SLAC Magnetic Measurements
Date: 03-24-2015
Time: 12:31:47
 
EPU Analysis
------------

Data File Header:
SLAC Magnetic Measurements
Date: 12-03-2014
Time: 12:08:28
Hall Probe Array Analysis
*************************
Bx, By, and Bz vs z:
     Z           Bx           By           Bz     
    (m)          (T)          (T)          (T)    
-----------  -----------  -----------  -----------

Analysis Parameters:
Input file directory = V:\MET\MagServe\MagData\DELTA\Delta data\Assembled Measurements\Final Measurements\LP24N\KR0565\
Input file name = hall2_anal_probe1_field.dat
Input file type = ZBXYZH
Correction required = 0
Correction, Bx multiplicative factor = 1.000000 
Correction, By multiplicative factor = 1.000000 
Correction, Bx additive constant = -0.000005 T
Correction, By additive constant = -0.000013 T
Correction Bxy additive file = none
Correction Bxy additive file type = CORR_ZBXY
Electron gamma = 26671.590000
Electron energy = 13.629158 Gev
Nominal undulator period = 0.000000 m
Nominal K value = 0.000000
Nominal radiation wavelength = 0.000000e+00 m
Number of undulator poles = 196
Number of end poles (used in analysis) = 4
Cell length = 3.656000 m
Nominal phase change through cell = 709.999940 rad
Nominal phase of pole after end poles = 61.261057 rad
Number of poles for entrance and exit phase error statistics = 5

Bx Peak And Zero Field Summary:
Number of Poles = 198
Number of End Poles (excluded in statistics) = 4
Peak Fields: Ave = 0.480399 T, RMS = 0.011756 T
Peak Field Spacing: Ave = 0.016002 m, RMS = 0.000095 m
Zero Field Spacing: Ave = 0.016003 m, RMS = 0.000088 m
Average Undulator Period = 0.032006 m

By Peak And Zero Field Summary:
Number of Poles = 196
Number of End Poles (excluded in statistics) = 4
Peak Fields: Ave = 0.514136 T, RMS = 0.010411 T
Peak Field Spacing: Ave = 0.016001 m, RMS = 0.000110 m
Zero Field Spacing: Ave = 0.016001 m, RMS = 0.000086 m
Average Undulator Period = 0.032002 m

Bx Field Harmonics:
In the undulator center, over an integer number of periods, expand Bx as
Bx(z) = a0 + Sum{ an cos(n 2 pi z / lambda_u) + bn sin(n 2 pi z / lambda_u) }
   n         an        bn   
            (T)       (T)   
--------  --------  --------
   0      -0.00015
   1      -0.01129  -0.46925
   2       0.00069   0.00036
   3       0.00025  -0.00022
   4      -0.00004  -0.00004
   5      -0.00434  -0.01000
   6       0.00004  -0.00001
   7      -0.00002  -0.00004
   8      -0.00001   0.00003
   9      -0.00008  -0.00016
  10       0.00001  -0.00003
  11      -0.00001  -0.00001
  12      -0.00001   0.00002
  13       0.00002  -0.00000
  14       0.00000  -0.00003
  15      -0.00002   0.00000
  16       0.00000   0.00002
  17       0.00002  -0.00001
  18      -0.00001  -0.00002
  19      -0.00002   0.00001
  20       0.00001   0.00002

By Field Harmonics:
In the undulator center, over an integer number of periods, expand By as
By(z) = a0 + Sum{ an cos(n 2 pi z / lambda_u) + bn sin(n 2 pi z / lambda_u) }
   n         an        bn   
            (T)       (T)   
--------  --------  --------
   0      -0.00007
   1      -0.00301   0.50445
   2      -0.00060  -0.00029
   3       0.00076   0.00062
   4       0.00006  -0.00002
   5       0.00227   0.00942
   6      -0.00009  -0.00001
   7      -0.00003   0.00007
   8       0.00003  -0.00002
   9       0.00015   0.00024
  10      -0.00002   0.00002
  11       0.00002   0.00001
  12       0.00001  -0.00002
  13      -0.00003  -0.00001
  14      -0.00001   0.00003
  15       0.00003   0.00001
  16       0.00001  -0.00003
  17      -0.00003  -0.00000
  18      -0.00000   0.00003
  19       0.00002  -0.00000
  20      -0.00001  -0.00002

