2007
DOI: 10.1103/physrevb.76.045430
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Symmetry-based approach to electron-phonon interactions in graphene

Abstract: We use the symmetries of monolayer graphene to write a set of constraints that must be satisfied by any electron-phonon interaction hamiltonian. The explicit solution as a series expansion in the momenta gives the most general, model-independent couplings between electrons and long wavelength acoustic and optical phonons. As an application, the possibility of describing elastic strains in terms of effective electromagnetic fields is considered in detail, with an emphasis on group theory conditions and the role… Show more

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Cited by 259 publications
(278 citation statements)
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“…Similar approaches can be applied to describe the appearance of Dirac bands in AG in semiconductors [13,14]. The general symmetries of the triangular lattice uniquely determine these couplings, which have the same form as graphene [39,40]. In particular, spatially patterning the hopping via STM atom manipulation allows the generation of both gauge (pseudo) electric and magnetic fields in molecular graphene (see Fig.…”
Section: Confining Electronsmentioning
confidence: 99%
“…Similar approaches can be applied to describe the appearance of Dirac bands in AG in semiconductors [13,14]. The general symmetries of the triangular lattice uniquely determine these couplings, which have the same form as graphene [39,40]. In particular, spatially patterning the hopping via STM atom manipulation allows the generation of both gauge (pseudo) electric and magnetic fields in molecular graphene (see Fig.…”
Section: Confining Electronsmentioning
confidence: 99%
“…40. In the long-wavelength limit, the TA and LA phonons are strictly transverse and longitudinal, respectively, 47 and the electronphonon interaction has a simple analytic representation in the two-dimensional pseudospin basis.…”
Section: Interaction With Acoustic Phononsmentioning
confidence: 99%
“…In the long-wavelength limit, the TA and LA phonons are strictly transverse and longitudinal, respectively, 47 and the electronphonon interaction has a simple analytic representation in the two-dimensional pseudospin basis. 40 Using the results of Ref. 40, the coupling matrix elements can be expressed in terms of the angles θ k , θ q , and θ k+q of the involved wave vectors.…”
Section: Interaction With Acoustic Phononsmentioning
confidence: 99%
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