2019
DOI: 10.1007/s10812-019-00865-7
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Photoluminescence Spectra of the 580-nm Center in Irradiated Diamonds

Abstract: The formation mechanisms of the zero-phonon line optical center at 580 nm (H19 center) in photoluminescence spectra of irradiated natural diamonds and those deposited from the vapor phase were studied after their hightemperature vacuum annealing. The photoluminescence band intensity of the H19 center was shown to increase exponentially as the annealing temperature increased. Temperature dependences of photoluminescence spectra and local mechanical stress effects on the position and full width at half-height of… Show more

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Cited by 14 publications
(4 citation statements)
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“…A different temperature dependence is observed in another group of bands with maxima at 335, 1390, 1415, and 1740 cm −1 . The intensity of all of these four bands synchronously increases in the temperature range of 1350-1650 • C, much faster than the intensity of the diamond peak and simultaneously with the strengthening of the 580 nm band of H19 center in PL spectra [76].…”
Section: Evidence Of New Raman Bands After High-temperature Annealingmentioning
confidence: 90%
“…A different temperature dependence is observed in another group of bands with maxima at 335, 1390, 1415, and 1740 cm −1 . The intensity of all of these four bands synchronously increases in the temperature range of 1350-1650 • C, much faster than the intensity of the diamond peak and simultaneously with the strengthening of the 580 nm band of H19 center in PL spectra [76].…”
Section: Evidence Of New Raman Bands After High-temperature Annealingmentioning
confidence: 90%
“…14) As the temperature rises, the ZPL gradually broadens, and the linewidth at temperature T, denoted as , w approximately follows the empirical formula. 33) g T 3 0 0 3…”
Section: Resultsmentioning
confidence: 99%
“…The ZPL quenching occurs due to the gradual replacement of radiative transitions with non-radiative ones for the same defect with the increase in the measurement temperature. In this case, the activation energy for thermal quenching of ZPL is equal to the energy difference between the crossover point of the excited and ground states and the minimum of the excited state [17]. The activation energies for thermal quenching are 119 meV, 124 meV, and 190 meV for the GR1, 550.3 nm, and 593 nm emissions, respectively.…”
Section: Resultsmentioning
confidence: 99%