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S30XL-LESA/LDMX
> Model number: AVO-9A-B-P-P3-SLAA
>
> Description: Laser Diode Driver (Pulsed Voltage) with IEEE-488.2 GPIB
> and RS-232 Computer Control Ports
>
> Polarity: positive
>
> Amplitude: 0 - 140 mA (see footnote 3 on datasheet)
>
> Maximum output of mainframe into 50 Ohms: 10V
>
> Pulse width (FWHM): 2 - 50 ns
>
> Maximum PRF: 50 kHz
>
> -P3-SLAA option: Provides an 8-pin socket for the QFLD-840-2SM. The
> positive output pulse is applied to pin 2 of the diode. All other pins
> are grounded. Rseries in the output module is approximately 42 Ohms,
> such that Rseries + Rdiode = 50 Ohms, approximately.
>
> Other: as per the standard AVO-9A-B-P, described at
> http://www.avtechpulse.com/laser/avo-9a
Notes: Output pulse looks like crap at lower amplitudes; use at least 5 V to minimize weirdness (plan is to always use 10 V, and use fixed RF attenuators to get the right amplitude for each diode). Narrow pulse widths come out narrower than advertised - a setting of 2 ns yields ~1 ns, 3 ns yields 2 ns, 4 ns yields 3 ns, etc. (This can apparently be calibrated - will do sometime if we decide we care.)
We have two AVX-S1-P3-SLAA (8-pin) and one AVX-S1-P4B (14-pin).
Barrel connector from diode to attenuator: ADAFC1 mounted on bracket ADABD2
Adjustable attenuator (up to 50 dB):
Collimator (in holder AD1109F):
Neutral density filter (anti-reflective coating, why not) for fixed attenuation (between two retaining rings SM05RR - needs spanner SPW603):
Lens (in holder S05TM09 - needs spanner SPW908):
Get some extra retaining rings (two per tube) in case we need to clamp down the lens holder or something, who knows.
3-inch lens tube: SM05M30
Lens tube clamps (two per tube for stability): SM05RC
Motor/encoders are Quicksilver QCI-A17H-3 for Z, QCI-A23H-5 for X and Y.
X and Y stages are Lintech 209205 rev. A.
Bottom of X stage is 3-3/8" high. Bottom edge of Z stage (Deltron LRS2-1) moves from 6-1/2" to 7-1/2" high.
Mounting plate sticks out 3.75" from the bottom edge of the Z stage.
About 1 m run from stage to the back of the hood; 1 m from back of hood to electronics.
Sensor is 320 um thick, so MIP = 124 keV, or 2e-14 J.
Assume 2 ns pulse width, then we need 2e-14 J/2e-9 s = 1e-5 W, or 10 uW. If we use wider pulses we need to attenuate more.
Filter damage: the narrower and more powerful of the two beams (1060 nm) is 2.4 mm diameter, so area is 4.5 mm^2; peak power density (factor of 2 is what Thorlabs says you should use for a Gaussian peak) is 2*10 mW/A = 0.4 W/cm^2. No actual spec on damage threshold for the AR coating, but the glass is definitely fine.