2022
DOI: 10.1126/sciadv.abl9402
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Imaging dark charge emitters in diamond via carrier-to-photon conversion

Abstract: Color centers capturing diffusive photo-induced charge carriers reveal otherwise invisible point defects in a crystal.

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Cited by 12 publications
(8 citation statements)
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“…The schematic in Figure a lays out our experimental protocol: We first implement multiple 632 nm, 6 mW laser scan across a (80 μm) 2 area to initialize SiVs into a nonfluorescing charge state (Supporting Information, Section II). We subsequently park a 532 nm, 3.6 mW laser at the center of the scanned plane for a variable time t p ; illumination at this wavelength is known to generate a continuous stream of free electrons and holes stemming from charge cycling of coexisting NVs. The ensuing carrier diffusion and capture produces a nonlocal change of the SiV charge state, which we subsequently image under 632 nm, 50 μW excitation.…”
mentioning
confidence: 99%
“…The schematic in Figure a lays out our experimental protocol: We first implement multiple 632 nm, 6 mW laser scan across a (80 μm) 2 area to initialize SiVs into a nonfluorescing charge state (Supporting Information, Section II). We subsequently park a 532 nm, 3.6 mW laser at the center of the scanned plane for a variable time t p ; illumination at this wavelength is known to generate a continuous stream of free electrons and holes stemming from charge cycling of coexisting NVs. The ensuing carrier diffusion and capture produces a nonlocal change of the SiV charge state, which we subsequently image under 632 nm, 50 μW excitation.…”
mentioning
confidence: 99%
“…Thereby a dark state is formed, and since the excitation laser is continually injecting carriers, the total fraction of SiV in the SiV − state remains small even with the existence of many SiV. 2,3 We now characterize the temperature-dependent ZPL peak shift for the 10 15 ions/cm 2 shift for the 10 10 ions/cm 2 fluence is also conducted and presented in the Supporting Information. 21 At temperatures below 100 K, the ZPL peak can be resolved into B and C optical transitions.…”
Section: ■ Resultsmentioning
confidence: 99%
“…We instead ascribe this observation to increased carrier lifetime at low temperature. , A SiV – loses its electron, leading to formation of SiV 0 , the emission of which is not monitored in this work. Thereby a dark state is formed, and since the excitation laser is continually injecting carriers, the total fraction of SiV in the SiV – state remains small even with the existence of many SiV. , …”
Section: Resultsmentioning
confidence: 99%
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“…22 Because every cycle of NV ionization and recombination leads to the successive injection of a free electron and a hole (see level diagram in Figure 1c), this stage in the protocol results in a stream of diffusing carriers, which we exploit to alter the charge state of the twin color center in the pair, namely, NV B or the "target" NV. To probe its charge state after a variable exposure time, we implement a single-shot charge state readout with the help of a low-power, 594 nm laser 23,24 (see Figure S1 of the Supporting Information); all experiments are performed at room temperature.…”
mentioning
confidence: 99%