2018
DOI: 10.1140/epjp/i2018-12137-4
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Magnetic dispersion of Dirac fermions in graphene under inhomogeneous field profiles

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Cited by 6 publications
(10 citation statements)
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“…The first-order intertwining method presented here generalizes the shape invariant technique that different authors have used previously to describe the behavior of an electron near to the Dirac points in a graphene layer with applied external magnetic fields [23][24][25][26][27][28]. Similarly as Figure 7: Second intertwining for the Morse potential with k = 6α, ν 1 = − 3 2 , ν 2 = − 1 2 , 1 = − 1 2 E − 1 = − 11α 2 2 , 2 = −E − 1 = −11α 2 : (a) generated potential V 2 (x, 2 ) (continuous line) and initial oneṼ 1 (x, 1 ) (dashed line), with energy levels E n (x)| 2 for the ground state (GS, blue) and the excited states n = 1, 2, 3 (red, green, purple); (d) current density for the excited states with the same colors that in (c).…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…The first-order intertwining method presented here generalizes the shape invariant technique that different authors have used previously to describe the behavior of an electron near to the Dirac points in a graphene layer with applied external magnetic fields [23][24][25][26][27][28]. Similarly as Figure 7: Second intertwining for the Morse potential with k = 6α, ν 1 = − 3 2 , ν 2 = − 1 2 , 1 = − 1 2 E − 1 = − 11α 2 2 , 2 = −E − 1 = −11α 2 : (a) generated potential V 2 (x, 2 ) (continuous line) and initial oneṼ 1 (x, 1 ) (dashed line), with energy levels E n (x)| 2 for the ground state (GS, blue) and the excited states n = 1, 2, 3 (red, green, purple); (d) current density for the excited states with the same colors that in (c).…”
Section: Discussionmentioning
confidence: 99%
“…The first-order intertwining method presented here generalizes the shape invariant technique that different authors have used previously to describe the behavior of an electron near to the Dirac points in a graphene layer with applied external magnetic fields [23][24][25][26][27][28]. Similarly as in [29], we have modified the form of the magnetic field without destroying the exact solvability of the system, by using Schrödinger seed solutions instead of solutions for the associated Riccati equation.…”
Section: Discussionmentioning
confidence: 99%
“…In this work, we have studied the Dirac fermion propagator for graphene-like systems in external magnetic fields. We have constructed the Dirac fermion propagator for graphene-like systems in the presence of non-trivial and inhomogeneous external magnetic fields generated by first-order intertwining operators from the solutions to the Dirac equation for a constant magnetic field and an exponetially decaying magnetic field [27,34,[37][38][39][40]. We constructed the propagator in the basis of the eigenfunctions of the operator (γ • Π) 2 .…”
Section: Final Remarksmentioning
confidence: 99%
“…In addition, the coherent state methods have been started to be applied recently to graphene subject to static homogeneous magnetic fields [179]. As can be seen, the SUSY methods applied to Dirac materials is a very active field which surely will continue its development in the near future [151][152][153][154][155][156][157][158][159][160][161].…”
Section: Recent Applications Of Susy Qmmentioning
confidence: 99%
“…Recently, the SUSY methods started to be used also in the study of Dirac electrons in graphene and some of its allotropes, when external electric or magnetic fields are applied [151][152][153][154][155][156][157][158][159][160][161]. It is worth to mention as well some systems in optics, since there is a well-known correspondence between Schrödinger equation and Maxwell equations in the paraxial approximation, which makes that the SUSY methods can be applied directly in some areas of optics [162][163][164][165][166][167][168][169].…”
Section: Introductionmentioning
confidence: 99%