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GLAST LAT Project Gamma-ray Large Area Space Telescope Integration and Test CDR Peer Review, March 28, 2003 GLAST Large Area Telescope: I & T Peer Review Particle Test Elliott Bloom SU-SLAC Subsystem Manager [email protected] 650-926-2469 Document: LAT-PR-01779-01 Section 8 - Page 1 GLAST LAT Project Integration and Test CDR Peer Review, March 28, 2003 Outline Flow of Requirements to/From Subsystems LAT Particle Tests Cosmic Rays and Van de Graaff Calibration Unit Beam Test Document: LAT-PR-01779-01 Section 8 - Page 2 GLAST LAT Project Integration and Test CDR Peer Review, March 28, 2003 LAT Functional Performance (SE and I&T) LATInstrumentPerformance Verification Plan LAT-M D-00408 T. Leisgang SubsystemTest Plans Tracker Tower Test Plan LAT-TD-00155 LAT Performance & Operation Test Plans Com ponent Aliveness Tests Subsystem IntegrationTests ACD Test Plan LATLim ited Perform ance Tests ACD-PLAN-000050 LAT Com prehensive Perform ance Tests E. Gawehn E-GSE LAT-M D-01533 M .Huffer R. Claus L. Wai LATOperational Perform ance Tests TEM EP PDU GASU LAT Contamination Control LAT-M D-00404 Plan J. Cullinan E. Gawehn LAT Instrumentation Plan LAT-M D-00890 M .Lovellette W. Davis Facilities LAT-M D-01386 LAT Survey & Alignment L. Wai LAT-M D-01586 LAT Survey Plan LAT-TD-00895 L. Wai M .Nordby M echanical Weight & CG LAT-M D-01598 E. Gawehn L. Wai LAT Dynamics Test Plan LAT-M D-01196 Y Ismael M .Lovellette •Structural and Mechanical Tests (cosmic ray survey) • Thermal Verification Tests (cosmic ray survey) • Instrument Monitoring (cosmic ray, Van de Graaff) • End-to-end test (cosmic rays at ~ 35,000 ft in a jet airplane during transport to NRL for environmental tests) (TBR) ElectricalPerformance Tests LAT-M D-01055 L. Wai ThermalTests LAT-M D-01837 M .Lovellette E. Gawehn LAT Thermal Test Plan LAT-M D-01600 M .Lovellette J. Wang LAT EM I Tests LAT-M D-01838 LAT EM I/EM C Test Plan No Number M .Lovellette T. Leisgang ElectronicsTest Plan LAT-TD-00296 SUI LAT Handling &Transportation Plan LAT-M D-00452 D-00649 M -GSE LAT-M D-01462 Dynamics Tests LAT-M D-01836 E. Gawehn M .Lovellette M echanicalS/S Test Plan LAT-SS-00493 LAT Flight Software Test Plan LAT-TD-00786 LATM echanicalIntegration LAT-PS-00676 E. Gawehn L. Wai Calorimeter Test Plan LAT-SS-00262 Thermal S/S Test Plan No Number LAT Integration & Test Plan LAT-M D-01376 E. Bloom M .Lovellette LAT SVAC Test Plan LAT-M D-01587 E. do Couto E Silva Particle Test Plan LAT-M D-00440 G.Godfrey Document: LAT-PR-01779-01 SVAC Plan LAT-M D-00446 E. Do Couto E Silva S. Ritz Produce a Working Instrument Section 8 - Page 3 GLAST LAT Project Integration and Test CDR Peer Review, March 28, 2003 Science Performance (SE, IS, and I&T ) LATPerformance Specification (LevelIIb) LAT-MD-00010 ACD Subsystem Spec. Tracker SubsystemSpec (levelIII) CAL Subsystem Spec. (levelIII) LAT-MD-00016 LAT-MD-00017 LAT-MD-0018 (levelIII) • • SVAC Plan LAT-MD-00446 • (levelIII) E. do Couto e Silva S. Ritz Particle tests (beam test, cosmic rays, Van de Graaff) Calibration (beam test, cosmic rays) Science verification tests (beam test, cosmic rays, Van de Graaff) LAT SVAC Test Plan Particle Test Plan LAT-MD-00440 (levelIV) G.Godfrey LAT-MD-01587 (levelIV) E. do Couto e Silva Engineering Model Calibration Unit LATIntegration LAT-MD-00573 (levelIV) LAT-MD-00574 (levelIV) LAT-MD-0575 (levelIV) E. do Couto e Silva E. do Couto e Silva E. do Couto e Silva Document: LAT-PR-01779-01 LATEnvironmental Tests LAT-MD-00576 (levelIV) E. do Couto e Silva LAT Mission Integration LAT-MD-00577 (levelIV) LAT Phase 0 OnOrbit LAT-MD-0581 (levelIV) E. do Couto e Silva E. do Couto e Silva Produce a Scientifically Working Instrument Section 8 - Page 4 GLAST LAT Project Integration and Test CDR Peer Review, March 28, 2003 Summary of Science Instrument Performance Verification (subset of Table 1 of LAT-SS-00010). Req’t # Req’t Title 1.Parameter Verification Method 5.2.1 Energy Range/ Effective Area At Normal Incidence: > 300 cm2 @ 20 MeV >3000 cm2 @ 100 MeV >6400 cm2 @ 300 GeV T=Test A=Analysis T and A 1) Van de Graaff 17.6 MeV g 2) Tagged photons 100 to 1500 MeV, norm incidence 3) Brems beam, simultaneously all g energy bins from 20 MeV to 28 GeV, variety of angles and transverse positions. 