Advanced Quantum Mechanics
... . Elastic scattering off immobile targets: here, the target is effectively so heavy that its mass can be considered infinite. In such cases, scattering is dominantly elastic, ∆E = −∆ = 0. The scattering target can be modelled by some potential distribution, fixed in real space, and arbitrary moment ...
... . Elastic scattering off immobile targets: here, the target is effectively so heavy that its mass can be considered infinite. In such cases, scattering is dominantly elastic, ∆E = −∆ = 0. The scattering target can be modelled by some potential distribution, fixed in real space, and arbitrary moment ...
What General Chemistry Students Know
... characters of an electron orbital Student2: The speedy electron. S: It would be, like, nucleus which we knew where it was and it would sort of be, like, a mess around it, and in that scribbled mess would be where you find the electron, somewhere in there. P: Mm-hmm. When you say where we would find ...
... characters of an electron orbital Student2: The speedy electron. S: It would be, like, nucleus which we knew where it was and it would sort of be, like, a mess around it, and in that scribbled mess would be where you find the electron, somewhere in there. P: Mm-hmm. When you say where we would find ...
(Haroche) File
... exchange excitation at the rate ilef. Such behavior is a well-known feature of the interaction of an atom with a classical monochromatic field. These so called "Rabi oscillations" are familiar in nuclear magnetic resonance and optical transient experiments. In cavity QED, however, the atom couples t ...
... exchange excitation at the rate ilef. Such behavior is a well-known feature of the interaction of an atom with a classical monochromatic field. These so called "Rabi oscillations" are familiar in nuclear magnetic resonance and optical transient experiments. In cavity QED, however, the atom couples t ...
A continued fraction resummation form of bath
... with one or more high-order corrections of K (2k) (k ≥ 2). For the leading-order QKE correction K (4), various resummation methods, e.g., the Pade approximation12 and the LandauZener approximation,32 have been well discussed previously. Although these approximations can significantly improve the sec ...
... with one or more high-order corrections of K (2k) (k ≥ 2). For the leading-order QKE correction K (4), various resummation methods, e.g., the Pade approximation12 and the LandauZener approximation,32 have been well discussed previously. Although these approximations can significantly improve the sec ...
Quantum Dot Computing Gates
... II-VI, III-V, or IV-IV. The size of QD ranges from several to tens of nanometers (10−9 m) in diameter, which is about 10-100 atoms’. A QD can contain from a single electron to several thousand electrons since the size of the quantum dot is designable. QD are fabricated in semiconductor material in s ...
... II-VI, III-V, or IV-IV. The size of QD ranges from several to tens of nanometers (10−9 m) in diameter, which is about 10-100 atoms’. A QD can contain from a single electron to several thousand electrons since the size of the quantum dot is designable. QD are fabricated in semiconductor material in s ...
Document
... space. Without them we are clueless as to how to manipulate and interact with a system. 2. The attributes are unchanging properties of a system, which can be determined from observable facts. The attributes determine the structure of the world. 3. The system Hamiltonian is one of the attributes, pla ...
... space. Without them we are clueless as to how to manipulate and interact with a system. 2. The attributes are unchanging properties of a system, which can be determined from observable facts. The attributes determine the structure of the world. 3. The system Hamiltonian is one of the attributes, pla ...
Physics 137B
... A particle of mass m is bound by the three-dimensional potential V (r) = −V0 e−r/a where !2 /mV0 a2 = 3/4. Use the variational method with the trial function e−αr to estimate an upper bound on the lowest energy eigenvalue. Note: You should find a quartic equation in (aα). You should show (by pluggin ...
... A particle of mass m is bound by the three-dimensional potential V (r) = −V0 e−r/a where !2 /mV0 a2 = 3/4. Use the variational method with the trial function e−αr to estimate an upper bound on the lowest energy eigenvalue. Note: You should find a quartic equation in (aα). You should show (by pluggin ...
Spin as Primordial Self-Referential Process
... generates our perceptions of spacetime. Do we have any supporting arguments? The answer is also „Yes.‰ As already discussed earlier, spin is deeply connected to the microscopic structure of spacetime as reflected by the Dirac equation for fermions (Dirac, 1928). Indeed, Penrose (1960 & 1967) had con ...
... generates our perceptions of spacetime. Do we have any supporting arguments? The answer is also „Yes.‰ As already discussed earlier, spin is deeply connected to the microscopic structure of spacetime as reflected by the Dirac equation for fermions (Dirac, 1928). Indeed, Penrose (1960 & 1967) had con ...
Paper
... for a noninteracting gas and a weakly interacting condensate in the simplest case of an isotropic harmonic potential. For a noninteracting ideal gas (both in the normal and in the Bose-condensed states), all modes have frequencies which are integer multiples of the harmonic trapping frequency n0 . I ...
... for a noninteracting gas and a weakly interacting condensate in the simplest case of an isotropic harmonic potential. For a noninteracting ideal gas (both in the normal and in the Bose-condensed states), all modes have frequencies which are integer multiples of the harmonic trapping frequency n0 . I ...
On the equivalence between non-factorizable mixed
... measured using Stern–Gerlach type detectors generating four quantum probabilities [4]. Players’ pay-off relations are expressed in terms of the pay-off entries of the corresponding bimatrix and the obtained quantum probabilities. Experimental realizations of quantum games are described elsewhere [20 ...
... measured using Stern–Gerlach type detectors generating four quantum probabilities [4]. Players’ pay-off relations are expressed in terms of the pay-off entries of the corresponding bimatrix and the obtained quantum probabilities. Experimental realizations of quantum games are described elsewhere [20 ...
The Large D Limit of Planar Diagrams arXiv:1701.01171v1 [hep
... it is then always possible to introduce natural localized probes and thus, in principle, to derive the large N emergent black hole geometry from first principles (see e.g. [10, 11]). Recently, such models were used to derive explicitly the quasi-normal behaviour at large N [12] and to discover inte ...
... it is then always possible to introduce natural localized probes and thus, in principle, to derive the large N emergent black hole geometry from first principles (see e.g. [10, 11]). Recently, such models were used to derive explicitly the quasi-normal behaviour at large N [12] and to discover inte ...
polarized quantum states
... Polarization is a useful and often used characteristic for coding of quantum info. The classical, and semiclassical description of polarization is unsatisfactory for quantum states. Other proposed measures have been discussed and compared. We have proposed to use the generalized visibility under (li ...
... Polarization is a useful and often used characteristic for coding of quantum info. The classical, and semiclassical description of polarization is unsatisfactory for quantum states. Other proposed measures have been discussed and compared. We have proposed to use the generalized visibility under (li ...
