'Hamiltonian' diaporamas de présentation

Journal Club: Introduction to Fluorescence Spectroscopy and Microscopy Avtar Singh 4/5/11

Journal Club: Introduction to Fluorescence Spectroscopy and Microscopy Avtar Singh 4/5/11. Introduction to Journal Club. discuss basic tools / ideas that are useful to all of us ask questions! topic-based or article-based? slides posted on DRBIO site. What is Fluorescence?.

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5. ATOMIC DYNAMICS IN AMORPHOUS SOLIDS

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The Study of Off-momentum Particle Motion with Independent Component Analysis

Weiming Guo Accelerator Physics Group / ASD Advanced Photon Source. The Study of Off-momentum Particle Motion with Independent Component Analysis. Acknowledgements. Katherine Harkay Xiaobiao Huang Michael Borland Jack Albert Chunxi Wang Hairong Shang.

374 views • 25 slides

PHY 7 11 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103

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Lectures 10-11: Multi-electron atoms

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Advanced FFAG and Cyclotron Design and Modeling Software using COSY infinity

Advanced FFAG and Cyclotron Design and Modeling Software using COSY infinity. Dr. C. Johnstone , Fermilab. FFAG13 13 th International Workshop on FFAGs TRIUMF Sept 23 2013 Vancouver, Canada. Recent Advances in Lattice Design and Optimization.

382 views • 22 slides

Helium

1.73k views • 18 slides

Effective Field Theory and Singular Potentials

Effective Field Theory and Singular Potentials. Kregg Philpott Grove City College. Advisor: Silas Beane University of Washington INT. August 20, 2001 University of Washington INT REU Program. Introduction - Effective Field Theory.

364 views • 18 slides

PARTITION FUNCTION

PARTITION FUNCTION. Defintion. The partition function Z is an important quantity that encodes the statistical properties of a system in thermodynamic equilibrium. It is a function of temperature and other parameters, such as the volume enclosing a gas. 1. Canonical partition function.

7.38k views • 18 slides

Stochastic Differential Equations

Stochastic Differential Equations. Langevin equations Fokker Planck equations Equilibrium distributions correlation functions Purely dissipative Langevin equation Simple example Generalised stochastic Markov processes Discretized Langevin equations. Simplest form of Langevin equation.

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The Potts Model Partition Function:

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Atomic units

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Communication from SYNERGIA about GSI benchmarking

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The Stark shift of a diatomic molecule

The Stark shift of a diatomic molecule. Contributions to the Stark shift. Hamiltonian for the Stark interaction:. Energy shift by perturbation theory, to second order. Zero. Small, when i and j differ only by rotation.

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Study of A=6 System by Complex-Scaled 4 He+N+N Model

Study of A=6 System by Complex-Scaled 4 He+N+N Model. Nozomi Kurihara Division of Physics, Graduate School of Science, Hokkaido University. Collaborators Yuma Kikuchi and Kiyoshi Kato Division of Physics, Graduate School of Science, Hokkaido University.

249 views • 14 slides

Graph Theory in Molecular Modeling

801 views • 11 slides

Permutations and Hamiltonian Circuits

Permutations and Hamiltonian Circuits. Larry Griffith Basic Notions Seminar October 10, 2007. Warning!. These slides are the FORMAL statements I will be doing informal examples and explanations. What is a Hamiltonian circuit?.

401 views • 10 slides

Weekly Report

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Consider the transition Ar (3p) 6 , 1 S 0 ? Ar (3p) 5 (4p), 1 P 1

Consider the transition Ar (3p) 6 , 1 S 0 ? Ar (3p) 5 (4p), 1 P 1 Is it an allowed transition, and if not, why not? (A) allowed (B) not allowed, because no spin change (C) not allowed, because promoting a p-electron to another p-orbital (D) not allowed, because J=0 ? J=1

218 views • 6 slides

A Method to Rapidly Predict the Injection Rate in Dye Sensitized Solar Cells.

A Method to Rapidly Predict the Injection Rate in Dye Sensitized Solar Cells. Daniel R. Jones and Alessandro Troisi Department of Chemistry and Centre for Scientific Computing, University of Warwick, Coventry, UK. Dye Coated Nanocrystalline TiO 2. Conductive Glass Electrode. Counter

159 views • 1 slides