Abstract

Negatively-charged nitrogen-vacancy (NV−^-) color centers in diamond have generated much interest for use in quantum technology. Despite the progress made in developing their applications, many questions about the basic properties of NV−^- centers remain unresolved. Understanding these properties can validate theoretical models of NV−^-, improve their use in applications, and support their development into competitive quantum devices. In particular, knowledge of the phonon modes of the 1A1^1A_1 electronic state is key for understanding the optical pumping process. Using pump-probe spectroscopy, we measured the phonon sideband of the 1E→1A1{^1}E\rightarrow{^1}A_1 electronic transition in the NV−^- center. From this we calculated the 1E→1A1{^1}E\rightarrow{^1}A_1 one-phonon absorption spectrum and found it to differ from that of the 3E→3A2{^3}E\rightarrow{^3}A_2 transition, a result which is not anticipated by previous group-theoretical models of the NV−^- electronic states. We identified a high-energy 169 meV localized phonon mode of the 1A1^1A_1 level.

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