to the whole? - Vasil Penchev
... 3. Y-function represents such a concrete asymmetry of a fractal structure in space-time. 4. Physical quantity representing a linear and Hermitian operator in Hilbert space (i.e. Y1Y2 transformation) means some movement of an object in space-time expressed by means of a change of its definitive asym ...
... 3. Y-function represents such a concrete asymmetry of a fractal structure in space-time. 4. Physical quantity representing a linear and Hermitian operator in Hilbert space (i.e. Y1Y2 transformation) means some movement of an object in space-time expressed by means of a change of its definitive asym ...
QUANTUM CRYPTOGRAPHY: PITFALLS AND ASSETS
... key is transmitted the encryption and decryption can ...
... key is transmitted the encryption and decryption can ...
Negative Quasi-Probability, Contextuality, Quantum Magic and the
... Frames and Quasi-probability representations The non-uniqueness of QPR is equivalent to choosing a frame and a dual frame for the Hilbert space of linear operators A frame of operators {F (λ)} is just a spanning set∗ , viz. an overcomplete basis, indexed by λ ∈ Λ. A Hermitian frame {F (λ)} and Herm ...
... Frames and Quasi-probability representations The non-uniqueness of QPR is equivalent to choosing a frame and a dual frame for the Hilbert space of linear operators A frame of operators {F (λ)} is just a spanning set∗ , viz. an overcomplete basis, indexed by λ ∈ Λ. A Hermitian frame {F (λ)} and Herm ...
Grid Enabled Molecular Dynamics: classical and quantum algorithms
... Foster and Kesselman (“The Grid: the blueprint for a new computing infrastructure”) [1], computational Grids are categorized into five major classes of applications. In summary, these classes identify a specific context of applications such as supercomputing applications, high-throughput computing, ...
... Foster and Kesselman (“The Grid: the blueprint for a new computing infrastructure”) [1], computational Grids are categorized into five major classes of applications. In summary, these classes identify a specific context of applications such as supercomputing applications, high-throughput computing, ...
Many-Body effects in Semiconductor Nanostructures Stockholm University Licentiat Thesis
... three dimensions, a partial quantization of energy is achieved. The resulting potential is called a quantum-well, the density of state of which can be seen in Fig. 1.1. By constraining the particle motion to one and then zero dimensions further quantization occurs until one has fully discretized ene ...
... three dimensions, a partial quantization of energy is achieved. The resulting potential is called a quantum-well, the density of state of which can be seen in Fig. 1.1. By constraining the particle motion to one and then zero dimensions further quantization occurs until one has fully discretized ene ...
The landscape of Anderson localization in a disordered medium
... function describing the external forces acting on the particle. The eigenvalues of the Hamiltonian correspond to the energies of these states. The electronic states inside a disordered medium can thus be modeled by introducing a random potential V to account for the material inhomogeneities. For ins ...
... function describing the external forces acting on the particle. The eigenvalues of the Hamiltonian correspond to the energies of these states. The electronic states inside a disordered medium can thus be modeled by introducing a random potential V to account for the material inhomogeneities. For ins ...
Factoring 51 and 85 with 8 qubits
... presented here should be considered as such. In our opinion a genuine implementation should use no knowledge of the value of the order r—including whether or not it is a power of two—because the objective of the quantum stage of the algorithm is to calculate r. Therefore we do not regard the factori ...
... presented here should be considered as such. In our opinion a genuine implementation should use no knowledge of the value of the order r—including whether or not it is a power of two—because the objective of the quantum stage of the algorithm is to calculate r. Therefore we do not regard the factori ...
The Church-Turing thesis in a quantum world
... Simulating physical systems There are quantum systems for which no efficient classical simulation is known, but which we can simulate on a universal quantum computer. What does it mean to “simulate” a physical system? According to the OED, simulation is “the technique of imitating the behaviour of ...
... Simulating physical systems There are quantum systems for which no efficient classical simulation is known, but which we can simulate on a universal quantum computer. What does it mean to “simulate” a physical system? According to the OED, simulation is “the technique of imitating the behaviour of ...
dicke-july2013x
... OK for fixed atoms, but I said we’d consider motion! • We’ve incorporated CoM coordinates into , the “cooperation” operator; does not commute with ! • Thus, these are not stationary eigenstates of . • Classically, relative motion of radiators causes decoherence, but radiators with a common velocity ...
... OK for fixed atoms, but I said we’d consider motion! • We’ve incorporated CoM coordinates into , the “cooperation” operator; does not commute with ! • Thus, these are not stationary eigenstates of . • Classically, relative motion of radiators causes decoherence, but radiators with a common velocity ...
Quantum Computation with Neutral Atoms
... Classical bit: we can find out if it is in state 0 or 1 and the measurement will not change the state of the bit. Qubit: we cannot just measure α and β and thus determine its state! We get either 0 or 1 with corresponding probabilities |α|2 and |β|2. ...
... Classical bit: we can find out if it is in state 0 or 1 and the measurement will not change the state of the bit. Qubit: we cannot just measure α and β and thus determine its state! We get either 0 or 1 with corresponding probabilities |α|2 and |β|2. ...
Gibbs' paradox and black-hole entropy
... between identity and indistinguishability [9]. In classical mechanics, different particles are not identical even if they are indistinguishable; in principle, they can be identified and have therefore to be counted separately.3 In quantum theory, on the other hand, one does not have ‘particles’, but ...
... between identity and indistinguishability [9]. In classical mechanics, different particles are not identical even if they are indistinguishable; in principle, they can be identified and have therefore to be counted separately.3 In quantum theory, on the other hand, one does not have ‘particles’, but ...
lowdin`s remarks on the aufbau principle and a philosopher`s view of
... that particular project had been carried out from the beginning in his laboratory. Very soon the term was being used for all kinds of accurate theoretical work which, at least at first sight, did not involve any fixing of paramenters. Regarding current ab initio calculations it is probably fair to s ...
... that particular project had been carried out from the beginning in his laboratory. Very soon the term was being used for all kinds of accurate theoretical work which, at least at first sight, did not involve any fixing of paramenters. Regarding current ab initio calculations it is probably fair to s ...
