Control of quantum systems using model
... encoding. Preparation of superposition of states is of great interest in order to exploit its inherent parallelism. An example is the preparation in many-particle qubit systems of entangled states, which offer information manipulation that is not possible with the classical binary bits [23]. The mos ...
... encoding. Preparation of superposition of states is of great interest in order to exploit its inherent parallelism. An example is the preparation in many-particle qubit systems of entangled states, which offer information manipulation that is not possible with the classical binary bits [23]. The mos ...
Document
... quantum energy saturates to a constant value hp2 i L2 , where L is the localization length. The dw-QKR shows a typical, exponentially localized, momentum distribution. However, for the cdw-QKR, the quantal Np is evidently asymmetric, but regains the DL form at large p. There is no net current in ...
... quantum energy saturates to a constant value hp2 i L2 , where L is the localization length. The dw-QKR shows a typical, exponentially localized, momentum distribution. However, for the cdw-QKR, the quantal Np is evidently asymmetric, but regains the DL form at large p. There is no net current in ...
The Scattering Green`s Function: Getting the Signs Straight
... It is worth taking a little time to discuss the statement that G+ (x, x0 ) is the Helmholtz Equation Green’s Function, namely (6.2.12), and use this to verify the overall minus sign. Take k = 0, in which case G+ (x, x0 ) is just −1/4π times the electrostatic potential at x for a unit charge located ...
... It is worth taking a little time to discuss the statement that G+ (x, x0 ) is the Helmholtz Equation Green’s Function, namely (6.2.12), and use this to verify the overall minus sign. Take k = 0, in which case G+ (x, x0 ) is just −1/4π times the electrostatic potential at x for a unit charge located ...
![arXiv:1412.5987v1 [hep-ex] 18 Dec 2014](http://s1.studyres.com/store/data/008057205_1-733500b8b6bd2637f9a7ffd625392271-300x300.png)
arXiv:1412.5987v1 [hep-ex] 18 Dec 2014
... damage detection or internal strain field mapping. The FBG sensors supposed to be located in fiber optic cable mounted in the sample. Furthermore, the key feature of FBGs sensors is that the information about perturbations is encoded in wavelength. Indeed, the main principle of FBG sensors work is t ...
... damage detection or internal strain field mapping. The FBG sensors supposed to be located in fiber optic cable mounted in the sample. Furthermore, the key feature of FBGs sensors is that the information about perturbations is encoded in wavelength. Indeed, the main principle of FBG sensors work is t ...
Unified rotational and permutational symmetry and selection rules in
... The nuclear spin wave function of N identical particles of spin I spans a representation of the product group SN×U(2I+1) Representation theory gives a simple prescription to find this! ...
... The nuclear spin wave function of N identical particles of spin I spans a representation of the product group SN×U(2I+1) Representation theory gives a simple prescription to find this! ...
Are Quantum Objects Propensitons
... interpretation; decoherence; consistent histories. None of these, in my view, provides us with a satisfactory version of quantum theory. For critical surveys and further literature see Squires (1986); Rae (2002, ch. 13); Bacciagaluppi (2003). ...
... interpretation; decoherence; consistent histories. None of these, in my view, provides us with a satisfactory version of quantum theory. For critical surveys and further literature see Squires (1986); Rae (2002, ch. 13); Bacciagaluppi (2003). ...
Dark Energy from Violation of Energy Conservation
... although the quantitative estimates in this Letter have been obtained for some specific examples, the results of our analysis are far more general and remain valid as long as the violation of energy conservation is of integrable type (5). This framework could therefore be used to rule out nonstandar ...
... although the quantitative estimates in this Letter have been obtained for some specific examples, the results of our analysis are far more general and remain valid as long as the violation of energy conservation is of integrable type (5). This framework could therefore be used to rule out nonstandar ...
PEPS, matrix product operators and the Bethe ansatz
... those “swaps” with the idenity; logarithmic derivative undoes all the other swaps, leaving the Heisenberg Hamiltonian! – It follows that eigenvectors ...
... those “swaps” with the idenity; logarithmic derivative undoes all the other swaps, leaving the Heisenberg Hamiltonian! – It follows that eigenvectors ...
Inhomogeneous liquid Superscript>4 Superscript>He: A density
... represents the c o m p a r i s o n o f X-l(q, to = 0) with the measurements o f C o w l e y a n d W o o d s ) 3 The agreement is satisfactory. It is w o r t h pointing out that the response X-l(q, 0) d e p e n d s only slightly on the p o w e r used to define Vt in the interval r = 0 to r = h. The f ...
