Extinction, σ/area. Energy (ev) D = 20 nm. t = 1.5 t 0. t = t 0
|
|
- Kelly Ward
- 5 years ago
- Views:
Transcription
1 Extinction, σ/area t = t 0 t = 0.7 t 0 t = t 0 t = 1.3 t 0 t = 1.5 t Energy (ev) = 20 nm t 1.3 Supplementary Figure 1: Plasmon epenence on isk thickness. We show classical calculations for isks of ifferent thicknesses (t in units of t 0 = a 0 / 3 = nm, see legen) an = 20 nm in iameter. The valence electron ensity is ajuste to have the same number of electrons in all cases. These results show that the plasmon energies an absorption profiles are rather inepenent on isk thickness, provie this is small compare with the iameter, which corroborates the robustness of our calculations with respect to the choice of film thickness. 1
2 y/ Without -ban screening (a) (b) (c) -1 1 Inuce charge ensity (arb. units.) Classical (g) - - = 3 nm - y/ Incluing -ban screening () = 9 nm - x/ = 15 nm (f) (e) y/ = 3 nm - x/ = 9 nm - x/ = 15 nm Supplementary Figure 2: Maps of inuce charge ensity corresponing to the lowest-orer ipolar plasmon of single-monolayer gol isks of ifferent iameters, as obtaine from our quantum mechanical escription (a-c,-f), compare with a classical, local calculation (g). The upper (lower) row shows results calculate without (with) inclusion of -ban electron screening. The classical calculation (g) is obtaine from the solution of Poisson s equation for a isk escribe by a resonant permittivity 1 1 /t, where t is the isk thickness. The ipolar patttern exhibits raial oscillations of a perio similar to the Frieel oscillations. The inclusion of -ban screening (2f) results in more complex patterns riven by the iscrete character of the backgroun ipoles. In all cases consiere, the ipolar character is clearly preserve an the inuce charge accumulates at the borer of the nanoisk as the iameter increases, thus approaching the behavior of a classical, local escription of the isk. 2
3 Fermi energy, E F (ev) Electronic ensity (nm -2 ) = 3 nm iameter, (nm) = 9 nm = 15 nm (a) (b) Position along iameter (nm) Fermi velocity, v F (10 6 m/s) Supplementary Figure 3: Filling of electron energy levels in a metallic isk. (a) Fermi energy E F relative to the bottom of the parabolic s-ban (left scale) an Fermi velocity v F = 2E F /m e (right scale) as a function of singlemonolayer gol isk (SMG) iameter. We consier a single (111) atomic layer of an fcc metal of lattice constant a 0 (e.g., a 0 = nm in gol). In practice, a single-layer isk of iameter has (π/ 3)(/a 0 ) 2 electrons that fill states of increasing energy up to a level that efines the Fermi energy E F. (b) Unperturbe valence electron ensity profiles for SMGs of ifferent iameters. 3
4 0.13 Absorbance, A 0.26 = 1.5 = 2 = 3 = 8nm l max = 1 l max = 4 l max = Energy (ev) Supplementary Figure 4: Multipolar effects in the interaction of isk arrays. We examine the valiity of the ipole approximation to represent each isk in the arrays consiere in the main paper. For simplicity, we present classical results, as we expect that the conclusions shoul be irectly applicable to quantum calculations as well. We use a layer KKR approach 2,3 to calculate the absorbance of perioic hexagonal arrays of = 8 nm gol isks with ifferent lattice parameters, with each isk represente through its scattering matrix, which is obtaine with the bounary-element metho (BEM). 4 We inclue multiples of orbital angular momentum l l max. The results are remarkably converge alreay with l max = 1 (ipolar approximation) for the two larger spacings uner iscussion, whereas for a perio equal to 1.5 times the isk iameter multipolar corrections are rather small. Therefore, we conclue that the ipolar approximation use in the main paper provies quantitatively correct results for the geometrical parameters uner consieration. 4
5 Absorbance, A = 30 nm Au Cu = 45 nm Ag oping charge ensity (10 13 cm -2 ) Energy (ev) Supplementary Figure 5: Electrical moulation of the absorbance of hexagonal perioic arrays forme by single atomic-layer isks mae of silver, gol, an copper. The structures are similar to those of Fig. 5 of the main paper, but now the isks are larger, leaing to lower-energy plasmons in the ev region. Silver is the less lossy of these three materials, an consequently, the optimum choice to maximize the optical tunability because its plasmons are narrower. Although the valence electron ensity is very similar in these metals, their plasmons occur at ifferent energies ue to variations in -ban screening. The geometrical an oping parameters are inicate by labels. The spectra are obtaine from classical calculations. 5