5.2.2 Energy Resolution On axis: 50 % 20–100 MeV 10 % .1-10 GeV 20% 10-300 GeV 6% >10 GeV, Incidence>60° T and A 1) Van de Graaff 17.6 MeV g 2) Tagged photons 100 to 1500 MeV, norm incidence 3) Positrons 1,2,5,10,28, 45 GeV, variety of angles and transverse positions 5.2.3 Peak Effective Area >8000 cm2 T and A 1) Brems beam, simultaneously all g energy bins from 20 MeV to 28 GeV, variety of angles and transverse positions. 5.2.4 Effective Area Knowledge A/A, 1 <50% 20-50 MeV <25% .05-300 GeV T and A 1) Brems beam, simultaneously all g energy bins from 20 MeV to 28 Gev, variety of angles and transverse positions. 5.2.5 Single Photon Ang Resolution 68% (onaxis) < 3.5° front @ 100 MeV < 6° back < 0.15° front @ 10-300 GeV < 0.3° back T and A 1) Brems beam, simultaneously all g energy bins from 20 MeV to 28 GeV, variety of angles and transverse positions. 2) Tagged photons 100 to 1500 MeV, norm incidence 5.2.6 Single Photon Ang Resolution 95% (onaxis) < 3 x 68% On-Axis T and A 1) Brems beam, simultaneously all g energy bins from 20 MeV to 28 GeV, variety of angles and transverse positions. 2) Tagged photons 100 to 1500 MeV, norm incidence 5.2.7 Single Photon Ang Resolution (off axis at 55°) < 1.7 times on-axis T and A 1) Brems beam, simultaneously all g energy bins from 20 MeV to 28 GeV, variety of angles and transverse positions. 5.2.8 Field of View > 2 sr T and A 1) Brems beam, simultaneously all g energy bins from 20 MeV to 28 GeV, variety of angles and transverse positions. 5.2.11 Time Accuracy Better than 10 usec relative to S/C time T and A 1) All Beam Test events record time from Linac RF 5.2.12 Background Rejection >105:1 (TBR) T and A 1) 200 K protons (Pattern rejection) 2) Cosmic rays on the ground (ACD rejection) 5.2.13 Dead Time <100 usec per event T and A 1) Ground cosmics 2) All Beam Test runs Document: LAT-PR-01779-01 Beam Tests relevant to the Verification Section 8 - Page 5 GLAST LAT Project Integration and Test CDR Peer Review, March 28, 2003 Beams • Cosmics rays on the ground – EM, CU, LAT • Van de Graff (17.6 Mev g) – EM, CU (TBR), LAT (TBR) • End Station A positrons (1-45 Gev) – CU • End Station A tagged photons (~100-1000 Mev) – CU • End Station A brems photons (> 20 Mev – 28 Gev) – CU • End Station A protons (~12 Gev) – CU • Cosmic rays in airplane (25,000 - 35,000 feet) (few hours) (TBR) – LAT Document: LAT-PR-01779-01 Section 8 - Page 6 GLAST LAT Project Integration and Test CDR Peer Review, March 28, 2003 Ground Cosmic Rays (Examples) • Each tower as it becomes available at SLAC – ~106 muons/day x 3 days (TBR) (use 3 in-a-row tracker trigger) – Natural cosmic solid angle distribution. External muon telescope. • Four Tower Calibration Unit – Inter tower survey. • Full LAT – ~108 muons/day (using 3 in-a-row tracker trigger) – Inter tower survey – Calibrate individual CsI xtals • ADC chans/MeV • Positional dependence – Calibrate tracker • Dead and noisy strip map • Straight tracks survey relative tray and tower positions – Calibrate ACD • ADC chans / MeV • Calibrate discriminator thresholds • Efficiency vs position – Trigger and DAQ • Efficiency vs position For a full list of calibrations see LAT-MD-00446. Document: LAT-PR-01779-01 Section 8 - Page 7 GLAST