2022
DOI: 10.1007/s11664-022-09498-7
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Structural, Electronic and Thermoelectric Properties of Bi2Se3 Thin Films Deposited by RF Magnetron Sputtering

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Cited by 24 publications
(17 citation statements)
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“…53 The opposite kind of peak shift in Bi and Se demonstrates the formation of the Bi−Se bond in the deposited film. 45,52 Figure 3a The peaks at 2θ values 24.9, 29.1, 35.9, 44.3, 48.1, 52.4, and 65.3°can be assigned to the (301), (040), (411), (314), (251), (610), and (522) Sb 2 Se 3 lattice planes, respectively (JCPDS number: 00-015-0861). 56,57 The other XRD peaks of the Mo foil are indexed in a manner similar to Figure 1d.…”
Section: Resultsmentioning
confidence: 99%
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“…53 The opposite kind of peak shift in Bi and Se demonstrates the formation of the Bi−Se bond in the deposited film. 45,52 Figure 3a The peaks at 2θ values 24.9, 29.1, 35.9, 44.3, 48.1, 52.4, and 65.3°can be assigned to the (301), (040), (411), (314), (251), (610), and (522) Sb 2 Se 3 lattice planes, respectively (JCPDS number: 00-015-0861). 56,57 The other XRD peaks of the Mo foil are indexed in a manner similar to Figure 1d.…”
Section: Resultsmentioning
confidence: 99%
“…The Raman spectrum of Bi 2 Se 3 on the Mo foil shows Raman peaks located at 73.6 (A 1g 1 ), 133.0 (E g 2 ), and 175.5 (A 1g 2 ) cm –1 as shown in Figure c. The A 1g 1 and A 1g 2 peaks are attributed to the out-of-plane vibrational mode, while the E g 2 peak corresponds to the in-plane vibrational Raman mode, and all the peaks correspond to the rhombohedral phase of Bi 2 Se 3 . , To investigate the crystal structure of Bi 2 Se 3 on the Mo foil, XRD was performed, and the data is presented in Figure d. The three peaks at 2θ values of 40.1, 58.7, and 73.6° correspond to the (110), (200), and (211) planes, respectively, of a pure Mo foil .…”
Section: Resultsmentioning
confidence: 99%
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“…Figure a shows the core-level scan of Bi 4f of the Bi 2 Se 3 /n-GaN hybrid structure where the two spin–orbital-coupled Bi (4f 7/2 , 4f 5/2 ) peaks are deconvoluted using a Voigt (mixed Lorentzian–Gaussian) function to Bi–Se, Bi–O, and Bi–Bi peaks, respectively. , Figure b shows the Se 3d narrow scan where, in addition to the deconvoluted spin–orbit-coupled Se 3d 3/2 and 3d 5/2 peaks, a feeble Se–O bond peak corresponding to both Se 3d 3/2 and 3d 5/2 peaks was also observed . The binding energy positions corresponding to each peak are given in Table .…”
Section: Resultsmentioning
confidence: 99%
“…Thus, the binding energy plays a crucial role in shifting the Raman modes. [ 32–34 ] Moreover, in the case of SiO 2 , there are three intrinsic Raman modes of bismuth selenide at 70.8, 128, and 174.2 cm −1 , while there is another Raman mode observed at 252 cm −1 . This particular mode at 252 cm −1 is due to selenium–selenium interaction and is known as H‐mode.…”
Section: Resultsmentioning
confidence: 99%