2013
DOI: 10.1007/978-3-319-00266-8_14
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The Topology of the Quantum Vacuum

Abstract: Topology in momentum space is the main characteristics of the ground states of a system at zero temperature, the quantum vacua. The gaplessness of fermions in bulk, on the surface or inside the vortex core is protected by topology, and is not sensitive to details of the microscopic physics (atomic or trans-Planckian). Irrespective of the deformation of the parameters of the microscopic theory, the energy spectrum of these fermions remains strictly gapless. This solves the main hierarchy problem in particle phy… Show more

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Cited by 81 publications
(114 citation statements)
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References 145 publications
(307 reference statements)
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“…In the present work, based on first-principles calculations and effective model analysis, we demonstrate that the antiperovskite Cu 3 PdN is a new candidate for realizing NLS and "drumhead"-like surface flat bands [12,[39][40][41][42][43], which may open an important route to achieving high-temperature superconductivity [44][45][46]. Strong SOC will drive NLS in Cu 3 PdN into Dirac semimetal state with three pairs of Dirac points, leading to exotic surface Fermi arcs which can be observed on various surfaces of this material.…”
mentioning
confidence: 99%
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“…In the present work, based on first-principles calculations and effective model analysis, we demonstrate that the antiperovskite Cu 3 PdN is a new candidate for realizing NLS and "drumhead"-like surface flat bands [12,[39][40][41][42][43], which may open an important route to achieving high-temperature superconductivity [44][45][46]. Strong SOC will drive NLS in Cu 3 PdN into Dirac semimetal state with three pairs of Dirac points, leading to exotic surface Fermi arcs which can be observed on various surfaces of this material.…”
mentioning
confidence: 99%
“…The protection of a nodal line can be inferred from the topological number of the form [39][40][41][42][43] …”
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confidence: 99%
“…Different Weyl points can be related to each other by symmetries: K 1 and K 2 (or K 3 and K 4 ) are related by Π (110) ≡ π (110) or T a 3 π (110) and therefore dubbed a 'Π pair', K 1 and K 3 (or K 2 and K 4 ) are related by Π (110) S and called a 'ΠS pair', and finally K 1 and K 4 (or K 2 and K 3 ) are related by S and named a 'S pair'. It is known [64][65][66] that a Weyl fermion can carry topological charge or chirality, which can be extracted from Chern number (CN) on a small spherical surface surrounding the Weyl point. Two Weyl points related by mirror symmetry have opposite Chern numbers while time reversal operation leaves Chern number of a Weyl point unchanged.…”
Section: B Weyl Semimetal Phase and Topological Mirrormentioning
confidence: 99%
“…This framework leads to a modified neutrino dispersion relation depending on the momentum of the neutrino.  The neutrino velocity can be modified by Fermi point splitting (for a recent review see [18]), which removes the degeneracy of zeros of the fermionic energy spectrum [19].  The neutrino dispersion relation can change because of environmental effects caused by fields that accumulate at the position of the Earth.…”
Section: Introductionmentioning
confidence: 99%