AN ABSTRACT for the THESIS of Jacqueline K. Garcia for the Degree of Master of Science in Radiation Health Physics Presented On
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Neutron Spin Echo Spectroscopy
Neutron Spin Echo Spectroscopy Peter Fouquet [email protected] Institut Laue-Langevin Grenoble, France Oxford Neutron School 2017 What you are supposed to learn in this tutorial 1. The length and time scales that can be studied using NSE spectroscopy 2. The measurement principle of NSE spectroscopy 3. Discrimination techniques for coherent, incoherent and magnetic dynamics 4. To which scientific problems can I apply NSE spectroscopy? NSE-Tutorial Mind Map Quantum Mechanical Model Resonance Spin-Echo Classical Model Measurement principle “4-point Echo” NSE spectroscopy Instrument Frustrated Components Magnets Bio- molecules Time/Space Map NSE around Surface the globe Diffusion Science Cases Paramagnetic Spin Echo Experiment planning and Interpretation Diffusion Glasses Polymers Models Coherent and Incoherent Scattering Data Treatment The measurement principle of neutron spin echo spectroscopy (quantum mechanical model) • The neutron wave function is split by magnetic fields • The 2 wave packets arrive at magnetic coil 1 magnetic coil 2 polarised sample the sample with a time neutron difference t • If the molecules move between the arrival of the first and second wave packet then coherence is lost • The intermediate scattering t λ3 Bdl function I(Q,t) reflects this ∝ loss in coherence strong wavelength field integral dependence Return The measurement principle of neutron spin echo spectroscopy Dynamic Scattering NSE spectra for diffusive motion Function S(Q,ω) G(R,ω) I(Q,t) = e-t/τ Fourier Transforms temperature up ⇒ τ down Intermediate VanHove -
Princeton University, Physics 311/312; NMR Andthe Spin Echo 1
Princeton University, Physics 311/312; NMR andthe Spin Echo 1 NUCLEAR MAGNETIC RESONANCE AND THE SPIN ECHO Introduction In this experiment we investigate the properties of several materials using pulsed nuclear magnetic resonance (NMR). The NMR technique is used extensively for medical imaging and as a tool in condensed matter and materials physics. The physical mechanism behind NMR is a resonant transition between the energy states of a precessing spin 1/2 particle, specifically a proton, in an external magnetic field. By illuminating the atoms in a liquid, gas or solid with pulses of radio frequency (RF) radiation of various lengths, one can examine the interaction of the spins with the external field, with each other, and with the “lattice.” À Consider a particle with classical angular momentum J in a constant external magnetic field ¼ .The = h  particle has a magnetic moment due to its angular momentum. From the classical equation of À motion we know that if ¼ and are not parallel, the magnetic moment will precess about the magnetic ! = À À ¼ field. The frequency of this precession, ¼ , is independent of the angle between and and is called the Larmor frequency. À In NMR, a sample is placed in a constant magnetic field ¼ as shown in Figure 1. All the spins of À the protons try to align with ¼ but the thermal motion (phonons) of the lattice, to some extent, prevents Å À ¼ this. There is still though a net magnetization, ¼ , parallel to . To manipulate the magnetization, we À apply an RF field perpendicular to ¼ . This results in an oscillating magnetic field that can be viewed as the superposition of two counter-rotating components; only the component rotating in the same direction as that of the spin’s precession has significant effect. -
Double Spin-Echo Sequence for Rapid Spectroscopic Imaging of Hyperpolarized 13C
Journal of Magnetic Resonance 187 (2007) 357–362 www.elsevier.com/locate/jmr Communication Double spin-echo sequence for rapid spectroscopic imaging of hyperpolarized 13C Charles H. Cunningham a,*, Albert P. Chen b, Mark J. Albers b, John Kurhanewicz b, Ralph E. Hurd c, Yi-Fen Yen c, John M. Pauly d, Sarah J. Nelson b, Daniel B. Vigneron b a Department of Medical Biophysics, Sunnybrook Health Sciences Centre, 2075 Bayview Ave., Toronto, Ont., Canada M4N 3M5 b Department of Radiology, University of California at San Francisco, San Francisco, CA, USA c GE Healthcare Technologies, Menlo Park, CA, USA d Department of Electrical Engineering, Stanford University, Stanford, CA, USA Received 2 