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Journal of Modern Optics
Journal of Modern Optics

... sections 3 and 4 the spatially periodic arrays of Gaussian and Laguerre–Gaussian beams of the first order are compared. Next, in section 5, in order to get an analytic solution for the macroscopic wavefunction C trapped by an optical vortex array, a special optical pancake-like potential (Figure 1) ...
Wednesday, Nov. 8, 2006
Wednesday, Nov. 8, 2006

Planetary motion, the hydrogen atom, and superintegrablity
Planetary motion, the hydrogen atom, and superintegrablity

Factorized S-Matrices in Two Dimensions as the Exact
Factorized S-Matrices in Two Dimensions as the Exact

Thesis - Institut für Physik
Thesis - Institut für Physik

... MCTDHB(M ) method reaches its limits in form of computational time and memory even for single digit values of M on typical workstations because of the exponential growth of the Hilbert space. In order to overcome these limitations and especially to take into account four and more modes in our simula ...
From molecular dynamics to Brownian dynamics
From molecular dynamics to Brownian dynamics

Conservation of Angular Momentum
Conservation of Angular Momentum

Lecture Notes in Physics Introduction to Plasma Physics Michael Gedalin
Lecture Notes in Physics Introduction to Plasma Physics Michael Gedalin

... charges of the opposite sign, thus making the system neutral. More precisely, we have to neutralize locally, so that the positive charge density should balance the negative charge density. Now let us add a test charge Q which make slight imbalance. We are interested to know what would be the electri ...
PDF (Author Accepted Manuscript) - CLoK
PDF (Author Accepted Manuscript) - CLoK

Josephson Effect for Photons in Two Weakly Linked Microcavities
Josephson Effect for Photons in Two Weakly Linked Microcavities

Work and Energy, Principle of Work and Energy, Principle of Work
Work and Energy, Principle of Work and Energy, Principle of Work

... By integrating the equation of motion,  Ft = mat = mv(dv/ds), the principle of work and energy can be written as  U1-2 = 1/2m(v2)2 – 1/2m(v1)2 or T1 +  U1-2 = T2 U1-2 is the work done by all the forces acting on the particle as it moves from point 1 to point 2. Work can be either a positive or n ...
1 Introduction. Measurable and Nonmea
1 Introduction. Measurable and Nonmea

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How JLab Makes The Beam

Quantum Decoherence and the - Philsci
Quantum Decoherence and the - Philsci

... that the chance that the wave function of a macroscopic system will collapse is overwhelmingly high at all times, whereas for microscopic system the dynamics practically does not differ from the Schrödinger equation. Albert’s approach to the foundations of statistical mechanics assumes that the meas ...
Real-time evolution for weak interaction quenches in quantum systems
Real-time evolution for weak interaction quenches in quantum systems

ch07-4 - Physics-YISS
ch07-4 - Physics-YISS

... Rain comes down with a velocity of -15 m/s and hits the roof of a car. The mass of rain per second that strikes the roof of the car is 0.060 kg/s. Assuming that rain comes to rest upon striking the car, find the average force exerted by the rain on the roof. ...
5 Path Integrals in Quantum Mechanics and Quantum Field Theory
5 Path Integrals in Quantum Mechanics and Quantum Field Theory

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20071031110012301

... T. McLoughlin, J. Minahan, R. Roiban, K. Zarembo for further collaborations ...
Download PDF
Download PDF

... essentially freeze into a stable configuration with very little subsequent dynamics (Video S3†). This discrepancy with respect to both simulations and experimental observations suggests that This journal is ª The Royal Society of Chemistry 2011 ...
A brief introduction to chiral perturbation theory
A brief introduction to chiral perturbation theory

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sclecture7

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Functional RG for few

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PHYSICS VS. SEMANTICS: A PUZZLING CASE

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l - Bryn Mawr College

Symmetries and Conservation Laws
Symmetries and Conservation Laws

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Relativistic quantum mechanics

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