ANL Tape Station Commissioning
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Transcript of ANL Tape Station Commissioning
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CARIBU System Results Conclusion Extras
First Commissioning Results with the TapeStation at CARIBU
Peter F. Bertone
Physics Division
Argonne National Laboratory
Heavy Ion Discussion15 June 2012
CARIBU Tape Station
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CARIBU System Results Conclusion Extras
Outline
Very Brief Overview of CARIBU
Tape Transport System
Results from Commissioning Runs
Summary and Conclusions
CARIBU Tape Station
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CARIBU System Results Conclusion Extras
CARIBU Tape Station
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CARIBU System Results Conclusion Extras
CARIBU Facility
Platform
Gas Cell
Figures: G. Savard, M. Sternberg
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CARIBU System Results Conclusion Extras
Beam Switch Yard and Tape Station
CARIBU Tape Station
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CARIBU System Results Conclusion Extras
Beam Switch YardSpherical Deflector
Photo: J. Van Schelt
CARIBU Tape Station
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CARIBU System Results Conclusion Extras
Beam Switch YardKicker
Photo: J. Van Schelt
CARIBU Tape Station
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CARIBU System Results Conclusion Extras
CARIBU Science
Figure: G. Savard
CARIBU Tape Station
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CARIBU System Results Conclusion Extras
CARIBU Science(No particular order)
Stopped Beam
Penning trap massmeasurements.
Trap-based studies of
-delayed neutronemission.
spectroscopy withX-Array.
Total absorption -rayspectroscopy (TAGS).
Half-life measurements.
Laser spectroscopy.
Re-Accelerated Beam
Neutron-addingreactions in 132Sn regionusing HELIOS.
Two nucleon-adding/removingreactions in neutron-richAZr region withHELIOS.
Coulex usingGammasphere.
Decay spectroscopy andcalorimetry withGammasphere.
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CARIBU System Results Conclusion Extras
The Purpose of a Tape Station
... is to transport implanted radioactivity to/from detectors. Implant-count-move cycle.
Detect activity in same location as implantation. Move activity to shielded location after set counting time. Avoid background from accumulation of longer-lived
daughter nuclei. e.g. studying shorter-lived nuclei.
Implant-move-count cycle.
Move activity to shielded detector location away from
implantation area. e.g. studying longer-lived nuclei. e.g. hostile implantation environment for detectors.
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CARIBU System Results Conclusion Extras
Possible Uses of a Tape Station
Diagnostics of CARIBU beams based on multiscaling.
Stopped beam experiments. Beam injected into ATLAS.
spectroscopy with X-Array. Half-life measurements.
Total Absorption Spectroscopy.
Transport of activity out/into Gammasphere or FMA focal
plane. And more ...
CARIBU Tape Station
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y
Tape Station Main Components
Implant/detection chamber.
Two apertures defining an implant point on tape. Plastic scintillator detector, light guide, PMT. One or two HPGe -ray detectors.
Tape drive/storage system.
Motor + various belts, gears, sprockets, pulleys. Tape + storage cartridge. Vacuum system.
Control system.
Programmable logic controller (PLC). Programmable motor controller. HV switch for beam kicker.
Data acquisition and electronics.
CARIBU Tape Station
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y
Design Concept
Modularity.
Tape storage/transport components detachable from
experiment-specific components. Portable - could, in principle, be moved to GS or FMA. Flexible - could change to implant-move-count cycle if
needed.
