Beam MC activity A.K.Ichikawa for beam group For more details,

Slides:



Advertisements
Similar presentations
CBM Calorimeter System CBM collaboration meeting, October 2008 I.Korolko(ITEP, Moscow)
Advertisements

Proposal for a new design of LumiCal R. Ingbir, P. Ruzicka, V. Vrba October 07 Malá Skála.
Beam direction and flux measured by MUMON K. Matsuoka (Kyoto) for the MUMON group Contents: 1.Beam stability (direction/flux) 2.Absolute  beam flux.
HARP Anselmo Cervera Villanueva University of Geneva (Switzerland) K2K Neutrino CH Meeting Neuchâtel, June 21-22, 2004.
Anne Dabrowski Northwestern University Collaboration Meeting 22 nd February 2005 Update Kmu3 Branching Ratio measurement A. Dabrowski, February
ISS, 23 September 2005E. Gschwendtner, CERN1 Beam Instrumentation at CNGS 1. Introduction 2. Layout 3. Beam Instrumentation 4. Summary.
Hall D Photon Beam Simulation and Rates Part 1: photon beam line Part 2: tagger Richard Jones, University of Connecticut Hall D Beam Line and Tagger Review.
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 capture and transport system for PRISM M. Yoshida Osaka Univ. 2005/8/28 NuFACT06 at UCI.
2015/6/23 1 How to Extrapolate a Neutrino Spectrum to a Far Detector Alfons Weber (Oxford/RAL) NF International Scoping Study, RAL 27 th April 2006.
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.
Study of two pion channel from photoproduction on the deuteron Lewis Graham Proposal Phys 745 Class May 6, 2009.
Status & Plans of Segmentation Y.P.Viyogi(V.E.C.C) Arun Prakash(B.H.U)
Photon reconstruction and calorimeter software Mikhail Prokudin.
1 Induced radioactivity in the target station and in the decay tunnel from a 4 MW proton beam S.Agosteo (1), M.Magistris (1,2), Th.Otto (2), M.Silari (2)
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.
HLab meeting 10/14/08 K. Shirotori. Contents SksMinus status –SKS magnet trouble –Magnetic field study.
 A GEANT4-based simulation was performed of the production target, solenoid, selection channel, and spectrometer.  The acceptance was found to be 8.3x10.
Results from Step I of MICE D Adey 2013 International Workshop on Neutrino Factories, Super-beams and Beta- beams Working Group 3 – Accelerator Topics.
Shifting the Position of Focal Point of Proton Beam Relative to Intersection Point with Fixed Emittance for IDS120h Configuration X. Ding, UCLA Target.
Secondary Particle Production and Capture for Muon Accelerator Applications S.J. Brooks, RAL, Oxfordshire, UK Abstract Intense pulsed.
N. Saoulidou Fermilab 1 Status & Update of track reconstruction in the Near Detector N. Saoulidou, Fermilab
Anne Dabrowski 26 February Semileptonic Analysis from Low Intensity Run Anne Dabrowski Northwestern University NA48 Collaboration Meeting 26 February.
J. Pasternak First Ideas on the Design of the Beam Transport and the Final Focus for the NF Target J. Pasternak, Imperial College London / RAL STFC ,
S. Kahn 5 June 2003NuFact03 Tetra Cooling RingPage 1 Tetra Cooling Ring Steve Kahn For V. Balbekov, R. Fernow, S. Kahn, R. Raja, Z. Usubov.
Mass production (Super-K) Setup of jnubeam – 3 horn 250 kA – 30-GeV proton beam of Gaussian distribution (  x,y = cm) – On center, parallel beam.
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,
First Look at Data and MC Comparisons for Cedar and Birch ● Comparisons of physics quantities for CC events with permutations of Cedar, Birch, Data and.
Studies on pion/muon capture at MOMENT Nikos Vassilopoulos IHEP, CAS August 11, 2015.
Photon reconstruction and matching Prokudin Mikhail.
Beam MC progresses for beam MC sub-group. Summary of update in 09b,c,10a 09b Geometry of baffle, target, 1st horn, dump and MUMON is updated. 09c MUMON.
Interaction Length A. Murakami. L = (interaction length of proton in carbon by PDG) change of constant : means uncertainty of L (change 0.8, 0.9,
7 November 2003 Status of CNGS NBI presented by K. Elsener 1 Status of CNGS Konrad Elsener CERN – Accelerators+Beams Division.
