Last updated 04:00 – 03/27/03 js
Date |
Cell |
Style |
Density |
Sat. Pol. |
Pol. |
Lifetime |
<Wall AB>
|
<Wall BA>
|
Win
A |
Win
B |
12/03/02 |
Proteus |
Right IC |
6.90 |
48.9% |
42.6% |
74 |
|
|
|
|
08/07/02 |
Patton |
Right IC |
6.97 |
~40%* |
- |
58 |
|
|
|
|
11/20/02 |
Phubar |
Right IC |
6.82 |
39.3% |
37.3% |
46 |
|
|
|
|
06/20/02 |
Prasch |
Right IC |
6.96 |
35.3% |
32.0% |
33 |
|
|
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|
01/14/03 |
Priapus |
40 cm |
8.96 |
|
|
56 |
|
|
|
|
02/25/03 |
Penelope |
40 cm |
9.28 |
|
|
54 |
|
|
|
|
03/26/03 |
Powell |
40 cm |
9.25 |
39.0% |
37.9% |
25 |
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This is the current list of cells that could be used in sGDH. All cells are made of C1720 by Mike Souza @ Princeton. Most numbers are from characterizations done at UVa.
All lifetime numbers have been corrected for AFP Loss if possible. Data is posted as it is taken.
The most up-to-date data & raw data can be attained by emailing me at (Jaideep Singh) js7uq@virginia.edu.
Date |
Cell |
Style |
Sat.
Pol. |
TC |
Pol |
Lifetime |
RAW |
He-He Dipole |
“Wall” |
12/03/02 |
Proteus |
Right IC |
48.9% |
27.1 hrs |
42.6% |
74 |
70 |
108 |
236 |
08/07/02 |
Patton |
Right IC |
~40%* |
- |
- |
58 |
53 |
107 |
127 |
11/20/02 |
Phubar |
Right IC |
39.3% |
18.3 hrs |
37.3% |
46 |
44 |
109 |
80 |
06/20/02 |
Prasch |
Right IC |
35.3% |
12.5 hrs |
32.0% |
33 |
32 |
107 |
48 |
|
|
|
|
|
|
|
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|
|
01/14/03 |
Priapus |
40 cm |
|
|
|
56 |
53 |
83 |
172 |
02/25/03 |
Penelope |
40 cm |
|
|
|
54 |
54 |
80 |
165 |
03/27/03 |
Powell |
40 cm |
39.0% |
12.7 hrs |
37.9% |
25 |
25 |
80 |
36 |
|
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Saturation polarization & TC are from the fit of the spinup. Pol is the highest polarization measured via the EPR Freq shift method. Lifetimes are corrected for AFP losses.
The “RAW” numbers are from fits to exp. Decay w/o correcting for afp losses. The reason these two numbers are very close is b/c we intentionally make the avg time interval
between measurements very long to minimize the effect of the afp losses. He-He dipole is the theoretical maximum lifetime. “Wall” is the lifetime subtracting out the dipole interaction
Date |
Cell |
He3
<Dens> |
He3
D1 |
He3
D2 |
He3
<D1/D2> |
He3
Fill |
N2
Fill |
12/03/02 |
Proteus |
|
|
|
|
6.90 |
0.0920 |
08/07/02 |
Patton |
|
|
|
|
6.97 |
0.0871 |
11/20/02 |
Phubar |
|
|
|
|
6.82 |
0.0846 |
06/20/02 |
Prasch |
6.96 |
6.96 |
6.96 |
6.96 |
6.96 |
0.0845 |
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01/14/03 |
Priapus |
|
|
|
|
8.96 |
0.0962 |
02/25/03 |
Penelope |
|
|
|
|
9.28 |
0.0939 |
03/26/03 |
Powell |
|
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|
|
9.25 |
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The fill numbers come from calculating the number of particles of gas put into the cell divided by the volume. The pressure broadening density is attained from fitting the Rb absorption lines at D1 – 795nm and D2 – 780nm to an asymmetric Lorentzian lineshape. From the fit we extract the width of the lineshape which is linearly proportional to the density of the perturbing gases in the cell. Broadening due to the Doppler effect, wall collisions, and collisions with other Rb atoms are tiny and therefore neglected. However, the raw data is corrected for the temperature of the cell and for the broadening due to collisions with N2. Each are <1% corrections. 1 amagat = 2.6e25 particles per cubic meter.
