2012
DOI: 10.1088/0268-1242/27/6/065019
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Effect of doping on electronic states in B-doped polycrystalline CVD diamond films

Abstract: High-resolution Laplace deep-level transient spectroscopy (LDLTS) and thermal admittance spectroscopy (TAS) have been used to determine the effect of boron (B) concentration on the electronic states in polycrystalline chemical vapour deposition diamond thin films grown on silicon by the hot filament method. A combination of high-resolution LDLTS and direct-capture cross-sectional measurements was used to investigate whether the deep electronic states present in the layers originated from point or extended defe… Show more

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Cited by 10 publications
(7 citation statements)
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“…Deep trap with the similar activation energy as identified in these measurements has been observed before in unintentionally doped HPHT type IIa and Ib diamond [33], in B-doped polycrystalline CVD diamonds [34], as well as in neutron irradiated scCVD diamond [35]. The origin of the defect has not been determined decisively.…”
Section: Charge Transient Spectroscopy (Qts)supporting
confidence: 63%
“…Deep trap with the similar activation energy as identified in these measurements has been observed before in unintentionally doped HPHT type IIa and Ib diamond [33], in B-doped polycrystalline CVD diamonds [34], as well as in neutron irradiated scCVD diamond [35]. The origin of the defect has not been determined decisively.…”
Section: Charge Transient Spectroscopy (Qts)supporting
confidence: 63%
“…However, in the case of an extended defect, the amplitude of the DLTS peak is proportional to the filling pulse width, as shown in the following equation 34 35 36 :…”
Section: Resultsmentioning
confidence: 99%
“…Figure S5a,b shows, respectively, the whole Raman spectra of the pristine BDD electrode and the U-BDD electrode after the chronoamperometry in 5 mM uranyl acetate and 0.1 M KClO 4 . Figure S5a reveals the characteristic Raman peaks for diamond at 1330 cm –1 (Fig mode). , …”
Section: Resultsmentioning
confidence: 99%