Particle Production of Carbon Target with 20Tto2T5m Configuration at 6.75 GeV (Updated) X. Ding, UCLA Target Studies April 3, 2014 14/3/14.

Slides:



Advertisements
Similar presentations
Comparison of Particle Production between MARS and FLUKA (Update) X. Ding, UCLA Target Studies Aug. 8, /8/13.
Advertisements

SUPERCONDUCTING SOLENOIDS - SHIELDING STUDIES 1. N. Souchlas BNL (Oct. 5, 2010)
Stefan Roesler SC-RP/CERN on behalf of the CERN-SLAC RP Collaboration
IDS120j WITH/WITHOUT GAPS SH#4 AZIMUTHAL DPD DISTRIBUTION ANALYSIS Nicholas Souchlas, PBL (3/14/2012) 1.
KT McDonald Target Studies Weekly Meeting July 10, Power Deposition in Graphite Targets of Various Radii K.T. McDonald, J. Back, N. Souchlas July.
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,
ISS, 23 September 2005E. Gschwendtner, CERN1 Beam Instrumentation at CNGS 1. Introduction 2. Layout 3. Beam Instrumentation 4. Summary.
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.
Pion yield studies for proton drive beams of 2-8 GeV kinetic energy for stopped muon and low-energy muon decay experiments Sergei Striganov Fermilab Workshop.
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.
MC/NF TARGET SHIELDING STUDIES. NICHOLAS SOUCHLAS (10/29/2010)‏ 1.
Proton Position Tracking X. Ding, D. Cline UCLA H. Kirk, J. S. Berg, BNL Phone Meeting on Aug. 25, 2009.
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.
SHIELDING STUDIES FOR THE MUON COLLIDER TARGET NICHOLAS SOUCHLAS BNL Nov 30, 2010 ‏ 1.
Above: Energy deposition in the superconducting magnet and the tungsten-carbide shield inside them. Approximately 2.4 MW must be dissipated in the shield.
Chapter 23 home work.
Optimization of Target Parameters for a Tungsten Target (Half Density) at 8GeV X. Ding Target Studies Nov. 2, 2010.
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.
1 Muon Yield Comparisons for Different ICOOL Versions and Lattices X. Ding Front End, Nov. 23, 2010.
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.
Proton Position Tracking X. Ding, UCLA Aug. 11, 2009.
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.
Above: On-axis field profiles of resistive, superconducting and all magnets, and bore-tube radius r = 7.5 (B/20T) −½ cm. Above: Hoop strain ε θ in resistive.
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.
Harold G. Kirk Brookhaven National Laboratory A MW Class Target System for Muon Beam Production AAC 2014 San Jose, Ca July 14-18, 2014.
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.
KT McDonald MAP Spring Meeting May 30, Target System Concept for a Muon Collider/Neutrino Factory K.T. McDonald Princeton University (May 28, 2014)
KT McDonald MAP Winter Meeting (SLAC) December 5, Solid Target Options for an Intense Muon Source K. McDonald Princeton U. (December 5, 2014) MAP.
IDS120j WITHOUT GAPS AND WITH MAXIMUM SIZE GAPS ( aka ''NIGHTMARE'' CASE SCENARIO ) SC#4, SC#7 AZIMUTHAL DPD DISTRIBUTION ANALYSIS. Nicholas Souchlas,
IDS120h GEOMETRY WITH MODIFIED Hg POOL VESSEL. SIMULATIONS FOR 60%W+40%He SHIELDING (P12 'POINT') WITH STST SHIELDING VESSELS EFFECTS OF Be WINDOW WATER.
SHIELDING STUDIES FOR THE MUON COLLIDER TARGET. (From STUDY II to IDS120f geometries) NICHOLAS SOUCHLAS (BNL)‏ ‏ 1.
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.
IDS120j WITH GAPS SC#3 AZIMUTHAL DPD DISTRIBUTION ANALYSIS WITH MAX GAPS SC#3, SC#4 AZIMUTHAL DPD DISTRIBUTION ANALYSIS, DP AND SC TOTAL DP WITH VARYING.
IDS120h GEOMETRY WITH MODIFIED Hg POOL VESSEL. SIMULATIONS FOR 60%W+40%He SHIELDING (P12 'POINT') WITH STST SHIELDING VESSELS. BP#1(STST/W), SH#1, BeWindow,SC#8.
Particle Production at 3 GeV (update) X. Ding, UCLA Target Studies Sept. 23, /23/13.
Monte Carlo methods in ADS experiments Study for state exam 2008 Mitja Majerle “Phasotron” and “Energy Plus Transmutation” setups (schematic drawings)
Beam MC activity A.K.Ichikawa for beam group For more details,
FRONTEND DESIGN & OPTIMIZATION STUDIES HISHAM KAMAL SAYED BROOKHAVEN NATIONAL LABORATORY June 26, 2014 Collaboration: J. S. Berg - X. Ding - V.B. Graves.
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,
Studies on pion/muon capture at MOMENT Nikos Vassilopoulos IHEP, CAS August 11, 2015.
RF source, volume and caesiated extraction simulations (e-dump)
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.
Meson Production at Low Proton Beam Energy (Update) X. Ding, UCLA Target Studies May 9, /9/113.
IDS120i GEOMETRY. SIMULATIONS FOR 60%W+40%He SHIELDING WITH STST SHIELDING VESSELS. Hg vs. Ga DEPOSITED POWER DISTRIBUTION. (using Ding's optimized parameters)
Optimized Target Parameters and Meson Production by IDS120h with Focused Gaussian Beam and Fixed Emittance (Update) X. Ding, UCLA AAG June 27, /27/12.
KT McDonald MAP Spring Meeting May 30, Target System Concept for a Muon Collider/Neutrino Factory K.T. McDonald Princeton University (May 28, 2014)
X. Ding, UCLA MAP Spring 2014 Meeting May 2014 Fermilab
Report to Delta Review: Hadronic Validation
Meson Production Efficiencies
Update on Data Analysis
Antoine Cazes Université Claude Bernard Lyon-I December 16th, 2008
Hit density at scoring planes at r=10, 30, and 50 cm.
Low Energy Electron-Ion Collision
JLEIC Reaching 140 GeV CM Energy: Concept and Luminosity Estimate
MEIC Alternative Design Part III
Presentation transcript:

