Real-time electron-spin-resonance measurement of plasma induced surface interactions
|
|
- Scarlett McDaniel
- 5 years ago
- Views:
Transcription
1 Realtime electronspinresonance measurement of plasma induced surface interactions 1 Naoya Sumi, 1 Kenji Ishikawa, 2 Hideo Horibe, 2 Akihiko Kono, 1 Keigo Takeda, 1 Hiroki Kondo, 1,3 Makoto Sekine and 1,3 Masaru Hori 1 Nagoya Univ., 2 Kanazawa Inst. of Technol., 3 JSTCREST ISPlasma2011 1
2 Outline of this talk Background Comprehensive understanding of surface reaction Chemical bond breaking process under plasma process Experimental setup Real time in situ electronspinresonance (ESR) Results and discussion Hydrogen plasma on PTE (C 2 C 2 ) Not only individual effect but also synergistic interactions of ions, radicals, and photons Summary ISPlasma2011 2
3 Background of this study Plasmasurface interactions are complex! Electrons, Ions, reactive neutrals, and photons Gaseous radical Light illumination Plasma Individual role and synergistic effects > PAPE Electrons Ion irradiation Surface reactions Materials (Semiconductor, softflexible, biocompatible) ISPlasma2011 3
4 Background PAPE (Pallet for Plasma process Evaluation) Transparent windows and shadowing plates With or without gap between the surface Si Mg 2 Mg 2 psioch (a) Radical psioch (b) Light after Uchida, et al. J. Appl. Phys. 103, (2008). psioch (c) Radical and Light ISPlasma2011 4
5 Background In line measurements Rupture of chemicalbonds, then danglingbonds creation. Only in line methods was previously succeeded. in line method (w/o air exposure) Plasma reactor In situ analyzer after K. Ishikawa, et al Appl.Phys. Lett., 81, 1773 (2002). After processes, samples may be changed. Thus realtime in situ analysis is required. ISPlasma2011 5
6 Objective of this research Establishment of realtime ESR measurement for analyzing plasmainduced surface reactions Realtime measurement of poly(tetrafluoroethylene) (PTE) surface irradiated by H 2 plasma Strong bondenergy for C (5.05 ev) Candidates for biocompatibles H H Can H atoms break C? Analyzed by using ESR and PAPE C C C ISPlasma2011 6
7 ElectronSpinResonance (ESR) Energy Magnetic field Unpaired electron Zeeman splitting Absorption Microwave energy H d I d H Typical ESR spectrum gvalue Intensity ΔH pp H Resonance condition h g H B 0 h B : Planck s constant : Bohr magnetron H 0 g : requency of microwave : Magnetic field : g value Detect microscopic nature surrounding dangling bonds ISPlasma2011 7
8 Realtime ESR Measurement Setup Plasma source Gas Microwave (2.45 GHz) Radical d distance, d Plasma emission ESR cavity <Cross section> PTE Microwave Glass tube Φ10 mm Exhaust ESR Magnet <ESR condition> Microwave frequency Microwave power Modulation amplitude : 9.53 GHz : 20 mw : 2.0 G ESR Cavity Quartz tube PTE ESR Magnet Magnetic field ISPlasma2011 8
9 PAPE (Plasma process Evaluation) Radical Lights Shadowing plate Light (Plasma emissions) Radical Transparent window (Mg 2 or Quartz) Individual effects of species can be analyzed. ISPlasma2011 9
10 Intensity [arb.unit] C dangling bond creation by H 2 plasma <Experimental condition> H 2 : 50 sccm Microwave : 50 W d : 15 cm Pressure : 10 Pa Irradiation time : 15 min g Simulated spectrum of C 2 C*C 2 H 2 plasma irradiation initial g value C The ESR signal was identified as fluoroalkyl radicals. ISPlasma C C Hyperfine interaction from atom having nuclear spins [1] M. Kuzuya et al., Appl. Surf. Sci. 60/61 (1992).
