Yeah.. well 3/2 till something near 1mA at which point it becomes linear. (You can do a decent job measuring PD DC current with the uA input on a dec ent DMM.)
Here's a plot of count rate vs photodiode current (where I used the same LE D current for both measurments.)
Almost linear. (slope should be 1.0 'in theory') There are several things that 'screw up' the spad counts. At low count rates there is after pulsin g which gives you more counts. And then at high count rates you need to ta ke the dead time of the spad into account. I've 'semi'* corrected the data for the dead time effects.
Thanks for the IR led offer, but if I can't buy ~100's of them I'm not real ly interested. But drop me an email and I'll put some AND113R's in an env elope. (gherold-at-teachspin.com)(That's what gave the above data... In wh at might be called an extreme case of 'trud' polishing I filed the plastic lens of the 'spad' down to just above the active element and got lot's more counts with green photons.)
George H.
*so to first order the dead time correction says that the 'real' time I was measuring is the (gate time)-(dead time)*(number counts). But then there' s a second order effect that a second pulse during the dead time strecthes the dead time by a factor between 1 and 2... I ignored the second order cor rection.