2015
DOI: 10.1088/0957-4484/26/24/245501
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All-optical single-nanoparticle ratiometric thermometry with a noise floor of 0.3 K Hz−1/2

Abstract: We demonstrate a temperature noise floor of 0.3 K Hz(-1/2) and a long-term stability better than 0.6 K (peak-to-peak value) using a single crystal of diamond smaller than 50 nm across and containing about 100 nitrogen-vacancy centres as a temperature sensor. We compare the achieved characteristics to other single-particle sensors and show that it is one of the best ratiometric all-optical nano-probes of temperature to date.

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Cited by 71 publications
(88 citation statements)
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References 37 publications
(50 reference statements)
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“…TheZ PL center (l 0 )can be extracted by fitting the spectrum over 610-660 nm to aL orentzian function, along with an exponential function to correct the baseline. [13] Signal averaging over 6s by curve-fitting of 60 independent spectra yielded l 0 = 638.519 AE 0.013 nm for a9 5% confidence interval (inset in Figure 1b and Figure S2), which suggests at emperature measurement sensitivity of AE 2 8 8C/Hz 1/2 .…”
mentioning
confidence: 88%
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“…TheZ PL center (l 0 )can be extracted by fitting the spectrum over 610-660 nm to aL orentzian function, along with an exponential function to correct the baseline. [13] Signal averaging over 6s by curve-fitting of 60 independent spectra yielded l 0 = 638.519 AE 0.013 nm for a9 5% confidence interval (inset in Figure 1b and Figure S2), which suggests at emperature measurement sensitivity of AE 2 8 8C/Hz 1/2 .…”
mentioning
confidence: 88%
“…TheZ PL center (l 0 )can be extracted by fitting the spectrum over 610-660 nm to aL orentzian function, along with an exponential function to correct the baseline. [13] Signal averaging over 6s…”
mentioning
confidence: 99%
See 1 more Smart Citation
“…In the case of NV À centers, 532-nm (2.33-eV) excitation is commonly used. However, exciting along the 575-nm (2.16-eV) ZPL of the neutrally charged nitrogen-vacancy center ðNV 0 Þ aids in the stability of the NV À center [49], while exciting at 590 nm (2.10 eV) may be used to avoid the excitation of the other charge state altogether [50]. The charge stability of the electrostatic environment stems from other defects that are optically excited within the laser spot size.…”
Section: A Optically Detected Magnetic Resonance In Defect Spinsmentioning
confidence: 99%
“…The NV center can then relax to its ground state through radiative and nonradiative pathways. The radiative transitions produce broad photoluminescence spectra with a zero-phonon line at 637 nm, which can be used for accurate measurements of temperatures [26,27]. The nonradiative transition is due to intersystem crossing (ISC) to singlet states situated below the excited triplet state.…”
Section: Introductionmentioning
confidence: 99%