11 Influence of air exposure Intensity [arb.unit] After O 2 exposure C 2 COO*C 2 Before O 2 exposure C 2 C*C 2 5 <Experimental condition> Step1. H 2 plasma irradiation Step2. O 2 exposure: O 2 : 5 sccm Pressure : 10 Pa Exposure time : 15 min : C 2 C*C 2 reacted with O g value C 2 COO*C 2 was formed [2] [2] A. Oshima et al. Radiat. Phys. Chem. 55 (1999). no fluoroalkyl radical was observed by exsitu. ISPlasma
12 Results of Realtime Measurement Surface radical density [ cm 2 ] <Experimental condition> H 2 : : 50 sccm Microwave power: 50 : W50 W Pressure : 10 Pa d : : cm Irradiation time : 21 : min 21 min aster rate Time [min] Radical formation speed [ cm 2 min 1 ] Time [min] The realtime ESR enable us to measure dynamics of formation. ISPlasma
13 Effects of atomic H and Optical emissions <H atom> <Plasma emissions> Intensity [arb.unit] After irradiation initial g value No radical formation Intensity [arb.unit] After irradiation initial g value luoroalkyl radicals were formed. ISPlasma
14 Radical formation speed cm 2 min 1 ] Wavelength dependence of emissions light (Mg 2 t=1 mm) light (Mg 2 t= 5mm) light (quartz) Time [min] Quartz: No surface dangling bond formation Windows:Mg 2 (1, 5 mm thick), Quartz H 2 : 50 sccm Power : 50 W Pressure : 10 Pa distance : 20 cm Processing period : 21 min Shorter wavelength than 250 nm Mg 2 : ormation of surface dangling bonds Saturated rates with light intensity ISPlasma
15 Synergistic effects of atomic H and vacuum UV Radical formation speed [ cm 2 min 1 ] H atom vacuum UV only vacuum UV Time [min] Why plasma process enhances to reactions. ISPlasma
16 Synergistic effects of atomic H and vacuum UV < VUV > Rupture of C bonds recombine the bonds before was desorbed > slow rate H atom H H < H atom > Not enough energy to break C bonds > no reaction Light C C C Photocatalytic process enables to modify! ISPlasma
17 Concluding remarks We established the realtime ESR measurement setup. The synergistic enhancement of H atom and vacuum UV in modifying PTE was found. insitu measurement luoroalkyl radicals were formed when PTE film was irradiated with H 2 plasma because of peroxy radical was formed by air exposure. realtime measurement We found that a synergistic effect of yielding radicals by H atom and vacuum UV emissions. ISPlasma
18 Thank you for your attention. This was in part supported by Tokai region of the Knowledge cluster Initiative (The second stage). Author: Kenji Ishikawa Plasma Nanotechnology Research Center (PLANT) ISPlasma
24th Symposium on Plasma Science for Materials (SPSM-24) - Keynote
24th Symposium on Plasma Science for Materials (SPSM-24) - Keynote Electron-Spin Resonance (ESR) Analysis of Plasma-Surface Interaction Kenji Ishikawa, Naoya Sumi, *Akihiko Kono, *ideo oribe, Keigo Takeda,
More informationPenicillium digitatum spores interacted with plasmas
JSAP 2011 Fall 31a-ZD-10 Electron-spin-resonance (ESR) study of Penicillium digitatum spores interacted with plasmas Kenji Ishikawa, Sachiko Iseki, Takayuki Ohta*, Masafumi Ito*, Hiroshi Hashizume*, Hiroyuki
More informationBroadband ESR from 500 MHz to 40 GHz using superconducting coplanar waveguides
Broadband ESR from 500 MHz to 40 GHz using superconducting coplanar waveguides Martin Dressel 1. Physikalisches Institut, Universität Stuttgart, Germany Outline 1. Introduction ESR resonators 2. Strip
More informationA comparison of the defects introduced during plasma exposure in. high- and low-k dielectrics
A comparison of the defects introduced during plasma exposure in high- and low-k dielectrics H. Ren, 1 G. Jiang, 2 G. A. Antonelli, 2 Y. Nishi, 3 and J.L. Shohet 1 1 Plasma Processing & Technology Laboratory
More informationEffect of Spiral Microwave Antenna Configuration on the Production of Nano-crystalline Film by Chemical Sputtering in ECR Plasma
THE HARRIS SCIENCE REVIEW OF DOSHISHA UNIVERSITY, VOL. 56, No. 1 April 2015 Effect of Spiral Microwave Antenna Configuration on the Production of Nano-crystalline Film by Chemical Sputtering in ECR Plasma
More informationLast Updated:
Last Updated: 2014 07 30 Generation of the EPR ignal MR and EPR are similar in a way that the amount of absorption energy required to for a transition between atomic or molecular states. pectroscopy generally
More informationPHYSICAL AND CHEMICAL PROPERTIES OF ATMOSPHERIC PRESSURE PLASMA POLYMER FILMS
PHYSICAL AND CHEMICAL PROPERTIES OF ATMOSPHERIC PRESSURE PLASMA POLYMER FILMS O. Goossens, D. Vangeneugden, S. Paulussen and E. Dekempeneer VITO Flemish Institute for Technological Research, Boeretang
More informationELECTRON PARAMAGNETIC RESONANCE
ELECTRON PARAMAGNETIC RESONANCE = MAGNETIC RESONANCE TECHNIQUE FOR STUDYING PARAMAGNETIC SYSTEMS i.e. SYSTEMS WITH AT LEAST ONE UNPAIRED ELECTRON Examples of paramagnetic systems Transition-metal complexes
More informationPhotocatalysis: semiconductor physics
Photocatalysis: semiconductor physics Carlos J. Tavares Center of Physics, University of Minho, Portugal ctavares@fisica.uminho.pt www.fisica.uminho.pt 1 Guimarães Where do I come from? 3 Guimarães 4 Introduction>>
More informationInformation in Radio Waves
Summative Assessment: Natural Sources of Radio Performance expectation: Develop and use a model of two objects interacting through electric or magnetic fields to illustrate the forces between objects and
More informationChapter 2 On-wafer UV Sensor and Prediction of UV Irradiation Damage
Chapter 2 On-wafer UV Sensor and Prediction of UV Irradiation Damage Abstract UV radiation during plasma processing affects the surface of materials. Nevertheless, the interaction of UV photons with surface
More informationSynthesis of a Radical Trap
Chemistry Catalyzed oxidation with hydrogen peroxide Trapping of a free radical (spin trapping) Technique Acquisition and interpretation of ESR spectra Radical trap molecule that reacts with short-lived
More informationDETECTION OF UNPAIRED ELECTRONS
DETECTION OF UNPAIRED ELECTRONS There are experimental methods for the detection of unpaired electrons. One of the hallmarks of unpaired electrons in materials is interaction with a magnetic field. That
More informationMagnetic Resonance Spectroscopy EPR and NMR
Magnetic Resonance Spectroscopy EPR and NMR A brief review of the relevant bits of quantum mechanics 1. Electrons have spin, - rotation of the charge about its axis generates a magnetic field at each electron.