February 2007; revised 17 April 2007 Available online 2 June 2007 Abstract Dynamic nuclear polarization of metabolically active compounds labeled with 13C has been introduced as a means for imaging met- abolic processes in vivo. To differentiate between the injected compound and the various metabolic products, an imaging technique capa- ble of separating the different chemical-shift species must be used. In this paper, the design and testing of a pulse sequence for rapid magnetic resonance spectroscopic imaging (MRSI) of hyperpolarized 13C is presented. The pulse sequence consists of a small-tip exci- tation followed by a double spin echo using adiabatic refocusing pulses and a ‘‘flyback’’ echo-planar readout gradient. Key elements of the sequence are insensitivity to calibration of the transmit gain, the formation of a spin echo giving high-quality spectral information, and a small effective tip angle that preserves the magnetization for a sufficient duration. -
Anatomy of the Breast Doctors Notes Notes/Extra Explanation Please View Our Editing File Before Studying This Lecture to Check for Any Changes
Color Code Important Anatomy of the Breast Doctors Notes Notes/Extra explanation Please view our Editing File before studying this lecture to check for any changes. Objectives By the end of the lecture, the student should be able to: ✓ Describe the shape and position of the female breast. ✓ Describe the structure of the mammary gland. ✓ List the blood supply of the female breast. ✓ Describe the lymphatic drainage of the female breast. ✓ Describe the applied anatomy in the female breast. Highly recommended Introduction 06:26 Overview of the breast: • The breast (consists of mammary glands + associated skin & Extra connective tissue) is a gland made up of lobes arranged radially .around the nipple (شعاعيا) • Each lobe is further divided into lobules. Between the lobes and lobules we have fat & ligaments called ligaments of cooper • These ligaments attach the skin to the muscle (beneath the breast) to give support to the breast. in shape (مخروطي) *o Shape: it is conical o Position: It lies in superficial fascia of the front of chest. * o Parts: It has a: 1. Base lies on muscles, (حلمة الثدي) Apex nipple .2 3. Tail extend into axilla Extra Position of Female Breast (حلقة ملونة) Base Nipple Areola o Extends from 2nd to 6th ribs. o It extends from the lateral margin of sternum medially to the midaxillary line laterally. o It has no capsule. o It lies on 3 muscles: • 2/3 of its base on (1) pectoralis major* Extra muscle, • inferolateral 1/3 on (2) Serratus anterior & (3) External oblique muscles (muscle of anterior abdominal wall). o Its superolateral part sends a process into the axilla called the axillary tail or axillary process. -
Digital Mammography
Fleitz Continuing Education Jeana Fleitz, M.E.D., RT(R)(M) “The X-Ray Lady” 6511 Glenridge Park Place, Suite 6 Louisville, KY 40222 Telephone (502) 425-0651 Fax (502) 327-7921 Website www.x-raylady.com Email address [email protected] Mammography & Older Women Approved for 9 Category A CE Credit American Society of Radiologic Technologists (ASRT) Approved for 9 Category A CE Credits Course Approval Start Date 1/1/2011 Course Approval End Date 2/1/2016 Florida Radiation Control: Radiologic Technology Program Approved for Category 9 A CE Credits (00 –Technical) Course Approval Start Date 1/1/2011 Course Approval End Date 1/31/2017 Please call our office before the course approval end date for course renewal status. Please let us know if your mailing address or email address changes. A Continuing Education Course for Radiation Operators Course Directions Completing an X-Ray Lady® homestudy course is easy, convenient, and can be done from the comfort of your own couch. To complete this course read the reference corresponding to your posttest and answer the questions. If you have difficulty in answering any question, refer back to the reference. The test questions correspond with the reading and can be answered as you read through the text. How Do I Submit my Answers? Transfer your answers to the blank answer sheet provided and fill out your information. Make a copy of your answer sheet for your records Interactive Testing Center: Get your score and download certificate immediately! Sign up on our website by clicking on the “Online Testing” tab or contact our office. -
