Giovannini, D., Romero, J., Leach, J., Dudley, A, Forbes, A, and
... method is that MUBs need to be defined for the small Hilbert spaces of the subsystems rather than for the large space of the overall system. This becomes especially relevant where the definition or measurement of MUBs for the overall system is challenging. We illustrate this approach by implementing ...
... method is that MUBs need to be defined for the small Hilbert spaces of the subsystems rather than for the large space of the overall system. This becomes especially relevant where the definition or measurement of MUBs for the overall system is challenging. We illustrate this approach by implementing ...
First Law of Thermodynamics:
... The steric number of an inner atom uniquely determines the number and type of hybrid orbitals. Hybrid orbitals form localized bonds by overlap with atomic orbitals or with other hybrid orbitals. There is no need to hybridize orbitals on outer atoms, because atoms do not have limiting geometries. The ...
... The steric number of an inner atom uniquely determines the number and type of hybrid orbitals. Hybrid orbitals form localized bonds by overlap with atomic orbitals or with other hybrid orbitals. There is no need to hybridize orbitals on outer atoms, because atoms do not have limiting geometries. The ...
The Asymptotic Safety Scenario in Quantum Gravity
... problems and maintaining the credible physics premise of a functional integral picture is, in our view, more appropriate than evading the problems in exchange for a less credible physics premise. Of course in the absence of empirical guidance the ‘true’ physics of quantum gravity is unknown; so for ...
... problems and maintaining the credible physics premise of a functional integral picture is, in our view, more appropriate than evading the problems in exchange for a less credible physics premise. Of course in the absence of empirical guidance the ‘true’ physics of quantum gravity is unknown; so for ...
Classical analogy of Fano resonances
... increases, the phase increases from ϕ = 0 at ω = 0 to ϕ = π/2 at ω = ω0 (at resonance) and to π as ω → ∞. It means that if the displacement and the external force are in phase before the resonance, then they are out of phase after the resonance. 2.2. Two coupled oscillators Now we discuss the dynami ...
... increases, the phase increases from ϕ = 0 at ω = 0 to ϕ = π/2 at ω = ω0 (at resonance) and to π as ω → ∞. It means that if the displacement and the external force are in phase before the resonance, then they are out of phase after the resonance. 2.2. Two coupled oscillators Now we discuss the dynami ...
Topological Chern Indices in Molecular Spectra
... is not too strong, further splitting of the rovibrational structure into subbands can be clearly seen. The well-known example is the splitting of the triply degenerate vibrational structure for a spherically symmetrical molecule into three subbands due to the first-order Coriolis interaction [2,3]. ...
... is not too strong, further splitting of the rovibrational structure into subbands can be clearly seen. The well-known example is the splitting of the triply degenerate vibrational structure for a spherically symmetrical molecule into three subbands due to the first-order Coriolis interaction [2,3]. ...
The Compton-Schwarzschild correspondence from extended de
... to wave functions that are consistently defined for all energy scales. The underlying theory is an extended form of canonical non-relativistic quantum mechanics which, at first sight, appears to be non-gravitational, in the sense that the results obtained do not require the introduction of a classic ...
... to wave functions that are consistently defined for all energy scales. The underlying theory is an extended form of canonical non-relativistic quantum mechanics which, at first sight, appears to be non-gravitational, in the sense that the results obtained do not require the introduction of a classic ...
Quantum spin systems from the perspective of quantum
... thermodynamic limit (N!1) when P1=P2=L =P1 – Systematic way of constructing translational invariant states – MPS become dense in space of all states when D!1 ...
... thermodynamic limit (N!1) when P1=P2=L =P1 – Systematic way of constructing translational invariant states – MPS become dense in space of all states when D!1 ...
Quantum Physics 2005 Notes-8 Three-dimensional Schrodinger Equation Notes 8
... • We have already found the eigenfunctions of this operator. They are the spherical harmonics. • We have previously found that the eigenvalues of L2 are l(l+1) with l=integers 0, 1, 2, 3... if the potential is central. • Angular momentum manifests itself as a magnetic dipole moment when the particle ...
... • We have already found the eigenfunctions of this operator. They are the spherical harmonics. • We have previously found that the eigenvalues of L2 are l(l+1) with l=integers 0, 1, 2, 3... if the potential is central. • Angular momentum manifests itself as a magnetic dipole moment when the particle ...
Electrically induced spin resonance fluorescence. I. Theory
... maximum swing an oscillator can have and that c = 1 / b is the maximum angular frequency an oscillator can have. The quantity which parametrizes the different oscillators arises from the constant of integration which states that at Z = 0 the electron velocity is 具0 , vF cos共兲 , vF sin共兲典. Henc ...
... maximum swing an oscillator can have and that c = 1 / b is the maximum angular frequency an oscillator can have. The quantity which parametrizes the different oscillators arises from the constant of integration which states that at Z = 0 the electron velocity is 具0 , vF cos共兲 , vF sin共兲典. Henc ...
Coherent population trapping of an electron spin in a single
... controlled by varying the ratio of Rabi frequencies between the driving and probe optical fields. Therefore, we can prepare an arbitrary initial qubit state by using the CPT technique. In this scheme, the initialization rate is limited by the excited-state decay rate, which is of the order of 109 s− ...
... controlled by varying the ratio of Rabi frequencies between the driving and probe optical fields. Therefore, we can prepare an arbitrary initial qubit state by using the CPT technique. In this scheme, the initialization rate is limited by the excited-state decay rate, which is of the order of 109 s− ...
A definite resolution of the mystery of
... from first principles. For that purpose we fuse the large structure as well as the quantum scale of spacetime together and model it using certain Calabi-Yau manifold. That way we derive a rescaled energy-mass special relativity equation which includes quantum effects. The missing energy predicted by ...
... from first principles. For that purpose we fuse the large structure as well as the quantum scale of spacetime together and model it using certain Calabi-Yau manifold. That way we derive a rescaled energy-mass special relativity equation which includes quantum effects. The missing energy predicted by ...
pdf - ISI Foundation
... Given the drastic changes that take place across a quantum phase transition, one should expect the fidelity for nearby states to exhibit a drop across the boundary phase, signaling an enhanced distinguishability. Indeed, while in the thermodynamic limit the fidelity 共susceptibility兲 has a drop 共dive ...
... Given the drastic changes that take place across a quantum phase transition, one should expect the fidelity for nearby states to exhibit a drop across the boundary phase, signaling an enhanced distinguishability. Indeed, while in the thermodynamic limit the fidelity 共susceptibility兲 has a drop 共dive ...
Ionization of atoms in parallel electric and magnetic fields: The role
... nates as described in the Appendix. This removes the Coulomb singularity at the origin ~see also Ref. @12#!. A highorder Taylor integrator was used as described in Ref. @13#, which reduced computation times by a factor of approximately 3 compared to conventional Runge-Kutta methods. Trajectories wer ...
... nates as described in the Appendix. This removes the Coulomb singularity at the origin ~see also Ref. @12#!. A highorder Taylor integrator was used as described in Ref. @13#, which reduced computation times by a factor of approximately 3 compared to conventional Runge-Kutta methods. Trajectories wer ...
