Entangling Dipole-Dipole Interactions and Quantum Logic in Optical
... quantum states can be prepared by cooling to the vibrational ground state of the optical lattice using Raman sideband cooling [18], or perhaps by loading the lattice with a precooled sample of Bose-condensed atoms [19]. Both internal and external degrees of freedom can be further manipulated through ...
... quantum states can be prepared by cooling to the vibrational ground state of the optical lattice using Raman sideband cooling [18], or perhaps by loading the lattice with a precooled sample of Bose-condensed atoms [19]. Both internal and external degrees of freedom can be further manipulated through ...
From the Mendeleev periodic table to particle physics and back to
... number, respectively. They are connected to the chain of groups SO(3)⊃SO(2): the quantum number ℓ characterizes an IRC, of dimension 2ℓ + 1, of SO(3) and mℓ a one–dimensional IRC of SO(2). The principal quantum number n is such that n − ℓ − 1 is the number of nodes of the radial wave function associ ...
... number, respectively. They are connected to the chain of groups SO(3)⊃SO(2): the quantum number ℓ characterizes an IRC, of dimension 2ℓ + 1, of SO(3) and mℓ a one–dimensional IRC of SO(2). The principal quantum number n is such that n − ℓ − 1 is the number of nodes of the radial wave function associ ...
Von Neumann`s Impossibility Proof: Mathematics in - Philsci
... After the mathematical intermezzo of chapter II, chapter III (“The quantum mechanical statistics”) returns to the physical meaning of the formalism. In chapter I it had become clear that in the transition from classical theory to quantum mechanics the coordinates qj and momenta pj had to be replaced ...
... After the mathematical intermezzo of chapter II, chapter III (“The quantum mechanical statistics”) returns to the physical meaning of the formalism. In chapter I it had become clear that in the transition from classical theory to quantum mechanics the coordinates qj and momenta pj had to be replaced ...
Nonequilibrium entropy production in open and closed quantum
... terms of the time averaged Bures length [Bur68, Bur69]. The definition of the Bures length will also serve as our starting point for the derivation of the generalized Heisenberg uncertainty relation [MT45, ML98, LT09]. We will derive the minimal time that an isolated quantum system needs to evolve f ...
... terms of the time averaged Bures length [Bur68, Bur69]. The definition of the Bures length will also serve as our starting point for the derivation of the generalized Heisenberg uncertainty relation [MT45, ML98, LT09]. We will derive the minimal time that an isolated quantum system needs to evolve f ...
Continuous Variable Quantum Information: Gaussian States and
... (continuous variables), such as those associated to position and momentum of a particle. This second approach has witnessed considerable success due to its versatility, with implementations often encompassing different physical systems, e.g. light quadratures and collective magnetic moments of atomic ...
... (continuous variables), such as those associated to position and momentum of a particle. This second approach has witnessed considerable success due to its versatility, with implementations often encompassing different physical systems, e.g. light quadratures and collective magnetic moments of atomic ...
here.
... • There are still many physical situations where the implications of quantum mechanics have not been adequately understood due to a lack of experimental, conceptual or mathematical tools (e.g. quantum effects in sub-atomic physics or gravity, mesoscopic systems and the problem of measurement). So th ...
... • There are still many physical situations where the implications of quantum mechanics have not been adequately understood due to a lack of experimental, conceptual or mathematical tools (e.g. quantum effects in sub-atomic physics or gravity, mesoscopic systems and the problem of measurement). So th ...
Cabello`s nonlocality for generalized three
... P (D1 , U2 , D3 | + −−) = P (D1 , U2 , D3 | − +−) = 0.5, P (D1 , D2 , U3 | + −+) = P (D1 , D2 , U3 | − ++) = 0.5, P (D1 , D2 , D3 | + −−) = P (D1 , D2 , D3 | − +−) = 0.5, where only the nonzero probabilities have been written out. It is important to notice that the system of linear equations (18)-(2 ...
... P (D1 , U2 , D3 | + −−) = P (D1 , U2 , D3 | − +−) = 0.5, P (D1 , D2 , U3 | + −+) = P (D1 , D2 , U3 | − ++) = 0.5, P (D1 , D2 , D3 | + −−) = P (D1 , D2 , D3 | − +−) = 0.5, where only the nonzero probabilities have been written out. It is important to notice that the system of linear equations (18)-(2 ...
Phases in noncommutative quantum mechanics on (pseudo) sphere
... of such states is finite [13] (see also [14]). In appropriate limits the NCQM on a (pseudo)sphere should be reduced to the planar one. Hence, out of the (pseudo)spherical system originate, in some sense, the “phases” of planar NCQM. Although this issue was touched upon in Refs. [10, 17, 18, 21], the ...
... of such states is finite [13] (see also [14]). In appropriate limits the NCQM on a (pseudo)sphere should be reduced to the planar one. Hence, out of the (pseudo)spherical system originate, in some sense, the “phases” of planar NCQM. Although this issue was touched upon in Refs. [10, 17, 18, 21], the ...
TOPICS IN QUANTUM NANOSTRUCTURE PHYSICS: SPIN-ORBIT EFFECTS AND FAR-INFRARED RESPONSE TEMES DE F´
... the three spatial components of the density, which in addition is a simpler both conceptually and practically quantity to deal with. On the other hand, the exchange-correlation part of the electron-electron interaction, neglected or only partially taken into account in the above-mentioned approaches ...
... the three spatial components of the density, which in addition is a simpler both conceptually and practically quantity to deal with. On the other hand, the exchange-correlation part of the electron-electron interaction, neglected or only partially taken into account in the above-mentioned approaches ...
On the Faithful Interpretation of Pure Wave Mechanics
... superposition of states each of which [. . .] represent[s] the bodies with fairly well defined positions and momenta. Each of these states then propagates approximately according to classical laws, so that the general state can be viewed as a superposition of quasi classical states propagating accor ...
... superposition of states each of which [. . .] represent[s] the bodies with fairly well defined positions and momenta. Each of these states then propagates approximately according to classical laws, so that the general state can be viewed as a superposition of quasi classical states propagating accor ...
Hubbard model description of silicon spin qubits: charge stability
... along the y-direction in order to exhibit this property. This rescaling is simply a matter of convenience and convention, and does not affect any of our results or conclusions. In addition to the assumptions above, we further assume that the Si conduction band valley splitting is sufficiently large ...
... along the y-direction in order to exhibit this property. This rescaling is simply a matter of convenience and convention, and does not affect any of our results or conclusions. In addition to the assumptions above, we further assume that the Si conduction band valley splitting is sufficiently large ...
Cotunneling in the ν Robert Zielke, Bernd Braunecker,
... the renormalization group flow is cut off by bias V and temperature T such that the perturbative result is accurate. Our calculations show that the different charge carriers can be clearly distinguished by standard transport measurements. Our approach is also applicable to a setup of two separate FQ ...
... the renormalization group flow is cut off by bias V and temperature T such that the perturbative result is accurate. Our calculations show that the different charge carriers can be clearly distinguished by standard transport measurements. Our approach is also applicable to a setup of two separate FQ ...