More informationAppendix II - 1. Figure 1: The splitting of the spin states of an unpaired electron
Appendix II - 1 May 2017 Appendix II: Introduction to EPR Spectroscopy There are several general texts on this topic, and this appendix is only intended to give you a brief outline of the Electron Spin
More informationETCHING Chapter 10. Mask. Photoresist
ETCHING Chapter 10 Mask Light Deposited Substrate Photoresist Etch mask deposition Photoresist application Exposure Development Etching Resist removal Etching of thin films and sometimes the silicon substrate
More informationInorganic Spectroscopic and Structural Methods
Inorganic Spectroscopic and Structural Methods Electromagnetic spectrum has enormous range of energies. Wide variety of techniques based on absorption of energy e.g. ESR and NMR: radiowaves (MHz) IR vibrations
More informationExploration COMSOL in Modeling RLSA TM CVD Processes
Exploration COMSOL in Modeling RLSA TM CVD Processes Ar+H 2 +SiH 4 +C 2 H 6 and Dopant Gas Jozef Brcka 1 *, Sundar Gandhi 2, Raymond Joe 2 1 Tokyo Electron U.S. Holdings, Inc., U.S. Technology Development
More informationInvestigation of H 2 :CH 4 Plasma Composition by Means of Spatially Resolved Optical Spectroscopy
Vol. 114 (2008) ACTA PHYSICA POLONICA A No. 6 A Optical and Acoustical Methods in Science and Technology Investigation of H 2 :CH 4 Plasma Composition by Means of Spatially Resolved Optical Spectroscopy
More informationHotwire-assisted Atomic Layer Deposition of Pure Metals and Metal Nitrides
Hotwire-assisted Atomic Layer Deposition of Pure Metals and Metal Nitrides Alexey Kovalgin MESA+ Institute for Nanotechnology Semiconductor Components group a.y.kovalgin@utwente.nl 1 Motivation 1. Materials
More informationChapter 6. Summary and Conclusions
Chapter 6 Summary and Conclusions Plasma deposited amorphous hydrogenated carbon films (a-c:h) still attract a lot of interest due to their extraordinary properties. Depending on the deposition conditions
More informationPlasma-Induced Free Radicals of Polycrystalline Monocarbohydrates Studied by Electron Spin Resonance
February 1999 Chem. Pharm. Bull. 47(2) 273 278 (1999) 273 Plasma-Induced Free Radicals of Polycrystalline Monocarbohydrates Studied by Electron Spin Resonance Yukinori YAMAUCHI, Masami SUGITO, and Masayuki
More informationChemistry Instrumental Analysis Lecture 3. Chem 4631
Chemistry 4631 Instrumental Analysis Lecture 3 Quantum Transitions The energy of a photon can also be transferred to an elementary particle by adsorption if the energy of the photon exactly matches the
More informationModification of thin films and nanoparticles. Johannes Berndt, GREMI,Orléans
Modification of thin films and nanoparticles Johannes Berndt, GREMI,Orléans Low temperature plasmas not fully ionized Ionization degree 10-6 10-4 far away from thermodynamic equlilibrium T electron >>
More informationReference literature. (See: CHEM 2470 notes, Module 8 Textbook 6th ed., Chapters )
September 17, 2018 Reference literature (See: CHEM 2470 notes, Module 8 Textbook 6th ed., Chapters 13-14 ) Reference.: https://slideplayer.com/slide/8354408/ Spectroscopy Usual Wavelength Type of Quantum
More informationPlasma-Surface Interactions and Impact on Electron Energy Distribution Function
Plasma-Surface Interactions and Impact on Electron Energy Distribution Function N. Fox-Lyon(a), N. Ning(b), D.B. Graves(b), V. Godyak(c) and G.S. Oehrlein(a) (a) University of Maryland, College Park (b)
More informationGas utilization in remote plasma cleaning and stripping applications
Gas utilization in remote plasma cleaning and stripping applications B. E. E. Kastenmeier IBM Semiconductor Research and Development Center, 2070 Rt. 52, Zip E40, Hopewell Junction, New York 12533 G. S.
