4. Paras M. Agrawal and M. P. Saksena, Rotational relaxation in mixtures of hydrogen isotopes with noble gases, J. Phys. (U.K.) B8, 1575 (1975).
|
|
- Tracy Austin Floyd
- 6 years ago
- Views:
Transcription
1 Research papers. 1. M. P. Saksena, Paras M. Agrawal, and Harminder, Distribtion of relaxation times and ultrasonic absorption in ammonia, Indian J. Pure & Applied Physics 11, 563 (1973). 2. Paras M. Agrawal and M. P. Saksena, Rotational relaxation in polar gases, J. Chem. Phys. 61, 848 (1974). 3. Paras M. Agrawal and M. P. Saksena, Rotational relaxation in H2 and D2 due to collisions with noble gas atoms, Chem. Phys. Lett. 32, 123 (1975). 4. Paras M. Agrawal and M. P. Saksena, Rotational relaxation in mixtures of hydrogen isotopes with noble gases, J. Phys. (U.K.) B8, 1575 (1975). 5. Paras M. Agrawal and M. P. Saksena, Rotational relaxation in HD-inert gas mixtures, J. Chem. Phys. 65, 550 (1976). 6. Paras M. Agrawal and L. M. Raff, Consideration of the exit channel velocity effect upon inelastic cross sections computed by the infinite- order-sudden approximation, J. Chem. Phys. 74, 3292 (1981). 7. Paras M. Agrawal and L. M. Raff, Calculation of reaction probabilities and rate coefficients for collinear three-body exchange reaction using time-dependent wave packet methods, J. Chem. Phys. 74, 5076 (1981). 8. Paras M. Agrawal and L. M. Raff, IOSA investigations of the effects of potential surface topography upon elastic and inelastic scattering and rotational relaxation in the (He, CO2) system, J. Chem. Phys. 75, 2163 (1981). 9. R. Viswanathan, Paras M. Agrawal and L. M. Raff, Comparison of modified infinite order sudden theory with the experimentally measured state-to-state cross sections for R-T energy transfer in Ar-HF, J. Chem. Phys. 75, 3860 (1981). 10. Paras M. Agrawal and L. M. Raff, A semiclassical wavepacket model for the investigation of elastic and inelastic gassurface scattering, J. Chem. Phys. 77, 3946 (1982). 1
2 11. Paras M. Agrawal, N. C. Agrawal, R. Viswanathan and L. M. Raff, Rate calculations from timedependent wavepacket methods: The relationship of the pure state and canonical total reaction probability, J. Chem. Phys. 80, 760 (1984). 12. Paras M. Agrawal, V. Mohan and N. Sathyamurthy, Time-dependent wave mechanical study of the wings to the Lyman- á line in atomic hydrogen + molecular hydrogen reactive collisions, Chem. Phys. Lett. 114, 343 (1985). 13. Paras M. Agrawal and N. C. Agrawal, Rotational energy transfer in the rigid rotor CO2-Ar system and the energy dependence of the parameters of the power-gap law, Chem. Phys. Let. 117, 451 (1985). 14. Paras M. Agrawal and N. C. Agrawal, Integral inelastic cross sections for the rotational energy transfer in CO2-Ar system, Current Science (India) 54, 689 (1985). 15. Paras M. Agrawal, N. C. Agrawal and Vinod Garg, Power-gap law and the dynamical constraints on the angular momentum transfer in rotationally inelastic molecular collisions, Chem. Phys. Let. 118, 213, (1985). 16. C. B. Smith, L. M. Raff and Paras M. Agrawal, Semiclassical wavepacket studies of elastic and inelastic atom-surface scattering from a 3D model surface, J. Chem. Phys. 83, 1411 (1985). 17. Paras M. Agrawal, N. C. Agrawal and V. Garg, Dynamical constraints on the angular momentum transfer in rotationally inelastic molecular collisions, J. Chem. Phys. 83, 4444 (1985). 18. Paras M. Agrawal and Vinod Garg, Rotational energy transfer in CO2-He system and the two parameter power-gap model, Indian J. Pure & Applied Physics 23, 392 (1985). 19. Paras M. Agrawal and V. Garg, On the validity of the power-gap law and the exponential-gap law for rotational energy transfer in CO2-He system, Acta Physica Polonica A69, 103 (1986). 2
3 20. Paras M. Agrawal and N. C. Agrawal, Dynamical constraints on the angular momentum transfer between polar molecules, Chem. Phys. Let. 122, 37 (1985). 21. Paras M. Agrawal, L. M. Raff, and D. L. Thompson, Effect of the lattice model on the dynamics of dissociative chemisorption of H2 on a Si(111) surface, Surface Science 188, 402 (1987). 22. M. Jezercak, Paras M. Agrawal, C. B. Smith and L. M. Raff, Wave packet studies of gas-surface inelastic scattering and desorption rates, J. Chem. Phys. 88, 1264 (1988). 23. Paras M. Agrawal, D. L. Thompson and L. M. Raff, Computational Studies of Heterogeneous Reactions of SiH2 on Si(111) surfaces, Surface Science 195, 283 (1988). 24. Paras M. Agrawal, D. L. Thompson and L. M. Raff, Computational studies of SiH2 + SiH2 recombination reaction dynamics on a global potential surface fitted to ab initio and experimental data, J. Chem. Phys. 88, 5948 (1988). 25. Paras M. Agrawal, D. L. Thompson and L. M. Raff, Trajectory studies of unimolecular reactions of Si2H4 and SiH2 on a global potential surface fitted to ab initio and experimental data, J. Chem. Phys. 89, 741 (1988). 26. M. Jezercak, Paras M. Agrawal, D. L. Thompson and L. M. Raff, A perturbation-trajectory method for the study of gas-surface collision dynamics, J. chem. Phys. 90, 3363 (1989). 27. Paras M. Agrawal, D. L. Thompson and L. M. Raff, Computational studies of heterogeneous reactions of SiH2 on reconstructed Si(111)-(7x7) and Si(111)-(1x1) surfaces, J. Chem. Phys. 91, 5021 (1989). 28. Paras M. Agrawal, D. L. Thompson and L. M. Raff, Variational phase-space theory studies of Siliconatom diffusion on reconstructed Si(111)-(7x7) surfaces, J. Chem. Phys. 91, 6463 (1989). 29. Paras M. Agrawal, D. L. Thompson and L. M. Raff, Unimolecular dissociation dynamics of disilane, J. Chem. Phys. 92, 1069(1990). 3