Neutron Spin Echo Spectroscopy
Neutron Spin Echo Spectroscopy Peter Fouquet [email protected] Institut Laue-Langevin Grenoble, France September 2014 Hercules Specialized Course 17 - Grenoble What you are supposed to learn in this lecture 1. The length and time scales that can be studied using NSE spectroscopy 2. The measurement principle of NSE spectroscopy 3. Discrimination techniques for coherent, incoherent and magnetic dynamics 4. To which scientific problems can I apply NSE spectroscopy? The measurement principle of neutron spin echo spectroscopy (quantum mechanical model) The neutron wave function is split by magnetic fields magnetic coil 1 magnetic coil 2 polarised sample The 2 wave packets arrive at neutron the sample with a time difference t If the molecules move between the arrival of the first and second wave packet then coherence is lost t λ3 Bdl The intermediate ∝ scattering function I(Q,t) reflects this loss in coherence strong wavelength field integral dependence The measurement principle of neutron spin echo spectroscopy Dynamic Scattering NSE spectra for diffusive motion Function S(Q,ω) G(R,ω) I(Q,t) = e-t/τ Fourier Transforms temperature up ⇒ τ down Intermediate VanHove Correlation Scattering Function Function I(Q,t) G(R,t) Measured with Neutron Spin Echo (NSE) Spectroscopy Neutron spin echo spectroscopy in the time/space landscape NSE is the neutron spectroscopy with the highest energy resolution The time range covered is 1 ps < t < 1 µs (equivalent to neV energy resolution) The momentum transfer range is 0.01 < Q < 4 Å-1 Spin Echo The measurement principle -
Echo-Detected Electron Paramagnetic Resonance Spectra of Spin-Labeled Lipids in Membrane Model Systems Denis A
Subscriber access provided by MPI FUR BIOPHYS CHEM Article Echo-Detected Electron Paramagnetic Resonance Spectra of Spin-Labeled Lipids in Membrane Model Systems Denis A. Erilov, Rosa Bartucci, Rita Guzzi, Derek Marsh, Sergei A. Dzuba, and Luigi Sportelli J. Phys. Chem. B, 2004, 108 (14), 4501-4507• DOI: 10.1021/jp037249y • Publication Date (Web): 16 March 2004 Downloaded from http://pubs.acs.org on March 24, 2009 More About This Article Additional resources and features associated with this article are available within the HTML version: • Supporting Information • Links to the 1 articles that cite this article, as of the time of this article download • Access to high resolution figures • Links to articles and content related to this article • Copyright permission to reproduce figures and/or text from this article The Journal of Physical Chemistry B is published by the American Chemical Society. 1155 Sixteenth Street N.W., Washington, DC 20036 J. Phys. Chem. B 2004, 108, 4501-4507 4501 Echo-Detected Electron Paramagnetic Resonance Spectra of Spin-Labeled Lipids in Membrane Model Systems Denis A. Erilov,†,| Rosa Bartucci,*,† Rita Guzzi,† Derek Marsh,§ Sergei A. Dzuba,‡ and Luigi Sportelli† Dipartimento di Fisica and Unita` INFM, UniVersita` della Calabria, I-87036 ArcaVacata di Rende (CS), Italy, Abteilung Spektroskopie, Max-Planck-Institut fur biophysikalische Chemie, 37077 Gottingen, Germany, and Institute of Chemical Kinetics and Combustion, Russian Academy of Science, 630090 NoVosibirsk, Russian Federation ReceiVed: October 28, 2003; In Final Form: February 5, 2004 The dynamics of spin-labeled lipid chains in the low-temperature phases of dipalmitoyl phosphatidylcholine (DPPC) membranes, with and without equimolar cholesterol, have been investigated by pulsed electron paramagnetic resonance (EPR) spectroscopy. -
A New Mechanism for Electron Spin Echo Envelope Modulation ͒ John J
THE JOURNAL OF CHEMICAL PHYSICS 122, 174504 ͑2005͒ A new mechanism for electron spin echo envelope modulation ͒ John J. L. Mortona Department of Materials, Oxford University, Oxford OX1 3PH, United Kingdom Alexei M. Tyryshkin Department of Electrical Engineering, Princeton University, Princeton, New Jersey 08544 Arzhang Ardavan Clarendon Laboratory, Department of Physics, Oxford University, Oxford OX1 3PU, United Kingdom Kyriakos Porfyrakis Department of Materials, Oxford University, Oxford OX1 3PH, United Kingdom S. A. Lyon Department of Electrical Engineering, Princeton University, Princeton, New Jersey 08544 G. Andrew D. Briggs Department of Materials, Oxford University, Oxford OX1 3PH, United Kingdom ͑Received 21 January 2005; accepted 18 February 