More informationNonthermal and nonequilibrium effects in high-power pulsed ICP and application to surface modification of materials*
Pure Appl. Chem., Vol. 74, No. 3, pp. 435 439, 2002. 2002 IUPAC Nonthermal and nonequilibrium effects in high-power pulsed ICP and application to surface modification of materials* T. Ishigaki 1,, N. Okada
More informationA Plasmonic Photocatalyst Consisting of Silver Nanoparticles Embedded in Titanium Dioxide. Ryan Huschka LANP Seminar February 19, 2008
A Plasmonic Photocatalyst Consisting of Silver Nanoparticles Embedded in Titanium Dioxide Ryan Huschka LANP Seminar February 19, 2008 TiO 2 Applications White Pigment Photocatalyst Previous methods to
More informationSupplementary Information
Supplementary Information Supplementary Figure 1. fabrication. A schematic of the experimental setup used for graphene Supplementary Figure 2. Emission spectrum of the plasma: Negative peaks indicate an
More informationLecture 6: Physical Methods II. UV Vis (electronic spectroscopy) Electron Spin Resonance Mossbauer Spectroscopy
Lecture 6: Physical Methods II UV Vis (electronic spectroscopy) Electron Spin Resonance Mossbauer Spectroscopy Physical Methods used in bioinorganic chemistry X ray crystallography X ray absorption (XAS)
More informationThe chemistry of a CCl 2 F 2 radio frequency discharge
The chemistry of a CCl 2 F 2 radio frequency discharge W. W. Stoffels, E. Stoffels, M. Haverlag, G. M. W. Kroesen, and F. J. de Hoog Department of Physics, Eindhoven University of Technology, 5600 MB Eindhoven,
More information08 - Miscellaneous and historical detectors
08 - Miscellaneous and historical detectors Jaroslav Adam Czech Technical University in Prague Version 2 Jaroslav Adam (CTU, Prague) DPD_08, Miscellaneous and historical detectors Version 2 1 / 25 Streamer
More informationIn-beam measurement of the hydrogen hyperfine splitting: towards antihydrogen spectroscopy. Martin Diermaier LEAP 2016 Kanazawa Japan
In-beam measurement of the hydrogen hyperfine splitting: towards antihydrogen spectroscopy Martin Diermaier LEAP 2016 Kanazawa Japan Martin Diermaier Stefan-Meyer-Institute March th 2016 MOTIVATION Charge
More informationHong Young Chang Department of Physics, Korea Advanced Institute of Science and Technology (KAIST), Republic of Korea
Hong Young Chang Department of Physics, Korea Advanced Institute of Science and Technology (KAIST), Republic of Korea Index 1. Introduction 2. Some plasma sources 3. Related issues 4. Summary -2 Why is
More informationULTRASONIC IONIZATION SPECTROSCOPY ABSTRACT
ULTRASONIC IONIZATION SPECTROSCOPY Thomas Prevenslik Consultant 15 H, Greenwood Court, Discovery Bay, Hong Kong E-mail: micronenergy@yahoo.com Christopher Beling, Chor Keung Cheung Department of Physics
More informationElectronic Supporting Information
Electronic Supplementary Material (ESI) for Chemical Communications. This journal is The Royal Society of Chemistry 2015 Electronic Supporting Information Nickel as a co-catalyst for photocatalytic hydrogen
More information.O. Demokritov niversität Münster, Germany
Quantum Thermodynamics of Magnons.O. Demokritov niversität Münster, Germany Magnon Frequency Population BEC-condensates http://www.uni-muenster.de/physik/ap/demokritov/ k z k y Group of NonLinea Magnetic
More informationChemical Sputtering of Carbon Materials due to Combined Bombardment by Ions and Atomic Hydrogen
Chemical Sputtering of Carbon Materials due to Combined Bombardment by Ions and Atomic Hydrogen W. Jacob, C. Hopf, and M. Schlüter Max-Planck-Institut für Plasmaphysik, EURATOM Association, Boltzmannstr.
