QRLed Driver in Magnetic Field Jaroslav Zalesak Institute

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QRLed Driver in Magnetic Field Jaroslav Zalesak Institute of Physics of the ASCR, Prague

QRLed Driver in Magnetic Field Jaroslav Zalesak Institute of Physics of the ASCR, Prague Feb 20, 2009 CALICE meeting, Daegu, Korea QRL in Magnetic Field 1

Calibration Option 2: LED driver • Non-linearity correction, MIP calibration, Correction temperature variations •

Calibration Option 2: LED driver • Non-linearity correction, MIP calibration, Correction temperature variations • Two appr. : electrical or optical signal distribution - One LED / one tile or central driver plus fibres UV LEDs – short light pulses Notched fibers Each illuminates 12 tiles HBU CALIB module Option I QRLD board (ASCR Prague): „Quasi Resonant LED Driver Board“, 6 LEDs / 1 PCB Feb 20, 2009 CALICE meeting, Daegu, Korea QRL in Magnetic Field 2

QR-LED driver • • Option with optical fiber distribution Electronics: multi-channel prototype complete Optical

QR-LED driver • • Option with optical fiber distribution Electronics: multi-channel prototype complete Optical system: uniformity again competitive Multichannel LED driver • 1 PCB with the communication module µC, power regulator, 6 channels of QRLed driver • Communication module to PC via CAN bus or I 2 C • Controlling the amplitude and monitoring temperature and voltages • LED pulse width ~ 5 ns fixed, tunable amplitude up to 50 -100 MIPs is controlled by the V-calib signal • 2 LEDs can be monitored by a PIN photodiode +12 V Power regulator QRLED 1 F I B R E S T-calib µC AT 91 SA M 7 X 256 V-calib QRLED 6 Feb 20, 2009 CALICE meeting, Daegu, Korea QRL in Magnetic Field LED 6 3

Magnetic Field Test Setup • week ago tests in mag. field • one week

Magnetic Field Test Setup • week ago tests in mag. field • one week period at solenoid • DESY site up to 4 T available • QRL PCB fixed to movable rod • different positions to measure • 3 LEDs / channels → • 3 optical fibers outside meas. area, LV supply and CANbus wires from r/o area Feb 20, 2009 CALICE meeting, Daegu, Korea QRL in Magnetic Field 4

Data Readout • 3 r/o Photo detector channels: § 2 APDs @ low-gain §

Data Readout • 3 r/o Photo detector channels: § 2 APDs @ low-gain § 1 PIN diode + amplifiers • 1 Temp sensor @ APD (automatically in r/o only at the end) • LV + HV supplies • Slow control based on Lab. View • via CAN bus several LV/Temp control points from PCB recorded • Auto-implemented data transfer from scope (3+1 ch. Ampl) • Independent S/C for Magnet Feb 20, 2009 CALICE meeting, Daegu, Korea QRL in Magnetic Field 5

Magnetic Field Scan #1 - ‘middle’ • 1 st PCB position in the middle

Magnetic Field Scan #1 - ‘middle’ • 1 st PCB position in the middle solenoid parallel to line of magnet force, horizontally placed, homogeneous Mag. Field • about 2 hours scan 6. 5 up/down magnet + 7 min stable B • Variations in response @ (in) visible level (PIN x APD T- uncorr. ) Feb 20, 2009 CALICE meeting, Daegu, Korea QRL in Magnetic Field 6

Magnetic Field Scan #2 - ‘slantways’ • 2 nd PCB position in the middle

Magnetic Field Scan #2 - ‘slantways’ • 2 nd PCB position in the middle solenoid, placed on oblique surface ‘slantways’ ~25° angle, homogeneous Mag. Field • Variations in response @ (in) visible level (PIN x APD T- uncorr. ) • Overall scan ± 0. 5% difference (a bit more APDs), maybe B steps Feb 20, 2009 CALICE meeting, Daegu, Korea QRL in Magnetic Field 7

