Scientific Committe Organizing Committe - Harvard
... two large scattering lengths in the three.body system. Tuning is in principle possible for polarizable spin-zero systems with electric field [3]. The effect is strengthened by three simultaneously large scattering lengths but much more decisively influenced by a large mass ratio between two of the p ...
... two large scattering lengths in the three.body system. Tuning is in principle possible for polarizable spin-zero systems with electric field [3]. The effect is strengthened by three simultaneously large scattering lengths but much more decisively influenced by a large mass ratio between two of the p ...
Theoretical study of solitonic excitations in Bose
... (Summary of the Ph.D. thesis) On the basis of quantum mechanics and statistical physics it is verifiable theoretically that a macroscopical part of system of bosonic particles fills the same quantum state at low temperature. This effect was predicted in 1924, but the experimental observation has bee ...
... (Summary of the Ph.D. thesis) On the basis of quantum mechanics and statistical physics it is verifiable theoretically that a macroscopical part of system of bosonic particles fills the same quantum state at low temperature. This effect was predicted in 1924, but the experimental observation has bee ...
Excited states from time-dependent density functional theory
... extremely difficult to find, so often only exchange is used. In DFT, this is called exact exchange (EXX), since exchange is usually only treated approximately. EXX gives useful features such as derivative discontinuities and the correct asymptotic decay of the KS potential[160]. As we will see in Se ...
... extremely difficult to find, so often only exchange is used. In DFT, this is called exact exchange (EXX), since exchange is usually only treated approximately. EXX gives useful features such as derivative discontinuities and the correct asymptotic decay of the KS potential[160]. As we will see in Se ...
Regularity and Approximability of Electronic Wave Functions
... therefore becomes desirable that approximate practical methods of applying quantum mechanics should be developed, which can lead to an explanation of the main features of complex atomic systems without too much computation.” Physicists and chemists followed Dirac’s advice and invented, during the pr ...
... therefore becomes desirable that approximate practical methods of applying quantum mechanics should be developed, which can lead to an explanation of the main features of complex atomic systems without too much computation.” Physicists and chemists followed Dirac’s advice and invented, during the pr ...
Far-infrared-driven electron-hole correlations in a quantum dot with an internal... Roger Sakhel, Lars Jo¨nsson, and John W. Wilkins
... that are not accessible by direct optical excitation. For example, using sequences of NIR and FIR pulses we show that coherent optical excitations can be transferred between radiative and dark pairs of excited states, and that new FIR pathways are created by the Coulomb correlations. Although we thr ...
... that are not accessible by direct optical excitation. For example, using sequences of NIR and FIR pulses we show that coherent optical excitations can be transferred between radiative and dark pairs of excited states, and that new FIR pathways are created by the Coulomb correlations. Although we thr ...
Fault-tolerant quantum repeater with atomic ensembles and linear
... where the relative phase between the entangled states of the two pairs of the remote ensembles is denoted by +* = k+x with +x = xu − xd. In practice, a series of write pulses are sent into the atomic ensembles and the induced Stokes pulses are directed to the detectors. The time interval between nei ...
... where the relative phase between the entangled states of the two pairs of the remote ensembles is denoted by +* = k+x with +x = xu − xd. In practice, a series of write pulses are sent into the atomic ensembles and the induced Stokes pulses are directed to the detectors. The time interval between nei ...