4 30. Paras M. Agrawal, D. L. Thompson and L. M. Raff, Comparison of silicon-atom diffusion on the dimer-adatom-stacking fault and Binning et al. Models of the reconstructed Si(111)-(7x7) surface, J. Chem. Phys. 94, 6243 (1991). 31. Paras M. Agrawal and Vinod Gard, The dependence of rotationally inelastic cross sections on the parameters of the potential, Current Science 61, 43 (1991). 32. Paras M. Agrawal, V. Garg, and K. R. Patidar, Rotationally inelastic cross-sections and parameters of the potential energy surface, Indian Journal of Pure and Applied Physics 31, 187(1993). 33. Paras M. Agrawal V. Garg, and K. R. Patidar, Rotationally inelastic cross sections and the parameters of the potential, Chem. Phys. Let. 208, 204 (1993). 34. Paras M. Agrawal, V. Garg, and K. R. Patidar, Potential parameters and energy dependence of rotational energy transfer in molecular systems, Acta Physica Polonica 84, 247 (1993). 35. Paras M. Agrawal, K. R. Patidar, and N. K. Dabkara, Potential energy surface for NO-He system from the state-to-state rate coefficients, Indian Journal of Pure and Applied Physics 32, 750 (1994). 36. Paras M. Agrawal, D. L. Thompson and L. M. Raff, Theoretical investigation of nonstatistical dynamics, energy transfer, and intramolecular vibrational relaxation in isomerization reactions of matrixisolated HONO/Xe, J. Chem. Phys 101, 9937(1994). 37. Paras M. Agrawal, D. L. Thompson and L. M. Raff, Theoretical studies of the effects of matrix composition, lattice temperature, and isotopic substitution on isomerization reactions of matrix-isolated HONO/Ar, J. Chem. Phys. 102, 7000 (1995). 38. Paras M. Agrawal, D. C. Sorescu, L. M. Raff, and S. A. Abrash, Theoretical investigations of vinyl bromide dissociation in Xe and Kr matrices, J. Phys. Chem., 99, (1995). 39. Paras M. Agrawal, D. C. Sorescu, R. D. Kay, D. L. Thompson, L. M. Raff, J. B. Conrey and A. K. Jameson, Spectral line shapes in systems undergoing continuous frequency modulation, 4
5 J. Chem. Phys. 105, 2686 (1996). 40. Paras M. Agrawal, N. K. Dabkara, and S. Tilwankar, Rotational energy transfer in NO-Ar system and the validity of different forms of the potential, Chem. Phys. Let. 266, 481 (1997). 41. Paras M. Agrawal, N. K. Dabkara, and S. Tilwankar, Rotational energy transfer in NO-Ar system and the validity of the pairwise sum of the potential, Indian Journal of Pure and Applied Physics 35, 299 (1997). 42. Paras M. Agrawal, S. Tilwankar, and N. K. Dabkara, The hard ellipsoid potential model and the limit of rotational energy transfer in molecular collisions, J. Chem. Phys. 108, 4854 (1998). 43. Paras M. Agrawal and S. Tilwankar, Rotational energy transfer in molecular collisions and parameters of power-gap law, Acta Physica Polonica A93, 451 (1998). 44. N. K. Dabkara and Paras M. Agrawal, The maximum limit of rotational energy transfer in collisions of N2 with Ne and the power-gap law, Chem. Phys. Let. 299, 125 (1999). 45. Paras M. Agrawal, D. C. Sorescu, B. M. Rice and D. L. Thompson, A model for predicting the solubility of RDX in supercritical CO2: Isothermal- Isobaric Monte Carlo simulations, Fluid Phase Equilibria 155, 177 (1999). 46. Paras M. Agrawal, B. M. Rice, D. C. Sorescu, and D. L. Thompson, NPT-MC simulations of enhanced solubility of RDX in polar-modified supercritical CO2, Fluid Phase Equilibria 166, 1 (1999). 47. Paras M. Agrawal, B. M. Rice, D. C. Sorescu, and D. L. Thompson, Models for predicting solubilities of trinitrotluene (TNT) and 1,3,5-trinitro- 1,3,5-s-triazine (RDX) in supercritical CO2: isothermalisobaric Monte Carlo simulations, Fluid Phase Equilibria , 139 (2001). 48. Seong K. Kim, J. M. White, Paras M. Agrawal and D. L. Thompson, J. Chem. Phys. 115, 7657 (2001). 5
6 49. Paras M. Agrawal, B. M. Rice, and D. L. Thompson, Predicting trends in rate parameters for selfdiffusion on FCC metal surfaces, Surface Science 515, 21 (2002). 50. Paras M. Agrawal, Betsy M. Rice and Donald L. Thompson, Molecular Dynamics Study on the Effects of Voids and Pressure in Defect- Nucleated Melting Simulations, J. Chem. Phys. 118, (2003). 51. Paras M. Agrawal, Betsy M. Rice and Donald L. Thompson, Molecular Dynamics Study of the Melting of Nitromethane, J. Chem. Phys., 119, (2003). 6
The maximum amount of rotational energy transfer in F 2 -He system and hard ellipsoid potential model.
