Spectral Diffusion (in Rare-Earth-Doped Materials) Aislinn Daniels Spectrum Lab Seminar Fall 2015 Spectrum Lab Montana State University.

Slides:



Advertisements
Similar presentations
Inorganic Chemistry Laboratory
Advertisements

Zero-Phonon Line: transition without creation or destruction of phonons Phonon Wing: at T = 0 K, creation of one or more phonons 7. Optical Spectroscopy.
Quantum random walks Andre Kochanke Max-Planck-Institute of Quantum Optics 7/27/2011.
PHYS 206 Matter and Light At least 95% of the celestial information we receive is in the form of light. Therefore we need to know what light is and where.
Samansa Maneshi, Jalani Kanem, Chao Zhuang, Matthew Partlow Aephraim Steinberg Department of Physics, Center for Quantum Information and Quantum Control,
EMISSION SPECTROSCOPIC STUDIES OF LASER-INDUCED GRAPHITE PLASMAS László Nemes Research Laboratory for Materials and Environmental Chemistry, Chemical Research.
Sub-THz Component of Large Solar Flares Emily Ulanski December 9, 2008 Plasma Physics and Magnetohydrodynamics.
Pulsed Cathodic Arc Plasma Diagnostics Optical Emission Spectroscopy Results Aluminium.
Spectrum from a Prism. Example of a Spectrum Kirchoff’s Laws.
Quantum Entanglement of Rb Atoms Using Cold Collisions ( 韓殿君 ) Dian-Jiun Han Physics Department Chung Cheng University.
NMR spectra of some simple molecules Effect of spinning: averaging field inhomogeneity (nmr1.pdf pg 2)
Spectral analysis of starlight can tell us about: composition (by matching spectra). temperature (compare to blackbody curve). (line-of-sight) velocity.
Critical fields, vortex melting and the irreversibility line in quasi 2D organic superconductors Braunen E. Smith K. Cho, I. Mihut and C. C. Agosta Department.
Hyperfine Studies of Lithium using Saturated Absorption Spectroscopy Tory Carr Advisor: Dr. Alex Cronin.
Long coherence times with dense trapped atoms collisional narrowing and dynamical decoupling Nir Davidson Yoav Sagi, Ido Almog, Rami Pugatch, Miri Brook.
Photons of Light The smallest unit of light is a photon A photon is often called a particle of light The Energy of an individual photon depends on its.
Physics of fusion power Lecture 14: Collisions / Transport.
Quantum Computation Using Optical Lattices Ben Zaks Victor Acosta Physics 191 Prof. Whaley UC-Berkeley.
Terahertz Conductivity of Silver Nanoparticles Abstract: The electrical conductivity for bulk metal is described by the well-known Drude model. As the.
First year talk Mark Zentile
Nonlinear Spectroscopy: Characterizing Fluctuations Andrei Tokmakoff MIT Department of Chemistry 2009.
Dressed state amplification by a superconducting qubit E. Il‘ichev, Outline Introduction: Qubit-resonator system Parametric amplification Quantum amplifier.
1 DIELECTRIC RELAXATION IN POROUS MATERIALS Yuri Feldman Tutorial lecture 5 in Kazan Federal University.
Dynamical decoupling in solids
57 Mn Mössbauer collaboration at ISOLDE/CERN Emission Mössbauer spectroscopy of advanced materials for opto- and nano- electronics Spokepersons: Haraldur.
L. Perivolaropoulos Department of Physics University of Ioannina Open page.
NMR spectroscopy in solids: A comparison to NMR spectroscopy in liquids Mojca Rangus Mentor: Prof. Dr. Janez Seliger Comentor: Dr. Gregor Mali.
Christine Muschik and J. Ignacio Cirac Entanglement generated by Dissipation Max-Planck-Institut für Quantenoptik Hanna Krauter, Kasper Jensen, Jonas Meyer.
Energy-Dispersive X-ray Microanalysis in the TEM Anthony J. Garratt-Reed Neil Rowlands.
Pump/Probe Microwave-Optical Double Resonance (PPMODR) Study of Tungsten Carbide( WC) a and Platinum Carbide(PtC) b Funded by Fang Wang, Chengbing Qin,
Magnetism Physics T Soft Gamma Repeater , is the most powerful known magnetic object in the universe. Only 10 of these unusual objects.
Wave Packet Echo in Optical Lattice and Decoherence Time Chao Zhuang U(t) Aug. 15, 2006 CQISC2006 University of Toronto.
First Result of Urumqi 6cm Polarization Observations: Xiaohui Sun, Wolfgang Reich JinLin Han, Patricia Reich, Richard Wielebinski Partner Group of MPIfR.
ROTATIONAL SPECTROSCOPY
Confinement of spin diffusion to single molecular layers in layered organic conductor crystals András Jánossy 1 Ágnes Antal 1 Titusz Fehér 1 Richard Gaál.
Ultrafast carrier dynamics Optical Pump - THz Probe Ultrafast carrier dynamics in Br + -bombarded semiconductors investigated by Optical Pump - THz Probe.
Observation of ultrafast nonlinear response due to coherent coupling between light and confined excitons in a ZnO crystalline film Ashida Lab. Subaru Saeki.
Nonlinear Optics in Plasmas. What is relativistic self-guiding? Ponderomotive self-channeling resulting from expulsion of electrons on axis Relativistic.
60th International Symposium on Molecular Spectroscopy Discovery: GaAs:Er system, 1983 The coincidence of the transition wavelength with the absorption.
Drude weight and optical conductivity of doped graphene Giovanni Vignale, University of Missouri-Columbia, DMR The frequency of long wavelength.
W I S S E N T E C H N I K L E I D E N S C H A F T  Januar 13 Name und OE, Eingabe über > Kopf- und Fußzeile.
Radio Waves Interaction With Interstellar Matter
SEM- Schematic Overview. Electron Detection Tungsten Filament Electron Source.
Aislinn Daniels Spectrum Lab Seminar Fall 2015
Temperature and sample dependence of spin echo in SiC Kyle Miller, John Colton, Samuel Carter (Naval Research Lab) Brigham Young University Physics Department.
Goren Gordon, Gershon Kurizki Weizmann Institute of Science, Israel Daniel Lidar University of Southern California, USA QEC07 USC Los Angeles, USA Dec.
Magnetic properties and NMR data of Rb2MnCl4, RbMnCl3 Kang, Byeongki
Spectral Line Strength and Chemical Abundance: Curve of Growth
1 Department of Physics , University at Buffalo, SUNY APS March Meeting 2015 Phonon mediated spin relaxation in a moving quantum dot: Doppler shift, Cherenkov.
Microwave Spectroscopy Wave length ~ 1 cm to 100  m Wave number ~ 1 to 100 cm -1. Frequency ~ 3 x to 3 x Hz Energy ~ 10 to 1000 Joules/mole.
Chapter – 7 Line Width Line Width (natural) Oscillator strength
Spatial distributions in a cold strontium Rydberg gas Graham Lochead.
IR, NMR, and MS CHEM 315 Lab 8. Molecular Structure and Spectra The most powerful and efficient methods currently in use to characterize the structure.
MOLECULAR SPECTROSCOPY
Microwave Transitions Between Pair States Composed of Two Rb Rydberg Atoms Jeonghun Lee Advisor: Tom F. Gallagher Department of Physics, University of.
Raman Effect The Scattering of electromagnetic radiation by matter with a change of frequency.
JLEIC ion source: specifications, design, and R&D prospects
A 2.3 GHz BANDWIDTH STRUCTURE FOR CLIC_DDS
Excitation control of a cold strontium Rydberg gas
Solar Modulation Davide Grandi AMS Group-INFN Milano-Bicocca.
Chapter 10 Magnetic Properties Introduction 10
EM Waves, Superposition
Diatomic molecules
Fig. 4-1: Pure-crystal energy-band diagram
Velocity autocorrelation functions and cage correlation functions of
Marco Polo, Daniel Felinto and Sandra Vianna Departamento de Física
Spectral analysis of starlight can tell us about:
Theoretical systematics Integrating efficiency fitting
of the Canonical Ensemble: A Quantum System of Spins J
Cold Atom project 12/02/2019.
Presentation transcript:

