3 He Polarization Tests at UIUC Danielle Chandler David Howell UIUC.

Slides:



Advertisements
Similar presentations
Polarized 3 He Target for A1n-A J. P. Chen, June 11, 2013, Hall A Meeting Overview Design Progress Progress in target lab Progress from users.
Advertisements

Measuring the Neutron and 3 He Spin Structure at Low Q 2 Vincent Sulkosky College of William and Mary, Williamsburg VA Experimental Overview The.
PHYSICS OF MAGNETIC RESONANCE
HATTIE RING PRESENTATION FOR PHYS 250 4/22/2008 Magnetometry.
Magnetic Resonance Imaging
Trapping Electrons With Light Elijah K. Dunn PHSX 516, Dec. 6, 2011.
NMR Spectroscopy Tuning / Matching Shimming and Lock.
Lecture 2 1 H Nuclear Magnetic Resonance. Gas Chromatograph of Molecular Hydrogen at –100 °C Thermoconductivity Detector 12.
NMR Nuclear Magnetic Resonance Spectroscopy. Over the past fifty years nuclear magnetic resonance spectroscopy, commonly referred to as nmr, has become.
Chapter 29 Continued-Chapter 31- Chapter EMF Induced in a Moving Conductor Example 29-8: Force on the rod. To make the rod move to the right.
Another Route to CP Violation Beyond the SM – Particle Dipole Moments Dave Wark Imperial/RAL WIN05 Delphi June 10, 2005.
Noise near peak field is increased Peak width narrow Peak is symmetric Purpose: Resonate nuclei to prevent polarization. Matching the resonant frequencies.
Dipole-dipole interactions in Rydberg states. Outline Strontium experiment overview Routes to blockade Dipole-dipole effects.
Cavity QED as a Deterministic Photon Source Gary Howell Feb. 9, 2007.
Nuclear effects in the optically- detected magnetic resonance of electron spins in n-GaAs Benjamin Heaton John Colton Brigham Young University.
Spin-induced Precession and its Modulation of Gravitational Waveforms from Merging Binaries.
The Forbidden Transition in Ytterbium ● Atomic selection rules forbid E1 transitions between states of the same parity. However, the parity-violating weak.
Resonance condition. Pulse A coil of wire placed around the X axis will provide a magnetic field along the X axis when a direct current is passed through.
Magnetic Resonance MSN 506 Notes. Overview Essential magnetic resonance Measurement of magnetic resonance Spectroscopic information obtained by magnetic.
Optically Pumping Nuclear Magnetic Spin M.R.Ross, D.Morris, P.H. Bucksbaum, T. Chupp Physics Department, University of Michigan J. Taylor, N. Gershenfeld.
Designing High Power Single Frequency Fiber Lasers Dmitriy Churin Course OPTI
SPIN 2004 Oct. 14, 2004 W. Kim, S.S. Stepanyan, S. Woo, M. Rasulbaev, S. Jin (Kyungpook National University) S. Korea Polarization Measurements of the.
Chapter 12. Multimode and Transient Oscillation
1 On A Laboratory, “Magnetic Resonance” Experimental Set up This is an Animated feature Viewable ONLY with the MS PowerPoint XP Version. Other versions.
Forced Oscillations and Magnetic Resonance. A Quick Lesson in Rotational Physics: TORQUE is a measure of how much a force acting on an object causes that.
Detection of 3He with SQUIDs. Experimental parameters For B=300 Gauss The expected signal is 220 fT (specific geometry is taken into account), while the.
June 21st OSU Mol. Spect. Symp.TB02 8:42 a.m Observation of Infrared Free Induction Decay and Optical Nutation Signals from Nitrous Oxide Using.
T ECHNISCHE U NIVERSITÄT KAISERSLAUTERN K. Bergmann Lecture 6 Lecture course - Riga, fall 2013 Coherent light-matter interaction: Optically driven adiabatic.
September 12, 2013 PSTP 2013 G. Atoian a *, V. Klenov b, J. Ritter a, D. Steski a, A. Zelenski a, V. Zubets b a Brookhaven National Laboratory, Upton,
DHB, nEDM Collab. Mtg, 15/16 Apr 04 UIUC Test System (Beck, Chandler, Hertzog, Kammel, Newman, Peng, Sharp, Williamson, Yoder; Blackburn, Kenyon, Thorsland)
1 Plans for KEK/ATF 1. Introduction 2. Related Instrumentations at ATF 3. Experimental Plans for Fast Kicker R&D at ATF Junji Urakawa (KEK) at ILC Damping.
NMR in Medicine and Biology MRI- Magnetic Resonance Imaging (water) In-vivo spectroscopy (metabolites) Solid-state NMR (large structures) Solution NMR.
NMR in Medicine and Biology
1 Introduction to Biomolecular NMR. 2 Nuclear Magnetic Resonance Spectroscopy Certain isotopes ( 1 H, 13 C, 15 N, 31 P ) have intrinsic magnetic moment.
SAINT-PETERSBURG STATE UNIVERSITY EXPERIMENTAL STUDY OF SPIN MEMORY IN NANOSTRUCTURES ROMAN V. CHERBUNIN.
Considerations for the Optimal Polarization of 3 He Targets Brielin C. Brown University of Virginia October 10, 2008 SPIN 2008.
Chapter 21 Electromagnetic Waves. General Physics Exam II Curve: +30.
Dynamics of Polarized Quantum Turbulence in Rotating Superfluid 4 He Paul Walmsley and Andrei Golov.
Beam Polarimetry Matthew Musgrave NPDGamma Collaboration Meeting Oak Ridge National Laboratory Oct. 15, 2010.
Low–field NMR (or MRI) Images of Laser polarized Noble Gas.
Oscillator Oscillation Level Detector Current Source Oscillation Level at fixed frequency ‘ν’ When No ESR Oscillation Level reduced when there is ESR.
Resolution Limits for Single-Slits and Circular Apertures  Single source  Two sources.
3 He cell production at NIST M. Jon Dadras. Outline Basics of a 3 He cells Basics of a 3 He cells Blowing/Baking Blowing/Baking Filling Filling Uses Uses.
S. ChelkowskiSlide 1WG1 Meeting, Birmingham 07/2008.
2007/11/02nEDM BOSTON1 Dressing Field Study Pinghan Chu University of Illinois at Urbana-Champaign nEDM Collaboration Boston Dressed.
Plots from RCNP UCN Run (April 20-25, 2010). EDM Set-up Schematic H0H0 (RF) H 1 Spin Flipper RF Coil Spherical Coil Cell Valve EDM Cell Magnetized Foil.
Spin Precession Animation “DEMO”
Ultra-low Field Nuclear Magnetic Resonance Measurements with SQUIDs
Simulation of Spin Interference and Echo Effect Abstract Successively jumping across a depolarization resonance twice produces interesting spin dynamics.
Charles University Prague Charles University Prague Institute of Particle and Nuclear Physics Absolute charge measurements using laser setup Pavel Bažant,
A. Nass, M. Chapman, D. Graham, W. Haeberli,
SONA Transition Optimization in the Brookhaven OPPIS A. Kponou, A. Zelenski, S. Kokhanovski, V. Zubets & T. Lehn B. N. L.
Scisat Test Readiness Review MAESTRO Evaluation and Verification Tests University of Toronto 29 January 2003.
Daniel Craft, Dr. John Colton, Tyler Park, Phil White, Brigham Young University.
J.S. Colton, Universal scheme for opt.-detected T 1 measurements Universal scheme for optically- detected T 1 measurements (…and application to an n =
R Wyllie, R Wakai, T G Walker University of Wisconsin, Madison Spin-Exchange Relaxation Free Heart signal frequency spectrum from DC-100Hz Adult heart.
SACE Stage 2 Physics Light and Matter Electromagnetic Waves.
Biomolecular Nuclear Magnetic Resonance Spectroscopy
Date of download: 6/30/2016 Copyright © 2016 SPIE. All rights reserved. Trans-cis conformational change of the azo-dyes under light irradiation. (a) Equivalent.
Date of download: 7/11/2016 Copyright © 2016 SPIE. All rights reserved. Typical temperature increase inside (solid line) and on the surface (dashed line)
 The electron electric dipole moment (eEDM) is aligned with the spin and interacts with the giant (~84 GV/cm) effective internal electric field of the.
CLARIDGE CHAPTER 2.2; 3.2.
(Instrument part) Thanundon Kongnok M
E- source R&D update ILC source laser project Faraday rotation experiment A. Brachmann 05/07/07 SLAC R&D meeting.
Energy calibration issues for FCC-ee I. Koop, BINP, Novosibirsk
Today’s Plan Review 2-level system (Schordinger eq, Rabi, Bloch)
Theory of microwave 3-Wave mixing of chiral molecules
Tunable Slow Light in Cesium Vapor
University of California, Berkeley
Report on Electron Polarization Study
Presentation transcript:

