EUBET 2014: Applications of effective field theories to particle
... If there is new physics in the electroweak breaking sector, the failed LHC searches suggest a mass gap, so the Higgs itself can be a Goldstone boson (as are the longitudinal vector bosons too). We can then formulate an effective theory for their interactions. With it, we have calculated the one-loop ...
... If there is new physics in the electroweak breaking sector, the failed LHC searches suggest a mass gap, so the Higgs itself can be a Goldstone boson (as are the longitudinal vector bosons too). We can then formulate an effective theory for their interactions. With it, we have calculated the one-loop ...
Ch.1 Identical particles
... the quantization of Maxwell's equations without sources and currents, is only possible when commutation relations between the eld operators are imposed leading to Bose-Einstein statistics. Bosons can be identi ed by integer intrinsic spin appropriate for fundamental particles like photons and gluon ...
... the quantization of Maxwell's equations without sources and currents, is only possible when commutation relations between the eld operators are imposed leading to Bose-Einstein statistics. Bosons can be identi ed by integer intrinsic spin appropriate for fundamental particles like photons and gluon ...
Quantum Mechanics Booklet
... Twentieth Century physicists predicted that a perfect black body would give out radiation of an infinite density when it reached thermal equilibrium (when the black body was absorbing the same amount of energy as it was giving off) This prediction was called the ‘ultraviolet catastrophe’. “If this w ...
... Twentieth Century physicists predicted that a perfect black body would give out radiation of an infinite density when it reached thermal equilibrium (when the black body was absorbing the same amount of energy as it was giving off) This prediction was called the ‘ultraviolet catastrophe’. “If this w ...
The Learnability of Quantum States
... Belovs 2012: Explicit (n2/3) adversary lower bound for element distinctness There must be an explicit (n1/3) adversary lower bound for collision. So, find it! ...
... Belovs 2012: Explicit (n2/3) adversary lower bound for element distinctness There must be an explicit (n1/3) adversary lower bound for collision. So, find it! ...
Anyons in the fractional quantum Hall effect
... by totaly antisymmetric, and totaly symmetric wavefunctions, respectively. Furthermore, there is a connection between spin s and statistics α = 2πs ...
... by totaly antisymmetric, and totaly symmetric wavefunctions, respectively. Furthermore, there is a connection between spin s and statistics α = 2πs ...
Quantum computing with nanoscale infrastructure
... world are able to collect chains of 8-10 ionised atoms. Each of these atoms can be made to behave like a two-level spin-half system, called quantum bit or qubit. The bits are manipulated and flipped by laser radiation. Moreover, the ions are coupled together by their electric fields to a vibrating s ...
... world are able to collect chains of 8-10 ionised atoms. Each of these atoms can be made to behave like a two-level spin-half system, called quantum bit or qubit. The bits are manipulated and flipped by laser radiation. Moreover, the ions are coupled together by their electric fields to a vibrating s ...
Pdf
... A new cluster development for the logarithm of the grand partition function of a system of interacting particles is derived. The leading term in this expansion is the pressure exerted by an ideal Bose or Fermi gas at the same temperature and absolute activity Z as the actual system. Succeeding terms ...
... A new cluster development for the logarithm of the grand partition function of a system of interacting particles is derived. The leading term in this expansion is the pressure exerted by an ideal Bose or Fermi gas at the same temperature and absolute activity Z as the actual system. Succeeding terms ...
