Electron and Ion Optics MICRODEVICES Physics and Fabrication Technologies
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For Electrostatic Quadrupole Lens [Fishkova Et Al
Acknowledgments I would like to express my sincere thanks and deep gratitude to my supervisors Dr. Fatin Abdul Jalil Al–Moudarris for suggesting the present project, and Dr. Uday Ali Al-Obaidy for completing the present work and for their support and encouragement throughout the research. I am most grateful to the Dean of College of Science and Head and the staff of the Department of Physics at Al –Nahrain University, particularly Ms. Basma Hussain for her assistance in preparing some of the diagrams. The assistance given by the staff of the library of the College of Science at Baghdad University is highly appreciated. Finally, I most grateful to my parents, my brothers, Laith, Hussain, Firas, Mohamed, Omer and my sisters, Sundus, Enas and Muna for their patience and encouragement throughout this work, and to my friends particularly Fatma Nafaa, Suheel Najem and Yousif Suheel, for their encouragement and to for their support. Sura Certification We certify that this thesis entitled ‘‘ Determination of the Most Favorable Shapes for the Electrostatic Quadrupole Lens ’’ is prepared by Sura Allawi Obaid Al–Zubaidy under our supervision at the College of Science of Al–Nahrain University in partial fulfillment of the requirements for the degree of Master of Science in Physics . Signature: Signature: Name: Dr. Fatin A. J. Al–Moudarris Name: Dr. Uday A. H. Al -Obaidy Title: (Supervisor) Title: (Supervisor) Date: / 4 / 2007 Date: / 4 / 2007 In view of the recommendations, we present this thesis for debate by the examination committee. Signature: Name: Dr. Ahmad K. Ahmad (Assist. Prof.) Head of Physics Department Date: / 2 / 2007 ١ Chapter one Introduction 1- INTRODUCTION 1-1 Electrostatic Quadrupole Lens Electrostatic Quadrupole lens is not widely used in place of conventional round lenses because it is not easy to produce stigmatic and distortion-free images. -
Theoretical Study to Calculate the Focal Length of Focusing System
International Journal of ChemTech Research CODEN (USA): IJCRGG, ISSN: 0974-4290, ISSN(Online):2455-9555 Vol.10 No.13, pp 214-218, 2017 Theoretical Study to calculate some parameters of Ion Optical System *Bushra Joudah Hussein *Department of Physics/ College of Education for Pure Science (Ibn Al-Haitham)/University of Baghdad, Iraq Abstract: In this study Matlab program build to study the effect of main parameter of quadrupole magnet lens. The study included theoretical analysis using matrices representation to calculate the focal length, lens power, effective length and displacement (the bandwidth envelope) for Horizontal and Vertical plane. Results showed the increasing in effective length caused decreasing in focal length of the system for horizontal and vertical plane, the opposite action appeared with lens power. Furthermore the increasing in effective length caused decreasing in Horizontal displacement (beam envelope) for horizontal plane, the opposite action appeared for vertical plane. Key Words : Ion Optical, Focusing lenses, Quadrupole Magnet, Magnetic lens. 1. Introduction A charged particle motion is determined mainly by interaction with electromagnetic forces [1]. Focusing systems of most installations of particle-beam technology are really intended for beam focusing, that is, obtaining a very small beam cross section (point focusing) [2]. New types of focusing systems, such as quadruple lenses, edge focusing in sector-shaped magnets, alternating gradient focusing, and so on, were invented and contributed to the successful development of plasma physics with steadily increasing energies and improving performance characteristics [3]. Applying the formalism of geometric optics the quadruple magnetic lens can be described as a thin focusing lens [4]. The current research aims to study the focal length of quadrupole magnet system to get the best values that leading to minimum band width or best focusing which is achieved in more control on beam transport systems. -
Lecture 2, Magnetic Fields and Magnet Design