6 Energy (ev) light-line layer 10 layers layers Plasmon wavelength (nm) 1 Supplementary Figure 6: Plasmons an tunability of thin homogeneous gol layers. We represent the plasmon ispersion relations of layers consisting of 1 an 10 atomic monolayers oriente along the (111) irection. The results are obtaine from classical electromagnetic theory, using optical ata for the ielectric function, 5 moifie as escribe in the main paper to inclue electrical oping. The plasmons of unope layers (soli curves) are compare with those preicte for an aitional ensity of cm 2 electrons (ashe curves). The light line an the ispersion of surface plasmons in a semi-infinite gol layer are shown for comparison. We conclue that the single-layer gol film can unergo similar electrical tunability as the nanostructures consiere in the main paper. The plasmons of the single layer are relatively far from the light line, although they have sizable wavelengths of 100 s nm in the NIR spectral region. Like in graphene, the in/out-coupling of light to these plasmons represents a serious challenge, which can be overcome by ecorating the layer with aitional structures or by placing it near a grating of perio comparable to the plasmon wavelength. 6
7 Supplementary References [1] Fang, Z.; Thongrattanasiri, S.; Schlather, A.; Liu, Z.; Ma, L.; Wang, Y.; Ajayan, P. M.; Norlaner, P.; Halas, N. J.; García e Abajo, F. J. Gate tunability an hybriization of localize plasmons in nanostructure graphene. ACS Nano 2013, 7, [2] Stefanou, N.; Yannopapas, V.; Moinos, A. Heterostructures of photonic crystals: Frequency bans an transmission coefficients. Comput. Phys. Commun. 1998, 113, [3] Stefanou, N.; Yannopapas, V.; Moinos, A. MULTEM 2: A new version of the program for transmission an ban-structure calculations of photonic crystals. Comput. Phys. Commun. 2000, 132, [4] García e Abajo, F. J.; Howie, A. Retare fiel calculation of electron energy loss in inhomogeneous ielectrics. Phys. Rev. B 2002, 65, [5] Johnson, P. B.; Christy, R. W. Optical constants of the noble metals. Phys. Rev. B 1972, 6,
inflow outflow Part I. Regular tasks for MAE598/494 Task 1
MAE 494/598, Fall 2016 Project #1 (Regular tasks = 20 points) Har copy of report is ue at the start of class on the ue ate. The rules on collaboration will be release separately. Please always follow the
More informationGeneralization of the persistent random walk to dimensions greater than 1
PHYSICAL REVIEW E VOLUME 58, NUMBER 6 DECEMBER 1998 Generalization of the persistent ranom walk to imensions greater than 1 Marián Boguñá, Josep M. Porrà, an Jaume Masoliver Departament e Física Fonamental,
More informationNonlinear Dielectric Response of Periodic Composite Materials
onlinear Dielectric Response of Perioic Composite aterials A.G. KOLPAKOV 3, Bl.95, 9 th ovember str., ovosibirsk, 639 Russia the corresponing author e-mail: agk@neic.nsk.su, algk@ngs.ru A. K.TAGATSEV Ceramics
More information05 The Continuum Limit and the Wave Equation
Utah State University DigitalCommons@USU Founations of Wave Phenomena Physics, Department of 1-1-2004 05 The Continuum Limit an the Wave Equation Charles G. Torre Department of Physics, Utah State University,
More informationApplications of First Order Equations
Applications of First Orer Equations Viscous Friction Consier a small mass that has been roppe into a thin vertical tube of viscous flui lie oil. The mass falls, ue to the force of gravity, but falls more
More informationELECTRON DIFFRACTION
ELECTRON DIFFRACTION Electrons : wave or quanta? Measurement of wavelength an momentum of electrons. Introuction Electrons isplay both wave an particle properties. What is the relationship between the
More informationAverage value of position for the anharmonic oscillator: Classical versus quantum results
verage value of position for the anharmonic oscillator: Classical versus quantum results R. W. Robinett Department of Physics, The Pennsylvania State University, University Park, Pennsylvania 682 Receive
More informationSemiclassical analysis of long-wavelength multiphoton processes: The Rydberg atom
PHYSICAL REVIEW A 69, 063409 (2004) Semiclassical analysis of long-wavelength multiphoton processes: The Ryberg atom Luz V. Vela-Arevalo* an Ronal F. Fox Center for Nonlinear Sciences an School of Physics,
More information1 dx. where is a large constant, i.e., 1, (7.6) and Px is of the order of unity. Indeed, if px is given by (7.5), the inequality (7.