Particle Production of Carbon Target with 20Tto2T5m Configuration at 6.75 GeV (Updated) X. Ding, UCLA Target Studies April 3, /3/14.
Bartol Flux Calculation presented by Giles Barr, Oxford ICRR-Kashiwa December 2004.
Muon absolute flux measurement in anti-neutrino mode A.Ariga 1, C. Pistillo 1, S. Aoki 2 1 University of Bern, 2 Kobe University.
Beam Dump for Carbon Target with IDS120h Configuration at 6.75 GeV (Updated) X. Ding, UCLA Target Studies Jan. 24, /24/14.
Beam Extrapolation Fit Peter Litchfield  An update on the method I described at the September meeting  Objective;  To fit all data, nc and cc combined,
Muon detection in NA60  Experiment setup and operation principle  Coping with background R.Shahoyan, IST (Lisbon)
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.
Neutron measurement with nuclear emulsion Mitsu KIMURA 27th Feb 2013.
1 Constraining ME Flux Using ν + e Elastic Scattering Wenting Tan Hampton University Jaewon Park University of Rochester.
T2K muon measurement 2014 Momentum module A.Ariga, C. Pistillo University of Bern S. Aoki Kobe University 1.
Proposal for the study to define what is really necessary and what is not when the data from beam, ND and SK are combined A.K.Ichikawa 2008/1/17.
Status of E14 G.Y.Lim IPNS, KEK. E14 Experiment Step-by-step approach to precise measurement of Br( K L    ) KEK-PS E391a J-PARC E14 (Step-1) J-PARC.
IDS120j WITH AND WITHOUT RESISTIVE MAGNETS PION AND MUON STUDIES WITHIN TAPER REGION, III ( 20 cm GAPS BETWEEN CRYOSTATS ) Nicholas Souchlas, PBL (9/4/2012)
1 S, Fedele, Student Presentations, 2004/08/04S Amazing Title Slide Reworking the CES Cluster Reconstruction Algorithm By: Steve Fedele Advisor: Pavel.
Neutrino Beam MC We propose to adopt ‘jnubeam’ as the official T2K code for flux calculation. –It is well established and almost ready for flux calculation.
Meson Production at Low Proton Beam Energy (Update) X. Ding, UCLA Target Studies May 9, /9/113.
NUMI NUMI/MINOS Status J. Musser for the MINOS Collatoration 2002 FNAL Users Meeting.
Horns, Hadron production etc. (from hadron production to neutrino beam) A.K.Ichikawa KEK 200/9/26 Study on horns Changing -beam energy Hadron.
Beam direction and flux measured by MUMON K. Matsuoka (Kyoto) for the MUMON group Contents: 1.Horn focusing effect 2.Beam stability (direction/flux) 3.Beam.
2005/07/12 (Tue)8th ACFA Full simulator study of muon detector and calorimeter 8th ACFA Workshop at Daegu, Korea 2005/07/12 (Tue) Hiroaki.
A New Upper Limit for the Tau-Neutrino Magnetic Moment Reinhard Schwienhorst      ee ee
Extrapolation Techniques  Four different techniques have been used to extrapolate near detector data to the far detector to predict the neutrino energy.
FCAL Krakow meeting, 6. May LumiCal concept including the tracker R. Ingbir, P.Růžička, V. Vrba.
Optimized Target Parameters and Meson Production by IDS120h with Focused Gaussian Beam and Fixed Emittance (Update) X. Ding, UCLA AAG June 27, /27/12.
N_TOF EAR-1 Simulations The “γ-flash” A. Tsinganis (CERN/NTUA), C. Guerrero (CERN), V. Vlachoudis (CERN) n_TOF Annual Collaboration Meeting Lisbon, December.
Characterization of muon beam in T2K with emulsion detectors A. Ariga, T. Ariga, C. Pistillo AEC-LHEP University of Bern 1.
The MiniBooNE Little Muon Counter Detector
J. Musser for the MINOS Collatoration 2002 FNAL Users Meeting
X. Ding, UCLA MAP Spring 2014 Meeting May 2014 Fermilab
Global PID MICE CM43 29/10/15 Celeste Pidcott University of Warwick
Pure  exposure for e/ separation
MUMON / emulsion total flux uncertainty
Special Considerations for SIDIS
GEANT Simulations and Track Reconstruction
Geant4 in HARP V.Ivanchenko For the HARP Collaboration
Contents First section: pion and proton misidentification probabilities as Loose or Tight Muons. Measurements using Jet-triggered data (from run).
Antoine Cazes Université Claude Bernard Lyon-I December 16th, 2008
Presentation transcript:

Beam MC activity A.K.Ichikawa for beam group For more details,

Summary of update in 09a,b,c 09a – This is almost equivalent to 07a except some bugs were fixed. Those bugs would not influence the neutrino flux iteslef. 09b – Mainly, geometry of baffle, target, 1st horn, dump and MUMON is updated. 09c – MUMON structures were included. – Energy deposit in the MUMON detector can be stored. – Emittance and Twiss parameters can be specified via card. – Neutrino tracking is discarded. – The density of the dump concrete was changed from 2.2 to 2.3g/cm3.

Comparison among different versions K. Matsuoka

MUMON A few bugs introduced in 2009 were found and fixed. Mainly in horn1. Magnetic field (proportional to 1/r) starts from r=2.7cm – Horn1 inner conductor Inner radius = 2.7cm, outer radius=3cm – Originally it starts from 3cm – Actually, something between them (skin depth > 5mm) – For MUMON, a few% effect K. Matsuoka

Muon flux at muon pit Spring commissioning (1 st horn only) Emulsion v.s. MC A.Ariga et. al. 273kA Data/MC= kA Data/MC=0.75 0kA Data/MC=0.57

horn2 and horn3 Geometry update update from conceptual shape to real shape Horn2 – outer conductor radius : 40 cm -> cm – B-field region (Z-length) : 200 cm ->195.7 cm Horn3 – outer conductor radius : 70 cm  65.5 cm – B-field region (Z-length) : 250 cm  cm H.Kubo Muon decreased by 3%, profile shape is same

Horn2&3 geometry update neutrino flux 09b new Far/Near less than 5% difference upto 5GeV

Parents of muons in muon pit -pions- H.Kubo. K.Matsuoka Horn off 1 st Horn 273kA All horns 320kA

Proton information Store primary beam information in a common block and MUMON or neutrino ntuple. – libneubeam/beaminfo.inc integer gipart : Primary generated particle ID real gpos0(3) : Generation point – common /gbeam/gipart, gpos0 Accumulate POT w/ a flat proton beam. Weight the muon profile w/ an arbitrary proton profile by using gpos0. We do not need to make many MC data sets of various proton beam profile. K. Matsuoka

new ND flux calculation algorithm current filling routine – SK : treated as a “point”. generated neutrino is always filled acceptance of SK for each decay is included in “norm”. – ND : repeat parent’s decay randomly (uniformly in CM) by N times (default 1,000). only neutrinos which have proper angle are filled. New method : fill ND ntuple just the same method as one of SK. 1.choose a detection point (x, y) randomly in the ND plane 2.calculate weight (acceptance) for this direction using parent 4-momentum  same method with SK ntuple. Motivation – In the current version, high-energy pions are multiply used. Events are not independent. Simple error couting results in underestimate. Status – Coding is almost done. Under check. H.Kubo

Remaining issues towards Dec.(Jan.) mass production Received requests from ND280 beam group Received a request from Hiro – To check new ND280 algorithm, want flux in both old and new algorithm Need to be done – final(?) check of new ND algorithm – final(?) check of mag. field inside conductor – correct ND280 position – Optimization of proton beam area two flat area? – check of Nicolas commitment and decide which should be stored for mass production version – Random seed control?