PPT
... function and results in particle behavior. • Single photons can interfere with themselves because as long as no measurement has been performed to determine precisely which path the photon has taken, it will behave as a wave. ...
... function and results in particle behavior. • Single photons can interfere with themselves because as long as no measurement has been performed to determine precisely which path the photon has taken, it will behave as a wave. ...
Tunneling and the Vacuum Zero
... of the stochastic processes theory is the study of escape rates over a potential barrier. The theoretical approach, first proposed by Kramers [1], has many applications in chemistry kinetics, diffusion in solids, nucleation [2], and other phenomena [3]. The essential structure of the escape process ...
... of the stochastic processes theory is the study of escape rates over a potential barrier. The theoretical approach, first proposed by Kramers [1], has many applications in chemistry kinetics, diffusion in solids, nucleation [2], and other phenomena [3]. The essential structure of the escape process ...
Universal quantum interfaces
... quantum logic circuit of N logic gates can be built up using no more than O(d 2 nN) pairwise operations, where d is the typical dimension of a subsystem. If the systems are qubits then the quantum logic circuit can be built up in O(nN) operations. For example, the coupled systems could themselves be ...
... quantum logic circuit of N logic gates can be built up using no more than O(d 2 nN) pairwise operations, where d is the typical dimension of a subsystem. If the systems are qubits then the quantum logic circuit can be built up in O(nN) operations. For example, the coupled systems could themselves be ...
1 Universal entanglement dynamics Quantum Entanglement Growth
... Recommended with a commentary by Rahul Nandkishore, CU Boulder Quantum entanglement is a phenomenon whereby distinct degrees of freedom exhibit ‘quantum correlations’ such that the wavefunction of the entire system cannot be expressed simply as a product of the wavefunctions of individual degrees of ...
... Recommended with a commentary by Rahul Nandkishore, CU Boulder Quantum entanglement is a phenomenon whereby distinct degrees of freedom exhibit ‘quantum correlations’ such that the wavefunction of the entire system cannot be expressed simply as a product of the wavefunctions of individual degrees of ...
Experimental quantum teleportation articles
... a distant location one does not need the original parts and pieces— all that is needed is to send the scanned information so that it can be used for reconstructing the object. But how precisely can this be a true copy of the original? What if these parts and pieces are electrons, atoms and molecules ...
... a distant location one does not need the original parts and pieces— all that is needed is to send the scanned information so that it can be used for reconstructing the object. But how precisely can this be a true copy of the original? What if these parts and pieces are electrons, atoms and molecules ...
Program: DYNQUA - Toulon University - February
... strong pseudospectral effect, a tiny perturbation can dramatically modify the spectrum of such an operator. Hager & Sjöstrand have thus considered adding small random pertubations, and proved that the eigenvalues of the perturbed operator typically spread over the classical spectrum, satisfying a pr ...
... strong pseudospectral effect, a tiny perturbation can dramatically modify the spectrum of such an operator. Hager & Sjöstrand have thus considered adding small random pertubations, and proved that the eigenvalues of the perturbed operator typically spread over the classical spectrum, satisfying a pr ...
Teacher text
... quantum waves, i.e.: the particle cannot reach certain position, because it can reach that position in different ways. The reduction of the wave-packet demonstrates in a very conclusive way that quantum particles are not only waves; they also have a particle-aspect. When the position of a quantum-ob ...
... quantum waves, i.e.: the particle cannot reach certain position, because it can reach that position in different ways. The reduction of the wave-packet demonstrates in a very conclusive way that quantum particles are not only waves; they also have a particle-aspect. When the position of a quantum-ob ...
Proton tomography with Wigner distributions
... The classical interpretation of GPDs as Wigner quasiprobabilities is valid in deep DGLAP domain! ...
... The classical interpretation of GPDs as Wigner quasiprobabilities is valid in deep DGLAP domain! ...
Document
... Einstein used kinetic theory to show that this motion could be explained by the statistical process of many collisions of molecules Detailed predictions of properties of the motion verified three years later. So, atoms are real (still controversial at the time) Still an active area of research! ...
... Einstein used kinetic theory to show that this motion could be explained by the statistical process of many collisions of molecules Detailed predictions of properties of the motion verified three years later. So, atoms are real (still controversial at the time) Still an active area of research! ...
- City Research Online
... deformation parameter β used in [2] by τ employed in [1]. It is well known that when given only a non-Hermitian Hamiltonian, the metric operator can not be uniquely determined. However, as argued in [1] with the specification of the observable X, which coincides in [2] and [1], the outcome is unique ...
... deformation parameter β used in [2] by τ employed in [1]. It is well known that when given only a non-Hermitian Hamiltonian, the metric operator can not be uniquely determined. However, as argued in [1] with the specification of the observable X, which coincides in [2] and [1], the outcome is unique ...
Ohmic vs Markovian heat bath — two-page
... M q̂¨ = −V 0 (q̂) − η q̂˙ + Xt . In the high-T limit β → 0, the correlation tends to be time-local: βCXX (t) → 2ηδ(t). Thus the random force Xt becomes a classical white-noise: hXt Xu istoch = 2ηkB T δ(t − u). Now, replacing q̂ by q would yield the classical Langevin equation, its solution q(t) at V ...
... M q̂¨ = −V 0 (q̂) − η q̂˙ + Xt . In the high-T limit β → 0, the correlation tends to be time-local: βCXX (t) → 2ηδ(t). Thus the random force Xt becomes a classical white-noise: hXt Xu istoch = 2ηkB T δ(t − u). Now, replacing q̂ by q would yield the classical Langevin equation, its solution q(t) at V ...