Particle Production of Carbon Target with 20Tto2T5m Configuration at 6.75 GeV (Updated) X. Ding, UCLA Target Studies April 3, /3/14

Target Setting 20Tto2T5m Configuration (initial beam pipe radius of 13 cm) and Fieldmap (20T  2T); Code: MARS15(2014) with ICEM 4 = 1; Proton beam: 6.75 GeV (KE) and launched at z = -100 cm, Focal beam with waist at z= 0 m and emittance of 5 μm; Production Collection: (50 m downstream, 40 MeV < KE < 180 MeV). Graphite density = 1.8 4/3/142

Configuration 4/3/143

Energy Card Setting ENRG E0 EM EPSTAM EMCHR EMNEU EMIGA EMIEL E0: The incident particle kinetic energy; EM: The hadron threshold energy (Default: GeV); EPSTAM: The star production threshold kinetic energy (Default:0.03 GeV); EMCHR: The threshold energy applied collectively to muons, heavy ions and charged hadrons (Default: GeV); EMNEU: The threshold energy for neutrons (Default:10 -4 GeV) EMIGA: The threshold energy for γ (Default:10 -4 GeV); EMIEL: The threshold energy for e ± (Default: 5*10 -4 GeV) Use non-default setting: ENRG 1=6.75 2=0.02 3=0.3 4=0.01 5=0.05 6=0.01 7=0.01 4/3/144

