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Glossary Physics (I-Introduction)
1 Glossary Physics (I-introduction) - Efficiency: The percent of the work put into a machine that is converted into useful work output; = work done / energy used [-]. = eta In machines: The work output of any machine cannot exceed the work input (<=100%); in an ideal machine, where no energy is transformed into heat: work(input) = work(output), =100%. Energy: The property of a system that enables it to do work. Conservation o. E.: Energy cannot be created or destroyed; it may be transformed from one form into another, but the total amount of energy never changes. Equilibrium: The state of an object when not acted upon by a net force or net torque; an object in equilibrium may be at rest or moving at uniform velocity - not accelerating. Mechanical E.: The state of an object or system of objects for which any impressed forces cancels to zero and no acceleration occurs. Dynamic E.: Object is moving without experiencing acceleration. Static E.: Object is at rest.F Force: The influence that can cause an object to be accelerated or retarded; is always in the direction of the net force, hence a vector quantity; the four elementary forces are: Electromagnetic F.: Is an attraction or repulsion G, gravit. const.6.672E-11[Nm2/kg2] between electric charges: d, distance [m] 2 2 2 2 F = 1/(40) (q1q2/d ) [(CC/m )(Nm /C )] = [N] m,M, mass [kg] Gravitational F.: Is a mutual attraction between all masses: q, charge [As] [C] 2 2 2 2 F = GmM/d [Nm /kg kg 1/m ] = [N] 0, dielectric constant Strong F.: (nuclear force) Acts within the nuclei of atoms: 8.854E-12 [C2/Nm2] [F/m] 2 2 2 2 2 F = 1/(40) (e /d ) [(CC/m )(Nm /C )] = [N] , 3.14 [-] Weak F.: Manifests itself in special reactions among elementary e, 1.60210 E-19 [As] [C] particles, such as the reaction that occur in radioactive decay. -
Or Continuous Spectrum and Not to the Line Spectra. in the X-Ray Region, In
662 PHYSICS: W. D UA NE PROC. N. A. S. intensity is greatest close to -80 and that it falls off regularly as the angle departs therefrom. We conclude, therefore, that the momentum of the electron in its orbit uithin the atom does not affect the direction of ejection in the way denanded by the theory of Auger and Perrin. While this does not constitute definite evidence against the physical reality of electronic orbits, it is a serious difficulty for the conception. A detailed discussion of the general question here raised in the light of new experimental results will be published elsewhere. 1 Auger, P., J. Physique Rad., 8, 1927 (85-92). 2 Loughridge, D. H., in press. 3 Bothe, W., Zs. Physik, 26, 1924 (59-73). 4 Auger, P., and Perrin, F., J. Physique Rad., 8, 1927 (93-111). 6 Bothe, W., Zs. Physik, 26,1924 (74-84). 6 Watson, E. C., in press. THE CHARACTER OF THE GENERAL, OR CONTINUOUS SPEC- TRUM RADIA TION By WILLIAM DuANX, DJPARTMSNT OF PHysIcs, HARVARD UNIVERSITY Communicated August 6, 1927 The impacts of electrons against atoms produce two different kinds of radiation-the general, or continuous spectrum and the line spectra. By far the greatest amount of energy radiated belongs to the general, or continuous spectrum and not to the line spectra. In the X-ray region, in particular, the continuous, or general radiation spectrum carries most of the radiated energy. In spite of this, and because the line spectra have an important bearing on atomic structure, the general radiation has received much less attention than the line spectra in the recent de- velopment of fundamental ideas in physical science. -
Discrete-Continuous and Classical-Quantum
