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Lecture 6. Entropy of an Ideal Gas (Ch. 3) Find  (U,V,N,...) – the most challenging step S (U,V,N,...) = k B ln  (U,V,N,...) Solve for U = f (T,V,N,...)
Documents Lecture 6. Entropy of an Ideal Gas (Ch. 3) Find  (U,V,N,...) – the most challenging step S....

Slide 1 Lecture 6. Entropy of an Ideal Gas (Ch. 3) Find  (U,V,N,...) – the most challenging step S (U,V,N,...) = k B ln  (U,V,N,...) Solve for U = f (T,V,N,...) Today…

Fast N-Body Learning Nando de Freitas University of British Columbia
Documents Fast N-Body Learning Nando de Freitas University of British Columbia

Slide 1 Fast N-Body Learning Nando de Freitas University of British Columbia Slide 2 Historical Perspective Non-iterative or “direct” methods for eigenvalue problems…

Time-resolved analysis of large amplitude collective motion in metal clusters Metal clusters : close « cousins » of nuclei Time resolved : « Pump Probe
Documents Time-resolved analysis of large amplitude collective motion in metal clusters Metal clusters : close...

Slide 1 Time-resolved analysis of large amplitude collective motion in metal clusters Metal clusters : close « cousins » of nuclei Time resolved : « Pump Probe » laser…

Microscopic diagonal entropy, heat, and laws of thermodynamics Anatoli Polkovnikov, Boston University AFOSR Roman Barankov – BU Vladimir Gritsev – Harvard
Documents Microscopic diagonal entropy, heat, and laws of thermodynamics Anatoli Polkovnikov, Boston...

Slide 1 Microscopic diagonal entropy, heat, and laws of thermodynamics Anatoli Polkovnikov, Boston University AFOSR Roman Barankov – BU Vladimir Gritsev – Harvard Vadim…

1 Time Arrow, Statistics and the Universe II Physics Summer School 17 July 2002 K. Y. Michael Wong Outline: * Counting and statistical physics * Explaining
Documents 1 Time Arrow, Statistics and the Universe II Physics Summer School 17 July 2002 K. Y. Michael Wong.....

Slide 1 Slide 2 1 Time Arrow, Statistics and the Universe II Physics Summer School 17 July 2002 K. Y. Michael Wong Outline: * Counting and statistical physics * Explaining…

Control of Inhomogeneous Spin Ensembles. Robust Control of Inhomogeneous Spin Ensembles M x y M
Documents Control of Inhomogeneous Spin Ensembles. Robust Control of Inhomogeneous Spin Ensembles M x y M

Slide 1 Control of Inhomogeneous Spin Ensembles Slide 2 Robust Control of Inhomogeneous Spin Ensembles M x y M Slide 3 Compensation and Composite Pulses z x y Slide 4 Robust…

Pablo A. Parrilo ETH Zürich SOS Relaxations for System Analysis: Possibilities and Perspectives Pablo A. Parrilo ETH Zürich  parrilo
Documents Pablo A. Parrilo ETH Zürich SOS Relaxations for System Analysis: Possibilities and Perspectives...

Slide 1 Pablo A. Parrilo ETH Zürich SOS Relaxations for System Analysis: Possibilities and Perspectives Pablo A. Parrilo ETH Zürich control.ee.ethz.ch/~parrilo Slide 2…

Yangian Symmetry in Yang-Mills Theories S. G. Rajeev Seminar at Cornell University Dec 8 th 2004
Documents Yangian Symmetry in Yang-Mills Theories S. G. Rajeev Seminar at Cornell University Dec 8 th 2004

Slide 1 Slide 2 Yangian Symmetry in Yang-Mills Theories S. G. Rajeev Seminar at Cornell University Dec 8 th 2004 Slide 3 Work in Collaboration with Abhishek Agarwal Also…

What is information? Insights from Quantum Physics Benjamin Schumacher Department of Physics Kenyon College
Documents What is information? Insights from Quantum Physics Benjamin Schumacher Department of Physics Kenyon....

Slide 1 What is information? Insights from Quantum Physics Benjamin Schumacher Department of Physics Kenyon College Slide 2 Translation comedy English The spirit is willing…

Electron Scattering Length - Mean Free Path – le - Avg. distance between scattering Si - ~ 5nm; GaAs - ~ 100 nm Electrical Resistance is closely related
Documents Electron Scattering Length - Mean Free Path – le - Avg. distance between scattering Si - ~...

Slide 1 Slide 2 Electron Scattering Length - Mean Free Path – le - Avg. distance between scattering Si - ~ 5nm; GaAs - ~ 100 nm Electrical Resistance is closely related…