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Saito, R.1
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Pimenta, M.A.6
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54
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84929592795
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The phonon modes (Equation presented), and (Equation presented) of monolayer and related Raman-active modes of few-layer (Equation presented) are labeled as (Equation presented), and (Equation presented) of bulk (Equation presented) for convenience in discussion
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The phonon modes (Equation presented), and (Equation presented) of monolayer and related Raman-active modes of few-layer (Equation presented) are labeled as (Equation presented), and (Equation presented) of bulk (Equation presented) for convenience in discussion.
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55
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84929592796
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Lecture Notes in Nanoscale Science and Technology, edited by (Springer, Berlin)
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(Equation presented): Materials, Physics, and Devices, Lecture Notes in Nanoscale Science and Technology, edited by Z. M. Wang (Springer, Berlin, 2014).
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(2014)
(Equation Presented): Materials, Physics, and Devices
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Wang, Z.M.1
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84864536898
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EPJBFY 1434-6028
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A. Kumar and P. Ahluwalia, Eur. Phys. J. B 85, 186 (2012). EPJBFY 1434-6028 10.1140/epjb/e2012-30070-x
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Kumar, A.1
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58
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84908045379
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PRLTAO 0031-9007
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A. Chernikov, T. C. Berkelbach, H. M. Hill, A. Rigosi, Y. Li, O. B. Aslan, D. R. Reichman, M. S. Hybertsen, and T. F. Heinz, Phys. Rev. Lett. 113, 076802 (2014). PRLTAO 0031-9007 10.1103/PhysRevLett.113.076802
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Phys. Rev. Lett.
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Chernikov, A.1
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Aslan, O.B.6
Reichman, D.R.7
Hybertsen, M.S.8
Heinz, T.F.9
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59
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84908052982
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NATUAS 0028-0836
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Z. Ye, T. Cao, K. O'Brien, H. Zhu, X. Yin, Y. Wang, S. G. Louie, and X. Zhang, Nature (London) 513, 214 (2014). NATUAS 0028-0836 10.1038/nature13734
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Ye, Z.1
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Zhang, X.8
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60
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84929592797
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It is worth pointing out that our assignment of the (Equation presented)-point phonon for (Equation presented) is similar to that for (Equation presented) by Berkdemir [41], but in our case is based on a different intervalley process. Berkdemir [41] used a laser line (514.5 nm) which matches the (Equation presented)-point gap of (Equation presented) and therefore may trigger an intervalley electron-phonon process between the (Equation presented) and (Equation presented) points, both of which have almost the same band energy. Thus Berkdemir's model should be used for (Equation presented) and our model for (Equation presented)
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It is worth pointing out that our assignment of the (Equation presented)-point phonon for (Equation presented) is similar to that for (Equation presented) by Berkdemir [41], but in our case is based on a different intervalley process. Berkdemir [41] used a laser line (514.5 nm) which matches the (Equation presented)-point gap of (Equation presented) and therefore may trigger an intervalley electron-phonon process between the (Equation presented) and (Equation presented) points, both of which have almost the same band energy. Thus Berkdemir's model should be used for (Equation presented) and our model for (Equation presented).
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62
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33846340492
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PRBMDO 1098-0121
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J. Jiang, R. Saito, K. Sato, J. S. Park, G. G. Samsonidze, A. Jorio, G. Dresselhaus, and M. S. Dresselhaus, Phys. Rev. B 75, 035405 (2007). PRBMDO 1098-0121 10.1103/PhysRevB.75.035405
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Phys. Rev. B
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Jiang, J.1
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Jorio, A.6
Dresselhaus, G.7
Dresselhaus, M.S.8
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63
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PRBMDO 1098-0121
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J. Jiang, R. Saito, G. G. Samsonidze, A. Jorio, S. G. Chou, G. Dresselhaus, and M. S. Dresselhaus, Phys. Rev. B 75, 035407 (2007). PRBMDO 1098-0121 10.1103/PhysRevB.75.035407
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Phys. Rev. B
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Jiang, J.1
Saito, R.2
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Dresselhaus, G.6
Dresselhaus, M.S.7
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