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Implant/Detection Chamber
Simplified schematic:
0 0 0
0 0 0
0 0 0
0 0 0
0 0 0
0 0 0
0 0 0
0 0 0
0 0 0
0 0 0
0 0 0
0 0 00 0 00 0 00 0 00 0 00 0 00 0 00 0 00 0 0
1 1 1
1 1 1
1 1 1
1 1 1
1 1 1
1 1 1
1 1 1
1 1 1
1 1 1
1 1 1
1 1 1
1 1 11 1 11 1 11 1 11 1 11 1 11 1 11 1 11 1 1
0 0 0
0 0 0
0 0 0
0 0 0
0 0 0
0 0 0
0 0 0
0 0 0
0 0 0
0 0 0
0 0 0
0 0 00 0 00 0 00 0 00 0 00 0 00 0 00 0 00 0 0
1 1 1
1 1 1
1 1 1
1 1 1
1 1 1
1 1 1
1 1 1
1 1 1
1 1 1
1 1 1
1 1 1
1 1 11 1 11 1 11 1 11 1 11 1 11 1 11 1 11 1 1
00000000000000001111111111111111
HPGe Detector
Pulleys
Plastic Beta Detectors
Apertures
Mylar Tape
Aluminumcoated
HPGe Detector
To Tape Storage
Beam
Some specifics:
D 1 mm (70% 4).
D 2.5 cm.
30% HPGe detectors.
Apertures: 5.1 mm,6.8 mm, 6 in apart.
35 mm motion picturetape.
Aluminum coatedMylar (1000A).
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Implant/Detection Chamber
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Tape Drive/Storage System
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Tape Drive/Storage System
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Control System
000
000
000
111
111
111
Windows PCLaptop
Stepper Motor
20k step/inch
USB
toDB9
Controller
STAC6Si
LC880
Programmable
Logic
Controller DAQ
(Inhibit Input)
Fast HV
Switch
(Reset Input)
Latching Scaler
To Beam Kicker
HV Supply
MMI 8lead connectorDB9
USB
1
2
3
4
DB9
CAMAC
BNCx4
AMP25
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Commissioning Goals
Demonstrate reliable operation of all system components
under typical experimental conditions. Demonstrate accurate measurement of some known
half-lives.
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How to Measure a Half-LifeUndergrad Physics
Grow-in:(1 et)
Decay:et
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How to Measure a Half-LifeControl System Setup & Multiscaling
000000000111111111
Windows PC
Laptop
Stepper Motor
20k step/inch
USB
to
DB9
Controller
STAC6Si
LC880
Programmable
Logic
Controller DAQ
(Inhibit Input)
Fast HV
Switch
(Reset Input)
Latching Scaler
To Beam Kicker
HV Supply
MMI 8lead connectorDB9
USB
1
2
3
4
DB9
CAMAC
BNCx4
AMP25
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Commissioning RunsOverview
Run #1 - 142Cs Beam.
3 hrs with 1-2 kHz beam rate. , counting in singles.
Run #2 - 142Cs Beam. 6.25 hrs with 1 kHz beam rate. coincidence counting (TAC).
Run #3 - 144Cs Beam.
1.25 hrs with 200 Hz beam rate. coincidence counting (TAC).
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Commissioning RunsOverview (continued)
Run #4 - 146Cs Beam.
Beam rate weak, 10 Hz.
Problems with CARIBU - NO DATA. Run #5 - High speed endurance test (no beam).
Advance tape 5x more often, 2x speed. Mimics conditions for measuring 300 ms T1/2. See how long before something breaks.
