Chapter 4 Bohr`s model of the atom
... Chapter 4 Bohr’s model of the atom 4.5 Bohr’s postulate Bohr’s postulate (1913): (1) An electron in an atom moves in a circular orbit about the nucleus under the influence of the Coulomb attraction between the electron and the nucleus, obeying the laws of classical mechanics. (2) An electron move i ...
... Chapter 4 Bohr’s model of the atom 4.5 Bohr’s postulate Bohr’s postulate (1913): (1) An electron in an atom moves in a circular orbit about the nucleus under the influence of the Coulomb attraction between the electron and the nucleus, obeying the laws of classical mechanics. (2) An electron move i ...
Cavity dark states for quantum computing M.S. Shahriar , J.A. Bowers
... decay is thus reduced by nearly three orders of magnitude. Thus, the cavity dark state described here achieves the desired transfer of quantum information without being aected signi®cantly by the cavity decay, and yet does not take much longer than the original Pellizari scheme. To summarize, we ha ...
... decay is thus reduced by nearly three orders of magnitude. Thus, the cavity dark state described here achieves the desired transfer of quantum information without being aected signi®cantly by the cavity decay, and yet does not take much longer than the original Pellizari scheme. To summarize, we ha ...
Photon pairs with coherence time exceeding 1 μs
... (not shown in Fig. 1) are switched off and all the atoms are optically pumped to the ground level j1i. During the biphoton generation time, phase-matched Stokes (ωs ) and anti-Stokes (ωas ) paired photons are produced in opposing directions along the MOT longitudinal z axis in the presence of the co ...
... (not shown in Fig. 1) are switched off and all the atoms are optically pumped to the ground level j1i. During the biphoton generation time, phase-matched Stokes (ωs ) and anti-Stokes (ωas ) paired photons are produced in opposing directions along the MOT longitudinal z axis in the presence of the co ...
Many-body levels of optically excited and multiply charged InAs nanocrystals... by semiempirical tight binding
... double-barrier tunneling-junction configuration in STM tunneling measurements. ...
... double-barrier tunneling-junction configuration in STM tunneling measurements. ...
Chapter 28
... ANS: e 56. When electrons interact with a double slit, a. each electron passes through only one of the slits. b. each electron scatters from the sides of only one of the slits. c. each electron passes through both of the slits simultaneously. d. the diffraction pattern shows up on photographic film ...
... ANS: e 56. When electrons interact with a double slit, a. each electron passes through only one of the slits. b. each electron scatters from the sides of only one of the slits. c. each electron passes through both of the slits simultaneously. d. the diffraction pattern shows up on photographic film ...
PDF
... where the atom propagates through only one laser beam with a gaussian field profile. The atom is modeled as a wavepacket with a gaussian distribution in the momentum representation, and it’s evolution in the laser field is calculated numerically. From this the phase shift with rotation is obtained a ...
... where the atom propagates through only one laser beam with a gaussian field profile. The atom is modeled as a wavepacket with a gaussian distribution in the momentum representation, and it’s evolution in the laser field is calculated numerically. From this the phase shift with rotation is obtained a ...
What can we learn from hydrodynamic analysis at RHIC?
... region by using a “cutting edge” hybrid model (CGC + full 3D hydro + hadronic cascade). • This picture is manifestation of the sudden change of entropy density at Tc, namely ...
... region by using a “cutting edge” hybrid model (CGC + full 3D hydro + hadronic cascade). • This picture is manifestation of the sudden change of entropy density at Tc, namely ...
A Chern-Simons E ective Field Theory for the Pfaan Quantum Hall... E. Fradkin , Chetan Nayak , A. Tsvelik
... where Trj is the trace in the spin j representation of SU(2) and P denotes path-ordering. To obtain the degeneracy of the 2n quasihole states, we need to rst observe that the half- ux-quantum quasiholes carry the spin-1=2 representation of SU(2). Let's consider the four quasihole case; the extensio ...
... where Trj is the trace in the spin j representation of SU(2) and P denotes path-ordering. To obtain the degeneracy of the 2n quasihole states, we need to rst observe that the half- ux-quantum quasiholes carry the spin-1=2 representation of SU(2). Let's consider the four quasihole case; the extensio ...
Introduction to Quantum Information
... If we encoded each of the k distinct symbols as a distinct binary number, i.e., as a distinct string of 0’s and 1’s, we would need strings composed of log k bits to represent each symbol (2log k = k). Shannon’s analysis shows that messages produced by a stochastic source can be compressed, in the se ...
... If we encoded each of the k distinct symbols as a distinct binary number, i.e., as a distinct string of 0’s and 1’s, we would need strings composed of log k bits to represent each symbol (2log k = k). Shannon’s analysis shows that messages produced by a stochastic source can be compressed, in the se ...