Lectures Nine an Ten The WKB Approximation The WKB metho is a powerful tool to obtain solutions for many physical problems It is generally applicable to problems of wave propagation in which the frequency
More informationChapter 4. Electrostatics of Macroscopic Media
Chapter 4. Electrostatics of Macroscopic Meia 4.1 Multipole Expansion Approximate potentials at large istances 3 x' x' (x') x x' x x Fig 4.1 We consier the potential in the far-fiel region (see Fig. 4.1
More informationHomework 7 Due 18 November at 6:00 pm
Homework 7 Due 18 November at 6:00 pm 1. Maxwell s Equations Quasi-statics o a An air core, N turn, cylinrical solenoi of length an raius a, carries a current I Io cos t. a. Using Ampere s Law, etermine
More informationSolution to the exam in TFY4230 STATISTICAL PHYSICS Wednesday december 1, 2010
NTNU Page of 6 Institutt for fysikk Fakultet for fysikk, informatikk og matematikk This solution consists of 6 pages. Solution to the exam in TFY423 STATISTICAL PHYSICS Wenesay ecember, 2 Problem. Particles
More informationCENTURION UNIVERSITY OF TECHNOLOGY & MANAGEMENT,ODISHA CUEE-2015
CENTURION UNIVERSITY OF TECHNOLOGY & MANAGEMENT,ODISHA CUEE-015 PHYSICS 1. The imensional formula of angular momentum is a) ML T - b) MLT - c) MLT -1 ) ML T -1. If A B = B A, then the angle between A an
More informationQuantum optics of a Bose-Einstein condensate coupled to a quantized light field
PHYSICAL REVIEW A VOLUME 60, NUMBER 2 AUGUST 1999 Quantum optics of a Bose-Einstein conensate couple to a quantize light fiel M. G. Moore, O. Zobay, an P. Meystre Optical Sciences Center an Department
More informationSurface-state mediated three-adsorbate interaction
EUROPHYSICS LETTERS 15 July 2002 Europhys. Lett., 59 (2), pp. 265 271 (2002) Surface-state meiate three-asorbate interaction P. Hylgaar 1 an T. L. Einstein 2 1 Department of Applie Physics, Chalmers University
More informationCollective optical effect in complement left-handed material
Collective optical effect in complement left-hane material S.-C. Wu, C.-F. Chen, W. C. Chao, W.-J. Huang an H. L. Chen, National Nano Device Laboratories, 1001-1 Ta-Hsueh Roa, Hsinchu, Taiwan R.O.C A.-C.
More informationQuantum mechanical approaches to the virial
Quantum mechanical approaches to the virial S.LeBohec Department of Physics an Astronomy, University of Utah, Salt Lae City, UT 84112, USA Date: June 30 th 2015 In this note, we approach the virial from
More informationSUPPLEMENTARY INFORMATION
Long-istance coherent coupling in a quantum ot array Floris R. Braakman 1, Pierre Barthelemy 1, Christian Reichl, Werner Wegscheier, Lieven M.K. Vanersypen 1 1 Kavli Institute of Nanoscience, TU Delft,
More informationinvolve: 1. Treatment of a decaying particle. 2. Superposition of states with different masses.
Physics 195a Course Notes The K 0 : An Interesting Example of a Two-State System 021029 F. Porter 1 Introuction An example of a two-state system is consiere. involve: 1. Treatment of a ecaying particle.
More informationwater adding dye partial mixing homogenization time
iffusion iffusion is a process of mass transport that involves the movement of one atomic species into another. It occurs by ranom atomic jumps from one position to another an takes place in the gaseous,
More informationModel for Dopant and Impurity Segregation During Vapor Phase Growth
Mat. Res. Soc. Symp. Proc. Vol. 648, P3.11.1-7 2001 Materials Research Society Moel for Dopant an Impurity Segregation During Vapor Phase Growth Craig B. Arnol an Michael J. Aziz Division of Engineering
More informationensembles When working with density operators, we can use this connection to define a generalized Bloch vector: v x Tr x, v y Tr y
Ph195a lecture notes, 1/3/01 Density operators for spin- 1 ensembles So far in our iscussion of spin- 1 systems, we have restricte our attention to the case of pure states an Hamiltonian evolution. Toay
More informationCharacterization of lead zirconate titanate piezoceramic using high frequency ultrasonic spectroscopy
JOURNAL OF APPLIED PHYSICS VOLUME 85, NUMBER 1 15 JUNE 1999 Characterization of lea zirconate titanate piezoceramic using high frequency ultrasonic spectroscopy Haifeng Wang, Wenhua Jiang, a) an Wenwu
More informationInteraction force in a vertical dust chain inside a glass box
Interaction force in a vertical ust chain insie a glass box Jie Kong, Ke Qiao, Lorin S. Matthews an Truell W. Hye Center for Astrophysics, Space Physics, an Engineering Research (CASPER) Baylor University
