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2020
DOI: 10.1038/s41524-020-00451-y
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Stone–Wales defects in hexagonal boron nitride as ultraviolet emitters

Abstract: Many quantum emitters have been measured close or near the grain boundaries of the two-dimensional hexagonal boron nitride where various Stone–Wales defects appear. We show by means of first principles density functional theory calculations that the pentagon–heptagon Stone–Wales defect is an ultraviolet emitter and its optical properties closely follow the characteristics of a 4.08-eV quantum emitter, often observed in polycrystalline hexagonal boron nitride. We also show that the square–octagon Stone–Wales li… Show more

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Cited by 38 publications
(31 citation statements)
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References 43 publications
(71 reference statements)
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“…The C N O N pair has also been suggested to explain the 4.1 eV luminescence [24]. However, a stoichiometric Stone-Wales defect that does not involve carbon at all has also been recently proposed [25]. All these three defects are expected to emit in the UV, but the debate regarding the exact chemical nature of the 4.1 eV emitters seems to continue.…”
Section: Introductionmentioning
confidence: 99%
“…The C N O N pair has also been suggested to explain the 4.1 eV luminescence [24]. However, a stoichiometric Stone-Wales defect that does not involve carbon at all has also been recently proposed [25]. All these three defects are expected to emit in the UV, but the debate regarding the exact chemical nature of the 4.1 eV emitters seems to continue.…”
Section: Introductionmentioning
confidence: 99%
“…Examples include boron dangling bonds as source for single photon emission at 2.06 eV [41] which could explain the accumulation of emitters localized near crystal edges or grain boundaries [42,43]. UV emission at 4.08 eV was traced back to optically active, pentagon-hexagon Stone-Wales defects preferentially present in poly-crystalline h-BN [44]. Emitters with transition energies between 2.0 and 2.2 eV were also found to originate from carbonrelated defects [45].…”
Section: The Large Family Of Defect Centers In H-bnmentioning
confidence: 99%
“…S3 of the SI). In addition, in the case of defect systems with singlet GS and ES, we expect non-negligible differences between TDDFT and CDFT results, since the accurate description of a singlet ES requires a linear combination of at least two Slater determinants [14,69]. In that case the use of quantum embedding theories (QDET), should be preferable to describe strongly correlated states [70][71][72].…”
Section: A Zero-phonon Linesmentioning
confidence: 99%
“…As for many properties of condensed systems, Density Functional Theory (DFT) has turned out to be a valuable tool to compute PL spectra, which are used to interpret experiments as well as to provide predictions of the fingerprints of specific defects in materials [7][8][9]. For example, first principles spectra based on DFT have been recently reported for nitrides, e.g., GaN [10,11], AlN [12], and hexagonal born nitride (h-BN) [13][14][15][16][17][18], diamond [19][20][21][22][23][24][25][26][27][28][29], silicon carbide (SiC) [30][31][32][33], and monolayers of transition metal dichalcogenides (TMDC) [34]. These studies have been performed with several useful computational approaches; however, a systematic assessment of the theoretical and numerical approximations adopted in PL calculations has not yet been conducted.…”
Section: Introductionmentioning
confidence: 99%