VELO detector and available aperture in IR8

Slides:



Advertisements
Similar presentations
1 Accelerator Physics Aspects LHCb Accelerator Physics Aspects LHCb CERN SL/AP n Layout n Crossing Scheme n Luminosity n Collision.
Advertisements

Spectrometer compensation in IR2 and IR8 during the 450 GeV collision run September 11, 2006 LOC meeting Y. Papaphilippou Thanks to S. Fartoukh, W. Herr,
VELO Testbeam 2006 Tracking and Triggering Jianchun (JC) Wang Syracuse University VELO Testbeam and Software Review 09/05/2005 List of tasks 1)L0 trigger.
Patrick Robbe, LAL Orsay, for the LHCb Collaboration, 16 December 2014
2 February 2005Ken Moffeit Spin Rotation scheme for two IRs Ken Moffeit SLAC.
T. Horn, SHMS Optics Update SHMS Optics Update Tanja Horn Hall C Users Meeting 31 January 2009.
* IP5 IP1 IP2 IP8 vertical crossing angle at IP8 R. Bruce, W. Herr, B. Holzer Acknowledgement: S. Fartoukh, M. Giovannozzi, S. Redaelli, J. Wenninger.
GRD - Collimation Simulation with SIXTRACK - MIB WG - October 2005 LHC COLLIMATION SYSTEM STUDIES USING SIXTRACK Ralph Assmann, Stefano Redaelli, Guillaume.
The HiLumi LHC Design Study is included in the High Luminosity LHC project and is partly funded by the European Commission within the Framework Programme.
New ALICE Beam Pipe: Injection Protection C. Bracco on Behalf of ABT/BTP Acknowledgment: M. Giovannozzi.
The HiLumi LHC Design Study is included in the High Luminosity LHC project and is partly funded by the European Commission within the Framework Programme.
Bernhard Holzer, CERN-LHC Parameter Space for HL-LHC IR8 * IP5 IP1 IP2 IP8 LEB Meeting.
October 4-5, Electron Lens Beam Physics Overview Yun Luo for RHIC e-lens team October 4-5, 2010 Electron Lens.
Background Simulations for the LHCb Beam Condition Monitor Overview: ● The LHCb Beam Condition Monitor (BCM) – Purpose, Design and Function – Implementation.
With a lot of help from Reine Versteegen, John Jowett, Richard Jacobson, Burkhard Schmidt, Gilda Scioli, Werner Herr CERN-LHC * IP5 IP1 IP8 Spectrometer.
ILC luminosity optimization in the presence of the detector solenoid and anti-DID Reine Versteegen PhD Student CEA Saclay, Irfu/SACM International Workshop.
Simulation on beam loss from radiative Bhabha process Y. Funakoshi KEK.
Inputs from GG6 to decisions 2,7,8,15,21,27,34 V.Telnov Aug.24, 2005, Snowmass.
Orbit related issues of the spin tune control at RHIC V.Ptitsyn, M.Bai, W.MacKay, T.Roser.
Status VELO alignment 1.Alignment at IP8 Jo van den Brand Frans Mul June 2, 2006.
MEIC Detector and IR Integration Vasiliy Morozov, Charles Hyde, Pawel Nadel-Turonski MEIC Detector and IR Design Mini-Workshop, October 31, 2011.
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,
Detector / Interaction Region Integration Vasiliy Morozov, Charles Hyde, Pawel Nadel-Turonski Joint CASA/Accelerator and Nuclear Physics MEIC/ELIC Meeting.
