Optimization of Target Parameters for a Tungsten Target (Half Density) at 8GeV X. Ding Target Studies Nov. 2, 2010.

Slides:



Advertisements
Similar presentations
DPA and Gas Production from Protons on W and Be Brian Hartsell.
Advertisements

Comparison of Particle Production between MARS and FLUKA (Update) X. Ding, UCLA Target Studies Aug. 8, /8/13.
Proposal for a new design of LumiCal R. Ingbir, P. Ruzicka, V. Vrba October 07 Malá Skála.
Simulation of Neutrino Factory beam and quasielastic scattering off electrons in the near detector Yordan Karadzhov University of Sofia “St. Kliment Ohridski”
UCLA Experiments with short single e-bunch using preformed and beam ionized plasma Retain ability to run short single bunch with pre-ionized plasma Ken.
Magnetic Configuration of the Muon Collider/ Neutrino Factory Target System Hisham Kamal Sayed, *1 H.G Kirk, 1 K.T. McDonald 2 1 Brookhaven National Laboratory,
6/30/20091 Meson Production with Different Directional Incident Proton Beam X. Ding, D. Cline, UCLA H. Kirk, J. S. Berg, BNL.
Meson Production at 8 GeV for IDS120h X. Ding, UCLA Target Studies, Dec. 27, 2011.
Meson Production Comparison between Hg and Ga at 8 GeV X. Ding, UCLA Target Studies, Oct. 04, 2011.
Meson Production Comparison between HG and GA at 8 GeV (Update) X. Ding, UCLA Target Studies, Oct. 18, 2011.
Particle Production of a Carbon/Mercury Target System for the Intensity Frontier X. Ding, UCLA H.G. Kirk, BNL K.T. McDonald, Princeton Univ MAP Spring.
Operated by Brookhaven Science Associates for the U.S. Department of Energy A Pion Production and Capture System for a 4 MW Target Station X. Ding, D.
Pion capture and transport system for PRISM M. Yoshida Osaka Univ. 2005/8/28 NuFACT06 at UCI.
Energy Deposition of 4-MW Beam Power in a Mercury Jet Target Xiaoping Ding UCLA Target Studies Meeting, Feb. 9, 2010.
1 Optical Diagnostic Results of Hg Jet Target and Post-Simulation H. Park, H. Kirk, K. McDonald Brookhaven National Laboratory Princeton University Stonybrook.
Proton Position Tracking X. Ding, D. Cline UCLA H. Kirk, J. S. Berg, BNL Phone Meeting on Aug. 25, 2009.
MERIT Beam Collimator Design Nicholas Olesen 9 August 2006.
Harold G. Kirk Brookhaven National Laboratory Meson Production Efficiencies IDS Target Meeting CERN December 17, 2008.
1 Meson Production Simulations X. Ding, D. B. Cline UCLA H. Kirk, J. S. Berg BNL N u F a c t th International Workshop on Neutrino Factories, Superbeams.
3D Target Simulations with Front Tracking/Ghost Fluid Method Wurigen Bo (Sept. 9, 2009) Brookhaven National Lab.
Above: Energy deposition in the superconducting magnet and the tungsten-carbide shield inside them. Approximately 2.4 MW must be dissipated in the shield.
Energy Deposition of 4MW Beam Power in a Mercury Jet Target Xiaoping Ding UCLA Target Studies Mar. 9, 2010 (Update of talk on Feb. 9, 2010)
Harold G. Kirk Brookhaven National Laboratory Target System Update IDS-NF Plenary Meeting Arlington, VA October 18, 2011.
Harold G. Kirk Brookhaven National Laboratory Target Baseline IDS-NF Plenary CERN March 23-24, 2009.
IDS-NF Target Studies H. Kirk (BNL) July 8, 2009.
1 Comparison of Power Depositions X. Ding, D. B. Cline, UCLA H. Kirk, J. S. Berg, BNL Collaboration Meeting July 2, 2010.
The Heavy Ion Fusion Virtual National Laboratory Comparison of final focus magnetic systems for the Assisted Pinched Transport and the RPD-2002 J. Barnard,
Comparison of Power Deposition in SC1 Coil Xiaoping Ding UCLA Target Studies Jun. 29, 2010.
Power Deposition in SC1 Coil Xiaoping Ding UCLA Target Studies Apr. 20, 2010.
Harold G. Kirk Brookhaven National Laboratory Meson Production Calculations 1 st Princeton/Oxford High-Power Targets Workshop Oxford May 1-2, 2008.
Operated by Brookhaven Science Associates for the U.S. Department of Energy Optimized Parameters for a Mercury Jet Target X. Ding, D. Cline, UCLA, Los.
Wayne R. Meier Lawrence Livermore National Lab Heavy Ion Driver Model Update* ARIES IFE Meeting LLNL March 8-9, 2001 * This work was performed under the.
Finding the Density of an Aluminium Block
Meson Productions for Target System with GA/HG Jet and IDS120h Configuration X. Ding (Presenter), D. Cline, UCLA H. Kirk, J.S. Berg, BNL Muon Accelerator.
Angular resolution study of isolated gamma with GLD detector simulation 2007/Feb/ ACFA ILC Workshop M1 ICEPP, Tokyo Hitoshi HANO collaborated with Acfa-Sim-J.
Shifting the Position of Focal Point of Proton Beam Relative to Intersection Point with Fixed Emittance for IDS120h Configuration X. Ding, UCLA Target.
Harold G. Kirk Brookhaven National Laboratory Target Considerations for Nufact and Superbeams ISS Meeting RAL April 26, 2006.
1 Energy Deposition of 4MW Beam Power in a Mercury Jet Target X. Ding, D. B. Cline UCLA H. Kirk, J. S. Berg BNL The International Design Study for the.
Particle Production at 3 GeV (update) X. Ding, UCLA Target Studies Sept. 23, /23/13.
Honors Geometry. Find the angle formed by the hands of a clock at 11:20. A. 160 B. 120 C. 140 D. 90
Proton Delivery to Target Keith Gollwitzer Accelerator Division Fermilab MAP 2012 Winter Meeting March 7, 2012.
FRONTEND DESIGN & OPTIMIZATION STUDIES HISHAM KAMAL SAYED BROOKHAVEN NATIONAL LABORATORY June 26, 2014 Collaboration: J. S. Berg - X. Ding - V.B. Graves.
LITHIUM LENS FOR EFFECTIVE CAPTURE OF POSITRONS Alexander Mikhailichenko Cornell University, LEPP, Ithaca, NY Positron Source Meeting, Jan30-Feb2.
Gallium as a Possible Target Material for a Muon Collider or Neutrino Factory X. Ding, D. Cline, UCLA, Los Angeles, CA 90095, USA J.S. Berg, H.G. Kirk,
Math 9 Unit 4 – Circle Geometry. Activity 3 – Chords Chord – a line segment that joints 2 points on a circle. A diameter of a circle is a chord through.
Studies on pion/muon capture at MOMENT Nikos Vassilopoulos IHEP, CAS August 11, 2015.
Particle Production of Carbon Target with 20Tto2T5m Configuration at 6.75 GeV (Updated) X. Ding, UCLA Target Studies April 3, /3/14.
Beam Dump for Carbon Target with IDS120h Configuration at 6.75 GeV (Updated) X. Ding, UCLA Target Studies Jan. 24, /24/14.
Particle Production with Carbon Target and IDS120j Configuration at 3 GeV (update) X. Ding, UCLA Target Studies Nov. 14, /14/13.
Kinetic Energy Spectra of pi +, pi -, mu +, mu - and sum of all from the 20to4T5m Configuration X. Ding Front End Meeting June 23,
Meson Production of Carbon Target at 3 GeV X. Ding, UCLA Target Studies 17/18/13.
Carbon Target Design and Optimization for an Intense Muon Source X. Ding, UCLA H.G. Kirk, BNL K.T. McDonald, Princeton Univ MAP Winter Collaboration.
Circles Shape and Space. Formula for the area of a circle We can find the area of a circle using the formula radius Area of a circle = πr 2 Area of a.
04/06/07I.Larin pi0 systematic error 1  0 error budget Completed items (review) Updated and new items (not reported yet) Items to be completed.
Tungsten-Silicon Luminosity Detector with Flat Geometry Ronen Ingbir Tel Aviv University High Energy Physics Experimental Group.
TESLA DAMPING RING RF DEFLECTORS DESIGN F.Marcellini & D. Alesini.
Meson Production at Low Proton Beam Energy (Update) X. Ding, UCLA Target Studies May 9, /9/113.
Optimized Target Parameters and Meson Production by IDS120h with Focused Gaussian Beam and Fixed Emittance (Update) X. Ding, UCLA AAG June 27, /27/12.
11.4 Circumference and Arc length. Concept #1 Circumference H B X M.
Harold G. Kirk Brookhaven National Laboratory Muon Production and Capture for a Neutrino Factory European Strategy for Future Neutrino Physics CERN October.
10 mm is the same as... 1 cm. 20 mm is the same as... 2 cm.
Positron production rate vs incident electron beam energy for a tungsten target
Preliminary result of FCC positron source simulation Pavel MARTYSHKIN
X. Ding, UCLA MAP Spring 2014 Meeting May 2014 Fermilab

