'Higher order terms' presentation slideshows

CH3. Intro to Solids Lattice geometries Common structures Lattice energies Born-Haber model Thermodynamic effects

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Strongly Anisotropic Motion Laws, Curvature Regularization, and Time Discretization

705 views • 61 slides

The Chameleon A.C.Davis

The Chameleon A.C.Davis with P.Brax, C van deBruck, C.Burrage, J. Khoury, A.Weltman,D.Mota, C.Shelpe, D. Seery and D.Shaw PRD70(04)123518, PRL 99(07)121103; PRD76(07)085010; PRD76(07)124034; 0902.2320 +unpublished Outline Introduction to chameleon theories Chameleon cosmology

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DFT and VdW interactions

DFT and VdW interactions. Marcus Elstner Physical and Theoretical Chemistry, Technical Universi ty of Braunschweig. E ~ 1/ R 6. DFT and VdW interactions. 2 Problems: Pauli repulsion: exchange effect ~ exp( R ?? ) or 1 /R 12 ?? - attraction due to correlation

961 views • 49 slides

The Chameleon A.C.Davis

The Chameleon A.C.Davis. with P.Brax, C van deBruck, C.Burrage, J. Khoury, A.Weltman,D.Mota, C.Shelpe, D. Seery and D.Shaw PRD70(04)123518, PRL 99(07)121103; PRD76(07)085010; PRD76(07)124034; 0902.2320 +unpublished. Outline. Introduction to chameleon theories Chameleon cosmology

669 views • 49 slides

Dense Motion Estimation

CS 636 Computer Vision. Dense Motion Estimation. Nathan Jacobs. overview. any issues or questions? review from last time dense motion estimation relationship to feature-based today: simple motion models next time: more complex motion models. Motion and perceptual organization.

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QPOs and Nonlinear Pendulums

QPOs and Nonlinear Pendulums. Weizmann Institute - January 13th 2008. by Paola Rebusco. QPOs=. Q uasi (=nearly) P eriodic O scillation s Oceanography Electronic circuits Neural systems ASTROPHYSICS. QPOs. Lorentzian Peaks X-ray power spectra Highly Coherent 0.1-1200 Hz

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EMERGENCE OF ASYMMETRY IN EVOLUTION

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EKF , UKF Pieter Abbeel UC Berkeley EECS

EKF , UKF Pieter Abbeel UC Berkeley EECS Many slides adapted from Thrun , Burgard and Fox, Probabilistic Robotics. TexPoint fonts used in EMF. Read the TexPoint manual before you delete this box.: A A A A A A A A A A A A A. Kalman Filter.

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Announcements

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Synchro -beta resonance and noise in beam-beam interaction at LHC

Synchro -beta resonance and noise in beam-beam interaction at LHC. K. Ohmi (KEK) Crab 2008 @ BNL 25-26 Feb. 2008. Synchro -beta resonance in KEKB (weak-strong simulation). Half Crossing angle=11mrad 0 mrad

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Constraining Goldstinos with Constrained Superfields

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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.

375 views • 25 slides

Diffraction and ultraperipheral collisions at ALICE

Rencontres de Moriond : QCD and High Energy Interactions. Diffraction and ultraperipheral collisions at ALICE. Evgeny Kryshen o n behalf of the ALICE collaboration Petersburg Nuclear Physics Institute, Gatchina , Russia 15 March 2013. Contents. Ultra-peripheral physics potential

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An Introduction to leading and next-to-leading BFKL Act. Phys. Pol. B30 (1999) 3679, G.P. Salam

An Introduction to leading and next-to-leading BFKL Act. Phys. Pol. B30 (1999) 3679, G.P. Salam. Introduction BFKL describes the high-energy behavior of the scattering of hadronic objects within the pQCD ? = (O(1)) n

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Simple Harmonic Motion

Simple Harmonic Motion. A restoring force is one that moves a system back to an equilibrium position. Example: mass on frictionless table, attached to spring. Example: gravity acting on a mass hanging from a string. *. Example: gravity acting on a mass hanging from a spring.

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ChE 250 Numeric Methods

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Measurements of CO 2 Molar Mixing Ratio by Infrared Absorption Spectroscopy C, mole fraction ( ? mole mole -1 = ppm)

Measurements of CO 2 Molar Mixing Ratio by Infrared Absorption Spectroscopy C, mole fraction ( ? mole mole -1 = ppm) LI-COR analyzers measure absorbance at 4.26 ? m V = kA (voltage proportional to absorbance) ? c = P c /RT = CP/RT (molar density of absorber)

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Propagation of Errors ( Chapter 3, Taylor )

Propagation of Errors ( Chapter 3, Taylor ). Introduction Example: Suppose we measure the current (I) and resistance (R) of a resistor. Ohm's law relates V and I: V = IR If we know the uncertainties (e.g. standard deviations) in I and R, what is the uncertainty in V?

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