LAT Project Integration and Test CDR Peer Review, March 28, 2003 BGO Detector Array Elements of Scintillator Telescope to identify Cosmic Rays. BGO crystal array used to calibrate the energy of the tagged photon beam. Phototubes BGO crystals Document: LAT-PR-01779-01 Section 8 - Page 8 GLAST LAT Project Integration and Test CDR Peer Review, March 28, 2003 Van de Graaff Installed Beam Pipe Bldg 33 Clean Room Inside Clean room Heritage from previous use in Crystal Ball experiment by members of I&T. This VDG was used for 8 years at SLAC and then shipped to DESY (Hamburg, Germany). During this time it was used routinely for CB calibration using g lines produced by the VDG. Document: LAT-PR-01779-01 Section 8 - Page 9 GLAST LAT Project Integration and Test CDR Peer Review, March 28, 2003 Van de Graff Produced g Spectrum Gamma Spectrum from P+Li7 170.57 200 Counts / .27 MeV counts i 150 counts_u counts_d FitCB E i In Crystal Ball detector i 100 i FitEM E i 50 0 0 0 0 5 10 15 E i Energy [MeV] 20 25 30 26.73 1) The points are data (3335 events) from the Crystal Ball for the gammas from the reaction p+Li7. 2) The black solid curve is the sum of a Breit-Wigner (Eresonance =12 MeV , FWHM G=5 MeV) and a Gaussian (Eresonance=17.6 MeV, G ~ 10 keV, resolution = 1.3 MeV). The two curves have equal area and add up to the total number of counts in the data. 3) The red solid curve is what the EM would see with the GLAST LAT required resolution, assuming a sum of two Gaussians ( = 50%, 50%, relative efficiency = 0.7, 1.0 ). 4) The Li target produced 1060 Hz of gammas (E>7 MeV) into 4p solid angle (Measured in February with the Van de Graff and BGO calorimeter in Bldg 33). Document: LAT-PR-01779-01 Section 8 - Page 10 GLAST LAT Project Integration and Test CDR Peer Review, March 28, 2003 Absolute normalization of VDG Flux • VDG Absolute Flux needs to be known if VDG used to establish < 100 MeV Science requirements. – Required to establish > 300 cm2 effective area for LAT @ 20 MeV (TBR) • BGO normalization of the g flux during EM, CU, LAT Measurements – The g angular distribution from the target is expected to be isotropic. Measurements at 0 and 45 degrees have initially confirmed this. – Primary normalization method: The BGO calorimeter will be placed at ~135 degrees to the beam direction (i.e., behind the target) while the target is in front of the EM, CU, or LAT. Simultaneously counting the photons into the solid angle of the BGO will yield the number of photons going into the solid angle of the EM, CU, or LAT. – Secondary normalization method (less accurate): The Van de Graff operator will keep the energy and current of the accelerator constant during the run, and then use the flux versus current calibration to calculate the number of photons going into the solid angle of the EM, CU, or LAT. Document: LAT-PR-01779-01 Section 8 - Page 11 GLAST LAT Project Integration and Test CDR Peer Review, March 28, 2003 Simulated Energy Spectrum from the VDG source Linear Scale !!! EB-W =12 MeV , FWHM G=6 MeV and a Gaussian Eresonance=17.6 MeV, G ~ 10 keV) 90 000 MC signal events (0.5 h of data taking 50 Hz rate from VDG) Used as input to the MC Energy (MeV) Document: LAT-PR-01779-01 Section 8 - Page 12 GLAST LAT Project TKR - Number of TRACKS EM MC Integration and Test CDR Peer Review, March 28, 2003 TKR – number of CLUSTERS m m g g Cuts: TKR trigger Differential distribution Signal dominates Negative values are not shown Document: LAT-PR-01779-01 Cuts: TKR trigger Differential distribution Signal dominates Negative values are not shown Section 8 - Page 13 GLAST LAT Project EM Energy Spectrum (TKR only) Integration and Test CDR Peer Review, March 28, 2003 EM MC Photons only TKR energy (MeV) Document: LAT-PR-01779-01 Section 8 - Page 14 GLAST LAT Project EM MC Integration and Test CDR Peer Review, March 28, 2003 Photons only EM Energy Spectrum (CAL+TKR) in MeV True MC Spectrum Breit-Wigner (mean 11.4, FWHM = 6 MeV) Delta function (17.6 MeV) Event ratio 1:1 MC Reconstructed spectrum 90 000 MC signal events (0.5 h of data taking) Cuts: TKR trigger, TOT>0 below conversion layer, ECAL>0 Document: LAT-PR-01779-01 Section 8 - Page 15 GLAST LAT Project Integration and Test CDR Peer Review, March 28, 2003 Beam Test Measurement Strategy • • • First, calibrate Four Tower Calibration Unit energy response – 1– 45 Gev e+ with variety of x,y,θ (6 days) (small extrapolation to g with MC). – Calibrate tagged photon beam with BGO array (energy calibrated with VDG). – 100-1500 Mev tagged photons at normal incidence (2 days). – 17.6 MeV g from Van de Graff (< 100 MeV) TBR. Second, take photon data for testing the Monte Carlo (use CU for energy measurement). – Bremsstrahlung g beam at one e+ energy (28 Gev) ( 20 days) – Simultaneously measures all g energies from 20 Mev to 28 GeV – Bremsstrahlung spectrum has equal numbers of g per % width energy bin. – The already energy calibrated LAT bins the photons into ±25% energy bins. – An example of bin edges= [GeV] – .017, .026, .038, .057, .086, .129, .19, .29, .44, .65, .98, 1.5, 2.2, 3.3, 5.0, 7.4, 11, 17, 25 GeV Third, take hadron data for testing the simulation and measuring the pattern cut rejection factor. – ~200 K protons @ .0044 /pulse x 30 Hz x 30 days x .58 accelerator efficiency – This is the number of protons we recorded in 30 days in Beamtest 99. Document: LAT-PR-01779-01 Section 8 - Page 16 GLAST LAT Project Integration and Test CDR Peer Review, March 28, 2003 EXTRA SLIDES Document: LAT-PR-01779-01 Section 8 - Page 17 GLAST LAT Project Integration and Test CDR Peer Review, March 28, 2003 Background Rate Trigger rate = # of triggered events x 60000 cm2 x 1.67 /cm2/s /1,000,000 generated events Vertical Position (3-in-a-row only) = 15.33 Hz Vertical Position (W cut) = 13.94 Hz Horizontal Position (W cut) = 2.54 Hz W cut = 3-in-row reconstructed events that Converted inside the W foil (130.15 to 130.25 mm) Energy (MeV) Document: LAT-PR-01779-01 Section 8 - Page 18 GLAST LAT Project Z Integration and Test CDR Peer Review, March 28, 2003 Photons Highest Photon flux Highest Trigger efficiency Lowest CR flux Highest Trigger efficiency X UP Y TKR Highest CR flux Lowest Trigger efficiency Document: LAT-PR-01779-01 For cosmic rays YZ Plane: Trade off between Flux and Trigger efficiency XZ Plane: No Trade off between Flux and Trigger efficiency rate is dominated by trigger efficiency Section 8 - Page 19 GLAST LAT Project Integration and Test CDR Peer Review, March 28, 2003 TOT right below the converter where conversion happens m We should be able to see this difference in the VDG test if the TOT is working . MC We need to “calibrate” the TOT with muons g X – axis = TOT*cosz DAC counts Cuts: TKR trigger, TOT>0 below conversion layer. Found track along Z direction, needed to normalize to normal incidence. Document: LAT-PR-01779-01 Section 8 - Page 20 GLAST LAT Project Integration and Test CDR Peer Review, March 28, 2003 TOT “Calibration” with Muons Tower Vertical - MC This is the TOT one expects for Muons in a given TKR layer from Monte Carlo Simulations Muons: 1 Mip ~ 33 to 37 counts DAC counts Cuts : TKR trigger, 1 track and 1 vertex Document: LAT-PR-01779-01 Section 8 - Page 21 TOT “Calibration” from muons - DATA GLAST LAT Project Integration and Test CDR Peer Review, March 28, 2003 (using EGSE and the GTRC chip v3 that is in the EM ! At SLAC) Merci Johann !! Muons: 1 Mip ~ 15-20 counts This is the TOT already working with real data ! DAC counts Document: LAT-PR-01779-01 Section 8 - Page 22