Under consideration for publication in Math. Struct. in Comp. Science Discrete-continuous and classical-quantum T. Paul C.N.R.S., D.M.A., Ecole Normale Sup´erieure Received 21 November 2006 Abstract A discussion concerning the opposition between discretness and continuum in quantum mechanics is presented. In particular this duality is shown to be present not only in the early days of the theory, but remains actual, featuring different aspects of discretization. In particular discreteness of quantum mechanics is a key-stone for quantum information and quantum computation. A conclusion involving a concept of completeness linking dis- creteness and continuum is proposed. 1. Discrete-continuous in the old quantum theory Discretness is obviously a fundamental aspect of Quantum Mechanics. When you send white light, that is a continuous spectrum of colors, on a mono-atomic gas, you get back precise line spectra and only Quantum Mechanics can explain this phenomenon. In fact the birth of quantum physics involves more discretization than discretness : in the famous Max Planck’s paper of 1900, and even more explicitly in the 1905 paper by Einstein about the photo-electric effect, what is really done is what a computer does: an integral is replaced by a discrete sum. And the discretization length is given by the Planck’s constant. This idea will be later on applied by Niels Bohr during the years 1910’s to the atomic model. Already one has to notice that during that time another form of discretization had appeared : the atomic model. It is astonishing to notice how long it took to accept the atomic hypothesis (Perrin 1905). -
Resonance Raman Scattering of Light from a Diatomic Molecule
University of Nebraska - Lincoln DigitalCommons@University of Nebraska - Lincoln Electrical & Computer Engineering, Department P. F. (Paul Frazer) Williams Publications of May 1976 Resonance Raman scattering of light from a diatomic molecule D. L. Rousseau Bell Laboratories, Murray Hill, New Jersey P. F. Williams University of Nebraska - Lincoln, [email protected] Follow this and additional works at: https://digitalcommons.unl.edu/elecengwilliams Part of the Electrical and Computer Engineering Commons Rousseau, D. L. and Williams, P. F., "Resonance Raman scattering of light from a diatomic molecule" (1976). P. F. (Paul Frazer) Williams Publications. 24. https://digitalcommons.unl.edu/elecengwilliams/24 This Article is brought to you for free and open access by the Electrical & Computer Engineering, Department of at DigitalCommons@University of Nebraska - Lincoln. It has been accepted for inclusion in P. F. (Paul Frazer) Williams Publications by an authorized administrator of DigitalCommons@University of Nebraska - Lincoln. Resonance Raman scattering of light from a diatomic molecule D. L. Rousseau Bell Laboratories. Murray Hill, New Jersey 07974 P. F. Williams Bell Laboratories, Murray Hill, New Jersey 07974 and Department of Physics, University of Puerto Rico, Rio Piedras, Puerto Rico 00931 (Received 13 October 1975) Resonance Raman scattering from a homonuclear diatomic molecule is considered in detail. For convenience, the scattering may be classified into three excitation frequency regions-off-resonance Raman scattering for inciderit energies well away from resonance with any allowed transitions, discrete resonance Raman scattering for excitation near or in resonance with discrete transitions, and continuum resonance Raman scattering for excitation resonant with continuum transitions, e.g., excitation above a dissociation limit or into a repulsive electronic state. -
Raman Spectroscopy for In-Line Water Quality Monitoring — Instrumentation and Potential
Sensors 2014, 14, 17275-17303; doi:10.3390/s140917275 OPEN ACCESS sensors ISSN 1424-8220 www.mdpi.com/journal/sensors Review Raman Spectroscopy for In-Line Water Quality Monitoring — Instrumentation and Potential Zhiyun Li 1, M. Jamal Deen 1,2,4,*, Shiva Kumar 2 and P. Ravi Selvaganapathy 1,3 1 School of Biomedical Engineering, McMaster University, Hamilton, ON L8S 4K1, Canada; E-Mails: [email protected] (Z.L.); [email protected] (P.R.S.) 2 Electrical and Computer Engineering, McMaster University, Hamilton, ON L8S 4K1 Canada; E-Mail: [email protected] 3 Mechanical Engineering, McMaster University, Hamilton, ON L8S 4K1, Canada 4 Electronic and Computer Engineering, Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong, China * Author to whom correspondence should be addressed; E-Mail: [email protected] or [email protected]; Tel.: +1-905-525-9140 (ext. 27137); Fax: +1-905-521-2922. Received: 1 July 2014; in revised form: 7 September 2014 / Accepted: 9 September 2014 / Published: 