2005; published online 2 May 2005͒ Electron spin echo envelope modulation ͑ESEEM͒ has been observed for the first time from a coupled heterospin pair of electron and nucleus in liquid solution. Previously, modulation effects in spin-echo experiments have only been described in liquid solutions for a coupled pair of homonuclear spins in nuclear magnetic resonance or a pair of resonant electron spins in electron paramagnetic resonance. We observe low-frequency ESEEM ͑26 and 52 kHz͒ due to a new mechanism present for any electron spin with SϾ1/2 that is hyperfine coupled to a nuclear spin. In ͑ ͒ ͑ ͒ our case these are electron spin S=3/2 and nuclear spin I=1 in the endohedral fullerene N@C60. The modulation is shown to arise from second-order effects in the isotropic hyperfine coupling of an electron and 14N nucleus. © 2005 American Institute of Physics. ͓DOI: 10.1063/1.1888585͔ I. INTRODUCTION electron spins with different Larmor frequencies͒ results in no modulation effects from this mechanism: The heterospin Measuring the modulation of a spin echo in pulsed coupling energy changes its sign upon application of the re- magnetic-resonance experiments has become a popular tech- focusing pulse ͑because only one spin flips͒, and the magne- nique for studying weak spin-spin couplings. -
Lesion Enhancement in Radio-Frequency Spoiled Gradient-Echo Imaging: Theory, Experimental Evaluation, and Clinical Implications
Lesion Enhancement in Radio-Frequency Spoiled Gradient-Echo Imaging: Theory, Experimental Evaluation, and Clinical Implications 1 1 2 1 Scott Rand, Kenneth R. Maravilla, • and Udo Schmiedl PURPOSE: To investigate the lesser lesion conspicuity after gadolinium contrast infusion with radio-frequency spoiled gradient-echo (SPGR) sequences relative to conventional T1-weighted spin-echo techniques. METHODS: The influences of repetition time, echo time, and flip angle on spin-echo and SPGR signal were studied with mathematical modeling of the image signal amplitude for concentrations of gadopentetate dimeglumine solute from 0 to 10 mM. Predictions of signal strength were verified in vitro by imaging of a doped water phantom. The effects of standard (0.1 mmol/kg) and high-dose (0.3 mmol/kg) gadoteridol on spin-echo and SPGR images were also investigated in three patients. RESULTS: The measured amplitude of undoped water and the rate of increase of doped water signal with increasing gadopentetate concentration (slope) for spin echo 600/ 11/1/ 90° (repetition time/ echo time/excitations/flip angle) and SPGR (600/11/190°) were similar and exceeded those of SPGR (35/ 5/ 145°). Greater increases in SPGR doped water signal and its slope were produced by increasing TR than by varying echo-time or flip angle. The subjective lesion conspicuity and measured lesion contrast at 0.3 mmol/kg were greater with spin echo (600/11/ 1/90°) than with SPGR (35/5/145°) in all three patients; the measured lesion enhancement was similar for both techniques in two patients and decreased for SPGR in the third patient. -
Female Breast
FEMALE BREAST PROF. Saeed Abuel Makarem & DR.SANAA AL-SHAARAWI OBJECTIVES • By the end of the lecture, the student should be able to: • Describe the shape and position of the female breast. • Describe the structure of the mammary gland. • List the blood supply of the female breast. • Describe the lymphatic drainage of the female breast. • Describe the applied anatomy in the female breast. Parts, Shape & position of the Gland • It is conical in shape. • It lies in superficial fascia of the front of chest. • It has a base, apex and tail. • Its base : • extends from 2nd to 6th ribs. • It extends from the sternum to the midaxillary line laterally. • It has no capsule. POSITION OF FEMALE BREAST • Base : • 2/3 of its base lies on the pectoralis major muscle, while its inferolateral 1/3 lies on: • Serratus anterior & • External oblique muscles. • Its superolateral part sends a process into the axilla called the axillary tail or axillary process. POSITION OF FEMALE BREAST • Nipple : • It is a conical eminence that projects forwards from the anterior surface of the breast. • The nipple lies opposite 4th intercostal space. • It carries 15-20 narrow pores of the lactiferous ducts. • Areola : • It is a dark pink brownish circular area of skin that surrounds the nipple. • The subcutaneous tissues of nipple & areola are devoid of fat. STRUCTURE OF MAMMARY GLAND • It is non capsulated gland. • It consists of lobes and lobules which are embedded in the subcutaneous fatty tissue of superficial fascia. • It has fibrous strands (ligaments of cooper) which connect the skin with deep fascia of pectoralis major. -
