ABSTRACT RANDOM ROUTING AND CONCENTRATION IN QUANTUM SWITCHING NETWORKS
... crossbar concentrators. Sparse crossbar concentrators are rectangular grids of simple 2 × 2 switches or crosspoints, with the switches arranged such that any k inputs can be connected to some k outputs. We give the design of the quantum crosspoints for such concentrators and devise a self-routing me ...
... crossbar concentrators. Sparse crossbar concentrators are rectangular grids of simple 2 × 2 switches or crosspoints, with the switches arranged such that any k inputs can be connected to some k outputs. We give the design of the quantum crosspoints for such concentrators and devise a self-routing me ...
Superfluid Helium 3: Link between Condensed Matter Physics and
... Soon after the discovery of the phase transitions by Osheroff et al.12 it was possible to identify altogether three distinct stable superfluid phases of bulk 3 He ; these are referred to as the A, B and A1 phases. In zero magnetic field only the A and B phases are stable. In particular, in zero fiel ...
... Soon after the discovery of the phase transitions by Osheroff et al.12 it was possible to identify altogether three distinct stable superfluid phases of bulk 3 He ; these are referred to as the A, B and A1 phases. In zero magnetic field only the A and B phases are stable. In particular, in zero fiel ...
msc_f_p1b2 - Bhoj University
... does not show it distinctly. In some cases the size of h line is not same due to unavoidable reasons but it conveys the same meaning. Some conventions In the above discussion we have written = (). It is more convenient to follow some rules now onwards. Observe change in presentation that follows ...
... does not show it distinctly. In some cases the size of h line is not same due to unavoidable reasons but it conveys the same meaning. Some conventions In the above discussion we have written = (). It is more convenient to follow some rules now onwards. Observe change in presentation that follows ...
The Automorphic Universe
... if T −1 B = B (mod 0). In this case, there exist a T − invariant set B e = B (mod 0). A function f : X → R is T −invariant if UT f = f , that B i.e. f ◦ T = T . In this case, f is constant on every trajectory of the map T . Again, if T preserves a measure µ, then we say that f is T −invariant (mod 0 ...
... if T −1 B = B (mod 0). In this case, there exist a T − invariant set B e = B (mod 0). A function f : X → R is T −invariant if UT f = f , that B i.e. f ◦ T = T . In this case, f is constant on every trajectory of the map T . Again, if T preserves a measure µ, then we say that f is T −invariant (mod 0 ...
Interplay of driving, nonlinearity and dissipation in nanoscale and ultracold atom systems
... (i) Not all condensed matter systems are embedded in the ordinary threedimensional space. Reduced dimensionality arises in a lattice with strongly anisotropic interactions or when the degrees of freedom in a given spatial dimension are frozen due to a gap larger than the chemical potential in the co ...
... (i) Not all condensed matter systems are embedded in the ordinary threedimensional space. Reduced dimensionality arises in a lattice with strongly anisotropic interactions or when the degrees of freedom in a given spatial dimension are frozen due to a gap larger than the chemical potential in the co ...
String theory as a Lilliputian world
... the formalism know as dynamical triangulation (DT) was suggested as an alternative [2]. It discretized the independent intrinsic worldsheet geometry used in the Polyakov formulation of bosonic string theory [3] and the integration over these geometries were approximated by a summation over triangula ...
... the formalism know as dynamical triangulation (DT) was suggested as an alternative [2]. It discretized the independent intrinsic worldsheet geometry used in the Polyakov formulation of bosonic string theory [3] and the integration over these geometries were approximated by a summation over triangula ...
Quantum Heisenberg models and their probabilistic representations
... The graphs of physical relevance are regular lattices such as Zd (or large finite boxes in Zd ), and the factor 2#objects need be present. What should we expect in this case? A few hints come from the models of spatial random permutations, which also involve one-dimensional objects living in higher ...
... The graphs of physical relevance are regular lattices such as Zd (or large finite boxes in Zd ), and the factor 2#objects need be present. What should we expect in this case? A few hints come from the models of spatial random permutations, which also involve one-dimensional objects living in higher ...
Two-dimensional momentum imaging of Rydberg states using half-cycle pulse ionization
... operators. Details of the wave function remain mostly hidden. In (e,2e) experiments 关1兴, the wave function of an atom or molecule in its ground state is retrieved in momentum space using the fact that at sufficiently high energy (⬃1 keV) the electron-electron collision is impulsive. From the final m ...
... operators. Details of the wave function remain mostly hidden. In (e,2e) experiments 关1兴, the wave function of an atom or molecule in its ground state is retrieved in momentum space using the fact that at sufficiently high energy (⬃1 keV) the electron-electron collision is impulsive. From the final m ...
Coupling Quantum Tunneling with Cavity Photons
... could thus map photonic states onto electron tunneling states that can be read out in charge transport. This suggests new strategies for quantum readout and optical interconnects—for example, as a variable pulse delay element in dipolariton signal processing. Furthermore, interactions between dipola ...
... could thus map photonic states onto electron tunneling states that can be read out in charge transport. This suggests new strategies for quantum readout and optical interconnects—for example, as a variable pulse delay element in dipolariton signal processing. Furthermore, interactions between dipola ...
SU(3) symmetry and Baryon wave functions
... • Two ways to form a totally symmetric wave-function from spin and isospin states: 1. combine totally symmetric spin and isospin wave-function 2. combine mixed symmetry spin and mixed symmetry isospin states ...
... • Two ways to form a totally symmetric wave-function from spin and isospin states: 1. combine totally symmetric spin and isospin wave-function 2. combine mixed symmetry spin and mixed symmetry isospin states ...
The Two Slit Experiment
... We now repeat the experiment for a third time, but in this case we use electrons. Here we imagine that there is a beam of electrons incident normally on a screen with the two slits, with all the electrons having the same energy E and momentum p. The screen is a fluorescent screen, so that the arriva ...
... We now repeat the experiment for a third time, but in this case we use electrons. Here we imagine that there is a beam of electrons incident normally on a screen with the two slits, with all the electrons having the same energy E and momentum p. The screen is a fluorescent screen, so that the arriva ...
Practical Quantum Coin Flipping
... less than 1, unless computational assumptions are considered. In other words, a dishonest player can force the outcome of the coin flip with probability 1. In the quantum model, where the two parties share a quantum channel, it was also proven that perfect coin flipping is informationtheoretically i ...
... less than 1, unless computational assumptions are considered. In other words, a dishonest player can force the outcome of the coin flip with probability 1. In the quantum model, where the two parties share a quantum channel, it was also proven that perfect coin flipping is informationtheoretically i ...
Classical field records of a quantum system: Their internal
... A major consideration in our work here has been to remain independent of trap geometry. This basically requires working in the local density approximation (LDA). As an example of variations with geometry that can occur without an LDA approach, optimal energy cutoffs found on the basis of the distrib ...
... A major consideration in our work here has been to remain independent of trap geometry. This basically requires working in the local density approximation (LDA). As an example of variations with geometry that can occur without an LDA approach, optimal energy cutoffs found on the basis of the distrib ...