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Introductory quantum mechanics
Introductory quantum mechanics

... Take a classical example: A particle that are subjected to a gravity field U(x) = GMm/r is governed by the Newton equations of motion, ...
6. String Interactions
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on the canonical formulation of electrodynamics and wave mechanics
on the canonical formulation of electrodynamics and wave mechanics

... was an undergraduate student of Scott’s, he imparted to me a deep appreciation for mathematics and a particular interest in analysis. Scott was an excellent teacher and mentor, and under his guidance, my undergraduate research was awarded by the College of Liberal Arts and Sciences. Outside of the U ...
Dispersion relation of the nonlinear Klein
Dispersion relation of the nonlinear Klein

... matter of fact we are considering conservative systems, for which the dynamics can be mapped to the nonlinear oscillation of a point mass in a one-dimensional potential. The main goal of this article is to explore the effects of the nonlinearity on the solutions, providing simple and efficient appro ...
On two possible definitions of the free energy for collective variables
On two possible definitions of the free energy for collective variables

... the level sets of the collective variables. Other than the aforementioned free energy, this second free energy, which is intrinsically geometric in that it solely depends upon the foliation given by the collective variables, appears to be a common quantity for computing, e.g., transition rates betwe ...
Slide 1
Slide 1

... • If we do it classically we have to calculate f(x) many times. – It isn’t how easy it is to calculate f(x), it is how many times. – Need to go from 0 to N2 , this is a huge number of calculations for a 128 bit number! This could be 2(2*128) or ~1.16 x 1077 – The results have to be stored somewhere ...
A n - USM
A n - USM

... • Consider a particle subjected to some timeindependent but space-dependent potential V(x) within some boundaries • The behaviour of a particle subjected to a timeindependent potential is governed by the famous (1D, time independent, non relativistic) Schrodinger equation: ...
1 Analytic Representation of The Square
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... addition to the confined singularities and the additional attractive (repulsive) term, the effective mass of the composite acquires an oscillatory behavior. We also derive an alternate relationship between the Dirac equation (with minimal coupling) and the square-root equation that is much closer th ...
Parametric evolution of eigenstates: Beyond perturbation theory and
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The classical electromagnetism as used nowadays is not the theory
The classical electromagnetism as used nowadays is not the theory

Asymptotic Safety in Quantum Gravity and Diffeomorphic Non
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... then should we exclude g 0 from the picture and just retain g ? why not exclude g and retain g 0 instead ?. Therefore, all these mathematically distinct solutions obtained via the active diffeomorphisms r → ρ(r) are not physically distinguishable, but they represent one and the same physical solutio ...
on the fine structure of spacetime
on the fine structure of spacetime

String Backgrounds
String Backgrounds

Syllabus: Quantum computing - University of Hawaii Physics and
Syllabus: Quantum computing - University of Hawaii Physics and

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... AdS/CFT replaces strongly coupled quantum field theory with weakly coupled classical field theory – we can now do time dependent problems that the lattice can’t… ...
Lecture 4 Density instead of the wavefunction CHEM6085: Density
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Fermions coupled to gauge fields .1in with cond
Fermions coupled to gauge fields .1in with cond

Beyond Transition-State Theory: A Rigorous
Beyond Transition-State Theory: A Rigorous

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- Philsci

... of TRI, which I have just given, is in fact gibberish. It just doesn’t make sense to timereverse a truly instantaneous state of a system. Nevertheless, for the sake of brevity I stick with the usual definition; by curtailing the effect of T so that it only effects those changes logically necessitate ...
BPS Geometry, AdS/CFT, and String Theory
BPS Geometry, AdS/CFT, and String Theory

... We see fermion configurations corresponding to a single isolated strip, or set of strips. These fermions are the same as the ones that appear in 2d QCD on a cylinder, or SU (N ) group quantum mechanics. In (a) we display the ground state and in (b) we display an excited state. From the point of view ...
QFT on curved spacetimes: axiomatic framework and applications
QFT on curved spacetimes: axiomatic framework and applications

... these degrees of freedom influence each other. This is the principle of locality, more precisely expressed by the German word Nahwirkungsprinzip. It states that each degree of freedom is influenced only by a relatively small number of other degrees of freedom. This induces a concept of neighborhood ...
2-2-guided-notes
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dirac and majorana fermions
dirac and majorana fermions

High Energy Cross Sections by Monte Carlo
High Energy Cross Sections by Monte Carlo

... where u(p) is a 4-component positive energy spinor wavefunction solution of the Dirac equation and γ µ are Dirac gamma matrices. This amplitude defines the scattering of a photon from an electron for arbitrary photon polarizations and electron spin. To compare with the Compton cross section for spin ...
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Instanton

An instanton (or pseudoparticle) is a notion appearing in theoretical and mathematical physics. An instanton is a classical solution to equations of motion with a finite, non-zero action, either in quantum mechanics or in quantum field theory. More precisely, it is a solution to the equations of motion of the classical field theory on a Euclidean spacetime.
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