Multidimensional Hypergeometric Functions in Conformai Field
... For example, an Aomoto polylogarithm of order 1 is defined by two pairs of points L = (L0, Lt),M = (M 0 , M J on P^C) and is equal to an integral of the form (ßL = dln(z1/z0) over a path going from M1 to M 0 . flj(L;M) is equal to the logarithm of the cross ratio of the four points (L 0 , Ll9 M0, Mx ...
... For example, an Aomoto polylogarithm of order 1 is defined by two pairs of points L = (L0, Lt),M = (M 0 , M J on P^C) and is equal to an integral of the form (ßL = dln(z1/z0) over a path going from M1 to M 0 . flj(L;M) is equal to the logarithm of the cross ratio of the four points (L 0 , Ll9 M0, Mx ...
Fast Converging Path Integrals for Time
... as well as for the numerical calculation of path integrals. The described discretization procedure is most straightforwardly numerically implemented by the Path-Integral Monte-Carlo approach [55]. Note that the O(1/N ) convergence can be also achieved with other choices of space-time points at which ...
... as well as for the numerical calculation of path integrals. The described discretization procedure is most straightforwardly numerically implemented by the Path-Integral Monte-Carlo approach [55]. Note that the O(1/N ) convergence can be also achieved with other choices of space-time points at which ...
Reconstructing the dynamics of a movable mirror in a
... dynamics of a movable mirror in an optical cavity for arbitrary values of the detuning between the optical cavity and an input driving field. Our work, based on the use of linearized Langevin equations, allows for the exact reconstruction of the quantum statistical properties of the system at hand [ ...
... dynamics of a movable mirror in an optical cavity for arbitrary values of the detuning between the optical cavity and an input driving field. Our work, based on the use of linearized Langevin equations, allows for the exact reconstruction of the quantum statistical properties of the system at hand [ ...
Studies of effective theories beyond the Standard Model
... These theories often reside at high energies, and will therefore be manifest as effective theories at the low energies experienced here on Earth. A first example is extra-dimensional theories. From our four-dimensional point of view, particles which propagate through the extra dimensions will effect ...
... These theories often reside at high energies, and will therefore be manifest as effective theories at the low energies experienced here on Earth. A first example is extra-dimensional theories. From our four-dimensional point of view, particles which propagate through the extra dimensions will effect ...
Table of Contents
... Dynamics problems involving Newton’s second law of motion often involve second order linear differential equations as illustrated in the derivation of Equation (1) for a particle attached to a light spring. For an understanding of simple harmonic motion it is sufficient to investigate the solution o ...
... Dynamics problems involving Newton’s second law of motion often involve second order linear differential equations as illustrated in the derivation of Equation (1) for a particle attached to a light spring. For an understanding of simple harmonic motion it is sufficient to investigate the solution o ...
Time reversal in classical electromagnetism - Philsci
... to say, in such a circumstance one faces a choice: this theory with these quantities and these invariances or that theory with those quantities and those invariances. If the competing theories are empirically equivalent then one should make such a choice in the usual manner: on the basis of simplici ...
... to say, in such a circumstance one faces a choice: this theory with these quantities and these invariances or that theory with those quantities and those invariances. If the competing theories are empirically equivalent then one should make such a choice in the usual manner: on the basis of simplici ...
Document
... NB2: CB violates both lepton number and helicity and CB contains a calculable lepton neutrino condensate. NB3: A similar story holds for supernova neutrinos (they are believed to be ...
... NB2: CB violates both lepton number and helicity and CB contains a calculable lepton neutrino condensate. NB3: A similar story holds for supernova neutrinos (they are believed to be ...
Majorana Fermions - Physics | Oregon State University
... deconfinement physics expected for QSLs. Comparing these with recent dynamical calculations involving gauge flux excitations and Majorana fermions of the pure Kitaev model, we propose the excitation spectrum of α-RuCl3 as a prime candidate for fractionalized Kitaev physics. ...
... deconfinement physics expected for QSLs. Comparing these with recent dynamical calculations involving gauge flux excitations and Majorana fermions of the pure Kitaev model, we propose the excitation spectrum of α-RuCl3 as a prime candidate for fractionalized Kitaev physics. ...
B2.IV Nuclear and Particle Physics
... from fusion of hydrogen to helium inside the sun. It’s perhaps unlikely that this is what he intended. ...
... from fusion of hydrogen to helium inside the sun. It’s perhaps unlikely that this is what he intended. ...
A short review on Noether`s theorems, gauge
... (2.4) should not be overlooked: equation (2.4) holds for all x(t), y(t), z(t). This seems like a trivial statement in this example but it is a crucial property of action symmetries. Symmetries can take far more complicated forms. Let q i be a set of generalised coordinates. Then for an action I[q i ...
... (2.4) should not be overlooked: equation (2.4) holds for all x(t), y(t), z(t). This seems like a trivial statement in this example but it is a crucial property of action symmetries. Symmetries can take far more complicated forms. Let q i be a set of generalised coordinates. Then for an action I[q i ...