IOSR Journal of Applied Physics (IOSR-JAP) ISSN: 2278-4861. Volume 2, Issue 5 (Nov. - Dec. 2012), PP 01-05 The maximum amount of rotational energy transfer in F 2 -He system and hard ellipsoid potential
More informationINTERMOLECULAR FORCES
INTERMOLECULAR FORCES Their Origin and Determination By GEOFFREY C. MAITLAND Senior Research Scientist Schlumberger Cambridge Research, Cambridge MAURICE RIGBY Lecturer in the Department of Chemistry King's
More informationCross Sections: Key for Modeling
Cross Sections: Key for Modeling Vasili Kharchenko Department of Physics, University of Connecticut Harvard-Smithsonian Center for Astrophysics, Cambridge, USA 1. Introduction: a) non-thermal atoms and
More informationState-to-State Kinetics of Molecular and Atomic Hydrogen Plasmas
State-to-State Kinetics of Molecular and Atomic Hydrogen Plasmas MARIO CAPITELLI Department of Chemistry, University of Bari (Italy) CNR Institute of Inorganic Methodologies and Plasmas Bari (Italy) MOLECULAR
More informationMolecular Aggregation
Molecular Aggregation Structure Analysis and Molecular Simulation of Crystals and Liquids ANGELO GAVEZZOTTI University of Milano OXFORD UNIVERSITY PRESS Contents PART I FUNDAMENTALS 1 The molecule: structure,
More informationResonances in Chemical Reactions : Theory and Experiment. Toshiyuki Takayanagi Saitama University Department of Chemistry
Resonances in Chemical Reactions : Theory and Experiment Toshiyuki Takayanagi Saitama University Department of Chemistry What is Chemical Reaction? Collision process between molecules (atoms) containing
More informationFoundations of Chemical Kinetics. Lecture 19: Unimolecular reactions in the gas phase: RRKM theory
Foundations of Chemical Kinetics Lecture 19: Unimolecular reactions in the gas phase: RRKM theory Marc R. Roussel Department of Chemistry and Biochemistry Canonical and microcanonical ensembles Canonical
More informationPhoton Interaction. Spectroscopy
Photon Interaction Incident photon interacts with electrons Core and Valence Cross Sections Photon is Adsorbed Elastic Scattered Inelastic Scattered Electron is Emitted Excitated Dexcitated Stöhr, NEXAPS
More informationChapter VI: Ionizations and excitations
Chapter VI: Ionizations and excitations 1 Content Introduction Ionization in gases Ionization in solids Fano factor 2 Introduction (1) Ionizations created by charged particles (incident particles or particles
More informationBrazilian Journal of Physics, vol. 36, no. 3A, September,
Brazilian Journal of Physics, vol. 36, no. 3A, September, 2006 725 Effects of Molecular Rovibrational States and Surface Topologies for Molecule-Surface Interaction: Chemisorption Dynamics of D 2 Collision
More information(12) Large local energy fluctuations in water. H. Tanaka and I. Ohmine, J. Chem. Phys., 87, (1987).115
(01) Free energy of mixing, phase stability, and local composition in Lennard-Jones liquid mixtures. K. Nakanishi, Susumu Okazaki, K. Ikari, T. Higuchi, and J. Chem. Phys., 76, 629-636 (1982). 91 (02)
More informationProperties of Individual Nanoparticles
TIGP Introduction technology (I) October 15, 2007 Properties of Individual Nanoparticles Clusters 1. Very small -- difficult to image individual nanoparticles. 2. New physical and/or chemical properties
More informationA GENERAL TRANSFORMATION TO CANONICAL FORM FOR POTENTIALS IN PAIRWISE INTERMOLECULAR INTERACTIONS
1 A GENERAL TRANSFORMATION TO CANONICAL FORM FOR POTENTIALS IN PAIRWISE INTERMOLECULAR INTERACTIONS Jay R. Walton Department of Mathematics, Texas A & M University College Station, TX, USA Luis A. Rivera-Rivera,
More informationErrors in electron - molecule collision calculations (at low energies)
e - Errors in electron - molecule collision calculations (at low energies) Jonathan Tennyson University College London Outer region Inner region IAEA May 2013 Electron processes: at low impact energies
More informationPRINCIPLES OF ADSORPTION AND REACTION ON SOLID SURFACES
PRINCIPLES OF ADSORPTION AND REACTION ON SOLID SURFACES Richard I. Masel Department of Chemical Engineering University of Illinois at Urbana-Champaign Urbana, Illinois A WILEY-INTERSCIENCE PUBLICATION
More informationAcidic Water Monolayer on Ruthenium(0001)
Acidic Water Monolayer on Ruthenium(0001) Youngsoon Kim, Eui-seong Moon, Sunghwan Shin, and Heon Kang Department of Chemistry, Seoul National University, 1 Gwanak-ro, Seoul 151-747, Republic of Korea.