Particle Production vs. Target Length (10 6 events, no beam dump) 4/3/145 Target radius: 0.80 cm Beam angle to SC axis: 65 mrad Co-linear target and beam TR/BR=4

Particle Production vs. Target Radius (10 6 events, no beam dump) 4/3/146 Target length: 80 cm Beam angle to SC axis: 65 mrad Co-linear target and beam TR/BR=4

Particle Production vs. Beam Angle (10 6 events, no beam dump) 4/3/147 Target length: 80 cm Target radius: 0.80 cm Co-linear target and beam TR/BR=4

Energy Spectra of  , K ,   (10 6 events, no beam dump) 4/3/148 Best parameters: Target length: 80 cm Target radius: 0.80 cm Beam angle: 65 mrad Co-linear target and beam TR/BR=4

Remaining Protons (10 6 events, no beam dump) 4/3/149 Target length: 80 cm Target radius: 0.80 cm Beam angle: 65 mrad Co-linear target and beam TR/BR=4 Peak of protons(?) at 6.5 GeV gone at z = 16, 50 m. If true, no need for beam dump.

Remaining Protons with Beam Dump (10 6 events) 4/3/1410 Target length: 80 cm (z=-40 cm to z=40 cm) Target radius: 0.80 cm Beam angle: 65 mrad Co-linear target and beam TR/BR=4 Beam dump rod: (z=40 cm to z=160 cm, horizontal tilt: 33.7 mrad, vertical tilt: mrad) The radius of beam dump is same that of the target

Remaining Protons with Beam Dump (10 6 events) 4/3/1411 Target length: 80 cm (z=-40 cm to z=40 cm) Target radius: 0.80 cm Beam angle: 65 mrad Co-linear target and beam TR/BR=4 Beam dump rod (z=40 cm to z=160 cm, horizontal tilt: 33.7 mrad, vertical tilt: mrad) The radius of beam dump is twice that of the target

Remaining Protons with Beam Dump (10 6 events) 4/3/1412 Target length: 80 cm (z=-40 cm to z=40 cm) Target radius: 0.80 cm Beam angle: 65 mrad Co-linear target and beam TR/BR=4 Beam dump rod (z=40 cm to z=160 cm, horizontal tilt: 33.7 mrad, vertical tilt: mrad) The radius of beam dump is triple that of the target

Yield Comparison (no-tilt vs. tilt of proton beam to SC axis) 4/3/1413 Optimized target length is 80 cm and target radius is 0.64 cm when beam angle is fixed at 0 mrad. Co-linear target and beam. TR/BR=4 ~ 13% advantage to tilting the beam/target

Remaining Protons (KE > 0) 10 4 events, no beam dump, beam angle = 0 mrad 4/3/1414 z = 0.4 m z = 1.6 m

Remaining Protons (KE > 0) 10 4 events, no beam dump, beam angle = 0 mrad 4/3/1415 z = 5 m z = 50 m

Remaining Protons (KE > 6 GeV) 10 4 events, Beam angle = 0 mrad, target radius = 0.64 cm 4/3/1416 No beam dump Beam dump: 120cm long (z=40 to 160 cm), Triple of target radius z = 5 m

Remaining Protons with Beam Dump (10 6 events, Beam angle = 0 mrad) 4/3/1417 Target length: 80 cm (z=-40 cm to z=40 cm) Target radius: 0.64 cm Beam angle: 0 mrad Co-linear target and beam TR/BR=4 Beam dump rod is 120 cm long (z=40 cm to z=160 cm) The radius of beam dump is triple that of the target ? This plot shows a peak at GeV for z = 16, 50 m ??

Counting 10 4 events, 1MW beam, beam angle = 0 mrad L dump (cm) R dump / R target ZTotal KE (protons) ( r <23 cm) GeV Total KE (non-protons) GeV Protons KE>6 Protons KE>4.5 Yield at Z=50m 005m m m m m m m m m m /3/1418