3 He Polarization Tests at UIUC Danielle Chandler David Howell UIUC

Overview Confirmation of successful 3 He polarization using 1083-nm optical signal Use of optical signal to calibrate perturbing field (B 1 ) NMR setup and initial tests

Tests using optical signal cell light detector cell

Confirmation of 3 He Polarization Baseline drops on the 1083-nm light signal when B 0 is turned on 1083-nm light produced in cell decreases when 3 He is polarized because polarized atoms do not interact with the circularly-polarized laser light

Response of optical signal to continuous oscillatory B 1 field Scanned through the B 1 resonance frequency and recorded the optical signal At resonance, the perturbing field rotates the 3 He spins away from the B 0 axis, which makes the optical pumping more efficient… therefore there is a peak in the optical signal at resonance.

Results of B 1 frequency scans Non-zero width as B 0 → 0 reflects nonuniformity in B 0 /B 1 fields B 1 dependence suggests B 0 /B 1 nonuniformity

Response of optical signal as a function of time Amplitude of oscillation damps out as cell becomes depolarized Signal decays as laser light repolarizes the 3 He cell end of pulse Optical signal peaks when the pulse time gives a π pulse, since this should orient the spins antiparallel to the B 0 axis, making optical pumping maximally efficient

Using optical signal to calibrate π/2 burst pulse First maximum corresponds to π pulse T B 1 program voltage = 2.5 V pp For a given B 1 : Can use this optical method to calibrate B 1 :

NMR Measurement Setup Adiabatic fast passage method Free induction decay method

NMR Measurements With current setup, we observe the sensitivity to detect NMR signal at a level of 0.2 μ V Need to improve the design of the NMR for a better signal/noise ratio Calculate that NMR signal should be of the same order of magnitude Response of NMR coil to B 1 pulse burst

Conclusion Optical signal tests were successful and provide a method of calibrating B 1 Preparing to make improvements on NMR sensitivity (for example) increase number of turns on pickup coils optimize position and geometry of coils optimize Q-factor introduce second pair of pickup coils