List of good runs and kinematics detail
All good runs have coincident time centered at 99 ns.
Units: Energy in GeV, momentum in GeV/c, angle in degree.
Kinematics terms:
Liquid Deuterium runs on 2-pass (2.345 GeV) beam: protons in the LHRS and electrons in the RHRS
(1) LDK0 : Liquid Deuterium rus (15 cm Target) with momentum settings: LHRS 0.9803, RHRS 1.8875.
In all of the following 4-pass (4.6275 GeV) beam kinematics, electrons are detected in the LHRS and protons in the RHRS.
(2) LDK1 : Liquid Deuterium runs (15 cm Target) with momentum settings: LHRS 3.7612, RHRS 1.4515.
(3) LDK2 : Liquid Deuterium runs (4 cm Target) with momentum settings: LHRS 3.7612, RHRS 1.4515.
(4) LDK3 : Liquid Deuterium runs (4 cm Target) with momentum settings: LHRS 3.7232, RHRS 1.4315.
(5) CK1a : Carbon runs with momentum settings: LHRS 3.7612, RHRS 1.4515.
(6) CK1b : Carbon runs with momentum settings: LHRS 3.7232, RHRS 1.4515
(7) CK2 : Carbon runs with momentum settings: LHRS 3.7232, RHRS 1.4215.
(8) CK3 : Carbon runs with momentum settings: LHRS 3.7232, RHRS 1.3614.
Kinematics Table
Kinematics
|
Ee GeV
|
Ee' GeV
|
&thetae' degree
|
&omega GeV
|
Q2 (GeV/c)2
|
xB
|
&thetap degree
|
|q| GeV/c
|
Pmiss GeV/c
|
LDK0
|
2.3452
|
1.8875
|
-17.197
|
0.4577
|
0.3958
|
0.461
|
53.89
|
0.778
|
0.24
|
LDK1
|
4.6275
|
3.7612
|
19.5
|
0.8663
|
1.9966
|
1.229
|
-40.1
|
1.657
|
0.3
|
LDK2
|
4.6275
|
3.7612
|
19.5
|
0.8663
|
1.9966
|
1.229
|
-40.1
|
1.657
|
0.3
|
LDK3
|
4.6275
|
3.7232
|
19.5
|
0.9043
|
1.9765
|
1.165
|
-32
|
1.672
|
0.45
|
CK1a
|
4.6275
|
3.7612
|
19.5
|
0.8663
|
1.9966
|
1.229
|
-40.1
|
1.657
|
0.3
|
CK1b
|
4.6275
|
3.7232
|
19.5
|
0.9043
|
1.9765
|
1.165
|
-40.1
|
1.672
|
0.3
|
CK2
|
4.6275
|
3.7232
|
19.5
|
0.9043
|
1.9765
|
1.165
|
-35.8
|
1.672
|
0.4
|
CK3
|
4.6275
|
3.7232
|
19.5
|
0.9043
|
1.9765
|
1.165
|
-32
|
1.672
|
0.5
|
Run Numbers:
LDK0 : 1727-1734, 1736-1747, 1749, 1750, 1753-1757, 1765-1769.
Total Charge: 0.4781932 C.
LDK1 :1797-1804, 2056-2069, 2083-2098, 2103-2105.
Total Charge: 1.097451 C.
LDK2 : 1805-1808,1810-1824,1826-1830,1832-1849,1857-1859,1861-1863,1865,1867,2568-2574, 2577-2623.
Total Charge: 8.020035 C.
LDK3 : 3299, 3325-3327, 3329-3337, 3418-3424, 3426-3431.
Total Charge: 0.610306 C.
CK1a : 1868-1871, 1886, 1888, 1900-1903, 1913, 1915, 1917-1932, 1935, 1937-1961, 1965-1967, 1981-1997, 2000-2003, 2009-2017, 2019-2037,2039, 2043-2055, 2106-2116, 2129-2133, 2135-2137, 2139-2141, 2144-2152, 2154-2169, 2171-2175, 2181-2182, 2184-2186, 2190-2191, 2193-2194, 2198, 2200, 2206-2214, 2575-2576, 2624-2625, 2627, 2629-2636, 2638, 2641-2644, 2648-2651.
Total Charge: 8.2218461 C.
CK1b : 2655, 2657-2677, 2697-2716, 2718-2719, 2721, 2723-2737, 2739-2741, 2744-2766, 2768-2787, 2789-2794, 2797-2807, 2809, 2811-2816, 2818-2827, 2830-2846, 2853, 2858-2878, 2880-2882, 2884, 2887-2892, 2894, 2895.
Total Charge: 16.0233445 C.
CK2 : 2898, 2906-2911, 2914-2926, 2929-2952, 2954-2956, 2962-2997, 3003-3013, 3015-3033, 3042-3049, 3052-3061, 3064, 3067-3071, 3074-3078, 3080-3091, 3093-3095, 3108-3118, 3120, 3125-3144, 3179-3181, 3183-3184, 3186-3200, 3202, 3209.
Total Charge: 20.1580766 C.
CK3 : 3211, 3217-3266, 3273, 3276-3291, 3302-3315, 3320-3324, 3338-3342, 3345, 3353, 3365-3375, 3378, 3380-3386, 3389-3404, 3407-3414.
Total Charge: 14.4846965 C.
Some footnotes:
In calculating the total charge, "BCM u3" reading was used from the "End of Run" info.
Each of the following runs has two "End of run" info:
2627, 2754, 2779 and 3064.
During analysis, the analyzer crashes for the runs 2748 [after 148k events], 2963 [after 154k events] and 2980 [after 157k events] while the run 3220 has ThaSlotData-problem between the events 136 to 151 k.
Most of the runs from 1882 to 1916 do not have Coincident timing info [CT.ct_2by1 or CT.ct_1by2]. Many of them are junk.
Runs 1917 to 1967 do not have CT.ct_2by1. (but they have CT.ct_1by2).
Total charge of all the 4-pass carbon runs is about 59 C.
The numbers in the kinematics table are all "central" values.
Production data were taken in constant (q,&omega) kinematics by fixing electron kinematics. The recoil momenutm was varied by detecting the ejected proton at different angles with respect to q.
Maintained by: Ramesh Raj Subedi.
Last updated: Sept 4, 2006.