More informationQuantum Monte Carlo Benchmarks Density Functionals: Si Defects
Quantum Monte Carlo Benchmarks Density Functionals: Si Defects K P Driver, W D Parker, R G Hennig, J W Wilkins (OSU) C J Umrigar (Cornell), R Martin, E Batista, B Uberuaga (LANL), J Heyd, G Scuseria (Rice)
More informationDirect Molecular Simulation of Hypersonic Flows
Direct Molecular Simulation of Hypersonic Flows Thomas E. Schwartzentruber Aerospace Engineering & Mechanics University of Minnesota UMN Students and Researchers: Savio Poovathingal 1 Paul Norman 3 Chonglin
More informationEstimations of Rotational Relaxation Parameters in Diatomic Gases
Estimations of Rotational Relaxation Parameters in Diatomic Gases Vladimir V. Riabov Department of Mathematics and Computer Science, Rivier College, 420 S. Main St., Nashua, NH 03060, USA Abstract: The
More informationAcademic and Research Staff. Dr. C.H. Becker Dr. R.A. Gottscho Dr. M.L. Zimmerman Dr. T.A. Brunner Dr. A. Morales-Mori Dr. W.H.
V. ATOMIC RESONANCE AND SCATTERING Academic and Research Staff Prof. D. Kleppner Prof. D.E. Pritchard Dr. T.W. Ducas* Dr. M.B. Elbel Dr. J.R. Rubbmark Dr. J.A. Serri Dr. C.H. Becker Dr. R.A. Gottscho Dr.
More informationRotational-translational relaxation effects in diatomic-gas flows
Rotational-translational relaxation effects in diatomic-gas flows V.V. Riabov Department of Computer Science, Rivier College, Nashua, New Hampshire 03060 USA 1 Introduction The problem of deriving the
More informationEmily A. Carter. REPORT DOCUMENTATION PAGE OM8 No F 03 C) S
SECURITY CLASSIFICATION OF THIS PAGE la. REPORT SECURITY CLASSIFICATION Unclassified RN Form Approved REPORT DOCUMENTATION PAGE OM8 No. 0704.0188 lb. RESTRICTIVE MARKINGS 2a. SECURITY CLASSIFICATION AUTHORITY
More informationNeutron and X-ray Scattering Studies
Neutron and X-ray Scattering Studies Alexis G. Clare NYSCC Alfred NY Clare@alfred.edu clare@alfred.edu Scattering Studies4 1 Outline Review interpreting correlation functions Some more examples Inelastic
More informationLaser MEOP of 3 He: Basic Concepts, Current Achievements, and Challenging Prospects
Polarization in Noble Gases, October 8-13, 2017 Laser MEOP of 3 He: Basic Concepts, Current Achievements, and Challenging Prospects Pierre-Jean Nacher Geneviève Tastevin Laboratoire Kastler-Brossel ENS
More informationPHYSICS OF SEMICONDUCTORS AND THEIR HETEROSTRUCTURES
PHYSICS OF SEMICONDUCTORS AND THEIR HETEROSTRUCTURES Jasprit Singh University of Michigan McGraw-Hill, Inc. New York St. Louis San Francisco Auckland Bogota Caracas Lisbon London Madrid Mexico Milan Montreal
More informationConcepts in Surface Physics
M.-C. Desjonqueres D. Spanjaard Concepts in Surface Physics Second Edition With 257 Figures Springer 1. Introduction................................. 1 2. Thermodynamical and Statistical Properties of
More informationEffect of the Inner-Zone Vibrations on the Dynamics of Collision-Induced Intramolecular Energy Flow in Highly Excited Toluene
Notes Bull. Korean Chem. Soc. 2005, Vol. 26, No. 8 1269 Effect of the Inner-Zone Vibrations on the Dynamics of Collision-Induced Intramolecular Energy Flow in Highly Excited Toluene Jongbaik Ree, * Yoo
More informationSolid Surfaces, Interfaces and Thin Films
Hans Lüth Solid Surfaces, Interfaces and Thin Films Fifth Edition With 427 Figures.2e Springer Contents 1 Surface and Interface Physics: Its Definition and Importance... 1 Panel I: Ultrahigh Vacuum (UHV)
More informationVibrationally Mediated Bond Selective Dissociative Chemisorption of HOD on Cu(111) Supporting Information
Submitted to Chem. Sci. 8/30/202 Vibrationally Mediated Bond Selective Dissociative Chemisorption of HOD on Cu() Supporting Information Bin Jiang,,2 Daiqian Xie,,a) and Hua Guo 2,a) Institute of Theoretical
More informationDETERMINATION OF THE POTENTIAL ENERGY SURFACES OF REFRIGERANT MIXTURES AND THEIR GAS TRANSPORT COEFFICIENTS
THERMAL SCIENCE: Year 07, Vo., No. 6B, pp. 85-858 85 DETERMINATION OF THE POTENTIAL ENERGY SURFACES OF REFRIGERANT MIXTURES AND THEIR GAS TRANSPORT COEFFICIENTS Introduction by Bo SONG, Xiaopo WANG *,
More informationElastic and Inelastic Scattering in Electron Diffraction and Imaging
Elastic and Inelastic Scattering in Electron Diffraction and Imaging Contents Introduction Symbols and definitions Part A Diffraction and imaging of elastically scattered electrons Chapter 1. Basic kinematical
More information1. Cold Collision Basics
ICAP Summer School, Seoul, S. Korea, July 18, 2016 1. Cold Collision Basics Paul S. Julienne Joint Quantum Institute NIST and The University of Maryland Thanks to many colleagues in theory and experiment
More informationAn Introduction to Chemical Kinetics
An Introduction to Chemical Kinetics Michel Soustelle WWILEY Table of Contents Preface xvii PART 1. BASIC CONCEPTS OF CHEMICAL KINETICS 1 Chapter 1. Chemical Reaction and Kinetic Quantities 3 1.1. The
More informationMultiple Choices: Choose the best (one) answer. Show in bold. Multiple Choices: Choose the best answer. The correct answer is shown in bold character.
