Transport/Turtle Studies of present and new g-2 beam lines (p. pile 3/9/06) Present Transport is H. Brown’s as translated by P. Debevec –for001_g-2pimu_v4_upload.dat.

Slides:



Advertisements
Similar presentations
Optics and magnetic field calculation for the Hall D Tagger Guangliang Yang Glasgow University.
Advertisements

HLAB MEETING -- Paper -- T.Gogami 30Apr2013. Experiments with magnets (e,eK + ) reaction.
1 MICE Beamline: Plans for initial commissioning. Kevin Tilley, 16 th November. - 75days until commissioning Target, detectors, particle production Upstream.
January 14, 2004 TJR - - UPDATED 1/25/04 1 MICE Beamline Analysis Using g4beamline Including Jan 25 Updates for Kevin’s JAN04 Beamline Design Tom Roberts.
STARTER Put this number in scientific notation.
Eric Prebys, FNAL.  So far, we’ve talked about nice, periodic lattice, but that may not be all that useful in the real world. In particular, we generally.
24/01/08Energy deposition, LIUWG, Elena Wildner1 Upgrade phase 1: Energy deposition in the triplet Elena Wildner Francesco Cerutti Marco Mauri.
Pion capture and transport system for PRISM M. Yoshida Osaka Univ. 2005/8/28 NuFACT06 at UCI.
Paul drumm, mutac jan MICE Beamline Optics Design Kevin Tilley, RAL, 12th June MICE Needs Generic Solution Pion Injection & Decay Section (a) Inputs.
Beam line summary paul drumm for beam line group.
124/3/2010CM26 - Riverside1 m. apollonio ( ,P) matrix.
K.Walaron Fermilab, Batavia, Chicago 12/6/ Simulation and performance of beamline K.Walaron T.J. Roberts.
MICE Beam Line Design Oct 24 th 2005 Dean Adams, Kevin Tilley Based on TURTLE element definitions by K Walaron, T Roberts and K Tilley.
Fig. 3-1, p. 67. Fig. 3-2, p. 67 Fig. 3-3, p. 68.
Recirculating pass optics V.Ptitsyn, D.Trbojevic, N.Tsoupas.
March 30, 2004 TJR1 MICE Beamline Performance with New Magnet Descriptions Tom Roberts Illinois Institute of Technology March 30, 2004.
1 MICE Beamline Design: General principles & expected capabilities Kevin Tilley, 16 th November Charge to beamline & desirable beam General principles.
Lattice calculations: Lattices Tune Calculations Dispersion Momentum Compaction Chromaticity Sextupoles Rende Steerenberg (BE/OP) 17 January 2012 Rende.
T. Horn, SHMS Optics Update SHMS Optics Update Tanja Horn Hall C Users Meeting 31 January 2009.
$100 $200 $300 $400 $500 $100 $200 $300 $400 $500 $100 $200 $300 $400 $500 $100 $200 $300 $400 $500 $100 $200 $300 $400 $500 $100 $200 $300.
$100 $200 $300 $400 $500 $100 $200 $300 $400 $500 $100 $200 $300 $400 $500 $100 $200 $300 $400 $500 $100 $200 $300 $400 $500 $100 $200 $300.
The Overview of the ILC RTML Bunch Compressor Design Sergei Seletskiy LCWS 13 November, 2012.
SHMS Optics Studies Tanja Horn JLab JLab Hall C meeting 18 January 2008.
Beam line commissioning Preparations for Phase1 Kevin Tilley For Paul Drumm & the beam line group.
Status of GlueX Particle Identification Ryan Mitchell September 10, 2004.
Eric Prebys, FNAL.  In our previous discussion, we implicitly assumed that the distribution of particles in phase space followed the ellipse defined.
RAL Muon Beam Line Properties. ISIS 70 MeV H- injection Ring accelerates up to 800 MeV in about 10 ms 50 Hz cycle - Dual Harmonic System ~ 2 x 1.5 MHz;
June 17, 2004 / Collab Meeting Strategy to reduce uncertainty on a  to < 0.25 ppm David Hertzog University of Illinois at Urbana-Champaign n Present data.
Mark Rayner 14/8/08Analysis Meeting: Emittance measurement using the TOFs 1 Emittance measurement using the TOFs The question: can we use position measurements.
