Maximizing the entanglement of two mixed qubits
... how can one increase its linear entropy given a certain degree of entanglement? It was shown by Lewenstein and Sanpera 关26兴 that any two-qubit entangled state can be written as a mixture of a separable state and a single pure entangled state. The Werner state 共4兲 is recognizably of this form. All it ...
... how can one increase its linear entropy given a certain degree of entanglement? It was shown by Lewenstein and Sanpera 关26兴 that any two-qubit entangled state can be written as a mixture of a separable state and a single pure entangled state. The Werner state 共4兲 is recognizably of this form. All it ...
achieving 128-bit security against quantum attacks in openvpn
... (which is always possible because NAND is functionally complete), and then converting this circuit to a quantum circuit built from Toffoli gates, as described in [11]. For example, f can be implemented as a function that returns 0 if and only if the input is an AES-key for a certain plaintextciphert ...
... (which is always possible because NAND is functionally complete), and then converting this circuit to a quantum circuit built from Toffoli gates, as described in [11]. For example, f can be implemented as a function that returns 0 if and only if the input is an AES-key for a certain plaintextciphert ...
achieving 128-bit security against quantum attacks in openvpn
... (which is always possible because NAND is functionally complete), and then converting this circuit to a quantum circuit built from Toffoli gates, as described in [11]. For example, f can be implemented as a function that returns 0 if and only if the input is an AES-key for a certain plaintextciphert ...
... (which is always possible because NAND is functionally complete), and then converting this circuit to a quantum circuit built from Toffoli gates, as described in [11]. For example, f can be implemented as a function that returns 0 if and only if the input is an AES-key for a certain plaintextciphert ...
boltzmann`s entropy and time`s arrow
... RX. Now we see the problem with our definite assignment of a time order to the snapshots in the figure: Going from a macrostate Ma at time ta to another macrostate Mb at time tb (th = ta + r, r > 0) means that there is a microstate X in YM that gives rise to a microstate Y in TM (at time tb); but th ...
... RX. Now we see the problem with our definite assignment of a time order to the snapshots in the figure: Going from a macrostate Ma at time ta to another macrostate Mb at time tb (th = ta + r, r > 0) means that there is a microstate X in YM that gives rise to a microstate Y in TM (at time tb); but th ...
The Equivalence Myth of Quantum Mechanics
... we need to be clear about the meaning of ‘mathematical equivalence’ and of ‘physical theory’. We characterise these terms in (a); and we present the mathematical structures of matrix mechanics in (b) and those of wave mechanics in (c), as expounded in Part I, Sections 3 and 4, respectively. (a) The ...
... we need to be clear about the meaning of ‘mathematical equivalence’ and of ‘physical theory’. We characterise these terms in (a); and we present the mathematical structures of matrix mechanics in (b) and those of wave mechanics in (c), as expounded in Part I, Sections 3 and 4, respectively. (a) The ...
Compatibility of Quark and Resonant Picture Excited Baryon
... The quark model has historically served as the paradigm for understanding the general patterns of excited baryonic states. In important ways, however, this picture is unsatisfactory. In particular, it is entirely unclear how to obtain the quark model as a direct consequence of fundamental QCD intera ...
... The quark model has historically served as the paradigm for understanding the general patterns of excited baryonic states. In important ways, however, this picture is unsatisfactory. In particular, it is entirely unclear how to obtain the quark model as a direct consequence of fundamental QCD intera ...
On the Wave Function of the Photon
... that one would associate with a one-photon wave function, including also an acceptable probabilistic interpretation. Photons are much different from massive particles. They are also different from neutrinos since the photon number does not obey a conservation law. These differences are a source of c ...
... that one would associate with a one-photon wave function, including also an acceptable probabilistic interpretation. Photons are much different from massive particles. They are also different from neutrinos since the photon number does not obey a conservation law. These differences are a source of c ...
The Logic of Complementarity - Philsci
... It should be remarked that it seems to exist a discrepancy between Rosenfeld and Bohr in what concerns the way of understanding complementarity. This difference may justify Bohr’s refuse to accept that von Weizsäcker had described ’the logic os complementarity’, as we shall see below. Apparently, B ...
... It should be remarked that it seems to exist a discrepancy between Rosenfeld and Bohr in what concerns the way of understanding complementarity. This difference may justify Bohr’s refuse to accept that von Weizsäcker had described ’the logic os complementarity’, as we shall see below. Apparently, B ...
... the stable states of the system. Neural networks have been shown to be capable of recognizing even distorted patterns and process information with a high level of noise. Another novel approach to information processing is quantum computation, which makes use of quantum superpositions and entanglemen ...
Full-Text PDF
... where M is identified as the black hole ADM mass. In the case of LQBHs, we shall take, for practical purposes, the changing in the mass parameter m related with the black hole ADM mass through the Equation (7). Therefore, we shall consider that a reduction in the black hole ADM mass will correspond ...
... where M is identified as the black hole ADM mass. In the case of LQBHs, we shall take, for practical purposes, the changing in the mass parameter m related with the black hole ADM mass through the Equation (7). Therefore, we shall consider that a reduction in the black hole ADM mass will correspond ...
Unified rotational and permutational symmetry and selection rules in
... What can representation theory tell us? 1)U є U(2I+1) leaves ψ ψ invariant (U✝U=Id.) 2)P є SN describes permutation of particles ...
... What can representation theory tell us? 1)U є U(2I+1) leaves ψ ψ invariant (U✝U=Id.) 2)P є SN describes permutation of particles ...
ןב תטיסרבינוא - בגנב ןוירוג
... “enough” precision, to control its interaction with other qubits, and to do so during a time interval “much shorter” than the decoherence time. 1.5 Qubit-specific measurement capability. Theoretically, we should be able to measure the state of each qubit independently of any other parameters of the ...
... “enough” precision, to control its interaction with other qubits, and to do so during a time interval “much shorter” than the decoherence time. 1.5 Qubit-specific measurement capability. Theoretically, we should be able to measure the state of each qubit independently of any other parameters of the ...
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... complex plane - Cauchy’s theorem - multiple connected regions - Cauchy integral formula - Derivatives of analytic function - Taylor and Laurent series - Singularities - Residue theorem - Evaluation of real integrals Application: Potential theory - (1) Electrostatic fields and complex potentials - Pa ...
... complex plane - Cauchy’s theorem - multiple connected regions - Cauchy integral formula - Derivatives of analytic function - Taylor and Laurent series - Singularities - Residue theorem - Evaluation of real integrals Application: Potential theory - (1) Electrostatic fields and complex potentials - Pa ...