More informationHyperbolic Systems of Equations Posed on Erroneous Curved Domains
Hyperbolic Systems of Equations Pose on Erroneous Curve Domains Jan Norström a, Samira Nikkar b a Department of Mathematics, Computational Mathematics, Linköping University, SE-58 83 Linköping, Sween (
More informationA Model of Electron-Positron Pair Formation
Volume PROGRESS IN PHYSICS January, 8 A Moel of Electron-Positron Pair Formation Bo Lehnert Alfvén Laboratory, Royal Institute of Technology, S-44 Stockholm, Sween E-mail: Bo.Lehnert@ee.kth.se The elementary
More informationLuciano Maiani: Quantum Electro Dynamics, QED. Basic
Luciano Maiani:. Lezione Fermi 10 Quantum Electro Dynamics, QED. Basic 1. Fiels, waves an particles 2. Complex Fiels an phases 3. Lowest orer QED processes 4. Loops an ivergent corrections 5. Two preictions
More informationStable and compact finite difference schemes
Center for Turbulence Research Annual Research Briefs 2006 2 Stable an compact finite ifference schemes By K. Mattsson, M. Svär AND M. Shoeybi. Motivation an objectives Compact secon erivatives have long
More information(3-3) = (Gauss s law) (3-6)
tatic Electric Fiels Electrostatics is the stuy of the effects of electric charges at rest, an the static electric fiels, which are cause by stationary electric charges. In the euctive approach, few funamental
More informationPHY 114 Summer 2009 Final Exam Solutions
PHY 4 Summer 009 Final Exam Solutions Conceptual Question : A spherical rubber balloon has a charge uniformly istribute over its surface As the balloon is inflate, how oes the electric fiel E vary (a)
More information1.4.3 Elementary solutions to Laplace s equation in the spherical coordinates (Axially symmetric cases) (Griffiths 3.3.2)
1.4.3 Elementary solutions to Laplace s equation in the spherical coorinates (Axially symmetric cases) (Griffiths 3.3.) In the spherical coorinates (r, θ, φ), the Laplace s equation takes the following
More informationNUMERICAL METHODS FOR QUANTUM IMPURITY MODELS
NUMERICAL METHODS FOR QUANTUM IMPURITY MODELS http://www.staff.science.uu.nl/~mitch003/nrg.html March 2015 Anrew Mitchell Utrecht University Quantum impurity problems Part 1: Quantum impurity problems
More informationOptical wire-grid polarizers at oblique angles of incidence
JOURNAL OF APPLIED PHYSICS VOLUME 93, NUMBER 8 15 APRIL 003 Optical wire-gri polarizers at oblique angles of incience X. J. Yu an H. S. Kwok a) Center for Display Research, Department of Electrical an
More informationGoal of this chapter is to learn what is Capacitance, its role in electronic circuit, and the role of dielectrics.
PHYS 220, Engineering Physics, Chapter 24 Capacitance an Dielectrics Instructor: TeYu Chien Department of Physics an stronomy University of Wyoming Goal of this chapter is to learn what is Capacitance,
More informationNon-Equilibrium Continuum Physics TA session #10 TA: Yohai Bar Sinai Dislocations
Non-Equilibrium Continuum Physics TA session #0 TA: Yohai Bar Sinai 0.06.206 Dislocations References There are countless books about islocations. The ones that I recommen are Theory of islocations, Hirth
More informationModeling the effects of polydispersity on the viscosity of noncolloidal hard sphere suspensions. Paul M. Mwasame, Norman J. Wagner, Antony N.
Submitte to the Journal of Rheology Moeling the effects of polyispersity on the viscosity of noncolloial har sphere suspensions Paul M. Mwasame, Norman J. Wagner, Antony N. Beris a) epartment of Chemical
More informationCharacterization of dielectric barrier discharge in air applying current measurement, numerical simulation and emission spectroscopy
Characterization of ielectric barrier ischarge in air applying current measurement, numerical simulation an emission spectroscopy Priyaarshini Rajasekaran, ikita Bibinov an Peter Awakowicz nstitute for
More informationarxiv: v1 [physics.optics] 22 Jun 2011
Total light absorption in graphene Sukosin Thongrattanasiri, 1 Frank H. L. Koppens, 2 1, 3, and F. Javier García de Abajo 1 Instituto de Óptica - CSIC, Serrano 121, 28006 Madrid, Spain 2 ICFO-Institut
More information6 Wave equation in spherical polar coordinates
6 Wave equation in spherical polar coorinates We now look at solving problems involving the Laplacian in spherical polar coorinates. The angular epenence of the solutions will be escribe by spherical harmonics.