Introduction to Neutron Spin Echo Spectroscopy
6/15/12 Introduction to Neutron Spin Echo Spectroscopy Antonio Faraone NIST Center for Neutron research & Dept. of Material Science and Engineering, U. of Maryland Methods and Applicaons of SANS, NR, and NSE NCNR, June 18th – 23rd, 2012 Outline • History • Dynamic Neutron Scattering (Recap) • The principles of Neutron Spin Echo • Instrumental Setup of Neutron Spin Echo • Conclusion 1 6/15/12 The beginning F. Mezei, Z. Physik. 255, 146 (1972). NSE Today in the World SPAN MUSES RESEDA NG5-NSE IN11 J-NSE IN15 (SNS-NSE) iNSE + NSE option for triple-axis spectrometers! + developing ones! 2 6/15/12 What does a NSE Spectrometer Look Like? IN-11 @ ILL The first IN-11c @ ILL; Wide Detector Option 3 6/15/12 IN-15 @ ILL MUSES, Resonance Spin Echo @ LLB 4 6/15/12 NSE @ NCNR NSE @ SNS 5 6/15/12 NSE Publications 60 total number of Papers Spectrometer polymer 50 glass membrane SolidStatePhysics 40 Further improvement and development of P. G. de Gennes the NSE technique! Nobel Prize in Physics 1991 30 The technique papers Number ofPapers Number 20 discovery of the principle are still increasing by F. Mezei in 1972 10 polymer dynamics researches by D. Richter in 1980’s 0 1975 1980 1985 1990 1995 2000 2005 Year publication record; searched using web of science: keyword=neutron spin echo! 6 6/15/12 Static and Dynamic Scattering Sample ki, Ei θ ki Probe: photons (visible light, X-rays), kf Q neutrons, electrons, … kf, Ef Momentum Exchanged: Q=ki-kf Energy Exchanged: E=Ei-Ef Detector dσ d 2σ StaticScattering: ≈ S(Q) Dynamic Scattering: ≈ S(Q, E) dΩ dΩdE Static and Dynamic Scattering S(Q) = FTS {exp[−iQ(ri −r j )] } Fourier Transform of the Space Correlation Function S(Q, E) = FTT {exp[−iQ(r(t) −r(0))] }= FTT {I(Q,t)}= FTST {G(r,t)} Fourier Transform of the Space-Time Correlation Function I(Q,t) Intermediate Scattering Function (ISF) G(r,t) van Hove Correlation Function 7 6/15/12 S(Q,E) Inelastic Scattering Q=x.xx Å-1 excitation: neutrons Instrumental exchange energy with an Resolution oscillatory motion which has a finite energy transfer Quasielastic Ex: phonon, magnon, .. -
Pulsed Epr Primer
PULSED EPR PRIMER Dr. Ralph T. Weber Bruker Instruments, Inc. Billerica, MA USA Pulsed EPR Primer Copyright © 2000 Bruker Instruments, Inc. The text, figures, and programs have been worked out with the utmost care. However, we cannot accept either legal responsibility or any liability for any incorrect statements which may remain, and their consequences. The following publication is protected by copyright. All rights reserved. No part of this publication may be reproduced in any form by photocopy, microfilm or other proce- dures or transmitted in a usable language for machines, in particular data processing systems with- out our written authorization. The rights of reproduction through lectures, radio and television are also reserved. The software and hardware descriptions referred in this manual are in many cases registered trademarks and as such are subject to legal requirements. Preface I gratefully acknowledge the many useful comments and discus- sions with Professor Gareth Eaton of the University of Denver and Dr. Peter Hoefer of Bruker Analytik. This document is best viewed with Adobe AcrobatTM 4.0. If you are using a PC running Microsoft WindowsTM, you can also view the several animations that are interspersed throughout the text. Simply click the movie poster with the blue frame and the movie will play in a floating window. To close the floating win- dow, place your cursor in the frame and press the <Esc> key. A Movie Poster iv Table of Contents 1 Pulse EPR Theory..................................................................3 1.1 The Rotating Frame..................................................................................... 3 Magnetization in the Lab Frame ................................................................... 4 Magnetization in the Rotating Frame ........................................................... 6 Viewing the Magnetization from Both Frames: The FID ..........................