;                    BPM calibration constants
;                    =========================
  guse_bpm_in_recon  = 0   ; if 1 use bpm information for reconstruction
  guse_bpmc    = 1   ; if 1 use bpm c information for reconstruction
  gbpm_sample  = 500 ; number of events, which are used for average 
                     ; beam position ( <5000 ). Optimal value dep. on rate

; These are from CSA's initial bpm cal 4/5/99, runs 24950, 51, 
; 54, 57, and 59.
;  gbpm_kappa   = 1.500,1.302,1.330 ; sensitivity in cm
;  gbpm_alpha_x = 1.00, 1.00, 1.00  ; calibration gain: we may get them from the
;  gbpm_alpha_y = 1.00, 1.00, 1.00  ;  EPICS events, right now that's according to Paul's note
; According to Accel (from Paul G):
;  gbpm_kappa   = 1.889,1.889,1.889 ; sensitivity in cm
  gbpm_kappa   = 1.85,1.85,1.85     ; sensitivity in cm
  gbpm_alpha_x = 0.929157, 1.08666, 1.01899
  gbpm_alpha_y = 1.065, 1.03812, 0.956884

; The following offsets get added to the calculated positions
; These are from CSA's initial bpm cal 4/5/99, runs as above.
;  gbpm_x_off = 0.069,-0.045,-0.045
;  gbpm_y_off = 0.038,-0.097,0.022
  gbpm_x_off = 0.,0.,0.
  gbpm_y_off = 0.,0.,0.

; average beam positions: only used if 'guse_bpm=0' 
;  gbeam_xoff  = +0.18
  gbeam_xoff  = +0.00
  gbeam_xpoff = +0.00
  gbeam_yoff  = +0.00
  gbeam_ypoff = +0.00

; spectrometers would like to see these positions (from optics studies) 
; we treat SOS and HMS the same, however, we may change this if necessary
;  gspec_xoff  = +0.18
  gspec_xoff  = +0.00
  gspec_xpoff = +0.00
  gspec_yoff  = +0.00
  gspec_ypoff = +0.00

; Pedestals for BPM ADCs: from cosmic runs 24941 and 42,
; 4/5/99 (look at histos for X+, etc.; the peds file may
; include high-adc events). CSA.
  gbpm_xp_ped = 952.,  1041.,  954.
  gbpm_xm_ped = 1012., 1043.,  954.
  gbpm_yp_ped = 964.,  1013.,  887.
  gbpm_ym_ped = 1110., 969.,   954.

; positions of BPMs relative to target
  gbpm_zpos = 327.,231.,136.

;             Fast Raster calibration constants
;             =================================

; Various fast raster quantities: gUse* are flags

  gusefr               = 1  ; if 1 correct for FRY in reconstruction

  guse_frdefault       = 1  ; if 1 do no phase correction (default)
      gfr_cal_mom      = 3.245  ; = beam momnetum during calibration run 
;      gfrx_adcpercm    = 11328. ; = FR channels per cm deflection on target
;      gfry_adcpercm    = 10708. ; from run 9981, August 25, 1996, book X-22

; the 1.4125 and 1.5811 come from modified attenuation
; the 2.2/3.0 came from a recalibration against the cryotarget ladder motion.
; 7/28/99 -- Now change x gain from 0.02 to 0.06 and y gain from
; 0.04 to 1.0
      gfrx_adcpercm    = (11328./1.4125*2.2/3.0*0.06/0.02) ; -3 db attenuator added
      gfry_adcpercm    = (10708./1.5811*2.2/3.0*0.1/0.04) ; -10 db AND double gain on module.

                            ;if 0 apply phase correction 
      gfrx_dphase      = 0.0    ; phase shift (never measured for x so far) 
      gFrx_synccut     = 0.     ; should be zero if applied on centered distr.
      gfrx_adcmax      = 1000   ; ADC amplitude in channels.
      gfrx_maxsize     = 0.1    ; fast raster amplitude in centimeter.

      gfry_dphase      = 5.8    ; phase shift 
      gFry_synccut     = 0.     ; should be zero if applied on centered distr.
      gfry_adcmax      = 1000   ; ADC amplitude in channels.
      gfry_maxsize     = 0.1    ; fast raster amplitude in centimeter.

; The latest FR phase analysis from spring '96 showed, that there is no
; measurable phase shift. During early running (E91-13, E89-12) the FRY-phase
; was determined to be 5.8 degree.

; positions of FR magnets relative to target
  gfrx_dist  = 2111   ; cm
  gfry_dist  = 2071   ; cm