Fluctuations of kinematic quantities in p+p interactions at the CERN
... Very low momentum conservation hill visible at (0, π) on averaged distribution and on multiplicity bins distributions. Quite difficult to observe, because it is masked by: ...
... Very low momentum conservation hill visible at (0, π) on averaged distribution and on multiplicity bins distributions. Quite difficult to observe, because it is masked by: ...
Weyl calculus with respect to the Gaussian measure and L^p
... • ab is the Fourier-Plancherel transform of a, • the unitary operators exp(i(uX + vD)) on L2 (Rd , γ) are defined through the action exp(i(uX + vD))f (x) := exp(iux + 21 iuv )f (v + x) (formally apply the Baker-Campbell-Hausdorff formula and use the commutator relations, or note that it give a unita ...
... • ab is the Fourier-Plancherel transform of a, • the unitary operators exp(i(uX + vD)) on L2 (Rd , γ) are defined through the action exp(i(uX + vD))f (x) := exp(iux + 21 iuv )f (v + x) (formally apply the Baker-Campbell-Hausdorff formula and use the commutator relations, or note that it give a unita ...
What time reversal invariance is and why it matters
... classical electrodynamical world, and if the sequence of dynamical conditions corresponding to Si, …, Sf is Di, …, Df, and if we write the sequence of dynamical conditions corresponding to Sf, …, Si as RDf, …, RDi, then the transformation from Dk to RDk can involve nothing whatsoever other than reve ...
... classical electrodynamical world, and if the sequence of dynamical conditions corresponding to Si, …, Sf is Di, …, Df, and if we write the sequence of dynamical conditions corresponding to Sf, …, Si as RDf, …, RDi, then the transformation from Dk to RDk can involve nothing whatsoever other than reve ...
Topics in Ultracold Atomic Gases: Strong Interactions and Quantum
... of several specific systems. We find the Fermi gases across narrow Feshbach resonances are strongly interacting at low temperature even when the magnetic field is several widths away from the resonance. We also discuss an approach to describe the metastable repulsive branch of Bose and Fermi gases a ...
... of several specific systems. We find the Fermi gases across narrow Feshbach resonances are strongly interacting at low temperature even when the magnetic field is several widths away from the resonance. We also discuss an approach to describe the metastable repulsive branch of Bose and Fermi gases a ...
Spin Algebra, Spin Eigenvalues, Pauli Matrices Lecture 10
... This equation has two solutions: bbot (a) = btop (a) + ~, and bbot (a) = −btop (a). But bbot (a) must be smaller than btop (a), so only the second solution works. Therefore bbot (a) = −btop (a). Hence b, which is the eigenvalue of Sz , ranges from −btop (a) to btop (a). Furthermore, since S− lowers ...
... This equation has two solutions: bbot (a) = btop (a) + ~, and bbot (a) = −btop (a). But bbot (a) must be smaller than btop (a), so only the second solution works. Therefore bbot (a) = −btop (a). Hence b, which is the eigenvalue of Sz , ranges from −btop (a) to btop (a). Furthermore, since S− lowers ...
Many Body Physics
... ε and ε + dε. Its expression can be easily obtained by noting that the total number of states with an energy lower than ε is given by X L(ε) = θ(ε − εα ) ...
... ε and ε + dε. Its expression can be easily obtained by noting that the total number of states with an energy lower than ε is given by X L(ε) = θ(ε − εα ) ...
Dynamics of Open Quantum Systems
... subtleties typically also emerge with other approaches/methods to quantum dissipation; thus it is beneficial to dwell on these in some detail. Important features of the QLE are: • The QLE (2) is an operator equation that acts in the full Hilbert space of system and bath. The coupling between system a ...
... subtleties typically also emerge with other approaches/methods to quantum dissipation; thus it is beneficial to dwell on these in some detail. Important features of the QLE are: • The QLE (2) is an operator equation that acts in the full Hilbert space of system and bath. The coupling between system a ...
Development of semi-classical and quantum tools for the
... smaller and faster devices. Therefore, the simulations tools needed to be able, to understand the behavior of emerging electron devices and to improve them, have to be reinvented for each new generation of devices. The International Technology Roadmap for Semiconductors predicts that, in ten years, ...
... smaller and faster devices. Therefore, the simulations tools needed to be able, to understand the behavior of emerging electron devices and to improve them, have to be reinvented for each new generation of devices. The International Technology Roadmap for Semiconductors predicts that, in ten years, ...
Quantum nonlocality
... •Leibniz: “there are never in nature two exactly similar entities in which one cannot find an internal difference” We all know that two electrons exhibit no internal differences. •In classical physics one can try to “individuate” absolutely identical objects by considering their locations in space a ...
... •Leibniz: “there are never in nature two exactly similar entities in which one cannot find an internal difference” We all know that two electrons exhibit no internal differences. •In classical physics one can try to “individuate” absolutely identical objects by considering their locations in space a ...
Interacting Fock spaces: central limit theorems and quantum
... ii) we are able to construct the approximating sequence of random variables. The main technical tool used to reach such a theorem is given by a special class of interacting Fock spaces (IFS), namely the 1-mode type Free interacting Fock spaces. More precisely, after introducing a new basic operator ...
... ii) we are able to construct the approximating sequence of random variables. The main technical tool used to reach such a theorem is given by a special class of interacting Fock spaces (IFS), namely the 1-mode type Free interacting Fock spaces. More precisely, after introducing a new basic operator ...
Singularity of the time-energy uncertainty in adiabatic perturbation
... eigenstate would remain in the instantaneous eigenstate of the time-dependent Hamiltonian up to the dynamical and Berry phases11,12. It may seem quite reasonable then that all physical properties in the adiabatic limit should be obtainable from the instantaneous eigenstate. However, this conjecture ...
... eigenstate would remain in the instantaneous eigenstate of the time-dependent Hamiltonian up to the dynamical and Berry phases11,12. It may seem quite reasonable then that all physical properties in the adiabatic limit should be obtainable from the instantaneous eigenstate. However, this conjecture ...
Mirror QCD and Cosmological Constant
... the ground state energy of the universe. In particular, an invisible QCD sector reconstructing Dark Energy was suggested in Refs. [10,43] while a unified description of Dark Matter and Dark Energy originating from invisible QCD dynamics was proposed in Refs. [44,45]. Below, we will demonstrate that ...
... the ground state energy of the universe. In particular, an invisible QCD sector reconstructing Dark Energy was suggested in Refs. [10,43] while a unified description of Dark Matter and Dark Energy originating from invisible QCD dynamics was proposed in Refs. [44,45]. Below, we will demonstrate that ...