Lecture 2 Magnetic Fields and Magnet Design Jeff Holmes, Stuart Henderson, Yan Zhang USPAS January, 2009 Vanderbilt Definition of Beam Optics Beam optics: The process of guiding a charged particle beam from A to B using magnets. An array of magnets which accomplishes this is a transport system, or magnetic lattice. Recall the Lorentz Force on a particle: × 2 ρ γ F = ma = e/c(E + v B) = mv / , where m= m0 (relativistic mass) In magnetic transport systems, typically we have E=0. So, × γ 2 ρ F = ma = e/c(v B) = m0 v / Force on a Particle in a Magnetic Field The simplest type of magnetic field is a constant field. A charged particle in a constant field executes a circular orbit, with radius ρ and frequency ω. B To find the direction of ω the force on the particle, ρ use the right-hand-rule. v What would happen if the initial velocity had a component in the direction of the field? Dipole Magnets A dipole magnet gives us a constant field, B. The field lines in a magnet run from S North to South. The field shown at right is positive in the vertical direction. B Symbol convention: F x - traveling into the page, x • - traveling out of the page. In the field shown, for a positively charged N particle traveling into the page, the force is to the right. In an accelerator lattice, dipoles are used to bend the beam trajectory. The set of dipoles in a lattice defines the reference trajectory: s Field Equations for a Dipole Let’s consider the dipole field force in more detail. -
Accelerator Magnets and Magnetic Field Measurement Supervisor: Dr
Synchrotron Research Institute German-Armenian Joint Practical Course on Accelerator Physics Accelerator Magnets and Magnetic Field Measurement Supervisor: Dr. Vitali Khachatryan Supported by the German Federal Foreign Office under Kapitel 0504, Titel 68713 YEREVAN, ARMENIA 2019 Introduction ............................................................................................... 4 1 Mathematical fundamentals .................................................................. 4 1.1 Multipole expansions .......................................................................... 5 Cylindrical coordinate representation ............................................................................ 6 Cartesian coordinates ................................................................................................. 10 2 Accelerator magnets ............................................................................ 12 2.1 Dipole magnet .......................................................................................................... 12 2.2 Solenoid lens ............................................................................................................ 13 2.4 Quadrupole magnet .................................................................................................. 13 2.5 Particle tracks and transformation matrices ............................................................. 16 2.6 Drift .......................................................................................................................... -
Fundamental of Accelerators
Fundamental of Accelerators Fanglei Lin Center for Advanced Studies of Accelerators, Jefferson Lab 29th Annual Hampton University Graduate Studies Program HUGS 2014, Jefferson Lab, June 2-20, 2014 Definition of Beam Optics Beam Optics: the process of guiding a charged particle beam from A to B using magnets An array of magnets which accomplishes this is a transport system, or magnetic lattice Recall Lorentz Force on a particle d(γmυ) = q(E +υ × B) dt Energy changes from electric fields Direction changes (energy conservative) from magnetic fields 2 Force on a Particle in a Magnetic Field The simplest type of magnetic field is a constant field. A charged particle in a constant field executes a circular orbit, with radius ρ and frequency ω To find the direction of the force on the particle, use the right-hand-rule. B ω ρ What would happen if the initial velocity had v a component in the direction of the field ? 3 Dipole Magnets A dipole magnet gives a constant field B Field lines in a magnet run from the North to South Symbol convention: × : traveling into the page ● : traveling out of the page In the field shown, for a positively charged particle traveling into the page, the force is to the right. In an accelerator lattice, dipoles are used to bend the beam trajectory. The set of dipoles in a lattice defines the reference trajectory ᶩ p[GeV / c] ≈ 0.3B[T ]ρ[m] q[e] θ ρ l θ = 4 ρ Generating B Field from a Current A current in a wire generates a magnetic field B which curls around the wire: Winding many turns on a coil -
