Geonium A Fake but Useful Atom BoBo. Overview What is Geonium and why is it useful? A little bit of history What is a Penning trap? Penning trap components.

Slides:



Advertisements
Similar presentations
Motion of a Charged Particle in a Magnetic Field
Advertisements

Applications of the Motion of Charged Particles in a Magnetic Field AP Physics C Montwood High School R. Casao.
Lecture 11 Magnetism of Matter: Maxwell’s Equations Chp
Magnetic Force PH 203 Professor Lee Carkner Lecture 16.
Single particle motion and trapped particles
Example: A single square loop of wire is placed in the plane of a magnetic field with a strength of 200 mT directed to the right. The loop has sides 10.
Electric Fields The Electric Field Electric Fields Lines Field due to a Point Charge Field due to an Electric Dipole Field due to a Line of Charge Field.
2/xx/07184 Lecture 221 PHY 184 Week 6 Spring 2007 Lecture 22 Title: The Lorentz Force = q v x B.
Charged Particles in Electric and Magnetic Fields Motion of charged particles Lorentz Force Examples: cyclotron, mass spectrometer.
Chapter 4 Waves in Plasmas 4.1 Representation of Waves 4.2 Group velocity 4.3 Plasma Oscillations 4.4 Electron Plasma Waves 4.5 Sound Waves 4.6 Ion Waves.
Magnetic Field and Magnetic Forces
There are a total of n subshells, each specified by an angular momentum quantum number, and having an angular momentum of The allowed energy levels are.
Q free on inner surface - Q free on inner surface Interior points electric field must be zero - q bound + q bound Symmetry –
Physics 1502: Lecture 17 Today’s Agenda Announcements: –Midterm 1 distributed today Homework 05 due FridayHomework 05 due Friday Magnetism.
PHYS Quantum Mechanics PHYS Quantum Mechanics Dr Jon Billowes Nuclear Physics Group (Schuster Building, room 4.10)
Today’s Lecture ●Spatial Quantisation ●Angular part of the wave function ●Spin of the electron ●Stern – Gerlach experiment ●Internal magnetic fields in.
LECTURE 22 More Atom Building PHYSICS 420 SPRING 2006 Dennis Papadopoulos.
Q free on inner surface - Q free on inner surface Interior points electric field must be zero - q bound + q bound Symmetry –
Physics 121: Electricity & Magnetism – Lecture 9 Magnetic Fields Dale E. Gary Wenda Cao NJIT Physics Department.
Biot-Savart Law Moving charge produces a curly magnetic field
Physics 121: Electricity & Magnetism – Lecture 3 Electric Field
Chapter 19 NMR Spectroscopy. Introduction... Nuclear Magnetic Resonance Spectrometry is based on the measurement of absorption of electromagnetic radiation.
A bit on quantum mechanics and atomic physics Physics 114 Spring 2004 – S. Manly References and photo sources: K. Krane, Modern Physics, John Wiley and.
Step 1: Cut up the current distribution into pieces and draw  B. Origin: center of wire Vector r: Magnitude of r: A Long Straight Wire Unit vector:
Gravity and Orbits The gravitational force between two objects:
Particle accelerators and detectors -Short Answers.
Magnetic Field Lines for a Loop Figure (a) shows the magnetic field lines surrounding a current loop Figure (b) shows the field lines in the iron filings.
Proposed injection of polarized He3+ ions into EBIS trap with slanted electrostatic mirror* A.Pikin, A. Zelenski, A. Kponou, J. Alessi, E. Beebe, K. Prelec,
Consider a time dependent electric field E(t) acting on a metal. Take the case when the wavelength of the field is large compared to the electron mean.
12 Ion traps 12.1 The force on ions in an electric field 12.2 Earnsha’s theorem 12.3 The Paul trap 12.4 Buffer gas cooling 12.5 Laser cooling of trapped.
Lecture 12 Magnetism of Matter: Maxwell’s Equations Ch. 32 Cartoon Opening Demo Topics –Ferromagnetism –Maxwell equations –Displacement current Demos.
Lecture 2:Research frontiers 1 9/9/ FYPC Most recent long range planning reports: FYPC (Canada), NSAC (USA) Collision products at RHIC.
Light and Matter Tim Freegarde School of Physics & Astronomy University of Southampton Classical electrodynamics.
Lecture 14-1 Magnetic Field B Magnetic force acting on a moving charge q depends on q, v. (q>0) If q
Lecture 20: More on the deuteron 18/11/ Analysis so far: (N.B., see Krane, Chapter 4) Quantum numbers: (J , T) = (1 +, 0) favor a 3 S 1 configuration.
Ampere’s Law The product of can be evaluated for small length elements on the circular path defined by the compass needles for the long straight wire.
Phys 102 – Lecture 26 The quantum numbers and spin.
Magnetism Physics T Soft Gamma Repeater , is the most powerful known magnetic object in the universe. Only 10 of these unusual objects.
Lecture 37: FRI 21 NOV CH32: Maxwell’s Equations III James Clerk Maxwell ( ) Physics 2113 Jonathan Dowling.
Lecture 12 Magnetism of Matter: Maxwell’s Equations Chp. 32 Cartoon Warm-up problem Opening Demo Topics –Finish up Mutual inductance –Ferromagnetism –Maxwell.
Energy calibration at LHC J. Wenninger. Motivation In general there is not much interest for accurate knowledge of the momentum in hadron machines. 
Magnetism1 Review on Magnetism Chapter 28 Magnetism2 Refrigerators are attracted to magnets!
Magnetic Fields Chapter 29 (continued). Force on a Charge in a Magnetic Field v F B q m (Use “Right-Hand” Rule to determine direction of F)
Lecture 3 16/9/2003 Recall Penning Trap orbits cylindrical coordinates: ( , ,z); B = constant along z radial (  ) and axial (z) electric.
Physics 121 Practice Problem Solutions 09 Magnetic Fields
1 Chapter 19: Magnetism The nature of magnetism Iron ore found near Magnesia Compass needles align N-S: magnetic Poles North (South) Poles attracted to.
Electromagnetism Zhu Jiongming Department of Physics Shanghai Teachers University.
Magnetic field Chapter 28.
Electric Fields in Matter  Polarization  Electric displacement  Field of a polarized object  Linear dielectrics.
Magnetic Field and Magnetic Forces
Spectroscopy Spectral lines The Fraunhofer spectrum Charlotte Moore Sitterly (Allen!) –Multiplet table –Rowland table Formalism of spectroscopy.
Introduction to materials physics #3
Vibrational Motion Harmonic motion occurs when a particle experiences a restoring force that is proportional to its displacement. F=-kx Where k is the.
Atomic Physics Quantum Physics 2002 Recommended Reading: Harris Chapter 7.
Last Time (Cross Products: Mathematically) Electron Current and Conventional Current Calculating the Electron Current True vs. Useful Biot-Savart Law in.
Electrostatic field in dielectric media When a material has no free charge carriers or very few charge carriers, it is known as dielectric. For example.
Copyright © 2009 Pearson Education, Inc. Biot-Savart Law.
The Zeeman Effect in Mercury Casey Wall with Advisor Alan Thorndike Summer 2011 Purpose The purpose of this experiment was to observe the effect of a magnetic.
Raman Effect The Scattering of electromagnetic radiation by matter with a change of frequency.
Electric Field & Magnetic Field
Single particle motion and trapped particles
Lasers and effects of magnetic field
AP Physics C: Electricity & Magnetism – Charges & Electric Field
Diatomic molecules
Gross Properties of Nuclei
Pauli Paramagnetism.
The Free Electron Fermi Gas
Nuclear Magnetic Resonance (NMR) Spectroscopy
Magnetic Monopoles Does there exist magnetic charge, just like electric charge? An entity which carried such magnetic charge would be called a magnetic.
Chapter 28 Magnetic Fields
Presentation transcript:

Geonium A Fake but Useful Atom BoBo

Overview What is Geonium and why is it useful? A little bit of history What is a Penning trap? Penning trap components and diagram Measurement Techniques Overview of the g-Factor Useful Results

What is Geonium and Why is it Useful? Not an actual atom! A single electron (or positron) confined inside of a Penning trap Called “Geonium” because it is essentially an electron bound to the earth Can measure g-factor and electron radius to great precision e-e-

Some History Hans Dehmelt of the University of Washington first quasi-permanently trapped an electron in 1973 after 17 years of work On October 12, 1989 he and Wolfgang Paul of Bonn University receive the Nobel Prize for Physics for their work on isolating individual electrons and ions and making exact measurements of them

What is a Penning Trap? Predecessor in measuring electron magnetic moment and g-factor: electrons stored in the field of a positive-ion cloud diffusing in a dense inert gas, polarized by spin- exchange collisions with optically polarized sodium vapor and depolarized by magnetic resonance Problem: too many electrons Solution: the Penning trap replaces the space-charge field with a high-vacuum quadrupole trap and the alkali vapor with an atomic beam. (Liquid Helium Temperatures ~4K) Benefit: using the Penning trap, a single electron can be confined near the axis for many months!

Penning Trap Components Top and bottom conducting caps have charge -Q/2 and center tube has charge +Q --> quadrupolar electrostatic field described by scalar potential: Uniform magnetic field B o along the z-axis Magnetized nickel wire around the center of the electrode creates “bottle field” used to measure properties of trapped electron

The Basic Penning Trap -Q/2 +Q Magnetized nickel wire wrapped around center measures electron properties z x y

Electron Motion in the Trap Three types --> cyclotron, magnetron, and axial motion 1.Axial: electron moves along the symmetry axis of the trap (z) changing directions with sinusoidal frequency as it gets too close to the charged caps (A>0, same constant as potential) 2.Cyclotron: small circular orbits resulting from the opposition between the radial electric and centripetal magnetic forces 3.Magnetron: Slow drift around the symmetry axis

Electron Motion in the Trap *Neat Java Applet

Measurement The axial frequency is at radio/television range, acting like an LC oscillator, so a reference signal can be used and adjusted to see both the absorption and dispersion modes of the axial resonator ATTEN. A INTEGRATOR ~ V o =9.2V Error Signal

The electron spin g-factor or gyromagnetic ratio is the ratio of the magnetic dipole moment to the mechanical angular momentum of a system Contributes to Zeeman effect and thus can be calculated from spectral lines Can be used to find magnetic moment The g-Factor Spin resonance frequency

Geonium Energy Levels & the g-Factor n = (after removing QED shifts)