Laser manipulation of nuclear transitions: experiment.

Slides:



Advertisements
Similar presentations
The atom and its nucleus
Advertisements

Relativistic Effects in Gold Chemistry Jan Stanek Jagiellonian University Marian Smoluchowski Institute of Physics Krakow, Poland.
MR TRACKING METHODS Dr. Dan Gamliel, Dept. of Medical Physics,
Mössbauer Spectrometry Brent Fultz, California Institute of Technology Department of Applied Physics and Materials Science History Recoil-Free Fraction.
Gamma Decay Readings: Modern Nuclear Chemistry, Chap. 9; Nuclear and Radiochemistry, Chapter 3 Energetics Decay Types Transition Probabilities Internal.
High sensitivity CRDS of the a 1 ∆ g ←X 3 Σ − g band of oxygen near 1.27 μm: magnetic dipole and electric quadrupole transitions in different bands of.
Cphys351 c4:1 Chapter 4: Atomic Structure The Nuclear Atom The Atom as the smallest division of an element quantization of electric charge oil drop experiments.
© 2010 Pearson Education, Inc. PowerPoint ® Lectures for College Physics: A Strategic Approach, Second Edition Chapter 29 Atoms and Molecules.
Emission of Scission Neutrons: Testing the Sudden Approximation N. Carjan Centre d'Etudes Nucléaires de Bordeaux-Gradignan,CNRS/IN2P3 – Université Bordeaux.
Light. Photons The photon is the gauge boson of the electromagnetic force. –Massless –Stable –Interacts with charged particles. Photon velocity depends.
When an nucleus releases the transition energy Q (say 14.4 keV) in a  -decay, the  does not carry the full 14.4 keV. Conservation of momentum requires.
1 Light as a Particle In 1888, Heinrich Hertz discovered that electrons could be ejected from a sample by shining light on it. This is known as the photoelectric.
Physics at the end of XIX Century Major Discoveries of XX Century
Chapter 31 Atomic Physics Early Models of the Atom The electron was discovered in 1897, and was observed to be much smaller than the atom. It was.
Resonant photon absorption The Mossbauer effect Photon attenuation Radiation attenuation by: -- photoelectric effect -- compton scattering (E 
1 Quiz 7: 9am +q I2I2 I1I1 I3I3. Physics 7C Fa 2008 Quantum Mechanics Light as a particle Energy of light Energy levels in atoms.
Light Emission. Today’s Topics Excitation Emission Spectra Incandescence –Absorption Spectra.
Week 11 Lecture 27 Monday, Oct 30, 2006 NO CLASS : DPF06 conference Lecture 28 Wednesday, Nov 1, 2006 GammaDecaysGammaDecays Lecture 29 Friday, Nov 3,
ISP Astronomy Gary D. Westfall1Lecture 6 The Nature of Light Light and other forms of radiation carry information to us from distance astronomical.
Lesson 9 Gamma Ray Decay. Electromagnetic decay There are two types of electromagnetic decay,  -ray emission and internal conversion (IC). In both of.
Dr. Jie ZouPHY Chapter 42 Atomic Physics. Dr. Jie ZouPHY Outline Atomic spectra of gases Early models of the atom Bohr’s model of the hydrogen.
Electron Spin as a Probe for Structure Spin angular momentum interacts with external magnetic fields g e  e HS e and nuclear spins I m Hyperfine Interaction.
6-1 RFSS: Lecture 6 Gamma Decay Part 2 Readings: Modern Nuclear Chemistry, Chap. 9; Nuclear and Radiochemistry, Chapter 3 Energetics Decay Types Transition.
PHYS 580 Nuclear Structure Chapter5-Lecture1 GAMMA DECAY
When an nucleus releases the transition energy Q (say 14.4 keV) in a  -decay, the  does not carry the full 14.4 keV. Conservation of momentum requires.
Corey Thompson Technique Presentation 03/21/2011
Microwave Spectroscopy Rotational Spectroscopy
Nuclear Energy. Nuclear energy is all around us and can be used for medical purposes. Nuclear energy is when an atom is split and releases energy or particles.
Mossbauer Spectroscopy
Mössbauer spectroscopy References: J.P. Adloff, R. Guillaumont: Fundamentals of Radiochemistry, CRC Press, Boca Raton, 1993.
1 Lectures on Medical Biophysics Department of Biophysics, Medical Faculty, Masaryk University in Brno.
Laser-microwave double resonance method in superfluid helium for the measurement of nuclear moments Takeshi Furukawa Department of Physics, Graduate School.
Collinear laser spectroscopy of 42g,mSc
Funded by: NSF Timothy C. Steimle, Fang Wang a Arizona State University, USA & Joe Smallman b, Physics Imperial College, London a Currently at JILA THE.
Yb valence in YbMn 2 (Si,Ge) 2 J.M. Cadogan and D.H. Ryan Department of Physics and Astronomy, University of Manitoba Winnipeg, MB, R3T 2N2, Canada
Gamma Decay Energetics Decay Types Transition Probabilities
Spectroscopy of a forbidden transition in a 4 He BEC and a 3 He degenerate Fermi gas Rob van Rooij, Juliette Simonet*, Maarten Hoogerland**, Roel Rozendaal,
29 Atoms and Molecules Slide 29-2.
Chapters 30, 31 Light Emission Light Quanta
Sarah Newton University of Oregon Applied Physics.
Magnetization dynamics
The 68 th International Symposium on Molecular Spectroscopy, June 2013 Fang Wang a, Allan Adam b and Timothy C. Steimle Dept. Chem. & BioChem., Arizona.
Fang Wang & Timothy C. Steimle Dept. Chem. & BioChem., Arizona State University, Tempe, AZ,USA The 65 th International Symposium on Molecular Spectroscopy,
1 Electromagnetic Radiation and X-Rays "It's of no use whatsoever[...] this is just an experiment that proves Maestro Maxwell was right - we just have.
Starlight and Atoms Chapter 6. The Amazing Power of Starlight Just by analyzing the light received from a star, astronomers can retrieve information about.
1 XI International Workshop PST05 Tokyo, Japan, November 14-17, 2005 The Sb and HIO 3 Aligned Nuclear Targets for Investigation of Time Reversal Invariance.
Chapter 3: Spectral lines in stars. Emission and absorption of light Emission line spectrum Continuous spectrum (thermal, blackbody) Independent of composition.
Methods of excitation: nuclear reactions
A. Bondarevskaya Highly charged ion beam polarization and its application to the search for the parity nonconservation effects in ions
1 Mössbauer Effect J-H. Kim
Note that the following lectures include animations and PowerPoint effects such as fly-ins and transitions that require you to be in PowerPoint's Slide.
Optical Pumping Simulation of Copper for Beta-NMR Experiment Julie Hammond Boston University ISOLDE, CERN
Nuclear Decay. Radioactivity The emission of high-energy radiation or particles from the nucleus of a radioactive atom.
Unit 12: Part 2 Quantum Physics. Overview Quantization: Planck’s Hypothesis Quanta of Light: Photons and the Photoelectric Effect Quantum “Particles”:
Assessment of Physics, Applications and Construction Issues for the Proposed Magurele Short-Pulse Facility Silviu Olariu National Institute of Physics.
CHEM 312: Gamma Decay Readings: Modern Nuclear Chemistry, Chap. 9; Nuclear and Radiochemistry, Chapter 3 Energetics Decay Types Transition Probabilities.
Microwave Spectroscopic Investigations of the Xe-H 2 O and Xe-(H 2 O) 2 van der Waals Complexes Qing Wen and Wolfgang Jäger Department of Chemistry, University.
NUCLEAR CHEMISTRY Chapter 20. Nuclear Chemistry Radioactivity is the emission of subatomic particles or high- energy electromagnetic radiation by the.
Summary Blackbody radiation Einstein Coefficients
Mossbauer spectroscopy
PHY Precise Measurement of the Internal Conversion Coefficient for the E3 decay from the 111mCd Isomer Laura G. Pineda1,2, N. Nica2, J.C. Hardy2.
Zeeman effect HFS and isotope shift
Origin of The Electromagnetic (EM) Waves
Lasers and effects of magnetic field
CHEM 312: Lecture 6 Part 2 Gamma Decay
Hydrogen relativistic effects II
Sections 6.1 – 6.3 Electromagnetic Radiation and its Interaction with Atoms Bill Vining SUNY College at Oneonta.
Nuclear Magnetic Resonance (NMR) Spectroscopy
Mössbauer study of BaFe2(As1-xPx)2 iron-based superconductors
Ion-beam, photon and hyperfine methods in nano-structured materials
Presentation transcript:

Laser manipulation of nuclear transitions: experiment

Olga Kocharovskaya, Roman Kolesov, Elena Kuznetsova, Yuri Rostovtsev, Farit Vagizov Texas A&M University, College Station, TX and Silviu Olariu National Institute of Physics and Nuclear Engineering, Magurele, Bucharest, Romania

Nuclear and electronic transitions of 151 Eu

Calculated Mossbauer spectra of Eu 3+ :CaF 2 for the ground 7 F 0 and excited 5 D 0 electronic states

Quadrupole interactions between the 151 Eu nucleus and the 7 F 0, 5 D 0 electronic states in Eu 3+ :CaF 2 Quadrupole interaction: H Q = P[I z 2 – I(I+1)/3 +  (I + 2 +I - 2 )/6], I: angular momentum of nucleus, P: quadrupole constant,  : asymmetry parameter P = 3eQV zz /4I(2I-1) Q: nuclear quadrupole moment, V zz : electric field gradient Q g = 1.16 b, Q e = 1.6 b, Ig = 5/2, Ie = 7/2

Comparison of Mossbauer spectra for ground and excited optical states of 151 Eu 3+ Isomer shift  E M : difference in the energy of the  rays emitted by the 151 Eu nuclei when the electrons are in the 7 F 0 and respectively the 5 D 0 states Isotopic shift  E O : difference in the energy of the optical 7 F D 0 transitions for the 151 Eu and respectively the 153 Eu isotopes  E M /  E O =  M /  g  M : variation of the square of the nuclear radius between the 21.5 keV state and the ground nuclear state of 151 Eu  g : variation of the square of the nuclear radius between the 153 Eu and the 151 Eu nuclei  E O = 0.15 GHz,  M =0.019 fm 2,  g = fm 2, 1 fm = m:  E M = 5.2 MHz

Calculated Mossbauer spectra for a 17.6% population in the 5 D 0 electronic state and a 6 MHz isomer shift

Magnitude of the effect

Optical absorption in the Eu 3+ :CaF 2 sample

Fluorescence of the Eu 3+ :CaF 2 sample

Fluorescence of the Eu 3+ :CaF 2 sample for 532 nm excitation

Eu 3+ centers in CaF 2, according to van der Voort et al. (1992)

Effects of 532 nm laser radiation on the Mossbauer spectra of a 151 Eu 3+ :CaF 2 sample

Count difference between the Mossbauer spectra of the 151 Eu 3+ :CaF 2 sample with laser on and off

Comparison of the relative positions of the extremal points for the calculated and measured Mossbauer spectra

Excitation spectra of the emission at nm (red line) and at nm (olive line), at liquid helium temperature, for Eu 3+ :CaF 2, according to van der Voort et al. (1992)

End of the presentation

Questions time