HCCS CHEM 1405 PRACTICE EXAM IV: 5 th, 6 th and 7 th editions of Corwin s Introductory Chemistry textbook Multiple Choices: Choose the best (one) answer. Show in bold. Multiple Choices: Choose the best
More informationSTM spectroscopy (STS)
STM spectroscopy (STS) di dv 4 e ( E ev, r) ( E ) M S F T F Basic concepts of STS. With the feedback circuit open the variation of the tunneling current due to the application of a small oscillating voltage
More informationParticle Behavior of Light 1. Calculate the energy of a photon, mole of photons 2. Find binding energy of an electron (know KE) 3. What is a quanta?
Properties of Electromagnetic Radiation 1. What is spectroscopy, a continuous spectrum, a line spectrum, differences and similarities 2. Relationship of wavelength to frequency, relationship of E to λ
More informationMicroscopical and Microanalytical Methods (NANO3)
Microscopical and Microanalytical Methods (NANO3) 06.11.15 10:15-12:00 Introduction - SPM methods 13.11.15 10:15-12:00 STM 20.11.15 10:15-12:00 STS Erik Zupanič erik.zupanic@ijs.si stm.ijs.si 27.11.15
More information1.3 Molecular Level Presentation
1.3.1 Introduction A molecule is the smallest chemical unit of a substance that is capable of stable, independent existence. Not all substances are composed of molecules. Some substances are composed of
More informationCoherent elastic and rotationally inelastic scattering of N 2,O 2, and CH 4 froma10kcu 111 surface
JOURNAL OF CHEMICAL PHYSICS VOLUME 113, NUMBER 20 22 NOVEMBER 2000 Coherent elastic and rotationally inelastic scattering of N 2,O 2, and CH 4 froma10kcu 111 surface T. Andersson, F. Althoff, P. Linde,
More informationATOMS. Central field model (4 quantum numbers + Pauli exclusion) n = 1, 2, 3,... 0 l n 1 (0, 1, 2, 3 s, p, d, f) m l l, m s = ±1/2
ATOMS Central field model (4 quantum numbers + Pauli exclusion) n = 1, 2, 3,... 0 l n 1 (0, 1, 2, 3 s, p, d, f) m l l, m s = ±1/2 Spectroscopic notation: 2S+1 L J (Z 40) L is total orbital angular momentum
More informationSupplementary Fig. 1. Progress of the surface mediated Ullmann coupling reaction using STM at 5 K. Precursor molecules
Supplementary Fig. 1. Progress of the surface mediated Ullmann coupling reaction using STM at 5 K. Precursor molecules (4-bromo-1-ethyl-2-fluorobenzene) are dosed on a Cu(111) surface and annealed to 80
More informationMonte Carlo Modelling of Hot Particle Coronae
ling of Hot Particle Coronae H. Lichtenegger Space Research Institute, Austrian Academy of Sciences, Graz, Austria N2 Workshop, Helsinki/FMI 29-31 Oct 2007 1 Goal 3D Monte Carlo model of hot particle coronae
More informationFermions in the unitary regime at finite temperatures from path integral auxiliary field Monte Carlo simulations
Fermions in the unitary regime at finite temperatures from path integral auxiliary field Monte Carlo simulations Aurel Bulgac,, Joaquin E. Drut and Piotr Magierski University of Washington, Seattle, WA
More informationAtom-molecule molecule collisions in spin-polarized polarized alkalis: potential energy surfaces and quantum dynamics
Atom-molecule molecule collisions in spin-polarized polarized alkalis: potential energy surfaces and quantum dynamics Pavel Soldán, Marko T. Cvitaš and Jeremy M. Hutson University of Durham with Jean-Michel
More informationModeling the sputter deposition of thin film photovoltaics using long time scale dynamics techniques
Loughborough University Institutional Repository Modeling the sputter deposition of thin film photovoltaics using long time scale dynamics techniques This item was submitted to Loughborough University's
More informationT-matrix calculations for the electron-impact ionization of hydrogen in the Temkin-Poet model
T-matrix calculations for the electron-impact ionization of hydrogen in the Temkin-Poet model M. S. Pindzola, D. Mitnik, and F. Robicheaux Department of Physics, Auburn University, Auburn, Alabama 36849
More informationPH 548 Atomistic Simulation Techniques
PH 548 Atomistic Simulation Techniques Lectures: Lab: 2-0-2-6 Tuesday 12-1 PM Thursday 12-1 PM Monday 2-5 PM P. K. Padmanabhan PH548: Two Excellent Books How to do it? 1 2 F 12 F 23 3 F i = F ij j i F