More information2008 Brooks/Cole 2. Frequency (Hz)
Electromagnetic Radiation and Matter Oscillating electric and magnetic fields. Magnetic field Electric field Chapter 7: Electron Configurations and the Periodic Table Traveling wave moves through space
More informationEffects of Ultraviolet Exposure on the current-voltage characteristics of. high-k dielectric layers
Effects of Ultraviolet Exposure on the current-voltage characteristics of high-k dielectric layers H. Ren 1, A. Sehgal 1, G.A. Antonelli 2, Y. Nishi 3 and J.L. Shohet 1 1 Plasma Processing & Technology
More information3.1 Absorption and Transparency
3.1 Absorption and Transparency 3.1.1 Optical Devices (definitions) 3.1.2 Photon and Semiconductor Interactions 3.1.3 Photon Intensity 3.1.4 Absorption 3.1 Absorption and Transparency Objective 1: Recall
More informationChapter 6 Part 1 Structure of the atom
Chapter 6 Part 1 Structure of the atom What IS the structure of an atom? What are the properties of atoms? REMEMBER: structure affects function! Important questions: Where are the electrons? What is the
More information16. Reactions of the Radical Pairs. The I P Step of the Paradigm
16. Reactions of the Radical Pairs. The I P Step of the Paradigm Let us consider the product forming step in the general photochemical paradigm, i.e., the I P process shown in Figure 1. From the discussion
More informationInstrumentelle Analytik in den Geowissenschaften (PI)
280061 VU MA-ERD-2 Instrumentelle Analytik in den Geowissenschaften (PI) Handoutmaterial zum Vorlesungsteil Spektroskopie Bei Fragen bitte zu kontaktieren: Prof. Lutz Nasdala, Institut für Mineralogie
More informationAPEX CARE INSTITUTE FOR PG - TRB, SLET AND NET IN PHYSICS
Page 1 1. Within the nucleus, the charge distribution A) Is constant, but falls to zero sharply at the nuclear radius B) Increases linearly from the centre, but falls off exponentially at the surface C)
More informationMIT Department of Nuclear Science & Engineering
1 MIT Department of Nuclear Science & Engineering Thesis Prospectus for the Bachelor of Science Degree in Nuclear Science and Engineering Nicolas Lopez Development of a Nanoscale Magnetometer Through Utilization
More informationCHEMISTRY 110 EXAM 1 SEPTEMBER 20, 2010 FORM A
CHEMISTRY 110 EXAM 1 SEPTEMBER 20, 2010 FORM A 1. What are the correct numbers of protons, neutrons and electrons in a 39 K + ion? p n e A. 20 19 18 B. 20 19 19 C. 19 20 18 D. 19 20 19 E. 20 19 20 2. Which
More informationLECTURE 11 ELECTROMAGNETIC WAVES & POLARIZATION. Instructor: Kazumi Tolich
LECTURE 11 ELECTROMAGNETIC WAVES & POLARIZATION Instructor: Kazumi Tolich Lecture 11 2 25.5 Electromagnetic waves Induced fields Properties of electromagnetic waves Polarization Energy of electromagnetic
More informationMIDSUMMER EXAMINATIONS 2001 PHYSICS, PHYSICS WITH ASTROPHYSICS PHYSICS WITH SPACE SCIENCE & TECHNOLOGY PHYSICS WITH MEDICAL PHYSICS
No. of Pages: 6 No. of Questions: 10 MIDSUMMER EXAMINATIONS 2001 Subject PHYSICS, PHYSICS WITH ASTROPHYSICS PHYSICS WITH SPACE SCIENCE & TECHNOLOGY PHYSICS WITH MEDICAL PHYSICS Title of Paper MODULE PA266
More informationFundamentals of Spectroscopy for Optical Remote Sensing. Course Outline 2009
Fundamentals of Spectroscopy for Optical Remote Sensing Course Outline 2009 Part I. Fundamentals of Quantum Mechanics Chapter 1. Concepts of Quantum and Experimental Facts 1.1. Blackbody Radiation and
More informationSupplementary Information
Supplementary Information Chemical and Bandgap Engineering in Monolayer Hexagonal Boron Nitride Kun Ba 1,, Wei Jiang 1,,Jingxin Cheng 2, Jingxian Bao 1, Ningning Xuan 1,Yangye Sun 1, Bing Liu 1, Aozhen
More informationSupplementary Figure 1 Detailed illustration on the fabrication process of templatestripped
Supplementary Figure 1 Detailed illustration on the fabrication process of templatestripped gold substrate. (a) Spin coating of hydrogen silsesquioxane (HSQ) resist onto the silicon substrate with a thickness
More informationPlasma based modification of thin films and nanoparticles. Johannes Berndt, GREMI,Orléans
Plasma based modification of thin films and nanoparticles Johannes Berndt, GREMI,Orléans What is a plasma? A plasma is a ionized quasineutral gas! + electron electrons Neon bottle Ne atom Ne ion: Ne +
More informationWelcome to Organic Chemistry II
Welcome to Organic Chemistry II Erika Bryant, Ph.D. erika.bryant@hccs.edu Class Syllabus 3 CHAPTER 12: STRUCTURE DETERMINATION 4 What is this solution Soda Tea Coffee??? 5 What is this solution Soda Tea
More informationChapter 7. Plasma Basics
Chapter 7 Plasma Basics 2006/4/12 1 Objectives List at least three IC processes using plasma Name three important collisions in plasma Describe mean free path Explain how plasma enhance etch and CVD processes
More informationQ1 and Q2 Review large CHEMISTRY
