E166 Collaboration Meeting Princeton, 22-24 May 2006 Analyzer Magnetic Analysis K. Peter Schüler General Overview Spin and Magnetization Field Distribution.

Slides:



Advertisements
Similar presentations
POLARIMETRY of MeV Photons and Positrons Overview Beam Characterization – undulator photons – positrons Basics of the Transmission Method – for photon.
Advertisements

The E166 Experiment K. Peter Schüler e+ source options for the ILC undulator source scheme for ILC E166 – proof-of-principle demonstration of the undulator.
Fundamentals of Magnetism T. Stobiecki. Definitions of magnetic fields Induction: External magnetic field: Magnetizationaverage magnetic moment of magnetic.
Chapter 10 Time-Varying Fields and Maxwell’s Equations Two New Concepts: The electric field produced by a changing magnetic field (Faraday) The magnetic.
BUILD-UP SIMULATIONS FOR DAFNE WIGGLER W/ ELECTRODES Theo Demma.
Simulations with ‘Realistic’ Photon Spectra Mike Jenkins Lancaster University and The Cockcroft Institute.
Purpose Determine the charge to mass ratio (e/m) of an electron.
Magnets for the ESRF upgrade phase II
Fundamentals of Magnetism T. Stobiecki, Katedra Elektroniki AGH 2 wykład
Sources of Magnetic Field Chapter 28 Study the magnetic field generated by a moving charge Consider magnetic field of a current-carrying conductor Examine.
K. LaihemPrinceton meeting Princeton meeting Status Report Simulation studies E166 experiment Karim Laihem.
Status report about the e-  identifier Study of shielding against the stray magnetic field at the downstream end of the spectrometer F. Huveneers, Gh.
Topics in Magnetism I. Definitions and Atomic Sources
Left: The polarization of the undulator radiation as a function of energy. Right: Calculated positron longitudinal polarization as a function of energy.
K. LaihemE166 collaboration LCWS06 Bangalore March 12th 2006 The E166 experiment Development of a polarized positron source for the ILC. Karim Laihem on.
Undulator-Based Production of Polarized Positrons An experiment in the 50 GeV Beam in the SLAC FFTB E-166 Undulator-Based Production of Polarized Positrons.
Magnetism Any time electrical power is moving through a wire magnetism is created Any time magnetism moves past a wire electrical power is created.
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.
Basics in Magnetism Electromagnetism Force on a Current-Carrying Wire EM Induction Transformer Generators Electric Motors ELECTROMAGNETISM.
Foundations of Physics
AP Physics C Montwood High School R. Casao
ISNS Phenomena of Nature
Oct 15, 2003 Video Conference Energy Deposition Steve Kahn Page 1 Energy Deposition in MICE Absorbers and Coils Steve Kahn November 2, 2003.
A topic (in two parts) about the interaction between magnetic fields
Magnetic Flux and Faraday’s Law of Induction
Magnetic Flux and Faraday’s Law of Induction. Questions 1.What is the name of the disturbance caused by electricity moving through matter? 2.How does.
Unit 14 Magnetic Induction. Objectives: Discuss magnetic induction. List factors that determine the amount and polarity of an induced voltage. Discuss.
The PEPPo e - & e + polarization measurements E. Fanchini On behalf of the PEPPo collaboration POSIPOL 2012 Zeuthen 4-6 September E. Fanchini -Posipol.
6.11 Vocabulary Electromagnet: type of magnet in which the magnetic field is produced by a flow of electric current Core: metal (iron) center of an electromagnet.
Magnetism Opposite poles attract and likes repel
Experiment Rosen07: Measurement of R =  L /  T on Deuterium in the Nucleon Resonance Region. 1  Physics  Data Analysis  Cross Section calculation.
Beijing, Feb 3 rd, 2007 LEPOL 1 Low Energy Positron Polarimetry for the ILC Sabine Riemann (DESY) On behalf of the LEPOL Collaboration.
Status of the Beamline Simulation A.Somov Jefferson Lab Collaboration Meeting, May 11, 2010.
Lecture 8 MAGNETOSTATICS Magnetic Fields Fundamental Postulates of Magnetostatics in Free Space Prof. Viviana Vladutescu.