BL1U at TRIUMF UCN Beamline Septum & Dipole Magnets (April 12, 2010)
Positron source beamline lattice Wanming Liu, ANL
KEK Test Beam Phase I (May 2005) Makoto Yoshida Osaka Univ. MICE-FT Daresbury Aug 30th, 2005.
Magnetized hadronic calorimeter and muon veto for the K +   +  experiment L. DiLella, May 25, 2004 Purpose:  Provide pion – muon separation (muon veto)
HYBRID WARM-COLD SYNCHROTRON FOR THE MUON COLLIDER Al Garren July 28, 2011.
UPDATE ON THE FORWARD PROTON DETECTOR Gilvan Alves Lafex/CBPF Introduction Accelerator Roman Pots Detector Future Plans April 1, 1998 (no kidding)
Calculating with Negatives THE FOUR RULES AND NEGATIVE NUMBERS.
More beam (muons) from the AGS AGS RHIC Users Group Meeting EDM Workshop Brookhaven National Laboratory 7 June 2006 Phil Pile.
M. Bonesini - CM 22 RAL October 081 TOF0 status M. Bonesini Sezione INFN Milano Bicocca.
MEIC Detector and IR Integration Vasiliy Morozov, Charles Hyde, Pawel Nadel-Turonski MEIC Detector and IR Design Mini-Workshop, October 31, 2011.
Tuning of trigger simulation parameters (Bossi, Moulson, Palutan, Sciascia) Calorimeter trigger thresholds calibration using prompt photons from K S 
Beam collimation in the transfer line from 8 GeV linac to the Main Injector A. Drozhdin The beam transfer line from 8 GeV Linac to the Main Injector is.
1June 2 nd 2009MICE CM24 - RAL1 m. apollonio Beamline+( ,P) matrix.
Interaction Region Design and Detector Integration V.S. Morozov for EIC Study Group at JLAB 2 nd Mini-Workshop on MEIC Interaction Region Design JLab,
Beam Optics of the TTF2 Nina Golubeva DESY. Beam optics from the BC2 up to the undulators General introduction to linear optics: – constraints for different.
This presentation will describe the state of each element in the beam line with regards to the current update being undertaken. Firstly, it will describe.
J-Parc Neutrino Facility Primary Proton Beam Design A. K. Ichikawa(KEK), Y.Iwamoto(KEK) and K.Tanabe(Tokyo) et.al. 7 th Nov. 2003,
Min Huang g2p/GEp Collaboration Meeting April 18, 2011.
INFN - PadovaBeauty Measurements in pp with the Central Detector 1 Beauty Measurements in p-p with the Central Detector F. Antinori, C. Bombonati, A. Dainese,
THE LEVERS IN CLIL METODOLOGIE (Content and Language Integrated Learning)
Scientific Notation Objectives: SWBAT convert between standard notation and scientific notation by hand and by calculators.
Interaction Region and Detector
Motion Position, Speed and Velocity Graphs of Motion Acceleration.
Alternate Lattice for LCLS-II LTU Y
Whiteboard Review #1 What goes in the blanks??? (A) (B) (C) (D) (E)
Specifications for the JLEIC IR Magnets
Ion-Side Small Angle Detection Forward, Far-Forward, & Ultra-Forward
Details of K1.8BR Beam line
longitudinal shower profile
Geant4 in HARP V.Ivanchenko For the HARP Collaboration
Aim: How to use Dimensional Analysis to Convert from One unit to Another DO Now: Answer the following questions in your notebook in the following format.
Length 4.5m = 9cm on the scale drawing Scale 1cm to 0.5m
Rate of Change The rate of change is the change in y-values over the change in x-values.
Java Lessons 9 – 12 Mr. Kalmes.
Calculate 81 ÷ 3 = 27 3 x 3 x 3 3 x 3 x 3 x 3 ÷ 3 = This could be written as
Four Jaw Collimator.
Rough designs for The LEB and HEB for pCDR-100
Upgrade on Compensation of Detector Solenoid effects
7.2 x 10-7 N attraction 2.1 x 10-7 N repulsion A on B / B on A
An Alternative Ion Complex Agenda /some preliminary estimations/
Presentation transcript:

