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Results 1 - 10
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161
The factorized S-matrix of CFT/AdS
, 2004
"... We argue that the recently discovered integrability in the large-N CFT/AdS system is equivalent to diffractionless scattering of the corresponding hidden elementary excitations. This suggests that, perhaps, the key tool for finding the spectrum of this system is neither the gauge theory’s dilatati ..."
Abstract
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Cited by 240 (7 self)
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We argue that the recently discovered integrability in the large-N CFT/AdS system is equivalent to diffractionless scattering of the corresponding hidden elementary excitations. This suggests that, perhaps, the key tool for finding the spectrum of this system is neither the gauge theory’s
Quantum vs Classical Mechanics: role of elementary excitations
, 2003
"... Simple theorems relating a quantum mechanical system to the corresponding classical one at equilibrium and connecting the quantum eigenvalues to the frequencies of normal modes oscillations are presented. Corresponding to each quantum eigenfunction, a ‘classical eigenfunction ’ is associated. Those ..."
Magnetic elementary excitations effects on a Co
"... INTRODUCTION In the last few years, several attentions have been given to the development and the research on magnetic ultrathin films and the multi-layer one. This is due to both the interest towards the comprehension of magnetic properties in quasitwo -dimensional systems and their various potent ..."
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the importance of the magnetic elementary excitations contribution. In this work we present a preliminary study of a cobalt super-lattice in the framework of linear spin wave theory. The first Brillowin light scattering (BLS) investigation on a twodimensional systems performed by Kerkmann and al[14] has showed
Finding the elementary excitations of Bose-condensed neutral atoms in a trap
, 1995
"... We describe a method for finding the excitation frequencies of a Bosecondensed collection of trapped, neutral atoms. These excitations are the equivalents of the collisionless phonons in a homogeneous gas. Numerical results for a small assembly of trapped atoms are also presented. We discuss how one ..."
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Cited by 1 (0 self)
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We describe a method for finding the excitation frequencies of a Bosecondensed collection of trapped, neutral atoms. These excitations are the equivalents of the collisionless phonons in a homogeneous gas. Numerical results for a small assembly of trapped atoms are also presented. We discuss how
Correspondence to:
"... The term ‘scaling’, to many, is veiled in a nimbus of exciting mys-tery. At a basic level, part of the mystery simply comes from confu-sion of two connotations of the word—meaning either scale invariance (i.e. processes behaving similarly at small and large scales) or upscal-ing/downscaling (i.e. ag ..."
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.e. aggregating/disaggregating data). However, once this hurdle is surmounted, from whence does this excitement come and in what direction does it lead? If we follow the scale invariance track of enquiry, some hidden signature of hydrologic systems that can be encapsulated in beautifully simple equations
Anyons in an exactly solved model and beyond
, 2005
"... A spin 1/2 system on a honeycomb lattice is studied. The interactions between nearest neighbors are of XX, YY or ZZ type, depending on the direction of the link; different types of interactions may differ in strength. The model is solved exactly by a reduction to free fermions in a static Z2 gauge f ..."
Abstract
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Cited by 85 (2 self)
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properties of excitation depend on ν mod 16, whereas ν itself governs edge thermal transport. The paper also provides mathematical background on anyons as well as an elementary theory of Chern number for quasidiagonal matrices.
Gapped itinerant spin excitations account for missing entropy in the hidden-order state of URu2Si2.” Nat
- Phys
, 2007
"... Many correlated electron materials, such as high-temperature superconductors 1 , geometrically frustrated oxides 2 and lowdimensional magnets 3,4 , are still objects of fruitful study because of the unique properties that arise owing to poorly understood many-body effects. Heavy-fermion metals 5 -m ..."
Abstract
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Cited by 1 (0 self)
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. The gapping of these excitations, which corresponds to a loss of accessible states, accounts for the reduction in γ through the transition at 17.5 K.
On the Observation of Phase Transitions in Collisions of Elementary
, 2000
"... We investigate the excitation function of directed flow, which can provide a clear signature of the creation of the QGP and demonstrate that the minimum of the directed flow does not correspond to the softest point of the EoS for isentropic expansion. A novel technique measuring the compactness is i ..."
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We investigate the excitation function of directed flow, which can provide a clear signature of the creation of the QGP and demonstrate that the minimum of the directed flow does not correspond to the softest point of the EoS for isentropic expansion. A novel technique measuring the compactness
The Higgs Boson in the Periodic System of Elementary Particles
, 2013
"... Copyright © 2013 Ding-Yu Chung, Ray Hefferlin. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. It is proposed that the observed Higgs ..."
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exist in the lepton condensate as a composite of μ ’ and μ’ ± hidden leptons and their corresponding antileptons. The calculated average mass of the hidden lep-ton condensate is 128.8 GeV in good agreements with the observed 125 or 126 GeV. The masses of the hidden lepton con-densate and all elementary
Effect of Hidden Channels on Low-Lying Channels
, 1967
"... The channel coupling effect is discussed for the two-channel amplitude when the threshold of the second channel is very high. The amplitude is written as the sum of the pure elastic term and the channel coupling term. In the low energy region in the first cbannel, the channel coupling term can be ap ..."
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be approximated by the modified Born term of an elementary particle (Z3~0) or intermediate one (Z3=0) corresponding to the cases whether the pure elastic term of the second channel contains a bound state or not, respectively. It is proposed to classify particles and resonances to three categories according
Results 1 - 10
of
161
