Photon Localization Revisited
... Lorentz group), which is locally isomorphic to the semi-direct product H2 (C) o SL(2, C) of the Jordan algebra H2 (C) of Hermitian (2 × 2)-matrices and SL(2, C), consisting of the energy-momentum vector Pµ and of the Lorentz generators Mµν (composed of angular momenta Mij and of Lorentz boosts M0i ) ...
... Lorentz group), which is locally isomorphic to the semi-direct product H2 (C) o SL(2, C) of the Jordan algebra H2 (C) of Hermitian (2 × 2)-matrices and SL(2, C), consisting of the energy-momentum vector Pµ and of the Lorentz generators Mµν (composed of angular momenta Mij and of Lorentz boosts M0i ) ...
Quantum Information Processing through Nuclear Magnetic
... individual components. In other words, there exist no singleparticle states |φiA and |ηiB such as that |ψi could be written in the form: |ψi = |φiA ⊗ |ηiB ...
... individual components. In other words, there exist no singleparticle states |φiA and |ηiB such as that |ψi could be written in the form: |ψi = |φiA ⊗ |ηiB ...
2.2 Schrödinger`s wave equation
... 2.2 Schrödinger’s wave equation Slides: Video 2.2.1 Schrödinger wave equation introduction Text reference: Quantum Mechanics for Scientists and Engineers Section Chapter 2 introduction ...
... 2.2 Schrödinger’s wave equation Slides: Video 2.2.1 Schrödinger wave equation introduction Text reference: Quantum Mechanics for Scientists and Engineers Section Chapter 2 introduction ...
arXiv:hep-th/0006105v1 15 Jun 2000 Quotient Construction of `t
... In ’t Hooft’s opinion, at the atomic scale quantum states are equivalence classes of primordial states at the Planck scale. If we only care the temporal evolution of equivalence classes, the information within each equivalence class can be ignored. Then from a non-time-reversible evolution, which ch ...
... In ’t Hooft’s opinion, at the atomic scale quantum states are equivalence classes of primordial states at the Planck scale. If we only care the temporal evolution of equivalence classes, the information within each equivalence class can be ignored. Then from a non-time-reversible evolution, which ch ...
Document
... 1. Ion trap (qubit is the ground-state vs excited-state of an electron attached to an ion; “many” ions in one trap) 2. NMR (qubit is the spin of a nuclei on a molecule; “many” spins on a molecule) 3. Josephson-Junction qubits (magnetic flux) 4. Optical qubits (photons) ...
... 1. Ion trap (qubit is the ground-state vs excited-state of an electron attached to an ion; “many” ions in one trap) 2. NMR (qubit is the spin of a nuclei on a molecule; “many” spins on a molecule) 3. Josephson-Junction qubits (magnetic flux) 4. Optical qubits (photons) ...
Chirality is the property of an object to exist as distinguishable mirror
... c) There are several results that we have obtained and that evidence their importance in this context. By using the Clifford algebraic formulation of quantum mechanics we have given mathematical proof of the potentialityactualization transition that in quantum mechanics is admitted instead as postul ...
... c) There are several results that we have obtained and that evidence their importance in this context. By using the Clifford algebraic formulation of quantum mechanics we have given mathematical proof of the potentialityactualization transition that in quantum mechanics is admitted instead as postul ...
Exceptional Points and Dynamical Phase Transitions
... environment, the number of localized states does not change and the widths of the resonance states increase, as expected. Here, the exceptional points are of minor importance. In the other phase, the narrow resonance states are superimposed with a smooth background and the individual spectroscopic f ...
... environment, the number of localized states does not change and the widths of the resonance states increase, as expected. Here, the exceptional points are of minor importance. In the other phase, the narrow resonance states are superimposed with a smooth background and the individual spectroscopic f ...
