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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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Detalles Bibliográficos
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
Descripción
Sumario: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.