Poster PDF (4.4mb)
... [1] J. R. Abo-Shaeer, C. Raman, J. M. Vogels, and W. Ketterle, Science 292, 476 (2001). [2] Y.-J. Lin, R. L. Compton, K. Jimenez-Garcia, J. V. Porto, and I. Spielman, Nature 462, 628 (2009). [3] K. Jimenez-Garcia, L. J. LeBlanc, R. A. Williams, M. C. Beeler, A. R. Perry, and I. B. Spielman, Phys. Re ...
... [1] J. R. Abo-Shaeer, C. Raman, J. M. Vogels, and W. Ketterle, Science 292, 476 (2001). [2] Y.-J. Lin, R. L. Compton, K. Jimenez-Garcia, J. V. Porto, and I. Spielman, Nature 462, 628 (2009). [3] K. Jimenez-Garcia, L. J. LeBlanc, R. A. Williams, M. C. Beeler, A. R. Perry, and I. B. Spielman, Phys. Re ...
PDF ∗ , 88K - UCLA Chemistry and Biochemistry
... many types of electronic structure calculations. It is based on two powerful methods of quantum reactive scattering theory, flux-flux correlation function21 and channel decoupling methods.22,23 The imaginary potentials act to impose the correct outgoing boundary conditions on the terminal edges. In ...
... many types of electronic structure calculations. It is based on two powerful methods of quantum reactive scattering theory, flux-flux correlation function21 and channel decoupling methods.22,23 The imaginary potentials act to impose the correct outgoing boundary conditions on the terminal edges. In ...
Quantum Spacetime without Observers: Ontological
... formulation [1], has led to severe conceptual and technical diculties, nonstandard choices of canonical variables, such as in the Ashtekar formulation [2] and in loop quantum gravity [21], have been used as starting points for quantization. While some of the technical problems have been resolved by ...
... formulation [1], has led to severe conceptual and technical diculties, nonstandard choices of canonical variables, such as in the Ashtekar formulation [2] and in loop quantum gravity [21], have been used as starting points for quantization. While some of the technical problems have been resolved by ...
A Noncommutative Sigma Model by Mauritz van den Worm
... and norms squared are replaced by taking the trace of the product of an operator with its adjoint. We explore a finite dimensional σ-model based on the construction of the finite dimensional representation of the quantum torus. In this case we are able to determine an explicit partition function of ...
... and norms squared are replaced by taking the trace of the product of an operator with its adjoint. We explore a finite dimensional σ-model based on the construction of the finite dimensional representation of the quantum torus. In this case we are able to determine an explicit partition function of ...
20040929114512301
... – Decoherence is an interesting problem: heating rates of seconds gives loads of time for gates. – Quantum memories are harder to realize: few qubit applications? ...
... – Decoherence is an interesting problem: heating rates of seconds gives loads of time for gates. – Quantum memories are harder to realize: few qubit applications? ...
A note on the realignment criterion
... but f` (s1 , . . . , sm2 ) > B` (m, n). Therefore, the bound B` (m, n) can be used to detect entanglement for which the realignment criterion fails. Numerical estimations for these bounds were given for (m, n) = (2, 2) and (2, 3) in [10]. The numerical results also suggest that B̃` (2, 2) = B` (2, 2 ...
... but f` (s1 , . . . , sm2 ) > B` (m, n). Therefore, the bound B` (m, n) can be used to detect entanglement for which the realignment criterion fails. Numerical estimations for these bounds were given for (m, n) = (2, 2) and (2, 3) in [10]. The numerical results also suggest that B̃` (2, 2) = B` (2, 2 ...
The quantum field theory (QFT) dual paradigm in fun
... avoiding this catastrophe we have to suppose that C is not constant at all, but vanishes, in the limit T !0, as T 3, so to make !S finite, as it has to be. This means however, that near the absolute 0°C, there is a mismatch between the variation of the body content of energy, and the supply of energ ...
... avoiding this catastrophe we have to suppose that C is not constant at all, but vanishes, in the limit T !0, as T 3, so to make !S finite, as it has to be. This means however, that near the absolute 0°C, there is a mismatch between the variation of the body content of energy, and the supply of energ ...
Even-denominator fractional quantum Hall effect in bilayer graphene
... Graphene-on-substrate is an elastic membrane with (frozen) random height flucuations that cause strain 1) distortion (scalar) potentials; 2) random hopping integrals (gauge potentials) Calculate scattering time (Fermi golden rune) and mobility Scalar = screened Gauge = NOT screened ...
... Graphene-on-substrate is an elastic membrane with (frozen) random height flucuations that cause strain 1) distortion (scalar) potentials; 2) random hopping integrals (gauge potentials) Calculate scattering time (Fermi golden rune) and mobility Scalar = screened Gauge = NOT screened ...
Document
... (spin). A full description must include the spin, with the wavefunctions χsms (2-dimensional vectors in the spin space), which satisfy S 2 χsms = s(s + 1)h̄2χsms Sz χsms = msh̄χsms . If we ignore the interaction between the spin and other degrees of freedom, we can express the wavefunction by ...
... (spin). A full description must include the spin, with the wavefunctions χsms (2-dimensional vectors in the spin space), which satisfy S 2 χsms = s(s + 1)h̄2χsms Sz χsms = msh̄χsms . If we ignore the interaction between the spin and other degrees of freedom, we can express the wavefunction by ...