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Volumn 115, Issue 16, 2015, Pages

Berry Phase Modification to the Energy Spectrum of Excitons

Author keywords

[No Author keywords available]

Indexed keywords

FRUITS; LINEAR EQUATIONS; WAVE FUNCTIONS;

EID: 84945280168     PISSN: 00319007     EISSN: 10797114     Source Type: Journal    
DOI: 10.1103/PhysRevLett.115.166803     Document Type: Article
Times cited : (171)

References (43)
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  • 32
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    • The Berry curvature introduced here should not be confused with the exciton Berry curvature defined in
    • The Berry curvature introduced here should not be confused with the exciton Berry curvature defined in W. Yao and Q. Niu, Phys. Rev. Lett. 101, 106401 (2008). PRLTAO 0031-9007 10.1103/PhysRevLett.101.106401
    • (2008) Phys. Rev. Lett. , vol.101 , pp. 106401
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    • For details, see the derivation of Eq. (2) in Ref. [33]
    • For details, see the derivation of Eq. (2) in Ref. [33].
  • 39
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    • We note that there is a difference between 2D and 3D regarding the Darwin term. In 3D, for the Coulomb interaction (Equation presented), the Darwin term therefore only affects the energy levels of (Equation presented) states. In 2D this is no longer true: the Darwin term can affect states with nonzero angular momentum as well
    • We note that there is a difference between 2D and 3D regarding the Darwin term. In 3D, for the Coulomb interaction (Equation presented), the Darwin term therefore only affects the energy levels of (Equation presented) states. In 2D this is no longer true: the Darwin term can affect states with nonzero angular momentum as well.
  • 40
  • 43
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    • preceding Letter
    • A. Srivastava and A. Imamoʇlu, preceding Letter, Phys. Rev. Lett. 115, 166802 (2015). PRLTAO 0031-9007 10.1103/PhysRevLett.115.166802
    • (2015) Phys. Rev. Lett. , vol.115 , pp. 166802
    • Srivastava, A.1    Imamoʇlu, A.2


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