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Edge Sensors for the Schwarzschild-Couder Telescopes

Edge Sensors for the Schwarzschild-Couder Telescopes. David Hanna McGill University UCLA AGIS Meeting June 26-27, 2008. The Requirement: facets on the S-C telescopes need to be positioned to a tolerance of the order of 10 microns light-weight optical support structure will undergo

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Edge Sensors for the Schwarzschild-Couder Telescopes

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  1. Edge Sensors for the Schwarzschild-Couder Telescopes David Hanna McGill University UCLA AGIS Meeting June 26-27, 2008

  2. The Requirement: facets on the S-C telescopes need to be positioned to a tolerance of the order of 10 microns light-weight optical support structure will undergo deformations of at least this scale while tracking sources a system of actuators to dynamically correct the facets’ positions and orientations is planned a related system to measure the facets’ positions and orientations must be developed

  3. light source beam PSD Mirror 2 Mirror 1 Edge Sensors to measure the displacement of one mirror facet with respect to its neighbour we plan to use a system of position-sensitive detectors (PSDs) illuminated by diode lasers or collimated LEDs. relative motion of the two facets causes the position of the beam spot on the PSD to be displaced; the job of the actuators is to move the facets in order to put the spot back to its nominal position

  4. Position Sensitive Detectors (PSDs) for the PSD, we are evaluating a lateral-effect photodiode of the pin-cushion type ( Hamamatsu S5991). - electrodes on the edges of the silicon photodiode collect charges produced by the illumination of the PSD. - ratios of currents from electrodes on opposite sides are used to calculate the centroid of the light pool. - thus the device is non-imaging. - shaped electrodes increase linearity near the edges and produce the pin-cushion-shaped sensitive area. figure from Circuit Cellar (www.circuitcellar.com)

  5. 15 mm Hamamatsu S5991 - this PSD model is available for $30 each in large quantities. - resolution is 1.5 mm

  6. Light Sources: we have two options: laser diode and light-emitting diode (LED) LED – blue(465 nm) Optek Technology ~ $0.70 (shown here with collimator, 1 mm diameter 10 mm long) LASER diode- red (650 nm) BEA lasers ~ $60 The LED can be made bright enough for our purposes but the forward current (80 mA) is larger than the suggested maximum (20 mA) Probably OK since - collimator acts as a very effective heat sink - we can use the LED in a low-duty-cycle mode (needs study)

  7. System Evaluation Hamamatsu provides a circuit for reading out the PSD. We have carried out tests on accuracy and stability using the setup shown at the right; the collimated LED is attached to an X-Y-Z translation device which is used to make controlled scans across the PSD - the blue spot below the PSD shows the size of the beam spot obtained using the simple collimator

  8. Scan in x and y use micrometer translator to change laser spot position on PSD compare PSD reading with translator position repeat to test for reproducibility

  9. Overnight Stability Test leave LED on for 16 hours record x, y and current +/- 10 um sunrise

  10. Electronics Developments single PSD circuit op-amps turn currents into voltages for ADCs to digitize

  11. 4-PSD op-amp board

  12. Present status and future plans PSDs and op-amp circuits now at UCLA awaiting tests on mechanical setup new circuit which puts ADC near the op-amp (ie send digital information over cables to improve noise rejection) to be developed this summer at McGill

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