This memo gives a description of the new procedure to determine the value of the flag "HWP" and to monitor its stability. Also, I give some some results of this procedure, from the July run. August 30, 2006 (modified August 17, 2007; changes marked with ***) *********************************************************************** A. Quick-Check Procedure, to monitor stability of "HWP": *********************************************************************** (1) Mount a grid with wires vertical in front of a cold load, as shown in SHARP installation video. Use level to ensure accuracy within one degree. (***if you put grid on the exit aperture then you can change the ZA of the telescope to level the grid***) Vertical wires corresponds to Phi_Inst_cor = 90 (see April 13 memo for definition of Phi_Inst_cor). (2) Measure the hwp angle at which the V-channel has its lowest signal. Call this hwp angle "V_null". (***set gains to low; see cheatsheet***) (***you should level with a warm-load in front of the LN-2 bucket before each reading***) Note that all SHARP hwp angles can be expressed in two ways: (a) "actual values of hwp angle", which are the actual numbers read on the encoder. I will refer to the V_null expressed in this way as "V_null_encoder" and (b) "relative values of hwp angle", which are measured relative to the first hwp angle used for data-taking. (The first angle was 50 degrees for the July 2006 run.) I will refer to the V-null expressed in this way "V_null_rel". (3) Note that HWP = 2 * V_null_rel (***so we can write: HWP = 2 * (V_null_encoder - "first-angle") ***) (this is derived below) *********************************************************************** B. Procedure used to measure "HWP" accurately *********************************************************************** For a precise measurement of "HWP" we need to take a few standard polarimetry files and do a fit, rather than just finding the "null" of V as described in (A) above. The reason is that there might be systematic deviations from a perfect sine curve. *********************************************************************** C. Results from the July 2006 run *********************************************************************** From an inspection of the notes made in the instrument log during the July 2006 run, we crudely estimate the V_null for each quick-check: date value of of quick-check V_null_encoder 7/13 93-94 7/16 93-94 7/17 90-91 7/18 92-93 7/20 92-93 It can be seen that there are no large problems with encoder slipping, but fits could be done to more precisely locate the minimum to probe this further. We can derive a value of "HWP" from these data by taking an average: V_null_encoder (avg.) is 92.5 V_null_rel is 92.5 - 50 = 42.5 estimate for HWP is 2*(42.5) = 85 *********************************************************************** D. Derivation of the relationship HWP = 2 * V_null_rel *********************************************************************** The derivation has two steps: (1) Think through the relationship between V_null_rel and Phi_Inst_raw The April 13 memo gives the definition of Phi_Inst_raw in terms of Q and U, and also tells how Q and U are calculated from the raw measurements of H and V as a function of hwp angle. From this info, the following Table can be constructed: V_null_rel Q U Phi_Inst_raw 0 + 0 0 22.5 0 - 135 45 - 0 90 67.5 0 + 45 From this Table we see that Phi_Inst_raw = -2 * V_null_rel (2) Relate Phi_Inst_raw to HWP: The following two expressions come from April 13th memo: Phi_Inst_cor = -1.0 * Phi_Inst_raw + Instrument_Offset Instrument_Offset = -HWP - 90 Thus, for vertical wires, we have: Phi_Inst_raw = -HWP Putting the results of (1) and (2) together, we get the desired relationship between V_null_rel and HWP.