calice anl, mar18, 2008 ivo polak, ipascr, prague1 a fast led driver prototype for hcal calibration...

38
CALICE ANL, MAR18, 2008 Ivo Polak, IPASCR, Prague 1 A fast LED driver prototype for HCAL calibration CALICE meeting at ANL, USA

Upload: suzanna-scarlett-dennis

Post on 03-Jan-2016

217 views

Category:

Documents


0 download

TRANSCRIPT

  • A fast LED driver prototype for HCAL calibration CALICE meeting at ANL, USA

    Ivo Polak, IPASCR, Prague

  • Proposal for calibration systemFast LED driver is a key part of calibration systemA tunable calibration light in the range 0 to 100MIPSimplification of the optical system: one LED -> one side emitting fibre, one row of scintillator tilesSee Jaras talk Comments on optical system II

    Ivo Polak, IoP Prague

  • LED driver strategy not only for SiPM calibrationAt AHCAL prototype (uses SiPM), we used CMB, calibration system with UV-LED 400nm driven by very fast rectangular pulses (1ns rise/fall time).Steep Rectangular waveform satisfied the needs to vary pulse-width, BUT creates lots of harmonics electromagnetic crosstalk!We have found fixed pulse-width to about 6ns, we can go to use narrow band ->smooth waveform less RF interference = Quasi Resonant LED driver (single pulse)

    Ivo Polak, IoP Prague

  • Quasi-Resonant LED driverLC circuit, heavily dumped 2CH boardprimary testedWith printed Cu inductor 2ns pulse-widthPrototypingUsed my lovely single side copper foil PCBWe need more work on components optimization to recent LED Simulation pulse-width 5ns with 33nH inductance

    Ivo Polak, IoP Prague

  • 2CH QRLED board Consists of:Double sided PCB2 QRLED driver2PIN photodiode preampRate generator 1Hz to 10kHzVoltage regulatorsAmplitude controlV-calib and T-calib interface

    Ivo Polak, IoP Prague

  • 2CH QRLED boardThere is a detail of two QRLED driverPrinted inductors with taps, left is connected by tin jointTwo trimmers equalize delays between CH A and B

    Ivo Polak, IoP Prague

  • Principal schema of QRLed driverAA

    Ivo Polak, IoP Prague

  • PIN PD response to UVLEDLED current 1V => 1APIN

    Ivo Polak, IoP Prague

  • PIN PD response to UVLEDLED current 1V => 1A

    PIN

    Ivo Polak, IoP Prague

  • PIN PD response to UVLEDLED current 1V => 1APIN

    Ivo Polak, IoP Prague

  • Ivo Polak, IoP Prague

  • Further increase of the LED amplitudeWe see a change of the shapePIN 1mV/divLED current 1V => 1A

    Ivo Polak, IoP Prague

  • Further increase of the LED amplitudeWe see a change of the shapeLED current 1V => 1A

    PIN 2mV/div

    Ivo Polak, IoP Prague

  • Maximum amplitude of the LEDWe see a change of the shapeLED current 1V => 1A

    PIN 2mV/div

    Ivo Polak, IoP Prague

  • In wider time scale, increase of the amplitude PIN 2mV/div

    Ivo Polak, IoP Prague

  • In wider time scalePIN

    Ivo Polak, IoP Prague

  • In wider time scalePIN

    Ivo Polak, IoP Prague

  • Highest amplitude -> funny distortion PINLED current 1V => 1A At this amplitude LED is shining visible

    Ivo Polak, IoP Prague

  • A response to Slower PMT LED is over full powerPMTLED voltage at cathodesync

    Ivo Polak, IoP Prague

  • PIN crosstalk testPINReference amplitude

    LED current 1V => 1A

    Ivo Polak, IoP Prague

  • Optically shielded, same LED amplitude Electrical crosstalk to PIN

    NO crosstalk

    Ivo Polak, IoP Prague

  • Different LEDsMore different LEDs will be testedPPT UVLEDs 400nm are very fast!One blue pioneer has been testedEach type of the LED needs a bit of matching of 2 components at QRled driver

    Ivo Polak, IoP Prague

  • Another Blue LED, too slow!2ns -> 10nsPINLED current 1V => 1A

    Ivo Polak, IoP Prague

  • Another Blue LED, too slow!2ns -> 20nsElectrical opticalLED current 1V => 1A

    PIN

    Ivo Polak, IoP Prague

  • ConclusionQR LED driver is very promising technique to reduce Electro-Magnetic-Interferences2 PCBs of the two-channel QR LED driver are ready to further testMarch linearity testApril more assembled PCBs to testMay designing of multichannel system with light transfer in side-emitting fibers, first approach to mechanical integration to a new detector design

    Ivo Polak, IoP Prague

  • Backup slides

    Ivo Polak, IoP Prague

  • QR LED driver Simulationoscilloscopeoscilloscope

    Ivo Polak, IoP Prague

  • Simulation at 1.5V amplitudeXSC1: Upper trace - sync pulseLower trace voltage at LED hot end

    XSC2: Lower trace LED current

    Ivo Polak, IoP Prague

  • Simulation at 3VXSC1: Upper trace - sync pulseLower trace voltage at LED hot end

    XSC2: Lower trace LED current

    Ivo Polak, IoP Prague

  • Tests shows more power on LEDWe see response of PIN photodiode at oscilloscopeAmplitude up to 2mVpeak @ 50

    Ivo Polak, IoP Prague

  • Prototype of QR LED driver

    Ivo Polak, IoP Prague

  • Response to low amplitude at prototypeLED current (cyan) (voltage @ 10Ohm)PIN response (yellow)LED anode (violet)

    Ivo Polak, IoP Prague

  • Response to middle amplitude at prototypePulse width ~ 6ns

    Ivo Polak, IoP Prague

  • Response to high amplitude at prototype200mA current at LEDPulse width ~ 6ns

    Ivo Polak, IoP Prague

  • Response to high amplitude at prototypeThe Light from LED was optically blocked to PIN.

    Ivo Polak, IoP Prague

  • LED Current View of the LED pulse for a small amplitude (0.6 A)

    Measured with 1GHz voltage differential probe and 1GHz scope TDS4104 at 1 smd resistor

    4ns/div 0.5A/div

    Ivo Polak, IoP Prague

  • LED currentView of the LED pulse for a middle amplitude (1.0 A)

    Measured with 1GHz voltage differential probe and 1GHz scope TDS4104 at 1 smd resistor

    4ns/div 0.5A/div

    Ivo Polak, IoP Prague

  • LED currentView of the LED current pulse for the highest amplitude (2.3 A) Measured with 1GHz voltage differential probe and 1GHz scope TDS4104 at 1 smd resistor

    4ns/div 0.5A/div

    Ivo Polak, IoP Prague