Q1 and Q2 Review large CHEMISTRY Multiple Choice Identify the choice that best completes the statement or answers the question. 1. E = hv relates the following a. Energy to Planck s constant & wavelength
More informationX-Rays From Laser Plasmas
X-Rays From Laser Plasmas Generation and Applications I. C. E. TURCU CLRC Rutherford Appleton Laboratory, UK and J. B. DANCE JOHN WILEY & SONS Chichester New York Weinheim Brisbane Singapore Toronto Contents
More information高等食品分析 (Advanced Food Analysis) I. SPECTROSCOPIC METHODS *Instrumental methods: 1. Spectroscopic methods (spectroscopy): a) Electromagnetic radiation
*Instrumental methods: 1. Spectroscopic methods (spectroscopy): a) Electromagnetic radiation (EMR): γ-ray emission X-Ray absorption, emission, fluorescence and diffraction Vacuum ultraviolet (UV) absorption
More informationESH Benign Processes for he Integration of Quantum Dots (QDs)
ESH Benign Processes for he Integration of Quantum Dots (QDs) PIs: Karen K. Gleason, Department of Chemical Engineering, MIT Graduate Students: Chia-Hua Lee: PhD Candidate, Department of Material Science
More informationOptical SHG and RAS of molecular adsorption at Si(001) step edges
Optical SHG and RAS of molecular adsorption at Si(001) step edges Robert Ehlert, Jinhee Kwon and Michael C. Downer Department of Physics, The University of Texas at Austin, Austin TX 78712, USA. OSI VI:
More informationAtomic Structure and Periodicity
Atomic Structure and Periodicity Atoms and isotopes: Isotopes-#p + same for all but mass number is different b/c of # n o Average atomic mass is weighted average of all the isotopes for an element Average
More informationUNIAQ Department of Physics
Nano4water, 2 nd dissemination Workshop Chalkidiki, 24-25 April 2012 Dr. Luca Lozzi Department of Physics University of L Aquila Italy UNIAQ Department of Physics N-doped TiO 2 nanostructured coatings
More informationElectron Spin Resonance, Basic principle of NMR, Application of NMR in the study of Biomolecules, NMR imaging and in vivo NMR spectromicroscopy
Electron Spin Resonance, Basic principle of NMR, Application of NMR in the study of Biomolecules, NMR imaging and in vivo NMR spectromicroscopy Mitesh Shrestha Electron Spin Resonance Electron paramagnetic
More informationPART 2 Electronic Structure and the Periodic Table. Reference: Chapter 7 8 in textbook
PART 2 Electronic Structure and the Periodic Table Reference: Chapter 7 8 in textbook 1 Experiment to Discover Atom Structure -particle: He 2+ mass number = 4 Nucleus and Electron Model 2 Atomic Structure
More informationMeasurement of the hyperfine splitting of 133 Cs atoms in superfluid helium
Hyperfine Interact DOI 10.1007/s10751-014-1102-z Measurement of the hyperfine splitting of 133 Cs atoms in superfluid helium K. Imamura T. Furukawa X. F. Yang Y. Mitsuya T. Fujita M. Hayasaka T. Kobayashi
More information(002)(110) (004)(220) (222) (112) (211) (202) (200) * * 2θ (degree)
Supplementary Figures. (002)(110) Tetragonal I4/mcm Intensity (a.u) (004)(220) 10 (112) (211) (202) 20 Supplementary Figure 1. X-ray diffraction (XRD) pattern of the sample. The XRD characterization indicates
More informationVisualization of Xe and Sn Atoms Generated from Laser-Produced Plasma for EUV Light Source
3rd International EUVL Symposium NOVEMBER 1-4, 2004 Miyazaki, Japan Visualization of Xe and Sn Atoms Generated from Laser-Produced Plasma for EUV Light Source H. Tanaka, A. Matsumoto, K. Akinaga, A. Takahashi
More informationI. 16. Coloration of Polyethylene Terephthalate (PET) Film by 3MeV Proton Beams
CYRIC Annual Report 2001 I. 16. Coloration of Polyethylene Terephthalate (PET) Film by 3MeV Proton Beams Matsuyama S., Ishii K., Yamazaki H., Endoh H., Yuki H., Satoh T., Sugihara S., Amartaivan Ts., Tanaka
More informationSaturation Absorption Spectroscopy of Rubidium Atom
Saturation Absorption Spectroscopy of Rubidium Atom Jayash Panigrahi August 17, 2013 Abstract Saturated absorption spectroscopy has various application in laser cooling which have many relevant uses in
More informationMagnetic measurements (Pt. IV) advanced probes
Magnetic measurements (Pt. IV) advanced probes Ruslan Prozorov October 2018 Physics 590B types of local probes microscopic (site-specific) NMR neutrons Mossbauer stationary Bitter decoration magneto-optics
More informationLecture 14 Organic Chemistry 1
CHEM 232 Organic Chemistry I at Chicago Lecture 14 Organic Chemistry 1 Professor Duncan Wardrop February 25, 2010 1 CHEM 232 Organic Chemistry I at Chicago Mass Spectrometry Sections: 13.24-13.25 2 Spectroscopy
More informationOptogalvanic spectroscopy of the Zeeman effect in xenon
Optogalvanic spectroscopy of the Zeeman effect in xenon Timothy B. Smith, Bailo B. Ngom, and Alec D. Gallimore ICOPS-2006 10:45, 5 Jun 06 Executive summary What are we reporting? Xe I optogalvanic spectra
More informationCompendium of concepts you should know to understand the Optical Pumping experiment. \ CFP Feb. 11, 2009, rev. Ap. 5, 2012, Jan. 1, 2013, Dec.28,2013.
