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- Edlyn V. Levine
- Department of Physics , Harvard University , Cambridge, MA 02138 , USA
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- Matthew J. Turner
- Department of Physics , Harvard University , Cambridge, MA 02138 , USA
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- Pauli Kehayias
- Sandia National Laboratories , Albuquerque, NM 87123 , USA
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- Connor A. Hart
- Department of Physics , Harvard University , Cambridge, MA 02138 , USA
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- Nicholas Langellier
- Department of Physics , Harvard University , Cambridge, MA 02138 , USA
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- Raisa Trubko
- Department of Physics , Harvard University , Cambridge, MA 02138 , USA
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- David R. Glenn
- Department of Physics , Harvard University , Cambridge, MA 02138 , USA
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- Roger R. Fu
- Department of Earth and Planetary Sciences , Harvard University , Cambridge, MA 02138 , USA
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- Ronald L. Walsworth
- Harvard-Smithsonian Center for Astrophysics , Cambridge, MA 02138 , USA
説明
<jats:title>Abstract</jats:title><jats:p>We provide an overview of the experimental techniques, measurement modalities, and diverse applications of the quantum diamond microscope (QDM). The QDM employs a dense layer of fluorescent nitrogen-vacancy (NV) color centers near the surface of a transparent diamond chip on which a sample of interest is placed. NV electronic spins are coherently probed with microwaves and optically initialized and read out to provide spatially resolved maps of local magnetic fields. NV fluorescence is measured simultaneously across the diamond surface, resulting in a wide-field, two-dimensional magnetic field image with adjustable spatial pixel size set by the parameters of the imaging system. NV measurement protocols are tailored for imaging of broadband and narrowband fields, from DC to GHz frequencies. Here we summarize the physical principles common to diverse implementations of the QDM and review example applications of the technology in geoscience, biology, and materials science.</jats:p>
収録刊行物
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- Nanophotonics
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Nanophotonics 8 (11), 1945-1973, 2019-09-17
Walter de Gruyter GmbH