More informationThe effect of nonvertical shear on turbulence in a stably stratified medium
The effect of nonvertical shear on turbulence in a stably stratifie meium Frank G. Jacobitz an Sutanu Sarkar Citation: Physics of Fluis (1994-present) 10, 1158 (1998); oi: 10.1063/1.869640 View online:
More informationThe Coupling between the Hydration and Double Layer Interactions
7584 Langmuir 00, 18, 7584-7593 The Coupling between the Hyration an ouble Layer Interactions Eli Ruckenstein* an Marian Manciu epartment of Chemical Engineering, State University of New York at Buffalo,
More information6. Friction and viscosity in gasses
IR2 6. Friction an viscosity in gasses 6.1 Introuction Similar to fluis, also for laminar flowing gases Newtons s friction law hols true (see experiment IR1). Using Newton s law the viscosity of air uner
More informationLecture Notes: March C.D. Lin Attosecond X-ray pulses issues:
Lecture Notes: March 2003-- C.D. Lin Attosecon X-ray pulses issues: 1. Generation: Nee short pulses (less than 7 fs) to generate HHG HHG in the frequency omain HHG in the time omain Issues of attosecon
More informationCharacteristics of Dark Current and Photocurrent in Superlattice Infrared Photodetectors
Characteristics of Dark Current an Photocurrent in Superlattice Infrare Photoetectors Wen-Hsing Hsieh a, Chun-Chi Chen a,jet-mingchen a, Yuen-Wuu Suen b an Chieh-Hsiung Kuan a a Department of lectrical
More informationA SIMPLE ENGINEERING MODEL FOR SPRINKLER SPRAY INTERACTION WITH FIRE PRODUCTS
International Journal on Engineering Performance-Base Fire Coes, Volume 4, Number 3, p.95-3, A SIMPLE ENGINEERING MOEL FOR SPRINKLER SPRAY INTERACTION WITH FIRE PROCTS V. Novozhilov School of Mechanical
More informationElectron-phonon interaction in the three-band model
Electron-phonon interaction in the three-ban moel O. Rösch an O. Gunnarsson Max-Planck-Institut für Festkörperforschung, Postfach 800665, D-70506 Stuttgart, Germany We stuy the half-breathing phonon in
More informationCONSERVATION PROPERTIES OF SMOOTHED PARTICLE HYDRODYNAMICS APPLIED TO THE SHALLOW WATER EQUATIONS
BIT 0006-3835/00/4004-0001 $15.00 200?, Vol.??, No.??, pp.?????? c Swets & Zeitlinger CONSERVATION PROPERTIES OF SMOOTHE PARTICLE HYROYNAMICS APPLIE TO THE SHALLOW WATER EQUATIONS JASON FRANK 1 an SEBASTIAN
More information6 General properties of an autonomous system of two first order ODE
6 General properties of an autonomous system of two first orer ODE Here we embark on stuying the autonomous system of two first orer ifferential equations of the form ẋ 1 = f 1 (, x 2 ), ẋ 2 = f 2 (, x
More informationPHYS 414 Problem Set 2: Turtles all the way down
PHYS 414 Problem Set 2: Turtles all the way own This problem set explores the common structure of ynamical theories in statistical physics as you pass from one length an time scale to another. Brownian
More informationImplicit Differentiation
Implicit Differentiation Thus far, the functions we have been concerne with have been efine explicitly. A function is efine explicitly if the output is given irectly in terms of the input. For instance,
More informationSeparation of Variables
Physics 342 Lecture 1 Separation of Variables Lecture 1 Physics 342 Quantum Mechanics I Monay, January 25th, 2010 There are three basic mathematical tools we nee, an then we can begin working on the physical
More informationinduced _ electric _ field = = = = σ V
The Figure shows that the open-circuit voltage V (an hence the fiel strength ) is proportional to compressive stress T up to a maximum of 5 kv, which occurs at a stress of 50 MPa. Inuce electrical fiel
More informationA Simple Model for the Calculation of Plasma Impedance in Atmospheric Radio Frequency Discharges
Plasma Science an Technology, Vol.16, No.1, Oct. 214 A Simple Moel for the Calculation of Plasma Impeance in Atmospheric Raio Frequency Discharges GE Lei ( ) an ZHANG Yuantao ( ) Shanong Provincial Key
More informationAdsorption of H 2 O, NH 3, CO, NO 2, and NO on graphene: A first-principles study
Asorption of H 2 O, NH 3, CO, NO 2, an NO on graphene: A first-principles stuy O. Leenaerts,* B. Partoens, an F. M. Peeters Departement Fysica, Universiteit Antwerpen, Groenenborgerlaan 171, B-2020 Antwerpen,
More information5-4 Electrostatic Boundary Value Problems
11/8/4 Section 54 Electrostatic Bounary Value Problems blank 1/ 5-4 Electrostatic Bounary Value Problems Reaing Assignment: pp. 149-157 Q: A: We must solve ifferential equations, an apply bounary conitions
More informationResearch Article Relativistic Propagation of Linearly/Circularly Polarized Laser Radiation in Plasmas
ISRN Optics Volume 213, Article ID 642617, 8 pages http://x.oi.org/1.1155/213/642617 Research Article Relativistic Propagation of Linearly/Circularly Polarize Laser Raiation in Plasmas Sonu Sen, 1 Meenu
More informationSupplementary Information for. Vibrational Spectroscopy at Electrolyte Electrode Interfaces with Graphene Gratings