Meson Production Efficiencies
GLD IR optimization and background study
Feasibility of Reusing PEP-II Hardware for MEIC Electron Ring
Feasibility of Recuperation of Magnets in Decommissioned Storage Rings
Option 1: Reduced FF Quad Apertures
Presentation transcript:

Optimization of Target Parameters for a Tungsten Target (Half Density) at 8GeV X. Ding Target Studies Nov. 2, 2010

Tungsten Geometry 5 mm of target radius and 1.5 mm beam 50mrad of beam and tungsten to sol. axis 50cm long of tungsten in sol. axis

Meson Productions at 8GeV Target50% W (9.65 g/cm 3 ) w/t optimization Hg (13.54 g/cm 3 ) with optimization Meson27220 (pos: neg: 14018) (pos: neg: 15206)

Vary Target Radius Peak production efficiency at r= cm Efficiency reduction at r=1cm is 22% Fit: peak at 0.47cm

Vary Target Angle Target radius is 0.47 cm Fit: peak at 80 mrad

Vary Target Length Target radius is 0.47 cm and target angle is 80 mrad Fit: peak at 43.5 cm

Meson Productions at 8GeV Target50% W (9.65 g/cm 3 ) with optimization* Hg (13.54 g/cm 3 ) with optimization Meson29069 (pos: neg: 14970) (pos: neg: 15206) * Target radius: 0.47 cm, target angle: 80mrad, target length: 45cm

Backup

Raw Data (Vary Target Radius) e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e+02

Raw Data (Vary Target Angle) e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e e+02

Raw Data (Vary Target Length) e e e e e e e e e e e e e e e e e e e e+02