16 September 2014 Abstract: Worldwide, the access to safe drinking water is a huge problem. In fact, the number of persons without safe drinking water is increasing, even though it is an essential ingredient for human health and development. The enormity of the problem also makes it a critical environmental and public health issue. Therefore, there is a critical need for easy-to-use, compact and sensitive techniques for water quality monitoring. Raman spectroscopy has been a very powerful technique to characterize chemical composition and has been applied to many areas, including chemistry, food, material science or pharmaceuticals. -
Basics of Plasma Spectroscopy
Home Search Collections Journals About Contact us My IOPscience Basics of plasma spectroscopy This content has been downloaded from IOPscience. Please scroll down to see the full text. 2006 Plasma Sources Sci. Technol. 15 S137 (http://iopscience.iop.org/0963-0252/15/4/S01) View the table of contents for this issue, or go to the journal homepage for more Download details: IP Address: 198.35.1.48 This content was downloaded on 20/06/2014 at 16:07 Please note that terms and conditions apply. INSTITUTE OF PHYSICS PUBLISHING PLASMA SOURCES SCIENCE AND TECHNOLOGY Plasma Sources Sci. Technol. 15 (2006) S137–S147 doi:10.1088/0963-0252/15/4/S01 Basics of plasma spectroscopy U Fantz Max-Planck-Institut fur¨ Plasmaphysik, EURATOM Association Boltzmannstr. 2, D-85748 Garching, Germany E-mail: [email protected] Received 11 November 2005, in final form 23 March 2006 Published 6 October 2006 Online at stacks.iop.org/PSST/15/S137 Abstract These lecture notes are intended to give an introductory course on plasma spectroscopy. Focusing on emission spectroscopy, the underlying principles of atomic and molecular spectroscopy in low temperature plasmas are explained. This includes choice of the proper equipment and the calibration procedure. Based on population models, the evaluation of spectra and their information content is described. Several common diagnostic methods are presented, ready for direct application by the reader, to obtain a multitude of plasma parameters by plasma spectroscopy. 1. Introduction spectroscopy for purposes of chemical analysis are described in [11–14]. Plasma spectroscopy is one of the most established and oldest diagnostic tools in astrophysics and plasma physics 2. -
Fluorescent, Prussian Blue-Based Biocompatible Nanoparticle System for Multimodal Imaging Contrast
Supplementary Materials Fluorescent, Prussian Blue-Based Biocompatible Nanoparticle System for Multimodal Imaging Contrast László Forgách 1,*, Nikolett Hegedűs 1, Ildikó Horváth 1, Bálint Kiss 1, Noémi Kovács 1, Zoltán Varga 1,2, Géza Jakab 3, Tibor Kovács 4, Parasuraman Padmanabhan 5, Krisztián Szigeti 1,*,† and Domokos Máthé 1,6,7,*,† 1 Department of Biophysics and Radiation Biology, Semmelweis University, 1085 Budapest, Hungary; [email protected] (N.H.); [email protected] (I.H.); [email protected] (B.K.); [email protected] (N.K.); [email protected] (Z.V.) 2 Institute of Materials and Environmental Chemistry, Research Centre for Natural Sciences, 1117 Budapest, Hungary; [email protected] (Z.V.) 3 Department of Pharmaceutics, Semmelweis University, 1085 Budapest, Hungary; [email protected] 4 University of Pannonia, Institute of Radiochemistry and Radioecology, 8200 Veszprém, Hungary; [email protected] 5 Lee Kong Chian School of Medicine, Nanyang Technological University, 636921 Singapore, Singapore; [email protected] 6 In Vivo Imaging Advanced Core Facility, Hungarian Centre of Excellence for Molecular Medicine, 6723 Szeged, Hungary 7 CROmed Translational Research Centers, 1047 Budapest, Hungary * Correspondence: [email protected] (L.F.); [email protected] univ.hu (K.S.); [email protected] (D.M.); Tel.: +36-1-459-1500/60164 (L.F.); +36-1- 459-1500/60210 (D.M.) † These authors contributed equally to this work. Native, citrate-coated PBNPs The mean hydrodynamic diameter (intensity-based harmonic means or z-average) of citrate- coated PBNPs was 29.30 ± 2.08 (average ± SD, 푛 = 8), as determined by DLS. -
Ice Features in the Mid-IR Spectra of Galactic Nuclei?
