nitrogen-vacancy (NV) color centers in diamond are excellent quantum sensors possessing high sensitivity and nano-scale spatial resolution. Their integration in photonic structures is often desired, since it leads to an increased photon emission and also allows the realization of solid-state quantum...

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Autores principales: Volkova, Kseniia, Heupel, Julia, Trofimov, Sergei, Betz, Fridtjof, Colom, Rémi, MacQueen, Rowan W., Akhundzada, Sapida, Reginka, Meike, Ehresmann, Arno, Reithmaier, Johann Peter, Burger, Sven, Popov, Cyril, Naydenov, Boris
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9103819/
https://www.ncbi.nlm.nih.gov/pubmed/35564222
http://dx.doi.org/10.3390/nano12091516
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author Volkova, Kseniia
Heupel, Julia
Trofimov, Sergei
Betz, Fridtjof
Colom, Rémi
MacQueen, Rowan W.
Akhundzada, Sapida
Reginka, Meike
Ehresmann, Arno
Reithmaier, Johann Peter
Burger, Sven
Popov, Cyril
Naydenov, Boris
author_facet Volkova, Kseniia
Heupel, Julia
Trofimov, Sergei
Betz, Fridtjof
Colom, Rémi
MacQueen, Rowan W.
Akhundzada, Sapida
Reginka, Meike
Ehresmann, Arno
Reithmaier, Johann Peter
Burger, Sven
Popov, Cyril
Naydenov, Boris
author_sort Volkova, Kseniia
collection PubMed
description Nitrogen-vacancy (NV) color centers in diamond are excellent quantum sensors possessing high sensitivity and nano-scale spatial resolution. Their integration in photonic structures is often desired, since it leads to an increased photon emission and also allows the realization of solid-state quantum technology architectures. Here, we report the fabrication of diamond nano-pillars with diameters up to 1000 nm by electron beam lithography and inductively coupled plasma reactive ion etching in nitrogen-rich diamonds (type Ib) with [100] and [111] crystal orientations. The NV centers were created by keV-He ion bombardment and subsequent annealing, and we estimate an average number of NVs per pillar to be 4300 ± 300 and 520 ± 120 for the [100] and [111] samples, respectively. Lifetime measurements of the NVs’ excited state showed two time constants with average values of τ(1) ≈ 2 ns and τ(2) ≈ 8 ns, which are shorter as compared to a single color center in a bulk crystal (τ ≈ 10 ns). This is probably due to a coupling between the NVs as well as due to interaction with bombardment-induced defects and substitutional nitrogen (P1 centers). Optically detected magnetic resonance measurements revealed a contrast of about 5% and average coherence and relaxation times of T(2) [100] = 420 ± 40 ns, T(2) [111] = 560 ± 50 ns, and T(1) [100] = 162 ± 11 μs, T(1) [111] = 174 ± 24 μs. These pillars could find an application for scanning probe magnetic field imaging.
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spelling pubmed-91038192022-05-14 Optical and Spin Properties of NV Center Ensembles in Diamond Nano-Pillars Volkova, Kseniia Heupel, Julia Trofimov, Sergei Betz, Fridtjof Colom, Rémi MacQueen, Rowan W. Akhundzada, Sapida Reginka, Meike Ehresmann, Arno Reithmaier, Johann Peter Burger, Sven Popov, Cyril Naydenov, Boris Nanomaterials (Basel) Article Nitrogen-vacancy (NV) color centers in diamond are excellent quantum sensors possessing high sensitivity and nano-scale spatial resolution. Their integration in photonic structures is often desired, since it leads to an increased photon emission and also allows the realization of solid-state quantum technology architectures. Here, we report the fabrication of diamond nano-pillars with diameters up to 1000 nm by electron beam lithography and inductively coupled plasma reactive ion etching in nitrogen-rich diamonds (type Ib) with [100] and [111] crystal orientations. The NV centers were created by keV-He ion bombardment and subsequent annealing, and we estimate an average number of NVs per pillar to be 4300 ± 300 and 520 ± 120 for the [100] and [111] samples, respectively. Lifetime measurements of the NVs’ excited state showed two time constants with average values of τ(1) ≈ 2 ns and τ(2) ≈ 8 ns, which are shorter as compared to a single color center in a bulk crystal (τ ≈ 10 ns). This is probably due to a coupling between the NVs as well as due to interaction with bombardment-induced defects and substitutional nitrogen (P1 centers). Optically detected magnetic resonance measurements revealed a contrast of about 5% and average coherence and relaxation times of T(2) [100] = 420 ± 40 ns, T(2) [111] = 560 ± 50 ns, and T(1) [100] = 162 ± 11 μs, T(1) [111] = 174 ± 24 μs. These pillars could find an application for scanning probe magnetic field imaging. MDPI 2022-04-29 /pmc/articles/PMC9103819/ /pubmed/35564222 http://dx.doi.org/10.3390/nano12091516 Text en © 2022 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
Volkova, Kseniia
Heupel, Julia
Trofimov, Sergei
Betz, Fridtjof
Colom, Rémi
MacQueen, Rowan W.
Akhundzada, Sapida
Reginka, Meike
Ehresmann, Arno
Reithmaier, Johann Peter
Burger, Sven
Popov, Cyril
Naydenov, Boris
Optical and Spin Properties of NV Center Ensembles in Diamond Nano-Pillars
title Optical and Spin Properties of NV Center Ensembles in Diamond Nano-Pillars
title_full Optical and Spin Properties of NV Center Ensembles in Diamond Nano-Pillars
title_fullStr Optical and Spin Properties of NV Center Ensembles in Diamond Nano-Pillars
title_full_unstemmed Optical and Spin Properties of NV Center Ensembles in Diamond Nano-Pillars
title_short Optical and Spin Properties of NV Center Ensembles in Diamond Nano-Pillars
title_sort optical and spin properties of nv center ensembles in diamond nano-pillars
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9103819/
https://www.ncbi.nlm.nih.gov/pubmed/35564222
http://dx.doi.org/10.3390/nano12091516
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