Quantum simulations with cold trapped ions
... potential use as frequency standards (e.g. Dehmelt (1981) and references therein). Today, by using trapped ions as frequency standards unsurpassed accuracy and precision have been reached (e.g. Rosenband et al (2008) and references therein), and in addition, trapped ions are used for a wide range of ...
... potential use as frequency standards (e.g. Dehmelt (1981) and references therein). Today, by using trapped ions as frequency standards unsurpassed accuracy and precision have been reached (e.g. Rosenband et al (2008) and references therein), and in addition, trapped ions are used for a wide range of ...
Molecular dynamics: an account of its evolution
... The equations of motion are constructed from this Hamiltonian and then reinterpreted in real variables. Hoover [24] showed that a different set of non-Newtonian equations of motion, that is free of the time scaling introduced by Nosé, can be used to carry out canonical ensemble MD simulations. Many ...
... The equations of motion are constructed from this Hamiltonian and then reinterpreted in real variables. Hoover [24] showed that a different set of non-Newtonian equations of motion, that is free of the time scaling introduced by Nosé, can be used to carry out canonical ensemble MD simulations. Many ...
XVIIth International Workshop on Quantum Atomic and Molecular
... Since then, numerous phenomena related to this effect, completely absent, even unthinkable of in classical mechanics have been discovered and continue to be discovered at a regular rate, with also many applications in chemistry and molecular physics. We look forward to learning about some of the mos ...
... Since then, numerous phenomena related to this effect, completely absent, even unthinkable of in classical mechanics have been discovered and continue to be discovered at a regular rate, with also many applications in chemistry and molecular physics. We look forward to learning about some of the mos ...
Theory and applications of light-matter interactions in Gerasimos Angelatos
... â - bosonic field annihilation operator. Like associated modes f , denoted â(r; ω) if modes are continuous and âλ if they are discrete. σ̂ ± - Pauli raising/lowering matrices for quantum dot state. g - quantum optical coupling rate ΩR - Rabi field S 0 (ω) - bare spontaneous emission spectrum S(rD ...
... â - bosonic field annihilation operator. Like associated modes f , denoted â(r; ω) if modes are continuous and âλ if they are discrete. σ̂ ± - Pauli raising/lowering matrices for quantum dot state. g - quantum optical coupling rate ΩR - Rabi field S 0 (ω) - bare spontaneous emission spectrum S(rD ...
∗ ∗
... they can never warrant them. But physical theories can unambiguously show that whatever the ultimate reality may be, it will not conform to our common sense. And quantum mechanics is a particular striking illustration of the latter point. But what exactly is the trouble with quantum mechanics? Perha ...
... they can never warrant them. But physical theories can unambiguously show that whatever the ultimate reality may be, it will not conform to our common sense. And quantum mechanics is a particular striking illustration of the latter point. But what exactly is the trouble with quantum mechanics? Perha ...
Renormalisation of Noncommutative Quantum Field Theory
... Four-dimensional quantum field theory suffers from infrared and ultraviolet divergences as well as from the divergence of the renormalized perturbation expansion. Despite the impressive agreement between theory and experiments and despite many attempts, these problems are not settled and remain a bi ...
... Four-dimensional quantum field theory suffers from infrared and ultraviolet divergences as well as from the divergence of the renormalized perturbation expansion. Despite the impressive agreement between theory and experiments and despite many attempts, these problems are not settled and remain a bi ...
Electronic Transport in One-Dimensional - Goldhaber
... box. The data indicate a gate-induced transition between singlet and triplet ground states for the dot. (c) Magnetic field dependence of the conductance at the point marked by the white triangle in 4a (a,b) Magnetic field evolution of conductance versus bias voltage on the left (triplet) and right ( ...
... box. The data indicate a gate-induced transition between singlet and triplet ground states for the dot. (c) Magnetic field dependence of the conductance at the point marked by the white triangle in 4a (a,b) Magnetic field evolution of conductance versus bias voltage on the left (triplet) and right ( ...
Single and double bosonic stimulation of THz emission in polaritonic systems
... with the dark exciton THz emitter based on polaritonic cascade lasers (i.e. cases (i) and (ii), respectively) will be analysed using Eqs. 2 and 3. For the last type of the THz emitter (iii) the emission probability used was taken to W 5 103 s21. Polaritons are formed by coupled photons and excitons, ...
... with the dark exciton THz emitter based on polaritonic cascade lasers (i.e. cases (i) and (ii), respectively) will be analysed using Eqs. 2 and 3. For the last type of the THz emitter (iii) the emission probability used was taken to W 5 103 s21. Polaritons are formed by coupled photons and excitons, ...
A unification of photons, electrons, and gravitons under qbit
... A unification of photons, electrons, and gravitons under qbit models ...
... A unification of photons, electrons, and gravitons under qbit models ...
Improve The Convergence of Jarzynski Equality through Fast
... a long time to accomplish, based on recent work on transitionless quantum driving [14], we accelerate the adiabatic process by adding a control Hamiltonian to the original Hamiltonian. We study the convergence of Jarzynski equality under this fast-forward adiabatic process and a normal non-adiabatic ...
... a long time to accomplish, based on recent work on transitionless quantum driving [14], we accelerate the adiabatic process by adding a control Hamiltonian to the original Hamiltonian. We study the convergence of Jarzynski equality under this fast-forward adiabatic process and a normal non-adiabatic ...