Compendium of concepts you should know to understand the Optical Pumping experiment. \ CFP Feb. 11, 2009, rev. Ap. 5, 2012, Jan. 1, 2013, Dec.28,2013. What follows is specialized to the alkali atoms, of
More information3. Write ground-state electron configurations for any atom or ion using only the Periodic Table. (Sections 8.3 & 9.2)
Lecture 2: learning objectives, readings, topics, and resources: 1. Understand the significance of the quantum numbers, understand how they can be used to code for the electron energy levels within atoms
More informationName: COMBINED SCIENCE Topics 4, 5 & 6 LEARNING OUTCOMES. Maintain a record of your progress Use the booklet to guide revision
Name: COMBINED SCIENCE Topics 4, 5 & 6 LEARNING OUTCOMES Maintain a record of your progress Use the booklet to guide revision Close the Gap Contemporary record of the Topics / Learning outcomes that I
More informationSynthesis of 2 ) Structures by Small Molecule-Assisted Nucleation for Plasmon-Enhanced Photocatalytic Activity
Electronic Supplementary Material (ESI) for ChemComm. This journal is The Royal Society of Chemistry 2015 Electronic Supplementary Information Synthesis of Au@UiO-66(NH 2 ) Structures by Small Molecule-Assisted
More informationCore Level Spectroscopies
Core Level Spectroscopies Spectroscopies involving core levels are element-sensitive, and that makes them very useful for understanding chemical bonding, as well as for the study of complex materials.
More informationIntroduction. The analysis of the outcome of a reaction requires that we know the full structure of the products as well as the reactants
Introduction The analysis of the outcome of a reaction requires that we know the full structure of the products as well as the reactants Spectroscopy and the Electromagnetic Spectrum Unlike mass spectrometry,
More informationARGON EXCIMER LAMP. A. Sobottka, L. Prager, L. Drößler, M. Lenk. Leibniz Institute of Surface Modification
ARGON EXCIMER LAMP A. Sobottka, L. Prager, L. Drößler, M. Lenk 1 Introduction Ar-Zufuhr Excimer-Plasma Inertisierung Polymerfolie Sintermetall Inertisierung Post curing [1] EP 1050395 A2 2 Introduction
More informationSimple strategy for enhancing terahertz emission from coherent longitudinal optical phonons using undoped GaAs/n-type GaAs epitaxial layer structures
Presented at ISCS21 June 4, 21 Session # FrP3 Simple strategy for enhancing terahertz emission from coherent longitudinal optical phonons using undoped GaAs/n-type GaAs epitaxial layer structures Hideo
More informationAdjustment of electron temperature in ECR microwave plasma
Vacuum (3) 53 Adjustment of electron temperature in ECR microwave plasma Ru-Juan Zhan a, Xiaohui Wen a,b, *, Xiaodong Zhu a,b, Aidi zhao a,b a Structure Research Laboratory, University of Science and Technology
More informationLasers PH 645/ OSE 645/ EE 613 Summer 2010 Section 1: T/Th 2:45-4:45 PM Engineering Building 240
Lasers PH 645/ OSE 645/ EE 613 Summer 2010 Section 1: T/Th 2:45-4:45 PM Engineering Building 240 John D. Williams, Ph.D. Department of Electrical and Computer Engineering 406 Optics Building - UAHuntsville,
More information1 Electrons are emitted from a metal surface when it is illuminated with suitable electromagnetic radiation. ...[1]
1 Electrons are emitted from a metal surface when it is illuminated with suitable electromagnetic radiation. 1 (a) (b) Name the effect described above....[1] The variation with frequency f of the maximum
More informationPhotodarkening Phenomenon in Yb-Doped Fibers
Photodarkening Phenomenon in Yb-Doped Fibers Tomofumi Arai, 1 Kentaro Ichii, 1 Kenji kada, 1 Tomoharu Kitabayashi, 2 Shoji Tanigawa, 1 and Munehisa Fujimaki 1 Photodarkening phenomenon in ytterbium (Yb)-doped
More informationStrong Facet-Induced and Light-Controlled Room-Temperature. Ferromagnetism in Semiconducting β-fesi 2 Nanocubes
Supporting Information for Manuscript Strong Facet-Induced and Light-Controlled Room-Temperature Ferromagnetism in Semiconducting β-fesi 2 Nanocubes Zhiqiang He, Shijie Xiong, Shuyi Wu, Xiaobin Zhu, Ming
