q -entropies and the entanglement dynamics of two-qubits interacting with an... 408 A. Hamadou-Ibrahim et al.
... quantum phenomena that lie at the heart of the present understanding of the fabric of Nature [1–4]. There is nowadays wide consensus that entanglement constitutes the most distinctive feature of the quantum mechanical description of the physical world. The multiple manifestations of quantum entangle ...
... quantum phenomena that lie at the heart of the present understanding of the fabric of Nature [1–4]. There is nowadays wide consensus that entanglement constitutes the most distinctive feature of the quantum mechanical description of the physical world. The multiple manifestations of quantum entangle ...
International Journal of Mathematics, Game Theory and Algebra
... minus infinity and 1 at infinity), with only weights located on the unit sphere. We see that the weights required for u. a. p. are not necessary to be of an arbitrarily large magnitude. But what if they are too restricted. How can one learn approximation properties of networks with an arbitrarily re ...
... minus infinity and 1 at infinity), with only weights located on the unit sphere. We see that the weights required for u. a. p. are not necessary to be of an arbitrarily large magnitude. But what if they are too restricted. How can one learn approximation properties of networks with an arbitrarily re ...
L6 - Physics
... Therefore P2 = I and the parity operator is unitary. If the interaction Hamiltonian (H) conserves parity then [H,P]=0, and: PY(x, y, z) = Y(-x, -y, -z) = nY(x, y, z) with n = eigenvalue of P P2Y(x, y, z) = PPY(x, y, z) = nPY(x, y, z) = n2Y(x, y, z) Y(x, y, z) = n2Y(x, y, z) n2 = 1 so, n=1 or n=-1 ...
... Therefore P2 = I and the parity operator is unitary. If the interaction Hamiltonian (H) conserves parity then [H,P]=0, and: PY(x, y, z) = Y(-x, -y, -z) = nY(x, y, z) with n = eigenvalue of P P2Y(x, y, z) = PPY(x, y, z) = nPY(x, y, z) = n2Y(x, y, z) Y(x, y, z) = n2Y(x, y, z) n2 = 1 so, n=1 or n=-1 ...
On the Distribution of the Wave Function for Systems in Thermal
... are represented by probability distributions on the phase space. In quantum mechanics, ensembles are usually represented by density matrices. It is natural to regard these density matrices as arising from probability distributions on the (normalized) wave functions associated with the thermodynamica ...
... are represented by probability distributions on the phase space. In quantum mechanics, ensembles are usually represented by density matrices. It is natural to regard these density matrices as arising from probability distributions on the (normalized) wave functions associated with the thermodynamica ...
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 ...
Unconditionally Secure Quantum Signatures
... communication channels and in how many of, e.g., pairwise quantum channels are needed. All known information-theoretically secure “classical” signature schemes also use shared secret keys, which would have to be obtained in an information-theoretically secure way, for example using QKD, making them ...
... communication channels and in how many of, e.g., pairwise quantum channels are needed. All known information-theoretically secure “classical” signature schemes also use shared secret keys, which would have to be obtained in an information-theoretically secure way, for example using QKD, making them ...
Resonances, dissipation and decoherence in exotic and artificial atoms
... By the rather general term ’exotic atoms’ one usually refers to atomic systems in which an electron is replaced by a heavy negative particle, such as for example a muon or an antiproton. Such systems are of considerable interest, since they make it possible to study the dependence of the atomic leve ...
... By the rather general term ’exotic atoms’ one usually refers to atomic systems in which an electron is replaced by a heavy negative particle, such as for example a muon or an antiproton. Such systems are of considerable interest, since they make it possible to study the dependence of the atomic leve ...
An Introduction to Quantum Game Theory
... nondegenerate, there are N solutions for E, say En , n = 1, 2, . . ., N. The En eigenvalues, or energy levels, are associated with an N-eigenvector-basis for the state space of ψ . The following year Erwin Schrödinger, looking for an electromagnetic interpretation of the same phenomena, published h ...
... nondegenerate, there are N solutions for E, say En , n = 1, 2, . . ., N. The En eigenvalues, or energy levels, are associated with an N-eigenvector-basis for the state space of ψ . The following year Erwin Schrödinger, looking for an electromagnetic interpretation of the same phenomena, published h ...
Programmable architecture for quantum computing Jialin Chen, Lingli Wang, Edoardo Charbon,
... for scalable chip-based quantum computer architectures as it allows the interaction between distant qubits without SWAP gates so as to offer individual addressability. For this reason, we will concentrate on the qubus system [14,15]—an important kind of ancilla-based model—which combines both matter ...
... for scalable chip-based quantum computer architectures as it allows the interaction between distant qubits without SWAP gates so as to offer individual addressability. For this reason, we will concentrate on the qubus system [14,15]—an important kind of ancilla-based model—which combines both matter ...
Overview Andrew Jaramillo Research Statement
... Moreover, all of the above results were for quantizations of the standard Borel and parabolic subalgebras in Lie groups/algebras of type A. There are standard ways to define quantized coordinate rings in types B, C, D, and the exceptional types, both for q not a root of unity and q a root of unity. ...
... Moreover, all of the above results were for quantizations of the standard Borel and parabolic subalgebras in Lie groups/algebras of type A. There are standard ways to define quantized coordinate rings in types B, C, D, and the exceptional types, both for q not a root of unity and q a root of unity. ...