More informationDevelopment of a Water Cluster Evaporation Model using Molecular Dynamics
Development of a Water Cluster Evaporation Model using Molecular Dynamics Arnaud Borner, Zheng Li, Deborah A. Levin. Department of Aerospace Engineering, The Pennsylvania State University, University Park,
More informationCynthia J. Jameson University of Illinois at Chicago
19 F NMR The temperature dependence of chemical shifts: mechanisms and contributions Cynthia J. Jameson University of Illinois at Chicago T 1 outline the intramolecular shielding surface temperature dependence
More informationVibrationally resolved ion-molecule collisions
Vibrationally resolved ion-molecule collisions CRP: Atomic and Molecular Data for State-Resolved Modelling of Hydrogen and Helium and Their Isotopes in Fusion plasma Predrag Krstic Physics Division, Oak
More informationMultiscale Materials Modeling
Multiscale Materials Modeling Lecture 02 Capabilities of Classical Molecular Simulation These notes created by David Keffer, University of Tennessee, Knoxville, 2009. Outline Capabilities of Classical
More informationTHERMODYNAMICS AND TRANSPORT PROPERTIES OF ABLATED SPECIES
THERMODYNAMICS AND TRANSPORT PROPERTIES OF ABLATED SPECIES A D Angola 1,2, G. Colonna 2, L. D. Pietanza 2, M. Capitelli 2, F. Pirani 3, E. Stevanato 4 and A. Laricchiuta 2 1 Scuola di Ingegneria, Università
More informationTheory of Gas Discharge
Boris M. Smirnov Theory of Gas Discharge Plasma l Springer Contents 1 Introduction 1 Part I Processes in Gas Discharge Plasma 2 Properties of Gas Discharge Plasma 13 2.1 Equilibria and Distributions of
More informationModule 5: "Adsoption" Lecture 25: The Lecture Contains: Definition. Applications. How does Adsorption occur? Physisorption Chemisorption.
The Lecture Contains: Definition Applications How does Adsorption occur? Physisorption Chemisorption Energetics Adsorption Isotherms Different Adsorption Isotherms Langmuir Adsorption Isotherm file:///e
More informationTable of Contents [ttc]
Table of Contents [ttc] 1. Equilibrium Thermodynamics I: Introduction Thermodynamics overview. [tln2] Preliminary list of state variables. [tln1] Physical constants. [tsl47] Equations of state. [tln78]
More informationLecture 6: High Voltage Gas Switches
Lecture 6: High Voltage Gas Switches Switching is a central problem in high voltage pulse generation. We need fast switches to generate pulses, but in our case, they must also hold off high voltages before
More informationElectronic Processes on Semiconductor Surfaces during Chemisorption
Electronic Processes on Semiconductor Surfaces during Chemisorption T. Wolkenstein Translatedfrom Russian by E. M. Yankovskii Translation edited in part by Roy Morrison CONSULTANTS BUREAU NEW YORK AND
More informationDynamical Monte-Carlo Simulation of Surface Kinetics
Dynamical Monte-Carlo Simulation of Surface Kinetics V. Guerra and J. Loureiro Centro de Física dos Plasmas, Instituto Superior Técnico, 1049-001 Lisboa, Portugal Abstract. This wor presents a theoretical
More informationModel Question Paper PART A ANSWER ALL QUESTIONS:
Std: XI Standard Subject: Chemistry ANSWER ALL QUESTIONS: Model Question Paper PART A Time: 2.30 hours Max Marks: 75 Marks (15X1=15) 1. Which one of the following is a standard for atomic mass? a) 6 C
More informationLecture 3 Vacuum Science and Technology
Lecture 3 Vacuum Science and Technology Chapter 3 - Wolf and Tauber 1/56 Announcements Homework will be online from noon today. This is homework 1 of 4. 25 available marks (distributed as shown). This
More informationNumerical simulation of Vibrationally Active Ar-H2 Microwave Plasma
Numerical simulation of Vibrationally Active Ar-H2 Microwave Plasma F. Bosi 1, M. Magarotto 2, P. de Carlo 2, M. Manente 2, F. Trezzolani 2, D. Pavarin 2, D. Melazzi 2, P. Alotto 1, R. Bertani 1 1 Department
More informationAR-7781 (Physical Chemistry)
Model Answer: B.Sc-VI th Semester-CBT-602 AR-7781 (Physical Chemistry) One Mark Questions: 1. Write a nuclear reaction for following Bethe s notation? 35 Cl(n, p) 35 S Answer: 35 17Cl + 1 1H + 35 16S 2.
More information1. I can use Collision Theory to explain the effects of concentration, particle size, temperature, and collision geometry on reaction rates.
