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1961por Guo, Donghui, Kondo, Takahiro, Machida, Takahiro, Iwatake, Keigo, Okada, Susumu, Nakamura, Junji“…The charge carriers in graphene are massless Dirac fermions and exhibit a relativistic Landau-level quantization in a magnetic field. …”
Publicado 2012
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1962por Minami, Yasuo, Araki, Kotaro, Dao, Thang Duy, Nagao, Tadaaki, Kitajima, Masahiro, Takeda, Jun, Katayama, Ikufumi“…Among them, carriers in graphene and surface states of topological insulators are known to behave as massless Dirac fermions with a conical band structure in the two-dimensional momentum space, whereas electrons in semimetal bismuth (Bi) are expected to behave as massive Dirac-like fermions in the three-dimensional momentum space, whose dynamics is of particular interest in comparison with that of the massless Dirac fermions. …”
Publicado 2015
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1963“…The Kitaev honeycomb spin model provides a prominent example of exotic fractionalized quasiparticles, composed of itinerant Majorana fermions and gapped gauge fluxes. However, identification of the Majorana fermions in a three-dimensional honeycomb lattice remains elusive. …”
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1964“…Thus if the diphoton enhancement survives further scrutiny, and no charged fermions beneath 150 GeV are found, there must be new bosons far beneath the 10 TeV scale. …”
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1965“…We prove that the invariance of the N=2 superconformal quantum mechanics is controlled by subalgebras of a given twisted superalgebra made of 6 fermionic (nilpotent) generators and 6 bosonic generators (including a central charge). …”
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1966por Abrikosov, A.A., Jr.“…For relativistic Dirac fermions, variations of temperature lead to creation (annihilation) of particle - antiparticle pairs. …”
Publicado 1992
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1967“…We consider here two benchmark scenarios that exemplify the range of possibilities: one in which $\Phi$ is a singlet scalar or pseudoscalar boson whose production and $\gamma \gamma$ decays are due to loops of coloured and charged fermions, and another benchmark scenario in which $\Phi$ is a superposition of (nearly) degenerate CP-even and CP-odd Higgs bosons in a (possibly supersymmetric) two-Higgs doublet model also with additional fermions to account for the $\gamma \gamma$ decay rate. …”
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1968“…To this end we use the worldline formalism to expand the fermionic determinant in powers of 1/N. We consider the hadronic as well as the deconfining phase of the theory. …”
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1969“…We consider the dynamics of fermions with a spatially varying mass which couple to bosons through a Yukawa interaction term and perform a consistent weak coupling truncation of the relevant kinetic equations. …”
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1970“…We outline a full non-perturbative proof of planar (large-N) equivalence between bosonic correlators in a theory with Majorana fermions in the adjoint representation and one with Dirac fermions in the two-index (anti)symmetric representation. …”
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1971“…We study single production of excited electrons at the CERN LHC through contact interactions of fermions. Subsequent decays of excited electrons to ordinary electrons and light fermions via gauge and contact interactions are examined. …”
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1972“…We propose a new baryogenesis scenario based on coherent production and mixing of different fermionic species. The mechanism is operative during phase transitions, at which the fermions acquire masses via Yukawa couplings to scalar fields. …”
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1973“…Theoretically, it has been known that breaking spin degeneracy and effectively realizing spinless fermions is a promising path to topological superconductors. …”
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1974“…But to check whether this Higgs is the Standard Model (SM) Higgs boson or not depends on one of its fundamental properties i.e. it’s coupling to fermions. The sensitivity of Higgs decay to the fermionic final states (H->tau anti-tau, H->bottom anti-bottom) is still limited. …”
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1975por Baulieu, Laurent“…There is a superspace with 6 twisted fermionic directions, with solvable constraints.…”
Publicado 2010
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1976“…The generation of a matter-antimatter asymmetry in the Universe may be induced by the propagation of fermions in non-trivial, spherically asymmetric (and hence Lorentz violating) gravitational backgrounds. …”
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1977“…We present a class of models in which dark matter (DM) is a fermionic singlet under the Standard Model (SM) gauge group but is charged under a symmetry of flavour that acts as well on the SM fermions. …”
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1978“…Away from the singularity the gauge theory has world-sheet matter fields, bosons and fermions, associated with the generation of target space-time. …”
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1979“…Moreover, for massive fermions we give a simple representation of the amplitude for n( gamma ) emission ideally suited for numerical evaluation. …”
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1980“…The Lorentz violation in the Higgs sector is communicated at tree level to fermions (via Yukawa interactions) and to massive gauge bosons, although the most important effect comes from one-loop dia- grams for photons and from two-loop diagrams for fermions. …”
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info:eu-repo/semantics/article