Supplementary Information for Vibrational Spectroscopy at Electrolyte Electrode Interfaces with Graphene Gratings Supplementary Figure 1. Simulated from pristine graphene gratings at different Fermi energy
More informationPatterns in bistable resonant-tunneling structures
PHYSICAL REVIEW B VOLUME 56, NUMBER 20 Patterns in bistable resonant-tunneling structures 15 NOVEMBER 1997-II B. A. Glavin an V. A. Kochelap Institute of Semiconuctor Physics, Ukrainian Acaemy of Sciences,
More informationNuclear spin relaxation of sodium cations in bacteriophage Pf1 solutions
THE JOURNAL OF CHEMICAL PHYSICS 125, 244509 2006 Nuclear spin relaxation of soium cations in bacteriophage Pf1 solutions D. N. Sobieski, N. R. Krueger, S. Vyas, a an M. P. Augustine b Department of Chemistry,
More informationSelf-focusing and soliton formation in media with anisotropic nonlocal material response
EUROPHYSICS LETTERS 20 November 1996 Europhys. Lett., 36 (6), pp. 419-424 (1996) Self-focusing an soliton formation in meia with anisotropic nonlocal material response A. A. Zoulya 1, D. Z. Anerson 1,
More informationRFSS: Lecture 4 Alpha Decay
RFSS: Lecture 4 Alpha Decay Reaings Nuclear an Raiochemistry: Chapter 3 Moern Nuclear Chemistry: Chapter 7 Energetics of Alpha Decay Geiger Nuttall base theory Theory of Alpha Decay Hinrance Factors Different
More informationarxiv:cond-mat/ v1 12 Oct 2005
Creation an estruction of a spin gap in weakly couple quarter-fille laers B. Eegger,, H.G. Evertz, an R.M. Noack Institut für Theoretische Physik, Technische Universität Graz, A-8 Graz, Austria Institut
More informationLecture 9: Introduction to Metal Optics. 5 nm
Lecture 9: Introuction to Metal Optics 5 nm What happene at the previous lectures? Light interaction with small objects ( < λ) Insulators (Rayleigh Scattering, blue sky..) Semiconuctors (Size epenent absorption,
More informationConstruction of the Electronic Radial Wave Functions and Probability Distributions of Hydrogen-like Systems
Construction of the Electronic Raial Wave Functions an Probability Distributions of Hyrogen-like Systems Thomas S. Kuntzleman, Department of Chemistry Spring Arbor University, Spring Arbor MI 498 tkuntzle@arbor.eu
More informationPHOTOELECTRIC EMISSION MEASUREMENTS ON THE ANALOGS OF INDIVIDUAL COSMIC DUST GRAINS
The Astrophysical Journal, 645:324 336, 2006 July 1 # 2006. The American Astronomical Society. All rights reserve. Printe in U.S.A. A PHOTOELECTRIC EMISSION MEASUREMENTS ON THE ANALOGS OF INDIVIDUAL COSMIC
More information19 Eigenvalues, Eigenvectors, Ordinary Differential Equations, and Control
19 Eigenvalues, Eigenvectors, Orinary Differential Equations, an Control This section introuces eigenvalues an eigenvectors of a matrix, an iscusses the role of the eigenvalues in etermining the behavior
More informationThe Ritz Ballistic Theory & Adjusting the Speed of Light to c near the Earth and Other Celestial Bodies
College Park, MD 11 PROCDINGS of the NPA 1 The Ritz Ballistic Theory & Ajusting the Spee of Light to c near the arth an Other Celestial Boies Nina Sotina PhD in Physics, Mosco State University 448 Neptune
More informationThermal-Photon and Residual-Gas Scattering in the NLC Beam Delivery
Thermal-Photon an Resiual-Gas Scattering in the NLC Beam Delivery I. Reichel, F. Zimmermann, P. Tenenbaum, T.O. Raubenheimer Stanfor Linear Accelerator Center, Stanfor University, California 94309 Abstract
More informationLORENTZIAN DYNAMICS. Ronald R. Hatch, 1142 Lakme Ave., Wilmington, CA 90744
LORENTZIAN DYNAMICS. Ronal R. Hatch, 114 Lakme Ave., Wilmington, CA 90744 A number of moern physicists have espouse some form of absolute ether theory. But any such theory must explain a number of experiments
More information4. Important theorems in quantum mechanics
TFY4215 Kjemisk fysikk og kvantemekanikk - Tillegg 4 1 TILLEGG 4 4. Important theorems in quantum mechanics Before attacking three-imensional potentials in the next chapter, we shall in chapter 4 of this
More informationarxiv:physics/ v1 [physics.atom-ph] 19 Dec 2003
Using Atomic Diffraction of Na from Material Gratings to Measure Atom-Surface Interactions John D. Perreault, Alexaner D. Cronin University of Arizona, Tucson, Arizona 87 arxiv:physics/v [physics.atom-ph]
More informationA USER-FRIENDLY TOOL FOR SIMULATING THE TIME-DEPENDENT FIELD DISTRIBUTION IN PE INSULATION ON THE BASIS OF A PHYSICAL APPROACH
A USER-FRIENLY TOOL FOR SIMULATING THE TIME-EPENENT FIEL ISTRIBUTION IN PE INSULATION ON THE BASIS OF A PHYSICAL APPROACH Séverine LE ROY, Laboratoire Plasma et Conversion Energie, (France), severine.leroy@laplace.univ-tlse.fr
More informationChapter 6: Energy-Momentum Tensors
49 Chapter 6: Energy-Momentum Tensors This chapter outlines the general theory of energy an momentum conservation in terms of energy-momentum tensors, then applies these ieas to the case of Bohm's moel.