Chemical Changes and Structure Learning Outcomes SECTION 1 Controlling the Rate. Subsection (a) Collision Theory 1. I can use Collision Theory to explain the effects of concentration, particle size, temperature,
More informationFormation of the simplest stable negative molecular ion H 3. in interstellar medium
Formation of the simplest stable negative molecular ion H 3 in interstellar medium V. Kokoouline 1,2, M. Ayouz 1, R. Guerout 1, M. Raoult 1, J. Robert 1, and O. Dulieu 1 1 Laboratoire Aimé Cotton, CNRS,
More informationComputational Physics. J. M. Thijssen
Computational Physics J. M. Thijssen Delft University of Technology CAMBRIDGE UNIVERSITY PRESS Contents Preface xi 1 Introduction 1 1.1 Physics and computational physics 1 1.2 Classical mechanics and statistical
More informationMinimal Update of Solid State Physics
Minimal Update of Solid State Physics It is expected that participants are acquainted with basics of solid state physics. Therefore here we will refresh only those aspects, which are absolutely necessary
More informationPhase Equilibria of binary mixtures by Molecular Simulation and PR-EOS: Methane + Xenon and Xenon + Ethane
International Journal of ChemTech Research CODEN( USA): IJCRGG ISSN : 0974-4290 Vol.5, No.6, pp 2975-2979, Oct-Dec 2013 Phase Equilibria of binary mixtures by Molecular Simulation and PR-EOS: Methane +
More informationP. W. Atkins and R. S. Friedman. Molecular Quantum Mechanics THIRD EDITION
P. W. Atkins and R. S. Friedman Molecular Quantum Mechanics THIRD EDITION Oxford New York Tokyo OXFORD UNIVERSITY PRESS 1997 Introduction and orientation 1 Black-body radiation 1 Heat capacities 2 The
More informationEffect of small amounts of hydrogen added to argon glow discharges: Hybrid Monte Carlo fluid model
PHYSICAL REVIEW E, VOLUME 65, 056402 Effect of small amounts of hydrogen added to argon glow discharges: Hybrid Monte Carlo fluid model Annemie Bogaerts* and Renaat Gijbels Department of Chemistry, University
More informationCollisional energy transfer modeling in non-equilibrium condensing flows
Collisional energy transfer modeling in non-equilibrium condensing flows Natalia Gimelshein, Ingrid Wysong and Sergey Gimelshein ERC, Inc, Edwards AFB, CA 93524 Propulsion Directorate, Edwards AFB, CA
More informationSurface diffusion control of the photocatalytic oxidation in air/tio2 heterogeneous reactors
Phys. Chem. Comm. 5 (2002) 161-164 Surface diffusion control of the photocatalytic oxidation in air/tio2 heterogeneous reactors Roumen Tsekov Department of Physical Chemistry, University of Sofia, 1164
More informationHigh pressure core structures of Si nanoparticles for solar energy conversion
High pressure core structures of Si nanoparticles for solar energy conversion S. Wippermann, M. Vörös, D. Rocca, A. Gali, G. Zimanyi, G. Galli [Phys. Rev. Lett. 11, 4684 (213)] NSF/Solar DMR-135468 NISE-project
More informationAu-C Au-Au. g(r) r/a. Supplementary Figures
g(r) Supplementary Figures 60 50 40 30 20 10 0 Au-C Au-Au 2 4 r/a 6 8 Supplementary Figure 1 Radial bond distributions for Au-C and Au-Au bond. The zero density regime between the first two peaks in g
More informationReaction dynamics of molecular hydrogen on silicon surfaces
PHYSICAL REVIEW B VOLUME 54, NUMBER 8 Reaction dynamics of molecular hydrogen on silicon surfaces P. Bratu Max-Planck-Institut für Quantenoptik, D-85740 Garching, Germany W. Brenig Physik-Department, Technische
More informationThe Impact of Sodium Cations on the Adsorption of Carbon Dioxide in Zeolites
The Impact of Sodium Cations on the Adsorption of Carbon Dioxide in Zeolites Meghan Thurlow and Daniela Kohen Carleton College, Northfield, MN Introduction Separation of CO 2 from multi-species gas emissions
More information2) Atom manipulation. Xe / Ni(110) Model: Experiment:
2) Atom manipulation D. Eigler & E. Schweizer, Nature 344, 524 (1990) Xe / Ni(110) Model: Experiment: G.Meyer, et al. Applied Physics A 68, 125 (1999) First the tip is approached close to the adsorbate
More informationChemistry B11 Chapter 3 Atoms
Chapter 3 Atoms Element: is a substance that consists of identical atoms (hydrogen, oxygen, and Iron). 116 elements are known (88 occur in nature and chemist have made the others in the lab). Compound:
More informationR. Clark, D. Humbert, K. Sheikh Nuclear Data Section
Calculation of Atomic Data for Plasma Modeling: Introduction and Atomic Structure Part 1 R. Clark, D. Humbert, K. Sheikh Nuclear Data Section Overview Plasmas in fusion research Data needs for plasma modeling
More informationElectron Rutherford Backscattering, a versatile tool for the study of thin films
Electron Rutherford Backscattering, a versatile tool for the study of thin films Maarten Vos Research School of Physics and Engineering Australian National University Canberra Australia Acknowledgements:
More informationThermodynamic behaviour of mixtures containing CO 2. A molecular simulation study
Thermodynamic behaviour of mixtures containing. A molecular simulation study V. Lachet, C. Nieto-Draghi, B. Creton (IFPEN) Å. Ervik, G. Skaugen, Ø. Wilhelmsen, M. Hammer (SINTEF) Introduction quality issues
More informationThe Ozone Isotope Effect. Answers and Questions
The Ozone Isotope Effect Answers and Questions The Ozone Isotope Effect Answers and Questions Dynamical studies of the ozone isotope effect: A status report Ann. Rev. Phys. Chem. 57, 625 661 (2006) R.