Magnetic Field Scan #3 – ‘outer’ • 3 rd PCB position at the end

Magnetic Field Scan #3 – ‘outer’ • 3 rd PCB position at the end of solenoid – ‘outer’ position, horizontally placed, no-homogeneous Mag. Field • response seems to rise contrary previous measurements for highest magnetic field B. Feb 20, 2009 CALICE meeting, Daegu, Korea QRL in Magnetic Field 8

Magnetic Field – Long-term • Over 8 hours long-term behavior in constant 4 T

Magnetic Field – Long-term • Over 8 hours long-term behavior in constant 4 T magnetic field • Almost (Temp ~0. 1%) constant conditions • Variations in response invisible • Amplitudes < 0. 5%; PIN diodes ~0. 5% noise level, APD less Feb 20, 2009 CALICE meeting, Daegu, Korea QRL in Magnetic Field 9

Temperature dependence • Only, at the end of data measurement period automatically APD temperature

Temperature dependence • Only, at the end of data measurement period automatically APD temperature sensor in r/o implemented • Correction formulas determined to be applied to data • 2(? , gain/pos. sensor) diff APD dependence, NO PIN dependence Feb 20, 2009 CALICE meeting, Daegu, Korea QRL in Magnetic Field 10

Conclusion I q Calibration system – option II: electronic part QR LED driver reasonably

Conclusion I q Calibration system – option II: electronic part QR LED driver reasonably works incl. Slow control interfaces can be implemented into EUDET AHCAL prototype q Characteristics and function described in public paper EUDET report 2008 -7 Prague AHCAL group q Optical part – notched fibres in preparation → promising results Feb 20, 2009 CALICE meeting, Daegu, Korea QRL in Magnetic Field 11

Conclusion II, Outlook q Calibration system – QR LED driver in Magnetic field tests:

Conclusion II, Outlook q Calibration system – QR LED driver in Magnetic field tests: works very well q meas. system sensitive to < 0. 5% variations in response q During constant magnetic field (standard operation conditions) the measurements are stable (w/o reference to PD temp. ) q Expecting one more measurement period § more precise orientations of PCB in mag. field § to avoid temperature dependence P. S. Thanks to DESY staff to allow to make such measurement Note: these days we have obtained one new notched fiber, which seems to fulfill our request on uniformity (light output ± 10%) Feb 20, 2009 CALICE meeting, Daegu, Korea QRL in Magnetic Field 12

Backup slides Feb 20, 2009 CALICE meeting, Daegu, Korea QRL in Magnetic Field 13

Backup slides Feb 20, 2009 CALICE meeting, Daegu, Korea QRL in Magnetic Field 13

Option 2: Optical system • Idea: use one fiber for one row of tiles

Option 2: Optical system • Idea: use one fiber for one row of tiles (72) • Problems: Notched fiber: • uniformity of distributed light • enough intensity of distributed light • concentration of LED light into one fiber • Two fibres: • Side-emitting - exponential fall of intensity • Notched fibre - better uniformity of distributed light - need to mechanize production - R&D • No optical cross talk seen (< 1 -2 %) @ different amplitudes 2 MIPs 10 MIPs 25 MIPs Feb 20, 2009 CALICE meeting, Daegu, Korea QRL in Magnetic Field 14

Calibration system • • • Non-linearity correction, MIP calibration, Correction temperature variations Use gain

Calibration system • • • Non-linearity correction, MIP calibration, Correction temperature variations Use gain monitoring, adjust voltage → see G. Eigen’s talk Many procedures developed during last year’s analysis, but not finally proven yet Stability of saturation still an issue -> need dynamic range Two appr. : electrical or optical signal distribution - One LED / one tile or central driver plus fibres Differences inside the active gap, but same external interfaces Option 2: LED driver • Electronics: multi-channel prototype complete • Optical system: uniformity again competitive • Integration into active layer still an open issue • Multichannel LED driver • 1 PCB with the communication module µC, power regulator, 6 channels of QRLed driver • Communication module to PC via CAN bus or I 2 C • Controlling the amplitude and monitoring temperature and voltages • LED pulse width ~ 5 ns fixed, tunable amplitude up to 50 -100 MIPs is controlled by the V-calib signal • 2 LEDs can be monitored by a PIN photodiode Feb 20, 2009 CALICE meeting, Daegu, Korea QRL in Magnetic Field 15