Hall Probe Overall Field Integrals:
Int Bx dz =   -1.1641e-04 Tm
Int Int Bx dz dz =   -4.0333e-04 Tm^2
Int By dz =    1.0403e-05 Tm
Int Int By dz dz =   -1.1209e-04 Tm^2

Trajectory Exit Information:
X at exit =   -2.4655e-06 m
X slope at exit =    2.2883e-07
Y at exit =    8.8718e-06 m
Y slope at exit =    2.5606e-06

Calculated Undulator Parameters:
Keff = 2.068240
Beff = 0.692109 T
Lambda_rad = 7.060615e-11 m

Phase Integral:
PI = Int_(z_enter)^(z_exit) {[Int_(-inf)^(z) Bx(z*) dz*]^2 + [Int_(-inf)^(z) By(z*) dz*]^2} dz (T^2m^3)
PI =   1.930e-05 T^2m^3
PI Of Cell =   1.930e-05 T^2m^3

Effective Length:
Leff =   3.099883 m

Phase Fluctuations:
Slippage vs Z At Peaks Fitted Slope =    2.20616e-09
Undulator Period = 0.032004 m
Radiation Wavelength =    7.06062e-11 m
Phase Error (From Slippage vs Z Fit Residuals):
  Ave = 0.000000 deg, RMS = 14.194023 deg

Phase Relative To Nominal Radiation Wave:
Nominal Radiation Wavelength =    0.00000e+00 m, (if 0, use radiation wavelength)
Cell Length = 3.656000 m
Number Of End Poles = 4
Entrance:
  Phase Error Of First 5 Poles After The End Poles
  Ave = -1859.138064 deg, RMS = 4.450726 deg
Center:
  Phase Error Of All Poles In Undulator Center:
  Ave = -1883.694833 deg, RMS = 14.424885 deg
Exit:
  Phase Error To Cell Boundary Of Last 5 Poles Before The End Poles
  Ave = -1861.956944 deg, RMS = 8.720361 deg
Cell:
  Phase Change Of Cell =   36912.185 deg
  Nominal Phase Change Of Cell =   40680.000 deg
  Phase Error Of Cell =   -3767.815 deg

Spontaneous Radiation:
(Forward direction)
Single electron at fundamental:
  |Ex| = 1.178713e-11 (V/m), |Ey| = 1.081384e-11 (V/m)
  Angle_y - Angle_x = 2.658347 (deg)
Stokes Parameters:
  S0 = Ix + Iy = 2.558755e-22, S1 = Ix - Iy = 2.199742e-23 (V/m)^2
  S2 = I45 - I135 = 2.546539e-22, S3 = Ir - Il = 1.182364e-23 (V/m)^2
Polarization Rates:
  P1 = S1 / S0 = 0.085969, P2 = S2 / S0 = 0.995226
  P3 = S3 / S0 = 0.046209
Spectra:
(Ideal = calc field period using FT coeff repeated with no phase errors)
Harmonic   Energy   Ang Num Spect       Ideal        Efficiency 
   #       (keV)     (ph/sec/mrad^2/0.1%bw/0.1A)          %   
--------  --------  --------------  --------------  ------------
   1        17.560       8.040e+18       8.807e+18         91.29
   2        35.120       9.255e+16        ---            ---
   3        52.680       6.840e+18       1.278e+19         53.53
   4        70.240       1.568e+17        ---            ---
   5        87.800       1.933e+18       1.112e+19         17.38
   6       105.360       6.638e+16        ---            ---
   7       122.920       3.688e+17       8.902e+18          4.14
   8       140.480       3.635e+15        ---            ---
   9       158.040       5.511e+17       5.641e+18          9.77
  10       175.600       3.834e+16        ---            ---
  11       193.160       5.665e+17       4.501e+18         12.58
  12       210.720       7.770e+16        ---            ---
  13       228.280       3.164e+17       2.555e+18         12.38
  14       245.840       8.722e+16        ---            ---
  15       263.400       1.063e+17       2.577e+18          4.12
