Spin-Orbit Coupling for Photons and Polaritons in
... of the total intensity emitted by each level, with maxima located at the center of each micropillar, as expected from the tight-binding calculation, Eq. (2). The phase structure of the eigenmodes can be accessed by performing interferometric measurements in the following way [35]. The photoluminesce ...
... of the total intensity emitted by each level, with maxima located at the center of each micropillar, as expected from the tight-binding calculation, Eq. (2). The phase structure of the eigenmodes can be accessed by performing interferometric measurements in the following way [35]. The photoluminesce ...
Power-Law Entanglement Spectrum in Many-Body Localized
... many quasi-local integrals of motion (LIOMs) [11–13]. In addition to distinct dynamical properties, ergodic and MBL systems are sharply distinguished by the microscopic nature of their eigenstates. This difference can be probed via quantum-information measures, such as entanglement entropy (EE). Giv ...
... many quasi-local integrals of motion (LIOMs) [11–13]. In addition to distinct dynamical properties, ergodic and MBL systems are sharply distinguished by the microscopic nature of their eigenstates. This difference can be probed via quantum-information measures, such as entanglement entropy (EE). Giv ...
Mathematical foundation of quantum annealing
... introduced control parameter, which, by reducing slowly from a high value to zero, we hope to drive the system to the state with the lowest value of the energy 共cost function兲, reaching the solution of the optimization problem. The idea is that the system is expected to stay close to thermal equilib ...
... introduced control parameter, which, by reducing slowly from a high value to zero, we hope to drive the system to the state with the lowest value of the energy 共cost function兲, reaching the solution of the optimization problem. The idea is that the system is expected to stay close to thermal equilib ...
Lectures on Thermodynamics and Statistical Mechanics
... Mechanics which I taught during the fall term of 2014, and plan to teach again for the spring term 2016. This is a course meant for upper level undergraduate students in physics, so that is the level at which most topics are discussed. I have formatted the notes for easier reading. The material is f ...
... Mechanics which I taught during the fall term of 2014, and plan to teach again for the spring term 2016. This is a course meant for upper level undergraduate students in physics, so that is the level at which most topics are discussed. I have formatted the notes for easier reading. The material is f ...
QI Package for Mathematica 7.0 (version 0.3.27) - ZKSI
... Superoperator – Superoperator[kl] returns matrix representation of quantum channel given as a list of Kraus operators. Superoperator[fun,dim] is just am alternative name for ChannelToMatrix[fun,dim] and returns matrix representation of quantum channel, given as a pure function, acting on dim-dimensi ...
... Superoperator – Superoperator[kl] returns matrix representation of quantum channel given as a list of Kraus operators. Superoperator[fun,dim] is just am alternative name for ChannelToMatrix[fun,dim] and returns matrix representation of quantum channel, given as a pure function, acting on dim-dimensi ...
appendix 2 - School of Physics
... constant comparison process, the concept maps were revisited and analysed with respect to the concept of uncertainty. The concept label provided to the students was ‘Uncertainty Principle’, the way students used this label on their maps fell into three groups. The first group (5 maps) did not link u ...
... constant comparison process, the concept maps were revisited and analysed with respect to the concept of uncertainty. The concept label provided to the students was ‘Uncertainty Principle’, the way students used this label on their maps fell into three groups. The first group (5 maps) did not link u ...
Mutually Unbiased bases: a brief survey
... be free of some statistical error. Two questions arise at this point: Given a measurement and assuming an initial probability distribution for the unknown state how can we extract an estimate for the density matrix? What are the measurements that minimize the statistical error? Complete collections ...
... be free of some statistical error. Two questions arise at this point: Given a measurement and assuming an initial probability distribution for the unknown state how can we extract an estimate for the density matrix? What are the measurements that minimize the statistical error? Complete collections ...
Born approximation - BYU Physics and Astronomy
... A. To develop a formalism where we express the wave function in terms of Green’s functions B. To use Helmholtz equation instead of Schrödinger equation C. To find an approximate expression for when far away from the scattering center for a given potential V D. To express the scattering factor in t ...
... A. To develop a formalism where we express the wave function in terms of Green’s functions B. To use Helmholtz equation instead of Schrödinger equation C. To find an approximate expression for when far away from the scattering center for a given potential V D. To express the scattering factor in t ...
Schroedinger`s cat states generated by the environment
... thereby creating macroscopic GHZ like states [23] for the N spin ensemble. Since the bath spectrum is continuous, the formation of such perfect cat states is not possible. Yet, the formation of high-purity cat states may still be possible. For an Ohmic spectrum with the Debye cutoff ωD we find fM = ...
... thereby creating macroscopic GHZ like states [23] for the N spin ensemble. Since the bath spectrum is continuous, the formation of such perfect cat states is not possible. Yet, the formation of high-purity cat states may still be possible. For an Ohmic spectrum with the Debye cutoff ωD we find fM = ...
Spin-to-orbital conversion of the angular momentum of light and its
... a uniform birefringent phase retardation δ and a transverse optical axis pattern with a nonzero topological charge. The pattern is defined by the number q of rotations that the optical axis exhibits in a path circling once around the center of the plate, where a topological defect must be present (q ...
... a uniform birefringent phase retardation δ and a transverse optical axis pattern with a nonzero topological charge. The pattern is defined by the number q of rotations that the optical axis exhibits in a path circling once around the center of the plate, where a topological defect must be present (q ...
Decoherence and open quantum systems
... In quantum information theory entanglement is used as a source for many different applications, for instance in quantum cryptography, teleportation schemes or quantum computation. To keep this entanglement in the system as long as possible we have to protect it against different environmental influe ...
... In quantum information theory entanglement is used as a source for many different applications, for instance in quantum cryptography, teleportation schemes or quantum computation. To keep this entanglement in the system as long as possible we have to protect it against different environmental influe ...
Atomic Bose-Hubbard Systems with Single-Particle
... I would like to thank my advisor, Markus Greiner, for five wonderful years in his group. Markus is extremely supportive of every group member and very open to new ideas. He is an incredibly gifted experimentalist with an amazing ability to explain most of our experiments in terms of beamsplitters an ...
... I would like to thank my advisor, Markus Greiner, for five wonderful years in his group. Markus is extremely supportive of every group member and very open to new ideas. He is an incredibly gifted experimentalist with an amazing ability to explain most of our experiments in terms of beamsplitters an ...