Quantum Theory of Magnetic Quadrupole Lenses for Spin- 2 Particles∗
physics/9809032 1 Quantum theory of magnetic quadrupole lenses for spin- 2 particles∗ Sameen Ahmed KHAN Dipartimento di Fisica Galileo Galilei Universit`adiPadova Istituto Nazionale di Fisica Nucleare (INFN) Sezione di Padova Via Marzolo 8 Padova 35131 ITALY E-mail: [email protected], http://www.pd.infn.it/∼khan/welcome.html Abstract General guidelines for constructing a quantum theory of charged-particle beam optics starting ab initio from the basic equations of quantum mechanics, 1 appropriate to the situation under study. In the context of spin-2 particles, these guidelines are used starting with the Dirac equation. The spinor the- ory just constructed is used to obtain the transfer maps for normal and skew magnetic quadrupoles respectively. As expected the traditional transfer maps get modified by the quantum contributions. The classical limit of the quan- tum formalism presented, reproduces the well-known Lie algebraic formalism of charged-particle beam optics. 1 Keywords: Beam physics, Beam optics, Accelerator optics, Spin- 2 particle, Anoma- lous magnetic moment, Quantum mechanics, Dirac equation, Foldy-Wouthuysen transformation, Polarization, Thomas-Bargmann-Michel-Telegdi equation, Magnetic quadrupole lenses, Stern-Gerlach kicks, Quantum corrections to the classical theory. PACS: 29.20.-c (Cyclic accelerators and storage rings), 29.27.-a (Beams in particle accelerators), 29.27.Hj (Polarized beams), 41.75.-i (Charged-particle beams), 41.75.Ht (Relativistic electron and positron beams), 41.85.-p (Beam optics), 41.85.Ja (Beam transport), 41.85.Lc (Beam focusing and bending magnets). ∗Presented at the Workshop on “Quantum Aspects of Beam Physics”, 15th ICFA (International Committee for Future Accelerators) Advanced Beam Dynamics Workshop, January 4–9, 1998, Mon- terey, California, U.S.A. -
Dipole Magnets
Dipole magnets A dipole magnet gives a constant B-field. The field lines in a magnet run from North to South. The field shown at right is positive in the vertical direction. Symbol convention: × - traveling into the page ● - traveling out of page In the field shown, for a positively charged particle traveling into the page, the force is to the right. In an accelerator lattice, dipoles are used to bend the beam trajectory. The set of dipoles in a lattice defines the reference trajectory: Indian Institute of Technology Ropar Hans-Jürgen Wollersheim - 2016 Field Equations for a Dipole Let’s consider the dipole field force in more detail. Using the Lorentz Force equation, we can derive the following useful relations: For a particle of mass m, Energy E and momentum p in a uniform B-field: 1) The bending radius of the motion of the particle in the dipole field is given by: 1 = 2) Re-arranging (1), we define the “magnetic rigidity” to be the required magnetic bending strength for given radius and energy: = = 10 = 2.998 ∙ ∙ Indian Institute of Technology Ropar Hans-Jürgen Wollersheim - 2016 Generating a B-field from a current Recall that a current in a wire generates a magnetic B-field which curls around the wire Or, by winding many turns on a coil we can create a strong uniform magnetic field The field strength is given by one of Maxwell’s equation: × = 4 ∆ = 0 Indian Institute of Technology Ropar Hans-Jürgen Wollersheim - 2016 The Dipole Current-to-Field Relationship In an accelerator dipole magnet, we use current-carrying wires and metal cores of high μ to set up a strong dipole field: N turns of current I generate a small H=B/μ in the metal. -
Basic Course on Accelerator Optics