Spectral Diffusion (in Rare-Earth-Doped Materials) Aislinn Daniels Spectrum Lab Seminar Fall 2015 Spectrum Lab Montana State University

Summary What is Spectral Diffusion? What causes Spectral Diffusion? Effects on Measurements ◦Example Measuring Spectral Diffusion Reducing Spectral Diffusion Spectrum Lab Montana State University

What is Spectral Diffusion? Changes in an atom’s or ion’s transition frequency as a function of time Accumulated frequency shifts cause the ions to “random walk” in frequency space Causes spectral “broadening” of material Spectrum Lab Montana State University

What is Spectral Diffusion? Spectrum Lab Montana State University

What is Spectral Diffusion? Spectrum Lab Montana State University

What Causes Spectral Diffusion? Spectrum Lab Montana State University

Effects on Measurements from Magnetic Dipole Interactions Spectrum Lab Montana State University

Effects on Measurements from Magnetic Dipole Interactions, Example Spectrum Lab Montana State University

Effects on Measurements from Magnetic Dipole Interactions, Example Spectrum Lab Montana State University

Measuring Spectral Diffusion Use theoretical descriptions of spectral diffusion for the specific setup (as in example) to fit echo intensity data to find  eff Then, variations in other parameters (concentration of rare-earth ions, temperature, external magnetic field, etc.) can be used to find parameters  SD and R from  eff Why measure it? ◦Corrections for other measurements ◦Characterizes material Spectrum Lab Montana State University

Reducing Spectral Diffusion For rare-earth-doped materials with paramagnetic ions, ◦Lower temperature of system ◦Increase magnetic field (prevents dipole flips) ◦Reduce concentration of ions in crystal ◦For three-pulse echo systems, decrease T w and/or t 12 Similar approaches for other systems and pulse configurations Spectrum Lab Montana State University

References Böttger, Thomas, C. W. Thiel, Y. Sun, and R. L. Cone. "Optical Decoherence and Spectral Diffusion at 1.5 μ M in Er 3 : Y 2 SiO 5 versus Magnetic Field, Temperature, and Er 3 Concentration." Phys. Rev. B APS Physics 73.7 (2006): n. pag. Physical Review B. Web. 1 Dec Special thanks to Randy Babbitt for answering my questions. Spectrum Lab Montana State University