2010
DOI: 10.1088/1751-8113/43/21/215202
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Multiparticle equations for interacting Dirac fermions in magnetically confined graphene quantum dots

Abstract: Abstract. We study the energy of quasi-particles in graphene within the Hartree-Fock approximation.The quasi-particles are confined via an inhomogeneous magnetic field and interact via the Coulomb potential. We show that the associated functional has a minimizer and determines the stability conditions for the N -particle problem in such a graphene quantum dot.

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Cited by 15 publications
(30 citation statements)
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References 33 publications
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“…The numerical algorithm to obtain the HF ground state is standard and can be found, for instance, in Ref. 20…”
Section: B Numerical Approachesmentioning
confidence: 99%
See 1 more Smart Citation
“…The numerical algorithm to obtain the HF ground state is standard and can be found, for instance, in Ref. 20…”
Section: B Numerical Approachesmentioning
confidence: 99%
“…We then follow Sucher 29 and confine the Hilbert space to positive-energy eigenstates of the full singleparticle problem, i.e., we assume an inert filled Dirac sea. This projection approach has been successfully employed in the same context before, 19,20 and one can analyze also other values for the chemical potential. The accuracy of this method was carefully assessed in Ref.…”
Section: Introductionmentioning
confidence: 99%
“…When the field is switched off completely and correspondingly the factor exp(−ν 2 2 /2) omitted from the trial function (4.1) (such that the normalization constant reduces to N 2 = (2Z ) 3 2 +γ / 4πΓ(3 + 2γ) ), the energy functional is given by…”
Section: Stability Of Antibinding For Modified Trial Functionsmentioning
confidence: 99%
“…In accord with the experimental spectrum the electron mass is thereby set equal to zero [1]. Also a mathematical analysis of the two-dimensional confinement by this magnetic field was provided for the case of interacting massless multi-fermions [3].…”
Section: Introductionmentioning
confidence: 99%
“…In Sec. 5, we turn to a waveguide geometry, defined by a suitable inhomogeneous magnetic field [25,26,27,28,29,30,31,32,33,34]. We show that the SOIs give rise to inter-esting spin textures of the chiral states propagating in the waveguides.…”
Section: Introductionmentioning
confidence: 99%