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... As we can see, the LQBH metric brings quantum gravity corrections, expressed in terms of LQC parameters like P and a0 , to the black hole thermodynamical properties like temperature and entropy. Such corrections could induce modifications in the way how the black hole evaporates. In the following, w ...
... As we can see, the LQBH metric brings quantum gravity corrections, expressed in terms of LQC parameters like P and a0 , to the black hole thermodynamical properties like temperature and entropy. Such corrections could induce modifications in the way how the black hole evaporates. In the following, w ...
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... Abstract. We study the critical behavior of Ising quantum magnets with broadly distributed random couplings (J), such that P (ln J) ∼ | ln J|−1−α , α > 1, for large | ln J| (Lévy flight statistics). For sufficiently broad distributions, α < αc , the critical behavior is controlled by a line of fixe ...
... Abstract. We study the critical behavior of Ising quantum magnets with broadly distributed random couplings (J), such that P (ln J) ∼ | ln J|−1−α , α > 1, for large | ln J| (Lévy flight statistics). For sufficiently broad distributions, α < αc , the critical behavior is controlled by a line of fixe ...
Comments on the 2nd order bootstrap relation
... to solve it was incorrect. In this note we demonstrate that these objections are totally unfounded. They are a result of a misinterpretation of the potential used in [2], which is a different quantity as compared to the kernel used in [1,3]. We also derive the 2nd order bootstrap relation of [1] in ...
... to solve it was incorrect. In this note we demonstrate that these objections are totally unfounded. They are a result of a misinterpretation of the potential used in [2], which is a different quantity as compared to the kernel used in [1,3]. We also derive the 2nd order bootstrap relation of [1] in ...
Evolution as context-driven actualisation of potential: toward
... has several limitations, including the linearity of the Hilbert space, and the fact that it can only describe the extreme case where change of state is maximally contextual. Other mathematical theories, such as state–context–property (SCOP) systems,44 lift the quantum formalism out of its specific s ...
... has several limitations, including the linearity of the Hilbert space, and the fact that it can only describe the extreme case where change of state is maximally contextual. Other mathematical theories, such as state–context–property (SCOP) systems,44 lift the quantum formalism out of its specific s ...
Nicolas Gisin - Quantum Nonlocality
... Quantum nonlocality based on finite-speed causal influences leads to superluminal signalling, arXiv:1110.3795 Nature is nonlocal in the sense of discontinuous ...
... Quantum nonlocality based on finite-speed causal influences leads to superluminal signalling, arXiv:1110.3795 Nature is nonlocal in the sense of discontinuous ...
Quantum One-Way Communication is Exponentially Stronger Than
... Can quantum one-way communication be exponentially stronger than classical two-way communication in computing a function? Such a result might be the strongest possible separation between quantum communication and classical communication. There have been quite a few partial results in this direction. ...
... Can quantum one-way communication be exponentially stronger than classical two-way communication in computing a function? Such a result might be the strongest possible separation between quantum communication and classical communication. There have been quite a few partial results in this direction. ...
A family of spin-S chain representations of SU(2) k Wess
... quantization and statistics of spinons as the fundamental excitations of quantum spin chains [17]. In this respect, ...
... quantization and statistics of spinons as the fundamental excitations of quantum spin chains [17]. In this respect, ...
Quantum transport of two-species Dirac fermions in dual-gated three-dimensional topological insulators ARTICLE
... elemental charge and : is the Plank’s constant h divided by 2p. The zeroth LL at E0 ¼ 0 is equally shared between electrons and holes, giving rise to the half-integer shift in the quantized Hall conductivity sxy ¼ g(N þ 1/2)e2/h, where g is the number of degenerate species of Dirac fermions (for exa ...
... elemental charge and : is the Plank’s constant h divided by 2p. The zeroth LL at E0 ¼ 0 is equally shared between electrons and holes, giving rise to the half-integer shift in the quantized Hall conductivity sxy ¼ g(N þ 1/2)e2/h, where g is the number of degenerate species of Dirac fermions (for exa ...
Unit 2: Lorentz Invariance
... Time-reversal leads to conservation of energy. This happens to be a Lorentz Transformation also. ¨ Parity leads to conservation of momentum. This happens to be a Lorentz Transformation also ...
... Time-reversal leads to conservation of energy. This happens to be a Lorentz Transformation also. ¨ Parity leads to conservation of momentum. This happens to be a Lorentz Transformation also ...
Chap 12.
... by considering a concrete example–the ammonia molecule NH3 . In any symmetry operation on NH3 , the nitrogen atom remains fixed but the hydrogen atoms can be permuted in 3!=6 different ways. The axis of the molecule is called a C3 axis, since the molecule can be rotated about it into 3 equivalent or ...
... by considering a concrete example–the ammonia molecule NH3 . In any symmetry operation on NH3 , the nitrogen atom remains fixed but the hydrogen atoms can be permuted in 3!=6 different ways. The axis of the molecule is called a C3 axis, since the molecule can be rotated about it into 3 equivalent or ...
Quantum error correction
... the field of quantum error correction highly relies on classical error correction, initially there were several obstacles that prolonged the adaptation of classical correcting codes to quantum systems. In 1995 Shor published his paper on 9–qubit code [5] that can correct an arbitrary single–qubit er ...
... the field of quantum error correction highly relies on classical error correction, initially there were several obstacles that prolonged the adaptation of classical correcting codes to quantum systems. In 1995 Shor published his paper on 9–qubit code [5] that can correct an arbitrary single–qubit er ...
Planes, Chains, and Orbits: Quantum Oscillations and High
... and the lattice vibration (phonon) component vanishes as T3 . The two different power-laws ultimately arise from the different quantum statistics of electrons (fermions) and phonons (bosons). With the application of an intense magnetic field H, the electronic orbits are quantized in a Fermi liquid m ...
... and the lattice vibration (phonon) component vanishes as T3 . The two different power-laws ultimately arise from the different quantum statistics of electrons (fermions) and phonons (bosons). With the application of an intense magnetic field H, the electronic orbits are quantized in a Fermi liquid m ...