More informationReview Chemistry Paper 1
Atomic Structure Topic Define an atom and element. Use scientific conventions to identify chemical symbols Identify elements by chemical symbols Define compound Use chemical formulae to show different
More informationElements, Compounds Mixtures Physical and Chemical Changes
Elements, Compounds Mixtures Physical and Chemical Changes Fundamentals of Chemistry 1 Classification of Matter Matter is any substance having distinct physical characteristics and chemical properties.
More informationNumerical Simulation of the Rarefied Gas Flow through a Short Channel into a Vacuum
Numerical Simulation of the Rarefied Gas Flow through a Short Channel into a Vacuum Oleg Sazhin Ural State University, Lenin av.5, 6283 Ekaterinburg, Russia E-mail: oleg.sazhin@uralmail.com Abstract. The
More informationMolecular Dynamics Simulations of Fusion Materials: Challenges and Opportunities (Recent Developments)
Molecular Dynamics Simulations of Fusion Materials: Challenges and Opportunities (Recent Developments) Fei Gao gaofeium@umich.edu Limitations of MD Time scales Length scales (PBC help a lot) Accuracy of
More informationQuantum Monte Carlo Study of the Equation of State and Vibrational Frequency Shifts of Solid para-hydrogen
Quantum Monte Carlo Study of the Equation of State and Vibrational Frequency Shifts of Solid para-hydrogen Lecheng Wang, Robert J. Le Roy and Pierre-Nicholas Roy Chemistry Department, University of Waterloo
More informationCHEMISTRY Matter and Change. Chapter 12: States of Matter
CHEMISTRY Matter and Change Chapter 12: States of Matter CHAPTER 12 States of Matter Section 12.1 Section 12.2 Section 12.3 Section 12.4 Gases Forces of Attraction Liquids and Solids Phase Changes Click
More informationMolecular Driving Forces
Molecular Driving Forces Statistical Thermodynamics in Chemistry and Biology SUBGfittingen 7 At 216 513 073 / / Ken A. Dill Sarina Bromberg With the assistance of Dirk Stigter on the Electrostatics chapters
More informationAxion detection by atomic/molecular transitions
Axion detection by atomic/molecular transitions Dark matter axions may cause transitions between atomic states Due to very low interaction cross section, it necessary to look for axion induced transition
More informationSimulation of the cathode surface damages in a HOPFED during ion bombardment
Simulation of the cathode surface damages in a HOPFED during ion bombardment Hongping Zhao, Wei Lei, a Xiaobing Zhang, Xiaohua Li, and Qilong Wang Department of Electronic Engineering, Southeast University,
More informationGAS-SURFACE INTERACTIONS
Page 1 of 16 GAS-SURFACE INTERACTIONS In modern surface science, important technological processes often involve the adsorption of molecules in gaseous form onto a surface. We can treat this adsorption
More informationD. De Fazio, T. V. Tscherbul 2, S. Cavalli 3, and V. Aquilanti 3
D. De Fazio, T. V. Tscherbul, S. Cavalli 3, and V. Aquilanti 3 1 Istituto di Struttura della Materia C.N.R., 00016 Roma, Italy Department of Chemistry, University of Toronto, M5S 3H6, Canada 3 Dipartimento
More informationSurface physics, Bravais lattice
Surface physics, Bravais lattice 1. Structure of the solid surface characterized by the (Bravais) lattice + space + point group lattice describes also the symmetry of the solid material vector directions
More informationName: Date: Period: #: BONDING & INTERMOLECULAR FORCES
BONDING & INTERMOLECULAR FORCES Page 1 INTERMOLECULAR FORCES Intermolecular forces (van der Waals forces) relative weak interactions that occur between molecules. Most of the physical properties of gases,
More information31704 Dynamic Monte Carlo modeling of hydrogen isotope. reactive-diffusive transport in porous graphite
31704 Dynamic Monte Carlo modeling of hydrogen isotope reactive-diffusive transport in porous graphite * R. Schneider a, A. Rai a, A. Mutzke a, M. Warrier b,e. Salonen c, K. Nordlund d a Max-Planck-Institut
More informationDensity-Functional Theory and Chemistry in One Dimension
Density-Functional Theory and Chemistry in One Dimension Pierre-François Loos Research School of Chemistry, Australian National University, Canberra, Australia 14ème Rencontre des Chimistes Théoriciens
More informationMicrocanonical unimolecular rate theory at surfaces. III. Thermal dissociative chemisorption of methane on Pt 111 and detailed balance
THE JOURNAL OF CHEMICAL PHYSICS 123, 094707 2005 Microcanonical unimolecular rate theory at surfaces. III. Thermal dissociative chemisorption of methane on Pt 111 and detailed balance A. Bukoski, H. L.
More informationCOPYRIGHTED MATERIAL. Index
347 Index a AC fields 81 119 electric 81, 109 116 laser 81, 136 magnetic 112 microwave 107 109 AC field traps see Traps AC Stark effect 82, 84, 90, 96, 97 101, 104 109 Adiabatic approximation 3, 10, 32
More informationLiquids and Solutions
Liquids and Solutions Physical Chemistry Tutorials Mark Wallace, Wadham College mark.wallace@chem.ox.ac.uk CRL Floor 1 Office 1 Phone (2)75467 Taken from Thomas Group Website, Problems 1. The answers are
More informationChapter 3. Crystal Binding
Chapter 3. Crystal Binding Energy of a crystal and crystal binding Cohesive energy of Molecular crystals Ionic crystals Metallic crystals Elasticity What causes matter to exist in three different forms?
More information