A Sample Pressure Broadening scan of Tilghman can be found here.
Cell |
Archimedes Internal |
Fill Internal |
Calculated
Internal |
Archimedes External |
Calculated
External |
Pumping
Chamber |
Transfer
Tube |
Target Chamber |
Proteus |
|
235.0 |
234.1 |
|
276.7 |
91.1 |
3.38 |
140.4 |
Patton |
|
250.8 |
250.7* |
|
- |
105.28 |
5.2* |
140.3* |
Phubar |
|
247.2 |
252 |
|
297.5 |
102.5 |
4.42 |
142.7 |
Prasch |
|
256.6 |
257.7* |
|
- |
114.3* |
3.39* |
139.5* |
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Priapus |
|
207.7 |
195.4 |
|
252.4 |
114.2 |
4.04 |
83.3 |
Penelope |
|
203.9 |
187.4 |
|
243.6 |
106.1 |
4.17 |
85.4 |
Powell |
|
206.6 |
|
|
|
115.3 |
4.0 |
87.3 |
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The volumes of the various chambers are calculated using a model and external dimension measurements. They are then scaled to sum to the volume as measured from the Archimedes volume method.
* denotes measurements made directly by Willie using methanol.
Cell |
VD |
HD |
T2P |
TTL |
TTD |
TCL |
TCDA |
TCDB |
TCDC |
TCDD |
TCDE |
<TCD> |
Proteus |
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Patton |
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Phubar |
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Prasch |
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Priapus |
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Penelope |
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Powell |
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VD – vertical diameter of pumping chamber, equivalent to distance from top of pumping chamber to top of transfer tube
HD – horizontal diameter of pumping chamber
T2P – tipoff length, equivalent to distance from top of tipoff to top of pumping chamber
TTL – transfer tube length, equivalent to distance from bottom of pumping chamber to top of target chamber
TTD – transfer tube diameter
TCL – target chamber length, this is measured from tip of window to tip of window
TCDA – target chamber diameter on window tube
TCDB – target chamber diameter past window to main tube seal
TCDC – target chamber diameter past the transfer tube but before main tube to window tube seal
TCDD – target chamber diameter on opposite window tube
TCDE – target chamber diameter on the middle of the target chamber.
<TCD> - average target chamber diameter
“tops” and “bottoms” are arbitrary, however, every attempt is made to measure each cell using the same criteria for “top” and “bottom.
A diagram of this is shown above.
Cell |
A |
B |
C |
D |
E |
F |
G |
H |
I |
J |
K |
L |
M |
N |
O |
P |
Q |
R |
S |
Proteus |
0.6556 |
0.6121 |
0.6187 |
0.6069 |
0.6073 |
1.428 |
1.314 |
1.313 |
1.284 |
1.341 |
1.277 |
1.302 |
1.415 |
0.7113 |
0.7100 |
0.7115 |
0.7177 |
0.6915 |
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Patton |
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Phubar |
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Prasch |
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Priapus |
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Penelope |
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Powell |
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(REF CELLS) |
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Proust |
0.8622 |
0.8538 |
0.8382 |
0.8572 |
0.8487 |
0.8685 |
0.8688 |
1.147 |
1.250 |
1.177 |
1.178 |
1.083 |
1.014 |
1.111 |
1.190 |
1.436 |
0.8759 |
0.8874 |
0.8794 |
Pushkin |
0.7997 |
0.8351 |
0.8223 |
0.8397 |
0.8434 |
1.308 |
1.373 |
1.286 |
1.392 |
1.363 |
1.302 |
1.339 |
0.8674 |
0.8997 |
0.8328 |
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Pax |
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Cell |
Label
|
Optical |
Thin
|
Beam |
|
|
Proteus |
4 |
126.2 |
201.6 |
231.7 |
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Patton |
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Phubar |
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Prasch |
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Priapus |
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Penelope |
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Powell |
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REF CELLS |
Label |
Optical |
Thin |
Beam |
|
|
Proust |
|
129.1 |
374.2 |
379.5 |
|
|
Pushkin |
IX |
155.8 |
249.0 |
258.9 |
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Pax |
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