More informationEvent based Kalman filter observer for rotary high speed on/off valve
28 American Control Conference Westin Seattle Hotel, Seattle, Washington, USA June 11-13, 28 WeC9.6 Event base Kalman filter observer for rotary high spee on/off valve Meng Wang, Perry Y. Li ERC for Compact
More informationBifurcations and stability of gap solitons in periodic potentials
PHYSICAL REVIEW E 70, 036618 (2004) Bifurcations an stability of gap solitons in perioic potentials Dmitry E. Pelinovsky, 1 Anrey A. Sukhorukov, 2 an Yuri S. Kivshar 2 1 Department of Mathematics, McMaster
More informationarxiv: v1 [hep-lat] 19 Nov 2013
HU-EP-13/69 SFB/CPP-13-98 DESY 13-225 Applicability of Quasi-Monte Carlo for lattice systems arxiv:1311.4726v1 [hep-lat] 19 ov 2013, a,b Tobias Hartung, c Karl Jansen, b Hernan Leovey, Anreas Griewank
More informationNuclear Physics and Astrophysics
Nuclear Physics an Astrophysics PHY-302 Dr. E. Rizvi Lecture 2 - Introuction Notation Nuclies A Nuclie is a particular an is esignate by the following notation: A CN = Atomic Number (no. of Protons) A
More informationElectromagnet Gripping in Iron Foundry Automation Part II: Simulation
www.ijcsi.org 238 Electromagnet Gripping in Iron Founry Automation Part II: Simulation Rhythm-Suren Wahwa Department of Prouction an Quality Engineering, NTNU Tronheim, 7051, Norway Abstract This paper
More informationAnalytic Scaling Formulas for Crossed Laser Acceleration in Vacuum
October 6, 4 ARDB Note Analytic Scaling Formulas for Crosse Laser Acceleration in Vacuum Robert J. Noble Stanfor Linear Accelerator Center, Stanfor University 575 San Hill Roa, Menlo Park, California 945
More informationarxiv:cond-mat/ v1 [cond-mat.other] 14 Dec 2005
Managing the supercell approximation for charge efects in semiconuctors: finite size scaling, charge correction factors, the bangap problem an the ab initio ielectric constant. arxiv:con-mat/52v [con-mat.other]
More informationIn the usual geometric derivation of Bragg s Law one assumes that crystalline
Diffraction Principles In the usual geometric erivation of ragg s Law one assumes that crystalline arrays of atoms iffract X-rays just as the regularly etche lines of a grating iffract light. While this
More informationAPPROXIMATE SOLUTION FOR TRANSIENT HEAT TRANSFER IN STATIC TURBULENT HE II. B. Baudouy. CEA/Saclay, DSM/DAPNIA/STCM Gif-sur-Yvette Cedex, France
APPROXIMAE SOLUION FOR RANSIEN HEA RANSFER IN SAIC URBULEN HE II B. Bauouy CEA/Saclay, DSM/DAPNIA/SCM 91191 Gif-sur-Yvette Ceex, France ABSRAC Analytical solution in one imension of the heat iffusion equation
More informationA Quantitative Analysis of Coupling for a WPT System Including Dielectric/Magnetic Materials
Progress In Electromagnetics Research Letters, Vol. 72, 127 134, 2018 A Quantitative Analysis of Coupling for a WPT System Incluing Dielectric/Magnetic Materials Yangjun Zhang *, Tatsuya Yoshiawa, an Taahiro
More informationDot trajectories in the superposition of random screens: analysis and synthesis
1472 J. Opt. Soc. Am. A/ Vol. 21, No. 8/ August 2004 Isaac Amiror Dot trajectories in the superposition of ranom screens: analysis an synthesis Isaac Amiror Laboratoire e Systèmes Périphériques, Ecole
More informationEvaporating droplets tracking by holographic high speed video in turbulent flow
Evaporating roplets tracking by holographic high spee vieo in turbulent flow Loïc Méès 1*, Thibaut Tronchin 1, Nathalie Grosjean 1, Jean-Louis Marié 1 an Corinne Fournier 1: Laboratoire e Mécanique es
More informationImpurities in inelastic Maxwell models
Impurities in inelastic Maxwell moels Vicente Garzó Departamento e Física, Universia e Extremaura, E-671-Baajoz, Spain Abstract. Transport properties of impurities immerse in a granular gas unergoing homogenous
More informationarxiv:physics/ v4 [physics.class-ph] 9 Jul 1999
