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Collimator Studies. z location revisited new field map preliminary tilt studies some target boiling results. collimator z-location. back in January we were discussing the collimator design and the backgrounds Roger suggested trying to make the lower edge of the collimator defined - PowerPoint PPT Presentation
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Collimator Studies
• z location revisited
• new field map
• preliminary tilt studies
• some target boiling results
collimator z-location
back in January we were discussing the collimator design and thebackgrounds
Roger suggested trying to make the lower edge of the collimator definedin the most upstream collimator
this would help eliminate the lower edge of the “VT row 20” acceptance defining collimator as a large source of background
turns out that the hit we take because of finite target effects is just too big
collimator z-location
“VT row 20” try to define lower edge upstream
collimator z-location
Version original VT row 20
lower edge upstream
Rate
(MHz/octant)
813 638
<Q2>
(GeV2/c2)
.02611 .02740
Error on Qweak 4.27 4.55
bkgd from ep γ (%)
0.203
+/-.005
0.161
+/-.005
bkgd from mol e- (%)
1.369
+/-.151
2.828
+/-.152
bkgd from mol γ (%)
0.664
+/-.044
0.502
+/-.029
new field map
Compare Q2 distributions for old map (black), new map (red), BFIL 1.00
in April, Jim posted a new field map produced by Peiqing Wang and Willie Falk
the map was based on the “as manufactured” coils, which means that it is not identical in alloctants
Jim had tested the map and noticed that the focus wasn’t as good as with the old map, butit still fit on the bar
as I began testing my implementation of the new map, I discovered some problems with the read-in code having to do with the arrays
should be okay now!
new field map
“VT row 20” with BFIL 1.00 “25cm upstream” with BFIL 1.00
new map comparisonserror on Qweak vs. lower x
4.25
4.30
4.35
4.40
4.45
4.50
4.55
4.60
305 310 315 320 325 330
lower x (cm)
erro
r o
n Q
wea
k (%
) BFIL = 1.00
BFIL = 1.02
BFIL = 1.04
BFIL = 1.00 (old)
Rate vs. lower x
670
690
710
730
750
770
790
810
830
305 310 315 320 325 330
lower x (cm)
erro
r o
n Q
wea
k (%
) BFIL = 1.00
BFIL = 1.02
BFIL = 1.04
BFIL = 1.00 (old)
<Q2> vs. lower x
0.0250
0.0252
0.0254
0.0256
0.0258
0.0260
0.0262
0.0264
0.0266
0.0268
305 310 315 320 325 330
lower x (cm)
erro
r o
n Q
wea
k (%
) BFIL = 1.00
BFIL = 1.02
BFIL = 1.04
BFIL = 1.00 (old)
inelastic % vs. lower x
-0.01
0.09
0.19
0.29
0.39
0.49
0.59
0.69
0.79
0.89
305 310 315 320 325 330
lower x (cm)
erro
r o
n Q
wea
k (%
) BFIL = 1.00
BFIL = 1.02
BFIL = 1.04
BFIL = 1.00 (old)
new map comparisons
Old map, BFIL 1.00. New map, BFIL 1.00. New map, BFIL 1.04.