Francesco Cerutti ENERGY DEPOSITION ASPECTS FOR LHCb REQUEST 5th Joint HiLumi LHC - LARP Annual Meeting Oct 29, 2015 through L.S. Esposito’s work and essential.
Overview of Wire Compensation for the LHC Jean-Pierre Koutchouk CARE-HHH Meeting on beam-beam effects and beam-beam compensation CERN 08/28/2008.
Backgrounds at FP420 Henri Kowalski DESY 18 th of May 2006.
Present MEIC IR Design Status Vasiliy Morozov, Yaroslav Derbenev MEIC Detector and IR Design Mini-Workshop, October 31, 2011.
Compensation of Detector Solenoid G.H. Wei, V.S. Morozov, Fanglei Lin JLEIC Collaboration Meeting Spring, 2016.
Crossing Schemes Considerations and Beam-Beam Work plan T. Pieloni, J. Barranco, X. Buffat, W. Herr.
Plan for 500 GeV Development Vadim, Mei. Goals 1.Explore polarization transmission to the 500 Gev CM energy. 2. Inspect the luminosity aspects (with 2.
First collisions in LHC
y x Vincenzo Monaco, University of Torino HERA-LHC workshop 18/1/2005
C. Bracco, R. Bruce, B. Goddard, C. Wiesner, A. Lechner, M. Frankl
Operating IP8 at high luminosity in the HL-LHC era
Developing Radiation Hard Silicon for the Vertex Locator
M. Sullivan for the SLAC SuperB Workshop Jan , 2009
D0 and its integrability
The Interaction Region
Status on Work for Splitter FS and Dilution System FS
Large Booster and Collider Ring
Spectrometer Operation in IP2 & 8
Β*-reach in 2017 R. Bruce, S. Redaelli, R. De Maria, M. Giovannozzi, A. Mereghetti, D. Mirarchi Acknowledgement: collimation and optics teams, BE/ABP,
The LHC collider in Geneva
Collision bump amplitudes for the 450 GeV run
CNGS Proton beam line: news since NBI2002 OUTLINE 1. Overview
Interaction Region Design Options e+e- Factories Workshop
Global aperture measurements at 450 GeV with 170 mrad crossing angle
Luminometer Integration at IR2
Collision bump amplitudes for the 450 GeV run
HL-LHC operations with LHCb at high luminosity
Hall C Users Meeting 31 January 2009
The LHCb Level 1 trigger LHC Symposium, October 27, 2001
Thanks to S. Fartoukh, W. Herr, B. Jeanneret, M. Giovannozzi
Optics Measurements in the PSB
IR Lattice with Detector Solenoid
The LHCb VErtex LOcator
Progress in IR8 matching for b* squeeze
Triplet corrector layout and strength specifications
Yuri Nosochkov Yunhai Cai, Fanglei Lin, Vasiliy Morozov
JLEIC High-Energy Ion IR Design: Options and Performance
Fanglei Lin, Yuhong Zhang JLEIC R&D Meeting, March 10, 2016
Status and plans for crab crossing studies at JLEIC
Alternative Ion Injector Design
Compensation of Detector Solenoids
Integration of Detector Solenoid into the JLEIC ion collider ring
Upgrade on Compensation of Detector Solenoid effects
Fanglei Lin JLEIC R&D Meeting, August 4, 2016
Large emittance scenario for the Phase II Upgrade of the LHC
First results from the LHCb Vertex Locator
Saturday 29th October Friday during IP2 1 m squeeze test
Presentation transcript:

VELO detector and available aperture in IR8 LOC Meeting VELO detector and available aperture in IR8 Y. Papaphilippou Thanks to M. Giovannozzi, W. Herr and B. Jeanneret October 23rd, 2006

LOC Meeting, Y. Papaphilippou Internal crossing bump of IR8 with collision strength for the spectrometer dipole Internal crossing angle of ±2100μrad in the horizontal plane! Deflection of ±0.010m at MBXWH, corresponding to 29σ, as compared to 0.0006m (2σ) of the nominal bump 23/10/2006 LOC Meeting, Y. Papaphilippou

Aperture in IR8 with full spectrometer dipole strength BEAM 1 MBXWS MBXWH IP8 MBLW When crossing angle is added beam excursion of 0.011m (33σ) at MBXWH, as compared to 0.0004m (6σ) for the nominal scheme When polarity and external crossing angle sign are mismatched, two additional crossings occur ~15m left and right of the IP (in total 4 crossings) Biggest loss in aperture around MBXWH n1 correspond to even smaller values than MBWXS in mm [m] 23/10/2006 LOC Meeting, Y. Papaphilippou

Aperture loss in IR8 by element Equipment n1 nominal [σ] n1 full [σ] n1 nominal [m] n1 full [m] n1 nominal [%] n1 full [%] BPMSW.1L8 20 0.014 45 MBXWS.1L8 16 0.010 40 MBXWH.1L8 34 19 0.012 0.006 24 IP8 56 0.016 0.015 52 MBLW.1R8 111 95 0.037 0.031 58 50 MBXWS.1R8 BPMSW.1R8 Not important impact in any element apart MBXWH Available aperture of 6mm (with respect to 12mm), corresponding to 15σ of aperture loss Remaining aperture corresponds 24% of the available 23/10/2006 LOC Meeting, Y. Papaphilippou

LOC Meeting, Y. Papaphilippou VErtex Locator in LHCb Used for precise localization of track coordinates close to the interaction region in order to reconstruct production and decay vertices of b-hadrons Surrounding IP8 (from ~0.35m left to 0.75m right) Series of retractable silicon sensors closing down to an aperture of 5mm radius Sensor boxes can be centered around the beam by moving laterally (by 30mm) and up or down (by 5mm) M. Ferro-Luzzi, PH/LBD Ability to locate precisely the beam position from beam gas events The experiment is interested in closing the VELO to its minimum during the 450 GeV collisions’ run, for calibration purposes 23/10/2006 LOC Meeting, Y. Papaphilippou

Simple considerations regarding aperture β-function at the right side of the VELO is 10.07m at injection Beam size in this location is 0.28mm VELO minimum aperture of 5mm corresponds to 17.8σ 7σ corresponds to 2mm For nominal crossing angle of ±135μrad, the horizontal displacement at the right edge of the VELO is 0.1mm (0.4σ) For extreme crossing angle of ±2.1mrad, the horizontal displacement becomes 1.6mm (5.6σ) Peak orbit tolerance of 4mm corresponds to 14.3σ Mechanical tolerance of 2.2mm corresponds to 7.7σ For no crossing and separation, the VELO aperture has to be bigger than 9mm J. Van den Brand, PH/ULB Including above tolerances and an extra 20% for the beta beating and spurious dispersion, the VELO radius has to be higher than 12mm for the extreme crossing angle and 10.5mm for the nominal one Centring the VELO around the beam, allows a further 4mm of closure (8mm and 6.6mm) 23/10/2006 LOC Meeting, Y. Papaphilippou

Closure of the VELO for different scenarios The VELO apertures quoted allow n1 =7σ For the nominal scheme the VELO cannot be closed to less than 11.4mm (nominal internal crossing angle) Different spectrometer polarity has a minor influence in the available aperture Influence of the external crossing angle is also minimal Influence of the separation important mostly for small internal crossing angles After centring VELO around the CO, aperture can be closed down to 5.6mm (for no internal crossing angle) or to 7.1-7.2mm for the maximum crossing angle In all the simulations, a mechanical tolerance of 2.2mm was used and has to be refined It is important to know the precision with which the detector can be centred around the beam Any failure maybe catastrophic for the detector and its manipulation has to be included in machine protection loop Internal crossing angle [mrad] Vertical Separation External crossing angle VELO aperture [mm] With CO of 0.4mm Without CO 2.1 + 12.2 7.2 0.135 11.4 7.4 11.1 7.1 9.6 5.6 12.3 8.3 11.5 7.5 11.3 7.3 9.7 5.7 -2.1 12.4 8.4 -0.135 11.2 23/10/2006 LOC Meeting, Y. Papaphilippou