More informationSupplementary Materials
Supplementary Materials Sample characterization The presence of Si-QDs is established by Transmission Electron Microscopy (TEM), by which the average QD diameter of d QD 2.2 ± 0.5 nm has been determined
More informationl* = 109 nm Glycerol Clean Water Glycerol l = 108 nm Wavelength (nm)
1/ (rad -1 ) Normalized extinction a Clean 0.8 Water l* = 109 nm 0.6 Glycerol b 2.0 1.5 500 600 700 800 900 Clean Water 0.5 Glycerol l = 108 nm 630 660 690 720 750 Supplementary Figure 1. Refractive index
More informationEXTREME ULTRAVIOLET AND SOFT X-RAY LASERS
Chapter 7 EXTREME ULTRAVIOLET AND SOFT X-RAY LASERS Hot dense plasma lasing medium d θ λ λ Visible laser pump Ch07_00VG.ai The Processes of Absorption, Spontaneous Emission, and Stimulated Emission Absorption
More informationLecture 16 Light transmission and optical detectors
Lecture 6 Light transmission and optical detectors Charged particle traversing through a material can generate signal in form of light via electromagnetic interactions with orbital electrons of the atoms
More informationSkoog Chapter 6 Introduction to Spectrometric Methods
Skoog Chapter 6 Introduction to Spectrometric Methods General Properties of Electromagnetic Radiation (EM) Wave Properties of EM Quantum Mechanical Properties of EM Quantitative Aspects of Spectrochemical
More informationLectures Spectroscopy. Fall 2012
Lectures 19-20 Spectroscopy Fall 2012 1 spectroscopic principles (Chem 1M/1N exps. #6 and #11) 4 1 spectroscopic excitations ( E = h = hc/ ; = c ) (nm) (sec -1 ) radiation technique molecular excitation
More informationEffect of Gas Flow Rate and Gas Composition in Ar/CH 4 Inductively Coupled Plasmas
COMSOL CONFERENCE BOSTON 2011 Effect of Gas Flow Rate and Gas Composition in Ar/CH 4 Inductively Coupled Plasmas Keisoku Engineering System Co., Ltd., JAPAN Dr. Lizhu Tong October 14, 2011 1 Contents 1.
More informationRadiation Damage and Recovery in Polarized Ammonia Targets
Radiation Damage and Recovery in Polarized Ammonia Targets James Maxwell Univ. of Virginia Polarized Target Group Polarized Sources & Targets, Ferrara, Italia, 8.9.2009 Outline Spin Physics at TJNAF (Jefferson
More informationMagnetic measurements (Pt. IV) advanced probes
Magnetic measurements (Pt. IV) advanced probes Ruslan Prozorov 26 February 2014 Physics 590B types of local probes microscopic (site-specific) NMR neutrons Mossbauer stationary Bitter decoration magneto-optics
More informationLaser-produced extreme ultraviolet (EUV) light source plasma for the next generation lithography application
Laser-produced extreme ultraviolet (EUV) light source plasma for the next generation lithography application EUV light source plasma Tin icrodroplet Main pulse (CO2 laser pulse) Pre-pulse (Nd:YAG laser
More informationHeat of formation / enthalpy of formation!
165 Heat of formation / enthalpy of formation! What is the enthalpy change at standard conditions when 25.0 grams of hydrogen sulfide gas is reacted? 1 - Use Hess' Law to find the enthalpy change of the
More informationIntroduction to Electron Paramagnetic Resonance Spectroscopy
Introduction to Electron Paramagnetic Resonance Spectroscopy Art van der Est, Department of Chemistry, Brock University St. Catharines, Ontario, Canada 1 EPR Spectroscopy EPR is magnetic resonance on unpaired
More informationprogressive electromagnetic wave
LECTURE 11 Ch17 A progressive electromagnetic wave is a self-supporting, energy-carrying disturbance that travels free of its source. The light from the Sun travels through space (no medium) for only 8.3
More informationPlasmonic Hot Hole Generation by Interband Transition in Gold-Polyaniline
Supplementary Information Plasmonic Hot Hole Generation by Interband Transition in Gold-Polyaniline Tapan Barman, Amreen A. Hussain, Bikash Sharma, Arup R. Pal* Plasma Nanotech Lab, Physical Sciences Division,
More information