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ダイヤモンド中 NV 中心アンサンブルの環境ノイズ解析

睦子 波多野, Mutsuko Hatano

Published Mar 1, 2020• 0 citations
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ダイヤモンド中 NV 中心アンサンブルの環境ノイズ解析

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ダイヤモンド中 NV 中心アンサンブルの環境ノイズ解析

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NV 中心は量子情報分野での応用が期待されている。本研究では、様々なスピン濃度(窒素不純物(P1 中心)と NV 中心濃度の合計)を持つ 9 つのダイヤモンド試料に対し、ハーンエコー測定を行い理論式により解析を行った。その結果、スピン濃度が減少するにつれて、信号が指数関数的減衰から非指数関数的減衰に移り変わることが分かった。また、ノイズ相関時間とノイズ強度がスピン濃度に依存することが分かった。

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The fine structure of the neutral nitrogen‐vacancy center in diamond

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Abstract The nitrogen‐vacancy (NV) center in diamond is a widely utilized system due to its useful quantum properties. Almost all research focuses on the negative charge state (NV − ) and comparatively little is understood about the neutral charge state (NV 0 ). This is surprising as the charge state often fluctuates between NV 0 and NV − during measurements. There are potentially under‐utilized technical applications that could take advantage of NV 0 , either by improving the performance of NV 0 or utilizing NV − directly. However, the fine structure of NV 0 has not been observed. Here, we rectify this lack of knowledge by performing magnetic circular dichroism measurements that quantitatively determine the fine structure of NV 0 . The observed behavior is accurately described by spin‐Hamiltonians in the ground and excited states with the ground state yielding a spin‐orbit coupling of λ = 2.24 ± 0.05 GHz and a orbital g ‐factor of 0.0186 ± 0.0005. The reasons why this fine structure has not been previously measured are discussed and strain‐broadening is concluded to be the likely reason.

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Acta Optica Sinica•Jan 1, 2024•3 citations
NV 中心は量子情報分野での応用が期待されている。本研究では、様々なスピン濃度(窒素不純物(P1 中心)と NV 中心濃度の合計)を持つ 9 つのダイヤモンド試料に対し、ハーンエコー測定を行い理論式により解析を行った。その結果、スピン濃度が減少するにつれて、信号が指数関数的減衰から非指数関数的減衰に移り変わることが分かった。また、ノイズ相関時間とノイズ強度がスピン濃度に依存することが分かった。
Abstract The nitrogen‐vacancy (NV) center in diamond is a widely utilized system due to its useful quantum properties. Almost all research focuses on the negative charge state (NV − ) and comparatively little is understood about the neutral charge state (NV 0 ). This is surprising as the charge state often fluctuates between NV 0 and NV − during measurements. There are potentially under‐utilized technical applications that could take advantage of NV 0 , either by improving the performance of NV 0 or utilizing NV − directly. However, the fine structure of NV 0 has not been observed. Here, we rectify this lack of knowledge by performing magnetic circular dichroism measurements that quantitatively determine the fine structure of NV 0 . The observed behavior is accurately described by spin‐Hamiltonians in the ground and excited states with the ground state yielding a spin‐orbit coupling of λ = 2.24 ± 0.05 GHz and a orbital g ‐factor of 0.0186 ± 0.0005. The reasons why this fine structure has not been previously measured are discussed and strain‐broadening is concluded to be the likely reason.