Hyperpolarized relaxometry based nuclear T1 noise spectroscopy in diamond

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作者
A. Ajoy
B. Safvati
R. Nazaryan
J. T. Oon
B. Han
P. Raghavan
R. Nirodi
A. Aguilar
K. Liu
X. Cai
X. Lv
E. Druga
C. Ramanathan
J. A. Reimer
C. A. Meriles
D. Suter
A. Pines
机构
[1] National Laboratory University of California,Department of Chemistry, and Materials Science Division Lawrence Berkeley
[2] Dartmouth College,Department of Physics and Astronomy
[3] Berkeley National Laboratory University of California,Department of Chemical and Biomolecular Engineering, and Materials Science Division Lawrence
[4] CUNY-City College of New York,Department of Physics and CUNY
[5] Fakultät Physik,Graduate Center
[6] Technische Universität Dortmund,undefined
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The origins of spin lifetimes in quantum systems is a matter of importance in several areas of quantum information. Spectrally mapping spin relaxation processes provides insight into their origin and motivates methods to mitigate them. In this paper, we map nuclear relaxation in a prototypical system of 13C\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${}^{13}{\rm{C}}$$\end{document} nuclei in diamond coupled to Nitrogen Vacancy (NV) centers over a wide field range (1 mT-7 T). Nuclear hyperpolarization through optically pumped NV electrons allows signal measurement savings exceeding million-fold over conventional methods. Through a systematic study with varying substitutional electron (P1 center) and 13C\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${}^{13}{\rm{C}}$$\end{document} concentrations, we identify the operational relaxation channels for the nuclei at different fields as well as the dominant role played by 13C\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${}^{13}{\rm{C}}$$\end{document} coupling to the interacting P1 electronic spin bath. These results motivate quantum control techniques for dissipation engineering to boost spin lifetimes in diamond, with applications including engineered quantum memories and hyperpolarized 13C\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${}^{13}{\rm{C}}$$\end{document} imaging.
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