scholarly journals Absence of binding in the Nelson and piezoelectric polaron models

2019 ◽  
Vol 31 (02) ◽  
pp. 1950006
Author(s):  
Gonzalo A. Bley

In the context of the massless Nelson model, we prove that two non-relativistic nucleons interacting with a massless meson field do not bind when a sufficiently strong Coulomb repulsion between the nucleons is added to the Hamiltonian. The result holds for both the renormalized and unrenormalized theories, and can also be applied to the so-called piezoelectric polaron model, which describes an electron interacting with the acoustical vibrational modes of a crystal through the piezoelectric interaction. The result can then be interpreted as well as a no-binding statement about piezoelectric bipolarons. The methods used allow also for a significant reduction of about 30% over previously known no-binding conditions for the optical bipolaron model of H. Fröhlich.

1996 ◽  
Vol 54 (6) ◽  
pp. 4056-4067 ◽  
Author(s):  
Karlo Penc ◽  
Hiroyuki Shiba ◽  
Frédéric Mila ◽  
Takuya Tsukagoshi

2011 ◽  
Vol 89 (2) ◽  
pp. 213-217 ◽  
Author(s):  
Catherine J. Stevenson ◽  
Jordan Kyriakidis

We present results on spin and charge correlations in two-dimensional quantum dots as a function of increasing Coulomb strength (dielectric constant). We look specifically at the orbital occupation of both spin and charge. We find that charge and spin evolve separately, especially at low Coulomb strength. For the charge, we find that a hole develops in the core orbitals at strong Coulomb repulsion, invalidating the common segregation of confined electrons into an inert core and active valence electrons. For excitations, we find a total spin-projection Sz = –1/2 breaks apart into separate occupations of net positive and negative spin. This dissociation is caused by spin correlations alone. Quantum fluctuations arising from long-range Coulomb repulsion destroy the spin dissociation and eventually results in all orbitals carrying a negative spin.


2020 ◽  
Vol 62 (9) ◽  
pp. 1447
Author(s):  
А.О. Злотников ◽  
С.В. Аксенов ◽  
М.С. Шустин

Abstract In the second order of the operator form of the perturbation theory, the effective interactions in a superconducting nanowire have been obtained at the strong electron correlations, when the spin–orbit coupling parameter is comparable with the hopping integral. Using the exact diagonalization technique, in short nanowires with the open boundary conditions at the strong Coulomb repulsion, the excitations corresponding to the Majorana edge states with the energy below the value of a bulk superconducting gap have been demonstrated.


Author(s):  
Ganiyu Debo Adebanjo ◽  
Pavel Kornilovitch ◽  
James Peter Hague

Abstract The majority of fulleride superconductors with unusually high transition-temperature to kinetic-energy ratios have a face-centred-cubic (FCC) structure. We demonstrate that, within extended Hubbard models with strong Coulomb repulsion, paired fermions in FCC lattices have qualitatively different properties than pairs in other three-dimensional cubic lattices. Our results show that strongly bound, light, and small pairs can be generated in FCC lattices across a wide range of the parameter space. We estimate that such pairs can Bose condense at high temperatures even if thelattice constant is large (as in the fullerides).


2007 ◽  
Vol 98 (3) ◽  
Author(s):  
J. P. Hague ◽  
P. E. Kornilovitch ◽  
J. H. Samson ◽  
A. S. Alexandrov

2006 ◽  
Vol 322 (1-2) ◽  
pp. 193-199 ◽  
Author(s):  
Franz J. Kaiser ◽  
Michael Strass ◽  
Sigmund Kohler ◽  
Peter Hänggi

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