'6 ev' diaporamas de présentation

William A. Goddard, III, wag@kaist.ac.kr

Lecture 27, December 14, 2009. Nature of the Chemical Bond with applications to catalysis, materials science, nanotechnology, surface science, bioinorganic chemistry, and energy. Course number: KAIST EEWS 80.502 Room E11-101 Hours: 0900-1030 Tuesday and Thursday.

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Preparation Strategies

Preparation Strategies. Preparation of heterogeneous catalysts. Energy ranges. Energy. 0. E f. EB. The Photoemission Process. kinetic energy. work function. initial photon energy. binding energy. Photemission - classical.

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Spitzer 24 um image: l ~ 358 - 359

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William A. Goddard, III, wag@kaist.ac.kr

Lecture 7, September 24, 2009. Nature of the Chemical Bond with applications to catalysis, materials science, nanotechnology, surface science, bioinorganic chemistry, and energy. Course number: KAIST EEWS 80.502 Room E11-101 Hours: 0900-1030 Tuesday and Thursday.

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Claudia Lederer

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Nirmalendu Das ALL INDIA RADIO SILIGURI WEST BENGAL DARJEELING INDIA

Nirmalendu Das ALL INDIA RADIO SILIGURI WEST BENGAL DARJEELING INDIA. COMPLETE UNIFIED THEORY A New effulgence. INTRODUCTION

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photons

photons. Physics 100 Chapt 21. Photoelectric effect. cathode. anode. Vacuum tube. Photoelectric effect. Vacuum tube. Experimental results. Electron KE ( electron Volts). For light freq below f 0 , no electrons leave the cathode. f 0. Even if the light Is very intense.

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Gas-phase IR spectroscopic studies of polar neutral mass-selected complexes

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Electron collisions with the CF x radicals using the R -matrix method

Electron collisions with the CF x radicals using the R -matrix method. Iryna Rozum University College London Supervisors: Prof. J. Tennyson and Prof. N.J. Mason. CONTENT. Introduction The R -matrix method Electron collisions with the CF Electron collisions with the CF 2

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HERON: Projected precision & plans

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Ionization: A key chemical pathway in ices under radiation environment?

Ionization: A key chemical pathway in ices under radiation environment?. Murthy S. Gudipati Jet Propulsion Laboratory, California Institute of Technology, 4800 Oak Grove Drive, Pasadena, CA 91109. Contents. Radiation, Ice and Organic Impurities Ionization - A Quick Tour

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Radiation pressure: why cos 2 ?

Astro 300B: Jan. 24, 2011 Optical Depth Eddington Luminosity Thermal radiation and Thermal Equilibrium. Radiation pressure: why cos 2 ?. Each photon of energy E=h n has momentum h n /c. Want the component of the momentum normal To direction defined by dA, this will be.

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Supporting material for Lecture 3: Gamma-Ray Bursts and their counterparts Light extinction:

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Dynamics of clusters and molecules in strong electromagnetic fields: A TDDFT-MD approach

Environment. Laser. Projectile. Time-resolved dynamics. Dynamics of clusters and molecules in strong electromagnetic fields: A TDDFT-MD approach. Fondamental studies of mechanisms of irradiation and response of clusters coupled with environment. Ionization. Methods on the market.

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Insights into quantum matter from new experiments

Insights into quantum matter from new experiments. Detecting new many body states will require: Atomic scale resolution of magnetic fields Measuring and manipulating electron spins Spatially resolved spectral information on charge dynamics.

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methyl

methyl. ethene. allyl. butadiene. Stabilization energy. 0. eV. Interaction of p orbitals in polyenes at the Huckel level of theory. Energy eV. 12.3. 14.5. 24.8. Stabilization Energy. Energy of electon on isolated p orbital. 2 x. 2x (-11.4 eV). 2 x.

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(a)

n-Doping of Organic Electronic Materials using Air-Stable Organometallics Antoine Kahn, Princeton University, DMR 1005892. Stable 2x18e dimer. E a = 0.23 eV. (a).

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