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Sborlini - High Energy Physics
... 2. Solution: Some theorems (KLN) guarantee that they can be cancelled in the final physical result (if we are computing IR safe observables…). For instance, the cancellation can be implemented through the subtraction method. (See: Muta, Foundations of Quantum Chromodynamics) ...
... 2. Solution: Some theorems (KLN) guarantee that they can be cancelled in the final physical result (if we are computing IR safe observables…). For instance, the cancellation can be implemented through the subtraction method. (See: Muta, Foundations of Quantum Chromodynamics) ...
Paired states of fermions in two dimensions with breaking of parity
... mode physics, from those connected with topological effects, quasiparticle zero modes and Hall-type responses for unbroken symmetries. In this paper we will make extensive use of the methods for BCS paired states, and consider the transitions between the weak and strong coupling regimes in two dimen ...
... mode physics, from those connected with topological effects, quasiparticle zero modes and Hall-type responses for unbroken symmetries. In this paper we will make extensive use of the methods for BCS paired states, and consider the transitions between the weak and strong coupling regimes in two dimen ...
Summarising Constraints On Dark Matter At The Large Hadron
... fermion (spin-half particle) has a super-partner with spin-0, and each boson (integerspin) has a spin-half super-partner. Stable supersymmetric particles are possible weakly interacting massive particle (WIMP) candidates and thus also candidates for dark matter [5]. This means that dark matter could ...
... fermion (spin-half particle) has a super-partner with spin-0, and each boson (integerspin) has a spin-half super-partner. Stable supersymmetric particles are possible weakly interacting massive particle (WIMP) candidates and thus also candidates for dark matter [5]. This means that dark matter could ...
What can string theory teach us about condensed matter physics?
... field theory which is relativistically invariant (where the spin-wave velocity plays the role of the velocity of “light”). • The quantum field theory is invariant under scale and conformal transformations at the quantum critical point: a CFT3 ...
... field theory which is relativistically invariant (where the spin-wave velocity plays the role of the velocity of “light”). • The quantum field theory is invariant under scale and conformal transformations at the quantum critical point: a CFT3 ...
Pair Production and the Light-front Vacuum
... special theory of relativity and quantum mechanics in the late 1920s (Dirac, 1927), quantum vacuum has emerged as an extremely interesting medium with remarkable properties to investigate. QED has been extremely successful in explaining the physical phenomena involving the interaction between light ...
... special theory of relativity and quantum mechanics in the late 1920s (Dirac, 1927), quantum vacuum has emerged as an extremely interesting medium with remarkable properties to investigate. QED has been extremely successful in explaining the physical phenomena involving the interaction between light ...
Majorana Fermions - Physics | Oregon State University
... MFs in Quantum Spin Liquids? Just this month, Banerjee et al. have claimed to observe MFs in QSLs: Quantum spin liquids (QSLs) are topological states of matter exhibiting remarkable properties such as the capacity to protect quantum information from decoherence. Whereas their featureless ground sta ...
... MFs in Quantum Spin Liquids? Just this month, Banerjee et al. have claimed to observe MFs in QSLs: Quantum spin liquids (QSLs) are topological states of matter exhibiting remarkable properties such as the capacity to protect quantum information from decoherence. Whereas their featureless ground sta ...
The Scattering of α and β Particles by Matter and
... chance of a second encounter involving another large deflexion is very small. If, for example, the probability of a single deflexion φ in passing through a thickness t is 1/1000, the probability of two successive deflexions each of value φ is 1/106 , and is negligibly small. The angular distribution ...
... chance of a second encounter involving another large deflexion is very small. If, for example, the probability of a single deflexion φ in passing through a thickness t is 1/1000, the probability of two successive deflexions each of value φ is 1/106 , and is negligibly small. The angular distribution ...