Blue – Elastic electronsRed – Inelastic Electrons
new map comparisons
VersionGlobal
MediumField map /
BFIL / RRate
(MHz)
<Q2>
(GeV2/c2)error on
Qweak (%)inelastic %
(w/ x10 factor)
original VT heliumold /
1.00 / 313875 .0261 4.18 .086
original VT airold /
1.00 / 313822 .0262 4.26 .076
25 cm upstream
airold /
1.00 / 313798 .02572 4.32 .056
25 cm upstream
airnew /
1.00 / 315811 .02571 4.30 .039
25 cm upstream
airnew /
1.02 / 318814 .02569 4.29 .068
25 cm upstream
airnew /
1.04 / 320807 .02579 4.30 .066
collimator tilt studies
removed “cleanup” collimators
no beamline, new map BFIL 1.00
did not move the quartz bar (lower edge 315cm)
for pitch, roll and yaw ±5º
for x, z ±5 cm
Also assumed all plots were linear, though some obviously aren’t
collimator tilt studies
<Q4> as a function of shift
4.00E-04
5.00E-04
6.00E-04
7.00E-04
8.00E-04
9.00E-04
1.00E-03
1.10E-03
1.20E-03
-6 -4 -2 0 2 4 6
shift (cm or degrees)
<Q4>
Roll (degrees)
Yaw (degrees)
Pitch (degrees)
x (cm)
z (cm)
Rate as a function of shift
400
500
600
700
800
900
1000
1100
1200
1300
-6 -4 -2 0 2 4 6
shift (cm or degrees)
Rat
e (M
Hz/
oct
ant)
Roll (degrees)
Yaw (degrees)
Pitch (degrees)
x (cm)
z (cm)
<Q2> as a function of shift
1.90E-02
2.10E-02
2.30E-02
2.50E-02
2.70E-02
2.90E-02
3.10E-02
3.30E-02
-6 -4 -2 0 2 4 6
shift (cm or degrees)
<Q2> Roll (degrees)
Yaw (degrees)
Pitch (degrees)
x (cm)
z (cm)
par
roll (º) -0.0275 -0.0039 -0.0096
yaw (º) -0.0161 -0.0008 0.0014
pitch (º) -0.0005 0.0039 0.0001
x (cm) -0.0993 0.0505 0.0956
z (cm) 0.0077 -0.0078 -0.0137
par
Q
Q 2
2
1
par
R
R 1
par
Q
Q 4
4
1
Qweak beam tests
performed March 26th , 27th
target boiling studies
low current tests (see Mark’s talk)
beam current monitoring (Dave Mack)
Thanks to everyone who took shifts!
target boiling studies
target boiling studies30 Hz LUMI widths vs. Current
LH2, 8Hz fan, 1.2x1.2 raster
0
200
400
600
800
1000
1200
1400
1600
0 5 10 15 20 25 30 35
Current (uA)
LU
MI w
idth
(p
pm
)
LUMI1
LUMI2
LUMI3
LUMI5
LUMI6
LUMI7
LUMI8
30 Hz LUMI widths vs. CurrentLH2, 40Hz fan, 1.8x1.8 raster
0
100
200
300
400
500
600
700
0 5 10 15 20 25 30
Current (uA)
LU
MI w
idth
(p
pm
)
LUMI1
LUMI2
LUMI3
LUMI5
LUMI6
LUMI7
LUMI8
250 Hz LUMI widths vs. CurrentLH2, 8Hz fan, 1.2x1.2 raster
0
2000
4000
6000
8000
10000
12000
14000
0 5 10 15 20 25 30
Current (uA)
LU
MI w
idth
(p
pm
)
LUMI1
LUMI2
LUMI3
LUMI5
LUMI6
LUMI7
LUMI8
250 Hz LUMI widths vs. CurrentC, 8Hz fan, 1.2x1.2 raster
0
5000
10000
15000
20000
25000
0 5 10 15 20 25 30
Current (uA)
LU
MI w
idth
(p
pm
)LUMI1, C
LUMI2, C
LUMI3, C
LUMI5, C
LUMI6, C
LUMI7, C
LUMI8, C
250 Hz LUMI widths vs. CurrentLH2, 40Hz fan, 1.8x1.8 raster
0
2000
4000
6000
8000
10000
12000
0 5 10 15 20 25
Current (uA)
LU
MI w
idth
(p
pm
)
LUMI1
LUMI2
LUMI3
LUMI5
LUMI6
LUMI7
LUMI8
30 Hz LUMI widths vs. CurrentC, 8Hz fan, 1.2x1.2 raster
0
200
400
600
800
1000
1200
1400
1600
1800
0 5 10 15 20 25 30
Current (uA)
LU
MI w
idth
(p
pm
)
LUMI1, C
LUMI2, C
LUMI3, C
LUMI5, C
LUMI6, C
LUMI7, C
LUMI8, C
target boiling studies
30 Hz, 8Hz fan, 1.2x1.2 raster, C 30 Hz, 8Hz fan, 1.2x1.2 raster, C
250 Hz, 8Hz fan, 1.2x1.2 raster, C 250 Hz, 8Hz fan, 1.2x1.2 raster, C