... represents the c o m p a r i s o n o f X-l(q, to = 0) with the measurements o f C o w l e y a n d W o o d s ) 3 The agreement is satisfactory. It is w o r t h pointing out that the response X-l(q, 0) d e p e n d s only slightly on the p o w e r used to define Vt in the interval r = 0 to r = h. The f ...
Enhancement of quantum dot peak-spacing fluctuations
... in contrast with the experimental observations. This deviation from random-matrix theory was attributed to the importance of electronic correlations, which are not captured in the constant-interaction model. For strong magnetic fields, in particular in the fractional quantum Hall regime, electronic ...
... in contrast with the experimental observations. This deviation from random-matrix theory was attributed to the importance of electronic correlations, which are not captured in the constant-interaction model. For strong magnetic fields, in particular in the fractional quantum Hall regime, electronic ...
Course Syllabus - Guru Jambheshwar University of Science
... Energy stored in an electric and magnetic fields. Maxwell’s equations, power flow in an electromagnetic field and pointing theorem. Electromagnetic waves in a homogeneous medium-solution for free space conditions. Uniform plane waves, the wave equations for a conducting medium, Sinusoidal time varia ...
... Energy stored in an electric and magnetic fields. Maxwell’s equations, power flow in an electromagnetic field and pointing theorem. Electromagnetic waves in a homogeneous medium-solution for free space conditions. Uniform plane waves, the wave equations for a conducting medium, Sinusoidal time varia ...
Ashtekar.pdf
... For, just as the classical Riemannian geometry of Σ is determined by the triads Eia , all Riemannian geometry operators – such as the area operator ÂS associated with a 2-surface S or the volume operator V̂R associated with a region R – are constructed from Êia . However, since even the classical ...
... For, just as the classical Riemannian geometry of Σ is determined by the triads Eia , all Riemannian geometry operators – such as the area operator ÂS associated with a 2-surface S or the volume operator V̂R associated with a region R – are constructed from Êia . However, since even the classical ...
Two Body Perturbing Resonances in a Three Body System: Origin of
... (8) sigma meson mass. Such a sigma mass is close to that commonly used in Relativistic We now have all the required expressions re- Mean Field (RMF)[1] theory of nuclei. It quired to get the expectation value of the cou- could be that only one ∆ resonance resonance ...
... (8) sigma meson mass. Such a sigma mass is close to that commonly used in Relativistic We now have all the required expressions re- Mean Field (RMF)[1] theory of nuclei. It quired to get the expectation value of the cou- could be that only one ∆ resonance resonance ...
ISM 08
... Null cosmologies: Φ = Φ(x+ ) . No nonzero contraction so the mass term vanishes i.e. m2 (Φ) = 0. Similar story for gauge theory using lightcone gauge for convenience. Suppressing many details, but briefly, cubic/quartic interaction terms: multiplied by powers of gY M = eΦ/2 , unimportant near eΦ → 0 ...
... Null cosmologies: Φ = Φ(x+ ) . No nonzero contraction so the mass term vanishes i.e. m2 (Φ) = 0. Similar story for gauge theory using lightcone gauge for convenience. Suppressing many details, but briefly, cubic/quartic interaction terms: multiplied by powers of gY M = eΦ/2 , unimportant near eΦ → 0 ...
A Chapter in Physical Mathematics: Theory of Knots in the Sciences
... It was the discovery by Gauss of this very integral expressing the work done on a magnetic pole while describing a closed curve in presence of a closed electric current and indicating the geometric connexion between the two closed curves, that led him to lament the small progress made in the Geomet ...
... It was the discovery by Gauss of this very integral expressing the work done on a magnetic pole while describing a closed curve in presence of a closed electric current and indicating the geometric connexion between the two closed curves, that led him to lament the small progress made in the Geomet ...
document
... so called “consistent linear discretization scheme” [3–5] that meets the continuity requirements across interfaces exactly, using a tetrahedron mesh combined with a consistent linear interpolation of electric and magnetic field strengths. In this section we briefly present our discretization scheme. ...
... so called “consistent linear discretization scheme” [3–5] that meets the continuity requirements across interfaces exactly, using a tetrahedron mesh combined with a consistent linear interpolation of electric and magnetic field strengths. In this section we briefly present our discretization scheme. ...
