VCSEL-980nm Test for RMD 4 mm2 APD Changguo Lu Princeton U Feb 8, 2013

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VCSEL-980nm Test for RMD 4 mm2 APD Changguo Lu Princeton U Feb 8, 2013

Test setup An environmental chamber (EC) is employed to create a temperature controlled test environment. In this test, the temperature was controlled to be close to 20C. The APD and VCSEL(980nm) laser diode are placed inside of the EC. Internal view of the EC. EC chamber APD test box (4mm^2 APD) Optical fiber VCSEL laser diode box Collimation lens (Thorlabs CFC-11X-B)

Screen Capture of the Instrument Response Test dtinst = 3.97 ps = combined resolution of scope and MiniCircuits ZX60 amplifier.

Linearity of Laser-Diode Beam Power vs. APD/ZX60 Signal Amplitude Use Thorlabs PM100USB power/energy meter to measure the beam power. The APD/ZX60 signal vs. power shows good linearity: The neutral filters were employed to change the beam power.

Dependence of RMS Timing Jitter dt on APD Signal Amplitude ( V) Plots of dt vs. 1/V and dt vs. 1/sqrt(V) show that better linearity in the former than the later. The instrument response contribution (3.97 ps) to dt has been subtracted in quadrature.

dt Dependence on # of MIPs Since we already calibrated the laser beam power, we can convert the signal amplitude unit to equivalent MIPs: Repetition rate of laser diode is R = 10 MHz, 980nm photon energy is E980 = 2.03E-19 J, MIP equivalent # of photo-electron = 6000, and we assume that Q.E. of APD = 35%; Therefore the conversion from laser beam power P(W) to # of MIP is: # of MIPs = P(W)/R(Hz)/E980 (J)*QE/6000 = P(W)*2.88E+7 1 MIP equivalent time resolution ~12ps

Thomas’ 12/5/2013 Test Result Below is T. Tsang’s test result of 12/5/2012. http://puhep1.princeton.edu/~mcdonald/LHC/Tsang/time_jitter_dependence_on_MIP.ppt In the two scenarios, dt  1/MIP and 1/sqrt(MIP), neither shows good linearity for the entire tested range 0.4 ~ 11 MIP. Probably above 1 MIP the linearity between dt and 1/sqrt(MIP) is better and below 1.7 MIP, 1/MIP is better. > 1 MIP < 1.7 MIP