A&A 385, 1022–1041 (2002) Astronomy DOI: 10.1051/0004-6361:20020147 & c ESO 2002 Astrophysics Ice features in the mid-IR spectra of galactic nuclei? H. W. W. Spoon1,2,J.V.Keane2,A.G.G.M.Tielens2,3,D.Lutz4,A.F.M.Moorwood1, and O. Laurent4 1 European Southern Observatory, Karl-Schwarzschild-Strasse 2, 85748 Garching, Germany e-mail: [email protected]; [email protected] 2 Kapteyn Institute, PO Box 800, 9700 AV Groningen, The Netherlands e-mail: [email protected]; [email protected] 3 SRON, PO Box 800, 9700 AV Groningen, The Netherlands 4 Max-Planck-Institut f¨ur Extraterrestrische Physik (MPE), Postfach 1312, 85741 Garching, Germany e-mail: [email protected] Received 28 November 2001 / Accepted 24 January 2002 Abstract. Mid infrared spectra provide a powerful probe of the conditions in dusty galactic nuclei. They variously contain emission features associated with star forming regions and absorptions by circumnuclear silicate dust plus ices in cold molecular cloud material. Here we report the detection of 6–8 µm water ice absorption in 18 galaxies observed by ISO. While the mid-IR spectra of some of these galaxies show a strong resemblance to the heavily absorbed spectrum of NGC 4418, other galaxies in this sample also show weak to strong PAH emission. The 18 ice galaxies are part of a sample of 103 galaxies with good S/N mid-IR ISO spectra. Based on our sample we find that ice is present in most of the ULIRGs, whereas it is weak or absent in the large majority of Seyferts and starburst galaxies. -
Supporting Information Kerr Gated Raman Spectroscopy of Lipf6 Salt
Electronic Supplementary Material (ESI) for Physical Chemistry Chemical Physics. This journal is © the Owner Societies 2019 Supporting Information Kerr gated Raman spectroscopy of LiPF6 salt and LiPF6-based organic carbonate electrolyte for Li-ion batteries Laura Cabo-Fernandez,[a] Alex R. Neale,[a] Filipe Braga,[a] Igor V. Sazanovich,[b] Robert Kostecki,[c] Laurence J. Hardwick*[a] [a] Stephenson Institute for Renewable Energy, Department of Chemistry, University of Liverpool, Peach Street, Liverpool, L69 7ZF (United Kingdom). [b] Central Laser Facility, Research Complex at Harwell, STFC Rutherford Appleton Laboratory, Harwell Campus, Didcot, Oxfordshire, OX11 0QX (United Kingdom). [c] Environmental Energy Technologies Division, Lawrence Berkeley National Laboratory, Berkeley, CA 94720 (United States). * [email protected] S1 Principles of Raman spectroscopy When a sample is lightened by a laser, the molecule interacts with the incident photon through the virtual energy level and then another photon is scattered; therefore, scattering processes can be looked at as the absorption of one photon and the instantaneous emission of another photon. The process is elastic if the scattered photon has the same energy as the incident one (Es=Ei), in which case it is known as Rayleigh scattering, or if both photons have different energy (Es≠Ei) it is an inelastic process. Raman spectroscopy is based on these inelastic phenomena and it could be a Stokes scattering if the scattered photon has less energy than the incident one (Es< Ei) or if it has more energy (Es>Ei) an anti-Stokes scattering, as seen in Figure 1 (a). Fluorescence lifetime and quantum yields1 Fluorescence quantum yield (Q) defined as the ratio of photons emitted to the number of photons absorbed1 could be equal to 1, whereas the yield of Raman inelastic scattering can be several orders of magnitude lower. -
Time-Discretized Extreme and Vacuum Ultraviolet Spectroscopy of Spark
