Time Scan
Scanning over time and increasing it from 1 day to 2 weeks in intervals of one day, we get:
1 Week Measurement
Given one PAC week, using the SHMS and an 11 GeV beam on an 30% tensor polarized target, we can expect to get a good measurement from <math>0.8 > x > 1.8</math>
Beam Energy = 11.0 GeV
<math><x></math> |
<math>dA_{zz}^{stat}</math> |
<math>dA_{zz}^{sys}</math>
|
0.8 |
0.716E-02 |
0.526E-02
|
0.9 |
0.675E-02 |
0.120E-01
|
1.0 |
0.525E-02 |
0.249E-03
|
1.1 |
0.569E-02 |
0.307E-01
|
1.2 |
0.941E-02 |
0.667E-01
|
1.3 |
0.140E-01 |
0.924E-01
|
1.4 |
0.194E-01 |
0.998E-01
|
1.5 |
0.130E-01 |
0.100E+00
|
1.6 |
0.124E-01 |
0.100E+00
|
1.7 |
0.222E-01 |
0.100E+00
|
1.8 |
0.204E-01 |
0.100E+00
|
Spectrometer |
Total Rates (kHz) |
QE Physics Rates (W≤0.8) (kHz) |
SRC Physics Rates (W<0.8) (kHz)
|
HMS |
--- |
--- |
---
|
SHMS |
1.03 |
0.789 |
0.0273
|
Beam Energy = 8.8 GeV
<math><x></math> |
<math>dA_{zz}^{stat}</math> |
<math>dA_{zz}^{sys}</math>
|
0.8 |
0.345E-02 |
0.526E-02
|
0.9 |
0.324E-02 |
0.120E-01
|
1.0 |
0.387E-02 |
0.249E-03
|
1.1 |
0.264E-02 |
0.307E-01
|
1.2 |
0.416E-02 |
0.667E-01
|
1.3 |
0.565E-02 |
0.924E-01
|
1.4 |
0.101E-01 |
0.998E-01
|
1.5 |
0.967E-02 |
0.100E+00
|
1.6 |
0.131E-01 |
0.100E+00
|
1.7 |
0.169E-01 |
0.100E+00
|
1.8 |
0.286E-01 |
0.100E+00
|
Spectrometer |
Total Rates (kHz) |
QE Physics Rates (W≤0.8) (kHz) |
SRC Physics Rates (W<0.8) (kHz)
|
HMS |
|
|
|
SHMS |
|
|
|
Beam Energy = 6.6 GeV
<math><x></math> |
<math>dA_{zz}^{stat}</math> |
<math>dA_{zz}^{sys}</math>
|
0.8 |
0.146E-02 |
0.526E-02
|
0.9 |
0.141E-02 |
0.120E-01
|
1.0 |
0.167E-02 |
0.249E-03
|
1.1 |
0.204E-02 |
0.307E-01
|
1.2 |
0.377E-02 |
0.667E-01
|
1.3 |
0.154E-02 |
0.924E-01
|
1.4 |
0.205E-02 |
0.998E-01
|
1.5 |
0.268E-02 |
0.100E+00
|
1.6 |
0.464E-02 |
0.100E+00
|
1.7 |
0.387E-02 |
0.100E+00
|
1.8 |
0.476E-02 |
0.100E+00
|
Spectrometer |
Total Rates (kHz) |
QE Physics Rates (W≤0.8) (kHz) |
SRC Physics Rates (W<0.8) (kHz)
|
HMS |
|
|
|
SHMS |
|
|
|
Beam Energy = 4.4 GeV
<math><x></math> |
<math>dA_{zz}^{stat}</math> |
<math>dA_{zz}^{sys}</math>
|
0.8 |
0.906E-03 |
0.526E-02
|
0.9 |
0.782E-03 |
0.120E-01
|
1.0 |
0.816E-03 |
0.249E-03
|
1.1 |
0.115E-02 |
0.307E-01
|
1.2 |
0.153E-02 |
0.667E-01
|
1.3 |
0.231E-02 |
0.924E-01
|
1.4 |
0.247E-02 |
0.998E-01
|
1.5 |
0.108E-02 |
0.100E+00
|
1.6 |
0.127E-02 |
0.100E+00
|
1.7 |
0.149E-02 |
0.100E+00
|
1.8 |
0.234E-02 |
0.100E+00
|
Spectrometer |
Total Rates (kHz) |
QE Physics Rates (W≤0.8) (kHz) |
SRC Physics Rates (W<0.8) (kHz)
|
HMS |
|
|
|
SHMS |
|
|
|
Beam Energy = 2.2 GeV
<math><x></math> |
<math>dA_{zz}^{stat}</math> |
<math>dA_{zz}^{sys}</math>
|
0.8 |
0.954E-03 |
0.526E-02
|
0.9 |
0.895E-03 |
0.120E-01
|
1.0 |
0.661E-03 |
0.249E-03
|
1.1 |
0.900E-03 |
0.307E-01
|
1.2 |
0.135E-02 |
0.667E-01
|
1.3 |
0.137E-02 |
0.924E-01
|
1.4 |
0.134E-02 |
0.998E-01
|
1.5 |
0.119E-02 |
0.100E+00
|
1.6 |
0.160E-02 |
0.100E+00
|
1.7 |
0.169E-02 |
0.100E+00
|
1.8 |
0.220E-02 |
0.100E+00
|
Spectrometer |
Total Rates (kHz) |
QE Physics Rates (W≤0.8) (kHz) |
SRC Physics Rates (W<0.8) (kHz)
|
HMS |
|
|
|
SHMS |
|
|
|
--E. Long 15:47, 20 September 2013 (UTC)