AIAA-99-2144 PROPULSION THROUGH ELECTROMAGNETIC SELF-SUSTAINED ACCELERATION arxiv:physics/9906059v4 [physics.class-ph] 9 Jul 1999 Abstract As is known the repulsion of the volume elements of an uniformly
More informationarxiv:physics/ v2 [physics.ed-ph] 23 Sep 2003
Mass reistribution in variable mass systems Célia A. e Sousa an Vítor H. Rorigues Departamento e Física a Universiae e Coimbra, P-3004-516 Coimbra, Portugal arxiv:physics/0211075v2 [physics.e-ph] 23 Sep
More informationThermal conductivity of graded composites: Numerical simulations and an effective medium approximation
JOURNAL OF MATERIALS SCIENCE 34 (999)5497 5503 Thermal conuctivity of grae composites: Numerical simulations an an effective meium approximation P. M. HUI Department of Physics, The Chinese University
More informationHow the potentials in different gauges yield the same retarded electric and magnetic fields
How the potentials in ifferent gauges yiel the same retare electric an magnetic fiels José A. Heras a Departamento e Física, E. S. F. M., Instituto Politécnico Nacional, México D. F. México an Department
More informationCREOL, The College of Optics & Photonics, UCF. Anomalous Surface Plasmon Dispersion in Metallodielectric Multilayers
Anomalous Surface Plasmon Dispersion in Metalloielectric Multilayers Gray Webb-Woo an Pieter G. Kik CREOL, University of Central Floria, Orlano, FL SPIE San Diego Nanophotonics an Near-fiel Optics http://kik.creol.ucf.eu
More informationThe Principle of Least Action
Chapter 7. The Principle of Least Action 7.1 Force Methos vs. Energy Methos We have so far stuie two istinct ways of analyzing physics problems: force methos, basically consisting of the application of
More informationSynchrotron X-ray Absorption Spectroscopy
Synchrotron X-ray Absorption Spectroscopy Near-ege Spectra (I) Graham N. George Ingri J. Pickering Toay Near-ege spectra Nomenclature Selection rules an spectra What are near-ege spectra sensitive to?
More informationSpectral Flow, the Magnus Force, and the. Josephson-Anderson Relation
Spectral Flow, the Magnus Force, an the arxiv:con-mat/9602094v1 16 Feb 1996 Josephson-Anerson Relation P. Ao Department of Theoretical Physics Umeå University, S-901 87, Umeå, SWEDEN October 18, 2018 Abstract
More informationTransmission Line Matrix (TLM) network analogues of reversible trapping processes Part B: scaling and consistency
Transmission Line Matrix (TLM network analogues of reversible trapping processes Part B: scaling an consistency Donar e Cogan * ANC Eucation, 308-310.A. De Mel Mawatha, Colombo 3, Sri Lanka * onarecogan@gmail.com
More informationOptimization of Geometries by Energy Minimization
Optimization of Geometries by Energy Minimization by Tracy P. Hamilton Department of Chemistry University of Alabama at Birmingham Birmingham, AL 3594-140 hamilton@uab.eu Copyright Tracy P. Hamilton, 1997.
More informationDynamical approach to heavy ion-induced fission
EPJ Web of Conferences 91, 0000 5 (2015) DOI: 10.1051/ epjconf/ 20159100005 C Owne by the authors, publishe by EDP Sciences, 2015 Dynamical approach to heavy ion-inuce fission D.Y. Jeung 1, a, E. Williams
More informationSolutions to the Exercises of Chapter 9
9A. Vectors an Forces Solutions to the Exercises of Chapter 9. F = 5 sin 5.9 an F = 5 cos 5 4.8.. a. By the Pythagorean theorem, the length of the vector from to (, ) is + = 5. So the magnitue of the force
More informationA Novel Decoupled Iterative Method for Deep-Submicron MOSFET RF Circuit Simulation
A Novel ecouple Iterative Metho for eep-submicron MOSFET RF Circuit Simulation CHUAN-SHENG WANG an YIMING LI epartment of Mathematics, National Tsing Hua University, National Nano evice Laboratories, an
More informationAN INTRODUCTION TO AIRCRAFT WING FLUTTER Revision A
AN INTRODUCTION TO AIRCRAFT WIN FLUTTER Revision A By Tom Irvine Email: tomirvine@aol.com January 8, 000 Introuction Certain aircraft wings have experience violent oscillations uring high spee flight.
More information