Journal of Physics D: Applied Physics PAPER Related content - Photoionization capable, extreme and Time-discretized extreme and vacuum ultraviolet vacuum ultraviolet emission in developing low temperature plasmas in air J Stephens, A Fierro, S Beeson et al. spectroscopy of spark discharges in air, N2 and O2 - A nanosecond surface dielectric barrier discharge at elevated pressures: time- To cite this article: D Trienekens et al 2016 J. Phys. D: Appl. Phys. 49 035201 resolved electric field and efficiency of initiation of combustion I N Kosarev, V I Khorunzhenko, E I Mintoussov et al. - Optical emission spectroscopy study in the View the article online for updates and enhancements. VUV–VIS regimes of a developing low- temperature plasma in nitrogen gas A Fierro, G Laity and A Neuber Recent citations - Guided ionization waves: The physics of repeatability XinPei Lu and Kostya (Ken) Ostrikov - Practical considerations for modeling streamer discharges in air with radiation transport J Stephens et al - Photoionization capable, extreme and vacuum ultraviolet emission in developing low temperature plasmas in air J Stephens et al This content was downloaded from IP address 129.118.3.25 on 05/09/2018 at 18:26 IOP Journal of Physics D: Applied Physics Journal of Physics D: Applied Physics J. Phys. D: Appl. Phys. J. Phys. D: Appl. Phys. 49 (2016) 035201 (5pp) doi:10.1088/0022-3727/49/3/035201 49 Time-discretized extreme and vacuum 2016 ultraviolet spectroscopy of spark © 2016 IOP Publishing Ltd discharges in air, N2 and O2 JPAPBE D Trienekens1,2, -
Spectrum (Functional Analysis) - Wikipedia, the Free Encyclopedia
Spectrum (functional analysis) - Wikipedia, the free encyclopedia http://en.wikipedia.org/wiki/Spectrum_(functional_analysis) Spectrum (functional analysis) From Wikipedia, the free encyclopedia In functional analysis, the concept of the spectrum of a bounded operator is a generalisation of the concept of eigenvalues for matrices. Specifically, a complex number λ is said to be in the spectrum of a bounded linear operator T if λI − T is not invertible, where I is the identity operator. The study of spectra and related properties is known as spectral theory, which has numerous applications, most notably the mathematical formulation of quantum mechanics. The spectrum of an operator on a finite-dimensional vector space is precisely the set of eigenvalues. However an operator on an infinite-dimensional space may have additional elements in its spectrum, and may have no eigenvalues. For example, consider the right shift operator R on the Hilbert space ℓ2, This has no eigenvalues, since if Rx=λx then by expanding this expression we see that x1=0, x2=0, etc. On the other hand 0 is in the spectrum because the operator R − 0 (i.e. R itself) is not invertible: it is not surjective since any vector with non-zero first component is not in its range. In fact every bounded linear operator on a complex Banach space must have a non-empty spectrum. The notion of spectrum extends to densely-defined unbounded operators. In this case a complex number λ is said to be in the spectrum of such an operator T:D→X (where D is dense in X) if there is no bounded inverse (λI − T)−1:X→D. -
New Trends in Raman Spectroscopy: from High-Resolution Geochemistry to Planetary Exploration Olivier Beyssac
New Trends in Raman Spectroscopy: From High-Resolution Geochemistry to Planetary Exploration Olivier Beyssac To cite this version: Olivier Beyssac. New Trends in Raman Spectroscopy: From High-Resolution Geochemistry to Plan- etary Exploration. Elements, GeoScienceWorld, 2020. hal-03049557 HAL Id: hal-03049557 https://hal.archives-ouvertes.fr/hal-03049557 Submitted on 9 Dec 2020 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. New Trends in Raman Spectroscopy: From High-Resolution Geochemistry to Planetary Exploration Olivier Beyssac1 ABSTRACT This article reviews nonconventional Raman spectroscopy techniques and discusses actual and future applications of these techniques in the Earth and planetary sciences. Time-resolved spectroscopy opens new ways to limit or exploit luminescence effects, whereas techniques based on coherent anti-Stokes Raman scattering or surface- enhanced Raman spectroscopy allow the Raman signal to be considerably enhanced even down to very high spatial resolutions. In addition, compact portable Raman spectrometers are now routinely used out of the laboratory and are even integrated to two rovers going to Mars in the near future. Keywords: mineralogy, SERS/TERS, time-resolved Raman, luminescence, Mars exploration INTRODUCTION Raman spectroscopy is a valuable, commonly-used, technique in the Earth and planetary sciences.