Fully quantum-mechanical model of a SQUID ring coupled to an
... regions of strong coupling 共energy exchange兲 are significantly reduced compared to those seen in Fig. 4. As a further example, we show in Fig. 6 the computed results for our coupled system taking, as in Fig. 4, e ⫽ s but now with stronger coupling ( ⫽1/10). To make our results strictly compara ...
... regions of strong coupling 共energy exchange兲 are significantly reduced compared to those seen in Fig. 4. As a further example, we show in Fig. 6 the computed results for our coupled system taking, as in Fig. 4, e ⫽ s but now with stronger coupling ( ⫽1/10). To make our results strictly compara ...
![Dirac multimode ket-bra operators` [equation]](http://s1.studyres.com/store/data/023088225_1-3900fa8a2c451013a9516ce21d0ecd01-300x300.png)
Dirac multimode ket-bra operators` [equation]
... this work is mainly concentrated on developing Dirac ketbra operator’s integration theory in Q-ordering or P-ordering to multimode case and demenstrating how classical transformations can be mapped onto the ordered exponential operators through the integration, and the integration directly lead to o ...
... this work is mainly concentrated on developing Dirac ketbra operator’s integration theory in Q-ordering or P-ordering to multimode case and demenstrating how classical transformations can be mapped onto the ordered exponential operators through the integration, and the integration directly lead to o ...
Almost all decoherence models lead to shot noise scaling in
... Entanglement enhanced precision Hong-Ou-Mandel interference ...
... Entanglement enhanced precision Hong-Ou-Mandel interference ...
Unit 2 The Fundamental Interactions
... exchange of virtual particles between matter. Electricity and magnetism behaves differently at tiny distances than at larger distances, and so quantum electrodynamics (QED) was developed in order to describe electromagnetism at quantum scales and account for observed measurements. Quantum chromodyna ...
... exchange of virtual particles between matter. Electricity and magnetism behaves differently at tiny distances than at larger distances, and so quantum electrodynamics (QED) was developed in order to describe electromagnetism at quantum scales and account for observed measurements. Quantum chromodyna ...
The Membrane Vacuum State
... Nambu-Goto action principle, which equates the action with the worldvolume. We thus proceed by constructing a volume element from the induced metric on the worldvolume by pulling back the target space metric: gij (X) = ∂i X µ ∂j X ν ηµν ≡ Eiµ Ejν ηµν , ...
... Nambu-Goto action principle, which equates the action with the worldvolume. We thus proceed by constructing a volume element from the induced metric on the worldvolume by pulling back the target space metric: gij (X) = ∂i X µ ∂j X ν ηµν ≡ Eiµ Ejν ηµν , ...
Coupled quantum dots as quantum gates
... ~leading to wave-function compression!, or by an electric field E ~leading to level detuning!, or by varying the barrier height or equivalently the interdot distance 2a ~leading to a suppression of tunneling between the dots!. The dependence on these parameters is of direct practical interest, since ...
... ~leading to wave-function compression!, or by an electric field E ~leading to level detuning!, or by varying the barrier height or equivalently the interdot distance 2a ~leading to a suppression of tunneling between the dots!. The dependence on these parameters is of direct practical interest, since ...
Resonant Tunneling Between Quantum Hall Edge States
... quantized Hall coefficient as I = ν(e2 /h)VH . This immediately establishes the universal result within a given Hall plateau: g = ν. This remarkable fact makes the resonance line shape completely universal, model-independent and fully determined (up to an overall temperature scale). The fractional q ...
... quantized Hall coefficient as I = ν(e2 /h)VH . This immediately establishes the universal result within a given Hall plateau: g = ν. This remarkable fact makes the resonance line shape completely universal, model-independent and fully determined (up to an overall temperature scale). The fractional q ...
2 - arXiv
... standard approach of [2]. In [6] the so-called Schrieffer-Wolff formalism is generalized to Lindbladian dynamics; its basic form requires inversion of the nominal dynamics operator, which is not too practical and which we circumvent here for the derivation of the reduced slow master equation (15). T ...
... standard approach of [2]. In [6] the so-called Schrieffer-Wolff formalism is generalized to Lindbladian dynamics; its basic form requires inversion of the nominal dynamics operator, which is not too practical and which we circumvent here for the derivation of the reduced slow master equation (15). T ...
Web FTP - Visicom Scientific Software
... introduces a difficult problem for the information theorist and the student of consciousness alike. When the reader now considers information How can something with N configurations theory below bit scale, one cannot avoid but memorise and retrieve accurately what appears to conclude that the quantu ...
... introduces a difficult problem for the information theorist and the student of consciousness alike. When the reader now considers information How can something with N configurations theory below bit scale, one cannot avoid but memorise and retrieve accurately what appears to conclude that the quantu ...
PDF
... A function f : [a, b] → R is said to be generalized Riemann integrable on [a, b] if there exists a number L ∈ R such that for every > 0 there exists a gauge δ on [a, b] such that if Ṗ is any δ -fine partition of [a, b], then |S(f ; Ṗ) − L| < , where S(f ; Ṗ) is any Riemann sum for f using t ...
... A function f : [a, b] → R is said to be generalized Riemann integrable on [a, b] if there exists a number L ∈ R such that for every > 0 there exists a gauge δ on [a, b] such that if Ṗ is any δ -fine partition of [a, b], then |S(f ; Ṗ) − L| < , where S(f ; Ṗ) is any Riemann sum for f using t ...
Prog. Theor. Phys. Suppl. 138, 489 - 494 (2000) Quantum Statistical
... the role of a generating function from which all physical quantities of interest can be obtained. Physical quantities such as the energy and specific heat are given by ...
... the role of a generating function from which all physical quantities of interest can be obtained. Physical quantities such as the energy and specific heat are given by ...
A Filtration of Open/Closed Topological Field Theory
... set out in the 1970’s in work of Wilson, Friedan and others. This structure should play an important role in organizing and classifying QFTs, and in the study of the string landscape, allowing us to say when two theories are connected by finite variations of the couplings or by RG flows, when a sequen ...
... set out in the 1970’s in work of Wilson, Friedan and others. This structure should play an important role in organizing and classifying QFTs, and in the study of the string landscape, allowing us to say when two theories are connected by finite variations of the couplings or by RG flows, when a sequen ...
Probability density of quantum expectation values
... We make use of the following trick. Since χ (λ) is well behaved in zero and decays at infinity, it belongs to the space of tempered distribution S 0 (R). The Fourier transform is well defined for such functions and the result is again a tempered distribution. Actually for d ≥ 3, χ is also summable a ...
... We make use of the following trick. Since χ (λ) is well behaved in zero and decays at infinity, it belongs to the space of tempered distribution S 0 (R). The Fourier transform is well defined for such functions and the result is again a tempered distribution. Actually for d ≥ 3, χ is also summable a ...