Ultra-Compact Electrical Machines for Wind Energy DE-FOA : Demo Machine C. L. Goodzeit and M. J. Ball May 1, 2014 Part 1: Design and Construction.
Inductors An inductor is essentially a coil of wire with an iron core.
Polarimetry at the LC Source Which type of polarimetry, at which energies for LC ? Sabine Riemann (DESY), LEPOL Group International Workshop on Linear.
Beam Polarimetry Matthew Musgrave NPDGamma Collaboration Meeting Oak Ridge National Laboratory Oct. 15, 2010.
V s N s V p N p = 1. What is mutual induction, how does it work? 2. What is self induction, how does it work? 3. What is the significance of the turns.
The link between electricity & magnetism N S When a wire moves through a magnetic field a voltage is produced N Moving a magnet moves through a coil of.
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.
Polarimetry Report Sabine Riemann on behalf of the DESY/HUB group January 24, 2008 EUROTeV Annual Meeting, Frascati.
Oct 15, 2003 Video Conference Energy Deposition Steve Kahn Page 1 Energy Deposition in MICE Absorbers and Coils Steve Kahn November 2, 2003.
Magnetic Fields. MAGNETOSTATICS Magnetic Fields Fundamental Postulates of Magnetostatics in Free Space.
E166: Polarized Positrons & Polarimetry K. Peter Schüler ILC: - why polarized positrons - e+ source options - undulator source scheme E166 - proof-of-principle.
Design of DC septum magnets based on measurements and 3D calculation of an R&D septum magnet for Rapid Cycle Synchrotron of J-PARC Masao Watanabe, Accelerator.
Inductors ? circuit diagram symbol.
Magnetic Field Stability Measurements Joe DiMarco 23Oct07.
The force on a current-carrying wire A magnetic field exerts a force on a single moving charge, so it's not surprising that it exerts a force on a current-carrying.
An electron/positron energy monitor based on synchrotron radiation. I.Meshkov, T. Mamedov, E. Syresin, An electron/positron energy monitor based on synchrotron.
Experiment Rosen07: Measurement of R =  L /  T on Deuterium in the Nucleon Resonance Region.  Physics  Data Analysis  Cross Section calculation 
Chapter 35 Magnetic Properties of Materials. E0E0 qq q E0E0 To describe this weakness of the electric field in an insulator, with “dielectric constant”
Preliminary result of the target polarization 2004 Kaori Kondo COMPASS target team.
Biot-Savart Law for a Single Charge Electric field of a point charge: Moving charge makes a curly magnetic field: B units: T (tesla) = kg s -2 A -1 The.
Transformers and Impedance. Review Two types of current: –ac –dc Two fundamental principles: –Moving electrons create magnetic fields –Moving or changing.
1 :. Introduction These are special type of transformers used for the measurement of voltage, current, power and energy. As the name suggests, these transformers.
Magnetic Fields. Magnets Magnets are polarized Magnets are polarized –It has two distinct and opposite ends North-seeking pole North-seeking pole South-seeking.
Shri Navsari Paschim Vibhag Koli Samal Kalyankari Trust Sanchalit MAHATMA GANDHI INSTITUTE OF TECHNICAL EDUCATION & RESEARCH CENTER NAVSARI NPE Campus,
Dollan, Laihem, Lohse, Schälicke, Stahl 1 Monte Carlo based studies of polarized positrons source for the International Linear Collider (ILC)
Yingshun Zhu Design of Small Aperture Quadrupole Magnet for HEPS-TF
Lecture 12 Magnetism of Matter: Maxwell’s Equations Ch. 32 Cartoon Opening Demo Topics Finish up Mutual inductance Ferromagnetism Maxwell equations.
Preliminary Magnetic Analysis of the CCT Magnet for HL-LHC
Progress with Spin Tracking in GEANT4
© 2011 Cengage Learning Engineering. All Rights Reserved.
Current flowing out Current flowing in 14-1
Magnets, Magnetism & Electromagnetism
Reading Quiz 2. What is the shape of the trajectory that a charged particle follows in a uniform magnetic field? Helix Parabola Circle Ellipse Hyperbola.
Electromagnets How they work, and how to make them more powerful
Flux density produced by a long coil (solenoid)
ILC Baseline Design: Physics with Polarized Positrons
Presentation transcript:

E166 Collaboration Meeting Princeton, May 2006 Analyzer Magnetic Analysis K. Peter Schüler General Overview Spin and Magnetization Field Distribution Modeling Results from Flux and Field Measurements Electron Polarization of the Iron Remaining Work Analyzer Magnetic Analysis (Status Report) P. Schüler (DESY)

2 General Overview error in e- polarization is dominated by knowledge in effective magnetization M along the photon trajectory: active volume Photon Analyzer: 50 mm dia. x 150 mm long Positron Analyzer: 50 mm dia. x 75 mm long E166 Collaboration Meeting Princeton, May 2006 Analyzer Magnetic Analysis K. Peter Schüler P e ≈ 0.07 ΔP e /P e < 0.05 (aim of proposal) electron polarization of the iron: M = manetization n = electron density μ B = Bohr magneton g‘ = magneto-mechanical factor

3 Spin and Magnetization E166 Collaboration Meeting Princeton, May 2006 Analyzer Magnetic Analysis K. Peter Schüler g‘ = magneto-mechanical factor: obtained from Einstein - de Haas type experiments, related to gyromagnetic ratio: γ = (g‘/2) ∙ (e/m) the principle … and its ultimate implementation (Scott 1962) g‘ = ± for pure iron i.e. orbital effects contribute about 4% Note: g‘ = 2  M s / M = 1 (pure spin magnetization) γ = e/m g‘ = 1  M s / M = 0 (pure orbit magnetization) γ = ½ (e/m)

4 Analyzer Magnets E166 Collaboration Meeting Princeton, May 2006 Analyzer Magnetic Analysis K. Peter Schüler CsI-Detector e+ Analyzer Pickup Coils e+ Analyzer  Analyzer

5 Field Distribution Modeling (Vector Fields OPERA-2d) E166 Collaboration Meeting Princeton, May 2006 Analyzer Magnetic Analysis K. Peter Schüler R = 0 mm B z (T) Z (mm) longitudinal field distribution: B z (R,Z) field drops gradually towards the ends: L eff / L < 1 center end

6 Field Distribution in 2d (Vector Fields OPERA-2d) E166 Collaboration Meeting Princeton, May 2006 Analyzer Magnetic Analysis K. Peter Schüler longitudinal field distribution: B z (R,Z) R (mm) Z (mm)

7 Pickup Coils for Flux Measurements: Positron AnalyzerPhoton Analyzer Δz (mm) r (mm) n (turns) Δz (mm) r (mm) n (turns) upstream x 40 = ** center x 38 = x 40 = 160 downstream x 40 = 160* x 40 = 160 dummy E166 Collaboration Meeting Princeton, May 2006 Analyzer Magnetic Analysis K. Peter Schüler (*) positron downstream became dysfuntional after Oct at SLAC (**) photon upstream was damaged already at DESY used 4 turns of special coil wire with 40 wire strands: externally wired in series for 4 x 40 = 160 turns max.

8 Flux Measurements: E166 Collaboration Meeting Princeton, May 2006 Analyzer Magnetic Analysis K. Peter Schüler data taken by Zen - analyzed by Roman measure voltage transients in pickup coils upon current reversals Positron Analyzer (-60  +60 amps) Photon Analyzer (-60  +60 amps) Sawtooth from Waveform Generator (for calibration of time base)

9 Flux Data: E166 Collaboration Meeting Princeton, May 2006 Analyzer Magnetic Analysis K. Peter Schüler

10 Flux and Field Measurements: Results E166 Collaboration Meeting Princeton, May 2006 Analyzer Magnetic Analysis K. Peter Schüler Note: polarimetry was always done at full saturation over the central region (±60A) Z = 0 (center)

11 Flux and Field Measurements: E166 Collaboration Meeting Princeton, May 2006 Analyzer Magnetic Analysis K. Peter Schüler No significant field difference seen between „upstream“ and „center“ Z = -20 mm

12 electron polarization of the iron E166 Collaboration Meeting Princeton, May 2006 Analyzer Magnetic Analysis K. Peter Schüler preliminary result for the e+ analyzer: (6.94 ± 0.17) % - and the nitty-gritty:

13 Remaining Work E166 Collaboration Meeting Princeton, May 2006 Analyzer Magnetic Analysis K. Peter Schüler repeat magnetic modeling with correct central field values as measured choose finer mesh spacing same for photon magnet generate writeup