BASIC COURSE ON ACCELERATOR OPTICS J. Rossbach, Deutsches Elektronen-Synchrotron DESY P. Schmüser, II. Institut für Experimentalphysik, Universität Hamburg, F.R. Germany Abstract The main subject of this introductory course is transverse optics in cyclic high energy accelerators. It is based on three one-hour lectures on "Basic transverse optics" given at the CERN Accelerator Schools (P. Schmüser, 1986 [5], 1988, 1990, and J. Rossbach, 1992). Although the emphasis is on periodic solutions and their stability, application of the formalism to non-periodic structures is also treated. We have not expanded the material beyond what can be covered in 3 lectures, but the proofs are done more carefully and some examples and details have been added which might be useful in practice. After a brief introduction to the concepts of both weak and strong focusing of relativistic particle beams, types of magnetic lenses are discussed, followed by a careful treatment of the multipole expansion of transverse magnetic fields. Linear transverse single-particle dynamics is treated both in terms of transfer matrices and betatron oscillations. Transfer matrices of the most common accelerator lattice modules are explicitly given, including a brief introduction to quadrupole doublet imaging. Dispersion is treated, but no linear coupling. The concept of beam emittance, including Liouville's Theorem, is discussed from different points of view. Also effects of linear field errors, stability criteria and chromaticity are dealt with. FODO cells are treated in various respects. Finally, strong and weak focusing are compared quantitatively. 1 INTRODUCTION In any kind of accelerator there is exactly one curve - the design orbit - on which ideally all particles should move, see Fig. -
Setup of a Penning Trap for Precision Laser Spectroscopy at HITRAP
Setup of a Penning trap for precision laser spectroscopy at HITRAP Trapping, cooling and electronic detection of externally produced ions Dissertation zur Erlangung des Grades „Doktor der Naturwissenschaften“ im Promotionsfach Chemie am Fachbereich Chemie, Pharmazie und Geowissenschaften der Johannes Gutenberg-Universität Mainz Zoran Anđelković geb. in Belgrad, Serbien Mainz, den 22. März 2012 Contents Introduction xi 1. Laser spectroscopy of forbidden transitions in highly charged ions 1 1.1. Highly charged ions . 1 1.1.1. Heavy highly charged ions at the GSI accelerator facility . 4 1.1.2. Mid-Z highly charged ions and the HITRAP EBIT . 5 1.2. Forbidden transitions in highly charged ions . 7 1.2.1. Transition probabilities . 7 1.2.2. Fine-structure transitions . 9 1.2.3. Hyperfine structure transitions . 10 1.3. Laser spectroscopy in ion traps . 12 1.3.1. Laser induced fluorescence spectroscopy . 13 1.3.2. Broadening of spectral lines . 13 2. Ion storage, detection and cooling in a Penning trap 15 2.1. Principles of charged particle confinement . 16 2.1.1. Particle motion inside a Penning trap . 17 2.1.2. Space charge effects . 19 2.1.3. Open-endcap cylindrical Penning Trap . 20 2.1.4. Electric and magnetic field inhomogeneities . 22 2.2. Destructive ion detection . 22 2.3. Non-destructive ion detection . 24 2.3.1. Theory of resonant circuits . 25 2.3.2. Interaction between trap electrodes and charged particles . 27 2.3.3. Passive tuned-circuit noise detection . 29 2.4. Ion cooling . 31 2.4.1. Resistive cooling . 31 2.4.2. -
Lawrence Berkeley National Laboratory Recent Work
Lawrence Berkeley National Laboratory Recent Work Title A CROSSED BEAM APPARATUS FOR MEASURING DIFFERENTIAL CROSS SECTIONS FOR ION- NEUTRAL INTERACTIONS AT LOW COLLISION ENERGIES Permalink https://escholarship.org/uc/item/67d9f4mx Author Farrar, James M. Publication Date 1976-09-01 eScholarship.org Powered by the California Digital Library University of California U ...J LBL-5478, c. ... , A CROSSED BEAM APPARATUS FOR MEASURlNG DIFFERENTIAL CROSS SEC TIONS FOR ION -NEUTRAL INTERACTIONS AT LOW COLLISION ENERGIES James M. Farrar September 1976 Prepared for the U. S. Energy Research and Development Administration under Contract W -7405-ENG -48 For Reference Not to be taken from this room DISCLAIMER This document was prepared as an account of work sponsored by the United States Government. While this document is believed to contain correct information, neither the United States Government nor any agency thereof, nor the Regents of the University of California, nor any of their employees, makes any warranty, express or implied, or assumes any legal responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or service by its trade name, trademark, manufacturer, or otherwise, does not necessarily constitute or imply its endorsement, recommendation, or favoring by the United States Government or any agency thereof, or the Regents of the University of California. The views and opinions of authors expressed herein do not necessarily state or reflect those of the United States Government or any agency thereof or the Regents of the University of California.