Transport/Turtle Studies of present and new g-2 beam lines (p. pile 3/9/06) Present Transport is H. Brown’s as translated by P. Debevec –for001_g-2pimu_v4_upload.dat with dipole fringe on and D1 gap at 3.5” –Q11-end tuned to GeV/c for backward decay solutions Transport input for the present forward decay beam line is: – /pion/ ; Transport input for the backward decay beam lines is: – /pion/ ; The transport is first order and second order K1 and K2 collimators are “IN” for all fwd decay tunes, except as noted, with –K1=0.812 in (beam left)  K1K2 entrance cut =+0.81/-1.48 in –K2=1.14 in (beam right)  K12 exit cut =+1.00/-1.14 inK12 entrance and exit cuts are separated by 16 inches

The E821 beam line (1 % dp/p), 3.15 GeV/c pion beam (from Debevec) cm or cm/% x (cm) y (cm) dy/dp (cm/%) dx/dp (cm/%) meters

cm or cm/% x (cm) y (cm) dy/dp (cm/%) dx/dp (cm/%) meters The E821 beam line (1 % dp/p), 3.15 GeV/c pion beam (from Debevec) SECOND ORDER CALCULATION

*QUAD* Q m kG 9.52 cm *QUAD* Q m kG 9.52 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 9.52 cm *QUAD* Q m kG 9.52 cm *QUAD* Q9a m kG 4.76 cm *QUAD* Q9b m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q23a m kG 4.76 cm *QUAD* Q23b m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 9.84 cm *QUAD* Q m kG 9.84 cm The E821 beam line (1 % dp/p), 3.15 GeV/c pion beam (from Debevec)

cm or cm/% x (cm) y (cm) dy/dp (cm/%) dx/dp (cm/%) meters E969 beam line FWD DECAY 4X LOW FIELD fodo p116

cm or cm/% x (cm) y (cm) dy/dp (cm/%) dx/dp (cm/%) meters E969 beam line FWD DECAY 4X LOW FIELD fodo p116 2 nd Order Calculation

*QUAD* Q m kG 9.52 cm *QUAD* Q m kG 9.52 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 9.52 cm *QUAD* Q m kG 9.52 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q11a m kG 4.76 cm *QUAD* Q11b m kG 4.76 cm E969 beam line FWD DECAY 4X LOW FIELD fodo (set for 3.15 GeV/c)

*QUAD* Q19a m kG 4.76 cm *QUAD* Q19b m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q23a m kG 4.76 cm *QUAD* Q23b m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 9.84 cm *QUAD* Q m kG 9.84 cm E969 beam line FWD DECAY 4X LOW FIELD fodo

E969 beam line (2.5 % dp/p), 5.35 GeV/c pion beam, present pion decay channel quads (p119) cm or cm/% x (cm) y (cm) dy/dp (cm/%) dx/dp (cm/%) meters

E969 beam line (2.5 % dp/p), 5.35 GeV/c pion beam, present pion decay channel quads P119 with Q7-10 fit to GeV/c FODO(pile) cm or cm/% x (cm) y (cm) dy/dp (cm/%) dx/dp (cm/%) meters

E969 beam line (2.5 % dp/p), 5.35 GeV/c pion beam, present pion decay channel quads P119 with Q7-10 fit to GeV/c FODO(pile)

cm or cm/% x (cm) y (cm) dy/dp (cm/%) dx/dp (cm/%) meters E969 beam line BAK DECAY 2X fodo p115, initial fit at 5.35 GeV/c

*QUAD* Q m kG 8.26 cm *QUAD* Q m kG cm *QUAD* Q m kG 6.35 cm *QUAD* Q m kG 6.35 cm *QUAD* Q m kG 6.35 cm *QUAD* Q m kG 6.35 cm *QUAD* Q m kG 9.52 cm *QUAD* Q m kG 9.52 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q11b m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q12b m kG 4.76 cm *QUAD* Q m kG 4.76 cm E969 beam line FWD DECAY 2X fodo p115

*QUAD* Q17b m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q18b m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q23a m kG 4.76 cm *QUAD* Q23b m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 4.76 cm *QUAD* Q m kG 9.84 cm *QUAD* Q m kG 9.84 cm E969 beam line FWD DECAY 2X fodo p115

cm or cm/% x (cm) y (cm) dy/dp (cm/%) dx/dp (cm/%) meters E969 beam line BAK DECAY 2X fodo p115, final fit for Q7-Q10, all else fixed, 5.35GeV/c front GeV/c FODO to end

cm or cm/% x (cm) y (cm) dy/dp (cm/%) dx/dp (cm/%) meters E969 beam line BAK DECAY 2X fodo p115, final fit for Q7-Q10, all else fixed, 5.35GeV/c front GeV/c FODO to end, SECOND ORDER

E969 beam line BAK DECAY 2X fodo p115, final fit for Q7-Q10, all else fixed, 5.35GeV/c front GeV/c FODO to end

E969 beam line BAK DECAY 2X fodo p115, final fit for Q7-Q10, all else fixed, 5.35GeV/c front GeV/c FODO to end

E969 beam line (2.5 % dp/p), 5.35 GeV/c pion beam, 4x FODO, p cm or cm/% x (cm) y (cm) dy/dp (cm/%) dx/dp (cm/%) meters

cm or cm/% x (cm) y (cm) dy/dp (cm/%) dx/dp (cm/%) meters E969 beam line (2.5 % dp/p), 5.35 GeV/c pion beam, 4x FODO, p119, Q7-10 FIT TO GeV/c High Field FODO

cm or cm/% x (cm) y (cm) dy/dp (cm/%) dx/dp (cm/%) meters E969 beam line (2.5 % dp/p), 5.35 GeV/c pion beam, 4x FODO, p119, Q7-10 FIT TO GeV/c High Field FODO, SECOND ORDER

E969 beam line (2.5 % dp/p), 5.35 GeV/c pion beam, 4x FODO, p119, Q7-10 FIT TO GeV/c High Field FODO

E969 beam line (2.5 % dp/p), 5.35 GeV/c pion beam, 4x FODO, p119, Q7-10 FIT TO GeV/c High Field FODO

cm or cm/% x (cm) y (cm) dy/dp (cm/%) dx/dp (cm/%) meters E969 beam line (2.5 % dp/p), 5.35 GeV/c pion beam, 4x pion decay channel quads Low Field FODO