James M c Intyre University of Connecticut GlueX Collaboration Meeting JLab, Feb. 2-4, 2011.

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Presentation transcript:

James M c Intyre University of Connecticut GlueX Collaboration Meeting JLab, Feb. 2-4, 2011

Update on Delivered Prototype to JLab Preparations for Beam Test Lessons Learned J. M c Intyre, GlueX collaboration meeting, JLab, Feb. 2-4, Beam Test in Hall B Tagger Microscope  Testing:  Detector Alignment  Readout  Time Resolution  Efficiency  Cross-talk

Beam Test in Hall B (cont.) Active Collimator  Overview of Design  Goal:  Determine Bandwidth Limits of the Position Readout  Test Updated Readout  Test the Spatial Resolution  Confirm Diagnosis of Anomalies from 2007 Beam Test 3 J. M c Intyre, GlueX collaboration meeting, JLab, Feb. 2-4, 2011

Delivered to JLab on Oct. 7, 2010 ► Delivered to JLab on Oct. 7, 2010 ◄ 4 J. M c Intyre, GlueX collaboration meeting, JLab, Feb. 2-4,

Preparations for Beam Test  Setup Control Computer (Software setup on JLab computer as per JLab requirements)  Setup Readout/Control for Tagger Microscope  Installed controls for SiPM electronics  Motor controls for alignment of SciFi focal plane 5 J. M c Intyre, GlueX collaboration meeting, JLab, Feb. 2-4, 2011

Preparations for Beam Test  Bench Tests Performed Verified:  Ability to remotely control the step motors  Appropriate implementation of motor limits  Readout of the individual channels (pulse shape)  Readout via fDAC and F1TDC 6 J. M c Intyre, GlueX collaboration meeting, JLab, Feb. 2-4, 2011

7 Lessons Learned  Fusing vs. Gluing of Fibers (MSU Splicing Unit) Discussed during May 2010 Collaboration Meeting Stronger SciFi/waveguide joint Better light transmission Air bubbles in glue & gluing gaps avoided Specialized glass ferrules designed & ready to order

8 J. M c Intyre, GlueX collaboration meeting, JLab, Feb. 2-4, 2011 Lessons Learned  Board Layout Changes for Electronics Backplane Board  Component clearances – Too conservative  Components rearranged to provide better clearance through prototype top-plate

Lessons Learned  Board Layout Changes for Electronics Amplifier Board Changes to the board’s layout are being implemented: (Based on Fernando Barbosa’s recommendations)  Decrease inductance by... Optimization of layout/interconnections We saw some resonances in the amplifier spectrum & distinct ringing in the tail of the signals indicating inductance 9 J. M c Intyre, GlueX collaboration meeting, JLab, Feb. 2-4, 2011

Lessons Learned  Board Layout Changes for Electronics Amplifier Board  Decrease cross-talk by...  Optimize ground traces to improve Amp. circuit isolation  Improved layout of transistor DC level distribution islands  Spacing out the circuits, which is now possible due the new more spacious radiation-conscious chamber design 10 J. M c Intyre, GlueX collaboration meeting, JLab, Feb. 2-4, 2011

11 J. M c Intyre, GlueX collaboration meeting, JLab, Feb. 2-4, 2011 Lessons Learned  Neutron Radiation Damage to SiPMs SiPMs sensitive to neutron radiation GlueX-doc-1660-v2GlueX-doc-1660-v2 ⇒ Calc. of radiation damage of SiPM in GlueX SiPM Radiation Hardness TestSiPM Radiation Hardness Test ⇒ To predict life-time of SiPM detectors Neutron background estimates GlueX-doc-1646-v1GlueX-doc-1646-v1 ⇒ Neutron background estimates in tagger hall Solution Solution ⇒ Separate and Shield Electronics (i.e. SiPMs) Effective Damage to Si Detector Relative to 1MeV neutron Electron vacuum pipe to beam dump Origin of neutrons which arrive in the Tagger Microscope area

12 J. M c Intyre, GlueX collaboration meeting, JLab, Feb. 2-4, 2011 Lessons Learned  Neutron Shielding Shielding Material (Polyethylene) Use concrete floor as shielding

Tagger Microscope:  Performance Features Under Test Detector Alignment  Simulations show that when fiber axis is aligned to < 3 o of the e - trajectory ⇒ Adjacent signal amplitudes have a factor of 3 separation  Bench tests demonstrate alignment < 0.2 o Readout  First time SiPM signal will be read out with the designated GlueX fADC and F1TDC modules  Examine the output on the equipment actually intended for reading out this detector 13 J. M c Intyre, GlueX collaboration meeting, JLab, Feb. 2-4, 2011 Fiber Bundle D.o.F. e - Trajectory

