The Double Slit Experiment and Quantum Mechanics∗
... the outputs of the detectors on the screen, we got the superposition of two single slit patterns. These patterns are so much alike that their sum looks just like the single slit pattern in Figure 2. It seems that detecting which slit they go through forces them to go through one slit or the other an ...
... the outputs of the detectors on the screen, we got the superposition of two single slit patterns. These patterns are so much alike that their sum looks just like the single slit pattern in Figure 2. It seems that detecting which slit they go through forces them to go through one slit or the other an ...
1 Imaginary Time Path Integral
... Use of Imaginary Time Path Integrals Imaginary time path integrals are practically useful in problems in condensed matter physics and particle physics. Numerical techniques involving random numbers (so-called Monte Carlo methods) are available for evaluating high dimensional real integrals. A typica ...
... Use of Imaginary Time Path Integrals Imaginary time path integrals are practically useful in problems in condensed matter physics and particle physics. Numerical techniques involving random numbers (so-called Monte Carlo methods) are available for evaluating high dimensional real integrals. A typica ...
Nonequilibrium quantum fluctuations of a dispersive medium: Spontaneous emission, photon statistics,
... We study the implications of quantum fluctuations of a dispersive medium, under steady rotation, either in or out of thermal equilibrium with its environment. A rotating object exhibits a quantum instability by dissipating its mechanical motion via spontaneous emission of photons, as well as interna ...
... We study the implications of quantum fluctuations of a dispersive medium, under steady rotation, either in or out of thermal equilibrium with its environment. A rotating object exhibits a quantum instability by dissipating its mechanical motion via spontaneous emission of photons, as well as interna ...
Intensified antibunching via feedback
... statistics of a driven optical system, the number of excitations are initially not limited and new methods are needed to describe quantum feedback effects in driven-damped setups. While there are special cases where driven quantum systems can be considered analytically [25], for most cases a numeri ...
... statistics of a driven optical system, the number of excitations are initially not limited and new methods are needed to describe quantum feedback effects in driven-damped setups. While there are special cases where driven quantum systems can be considered analytically [25], for most cases a numeri ...
Complete Analytical Solutions of the Mie
... eigenfunctions of H(q) respectively, then the HFT states that ∂En (q) ∂H(q) = hΨn (q)| |Ψn (q)i . ...
... eigenfunctions of H(q) respectively, then the HFT states that ∂En (q) ∂H(q) = hΨn (q)| |Ψn (q)i . ...
Quasidistributions in nonlinear quantum optics
... It is well known from the papers by R.J. Glauber [1, 2] published in 1963, founding the modern quantum optics, that optical processes having completely quantum behavior, i.e. having no classical analogue, are described by means of quasidistributions, e.g. using the weighting function in the diagonal ...
... It is well known from the papers by R.J. Glauber [1, 2] published in 1963, founding the modern quantum optics, that optical processes having completely quantum behavior, i.e. having no classical analogue, are described by means of quasidistributions, e.g. using the weighting function in the diagonal ...
The Quantum World
... analogy with the 'real' world of everyday experience is direct. In classical physics I can know both where an electron is and what it is doing. In more technical language, its position and momentum can both simultaneously be known. Such an object is not so very different from a table or a cow, conce ...
... analogy with the 'real' world of everyday experience is direct. In classical physics I can know both where an electron is and what it is doing. In more technical language, its position and momentum can both simultaneously be known. Such an object is not so very different from a table or a cow, conce ...
Kirkwood−Buff Integrals for Finite Volumes
... This finite size effect was corrected by estimating h∞(r) (eq 9), resulting in G̃ R∞ and Ĝ R∞. They practically coincide with the KB integrals of the largest system L/σ = 40. In Figure 3 (right), the corresponding exact finite volume KB integrals GR are plotted as a function of σ/R. The R3 divergence ...
... This finite size effect was corrected by estimating h∞(r) (eq 9), resulting in G̃ R∞ and Ĝ R∞. They practically coincide with the KB integrals of the largest system L/σ = 40. In Figure 3 (right), the corresponding exact finite volume KB integrals GR are plotted as a function of σ/R. The R3 divergence ...
Non-relativistic limit in the 2+ 1 Dirac Oscillator: A Ramsey
... the Zitterbewegung, a helicoidal motion performed by the average position of a free relativistic fermion, can be reinterpreted with the language of Quantum Optics. This dynamical phenomenon also becomes observable in the spin and orbital degrees of freedom, where it can be surprisingly interpreted i ...
... the Zitterbewegung, a helicoidal motion performed by the average position of a free relativistic fermion, can be reinterpreted with the language of Quantum Optics. This dynamical phenomenon also becomes observable in the spin and orbital degrees of freedom, where it can be surprisingly interpreted i ...