Tagger Microscope:  Performance Features Under Test Time Resolution  Requirement: 200ps time resolution  BCF-20 SciFi → decay time 2.7ns  Collective photon emission time uncertainty goes as: 2.7ns / √(N γ ) ⇒ Minimum of 183 detected photons is required to meet 200ps time resolution specification  Simulations predict the mean photoelectron count > J. M c Intyre, GlueX collaboration meeting, JLab, Feb. 2-4, 2011

Tagger Microscope:  Performance Features Under Test Efficiency  Random arrival, in a single channel, of tagging e - result in the occasional overlap of these finite pulses ⇒ Resulting in the inability to resolve the two leading edges  While calculations are effective → measurement of the pulse selection efficiency fed by pulses from an e - beam would be extremely useful Cross-talk  Need to investigate the degree of cross-talk between channels in a live beam  Measure electronic cross-talk on the Amp. Board  Measure optical cross-talk between adjacent fiber-SiPM junctions 15 J. M c Intyre, GlueX collaboration meeting, JLab, Feb. 2-4, 2011

16 J. M c Intyre, GlueX collaboration meeting, JLab, Feb. 2-4, 2011

17 J. M c Intyre, GlueX collaboration meeting, JLab, Feb. 2-4, 2011 γ Beam Tungsten Ejected e - Insulator Tungsten Wedges Cathode (+) Anode (-) γ Beam Φ 5mm. Active Collimator Active Collimator ▶ Photon beam position monitor which will provide feedback to magnets upstream to ensure we thread through the collimators to the target.

Active Collimator:  Parasitic Beam Test  Goals:  Test the readout which was updated to 4 of 8 instruments (Since 2007 beam test)  Permits 2 complete opposing quadrants to be monitored continuously  Test the spatial resolution of the device  In absence of narrow upstream collimator (Present in 2007 beam test) 18 J. M c Intyre, GlueX collaboration meeting, JLab, Feb. 2-4, 2011

Active Collimator:  Parasitic Beam Test  Goals:  Determine the bandwidth limits of the position readout (signal noise vs. bandwidth of the detector signals)  Will be used to stabilize the photon beam position in Hall D using a controlled feedback loop to electron beam correctors up stream of the radiator 19 J. M c Intyre, GlueX collaboration meeting, JLab, Feb. 2-4, 2011

Active Collimator:  Parasitic Beam Test  Goals:  Confirm anomalies in the 2007 beam test were correctly diagnosed and remedied successfully  Larger than predicted currents ( Good thing ) (By Geant3 simulation)  Factor of 3.5 higher  Geant3 result was sensitive to the lower cutoff on the energy of the shower particles and deltas in the simulation  The P.E.E. that dominates photon absorption at energies < 100 keV is a complex Z-dependent function of energy that is described in an average way by Geant3 20 J. M c Intyre, GlueX collaboration meeting, JLab, Feb. 2-4, 2011

Active Collimator:  Parasitic Beam Test  Goals:  Confirm anomalies in the 2007 beam test were correctly diagnosed and remedied successfully  Cross-talk  Relatively large response on inner wedge when the photon beam interacts in the outer wedge (peaks at 15.5cm & 22.0cm)  Simulation < 5% of peak current vs. ~ 25% during beam test  Possibility  Possibility that the photon beam directed on the wedge not being readout caused charges to built up to a high voltage. Surface leakage currents drained the charge along the insulator to the nearest path to ground (which was through the adjacent wedge connected to the readout). 21 J. M c Intyre, GlueX collaboration meeting, JLab, Feb. 2-4, 2011

Active Collimator:  Parasitic Beam Test  Goals:  Confirm anomalies in the 2007 beam test were correctly diagnosed and remedied successfully  Middle Peaks (Remedy: Use of 90 o Connectors)  Peaks seen at 16.5cm & 21.0cm on both the inner and outer wedge readouts  Possibility  Possibility that the readout cables hanging down in front of the detector acted as a pre-shower. The asymmetry between left and right most likely comes from the fact that one cable (16.5cm) hangs down from above, while the other (21.0cm) starts out from below, the center of the photon beam. Therefore one interacts with a smaller fraction of the beam than the other. 22 J. M c Intyre, GlueX collaboration meeting, JLab, Feb. 2-4, 2011 Current measured on two outer wedges

23 J. M c Intyre, GlueX collaboration meeting, JLab, Feb. 2-4, 2011 Beam line

J. M c Intyre, GlueX collaboration meeting, JLab, Feb. 2-4, 2011