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Run #2 - 142Cs Beam
Raw multiscaled data:
Time (sec)0 5 10 15 20 25
(keV)
E
0
500
1000
1500
2000
2500
3000
Cs Beam142Run #2 - Cs Beam142Run #2 -
-gated -ray spectrum:
(keV)E0 200 400 600 800 1000 1200 1400
Counts/keV
0
1000
2000
3000
4000
5000
Cs Beam142Run #2 - Cs Beam142Run #2 -
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-rays Used in 142Cs Half-Life Determination
Ge1GM
Entries310508
Mean 438.6
RMS 355.9
(keV)E200 400 600 800 1000 1200 1400
Counts/k
eV
0
1000
2000
3000
4000
5000
Ge1GM
Entries310508
Mean 438.6
RMS 355.9Run #2
Ba142Cs142
359 keV27%
967 keV9.0%
1326 keV13%
1176 keV4%
Cs Beam142
142Cs -decay: Scott et al J. Phys. G: 6 1291 (1980)
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142Cs Half-Life Determination
Time (sec)0 5 10 15 20 25
(keV)
E
340
345
350
355
360
365
370
375
= 359 keV
Ba, Run #2, E142Cs142 = 359 keV
Ba, Run #2, E142Cs142
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142Cs Half-Life Determination
Time (sec)0 5 10 15 20 25
Counts/100
ms
0
50
100
150
200
250
300
350
400
= 1.68(2) sec1/2T
/n= 1.12
= 359 keV
Ba, Run #2, E142Cs142
Fit:
Background
Background
Tape
Move-DAQV
eto
Grow-in Decay
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142Cs Half-Life DeterminationPreliminaryResults
200 400 600 800 1000 1200 1400
E(keV)
1.2
1.25
1.3
1.35
1.4
1.45
1.5
1.55
1.6
1.65
1.7
1.751.8
1.85
1.9
1.95
2
2.05
2.1
T1/2
(sec)
Weighted Ave = 1.68(2) sec
142Cs Present Data (+/- 1)
(2/n = 1.1)
(1.0) (0.6)(1.2)
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142Cs Half-Life DeterminationComparison to Previous Measurements
1960 1970 1980 1990 2000 2010 2020Year
1.6
1.7
1.8
1.9
2
2.1
2.2
2.3
2.4
2.5
T1/2
(sec)
n,
PriorPresent
142Cs
1.684(14) [ENSDF]
1.68(2) [Present]n,
SFn
n,
?
,
?
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Run #3 - 144Cs Beam
Raw multiscaled data:
Time (sec)0 2 4 6 8 10 12 14 16
(keV)
E
0
200
400
600
800
1000
Cs Beam144Run #3 - Cs Beam144Run #3 -
-gated -ray spectrum:
(keV)E0 100 200 300 400 500 600 700 800
Counts/ke
V
0
50
100
150
200
250
300
350
Cs Beam144Run #3 -
Ba144Cs144
199 keV
144Cs -decay: Scott et al J. Phys. G: 6 1291 (1980)
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144
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144Cs Half-Life Determination
Time (sec)0 2 4 6 8 10 12 14 16
(keV)
E
160
180
200
220
240
= 199 keV
Ba, Run #3, E144Cs144 = 199 keV
Ba, Run #3, E144Cs144
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144C lf f
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144Cs Half-Life Determination
Time (sec)0 2 4 6 8 10 12 14 16
Counts/100
ms
0
10
20
30
40
50
= 0.99(5) sec1/2T
/n= 1.12
= 199 keV
Ba, Run #3, E144Cs144
Fit:
Background Background
Grow-in
Decay
TapeMove-DAQVeto
CARIBU Tape Station
CARIBU System Results Conclusion Extras
144C H lf Lif D i i
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144Cs Half-Life DeterminationPreliminaryResults and Comparison
1960 1970 1980 1990 2000 2010Year
0.88
0.9
0.92
0.94
0.96
0.98
1
1.02
1.04
1.06
1.08
1.1
1.12
1.14
1.16
1.18
1.2
T1/2
(sec)
144Cs
0.99(5) [Present]
0.994(6) [ENSDF] n
n,
n,
(n)
n
n,
n
SF
n
PriorPresent
CARIBU Tape Station
CARIBU System Results Conclusion Extras
R #5 Offli S d d E d T t
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Run #5 - Offline Speed and Endurance Test
In absence of short-lived beam, simulate experimentalconditions:
Set cycle appropriate for T1/2 300 ms measurement.
0.9 s background
0.9 s growth period (3T1/2) 1.8 s decay period (6T1/2) 0.5 s tape advance (2 m/s) 0.9 s background 5 s total cycle time (10% dead-time)
Voluntary termination after 16 hrs with no problems. Could have run longer/faster.
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Summary and ConclusionsAccomplishments
We have successfully assembled, installed andcommissioned a tape station for CARIBU.
We have measured half-lives for 142
Cs and 144
Cs, achievingreasonable precision for 142Cs, and excellent agreement withadopted values in both cases.
We have demonstrated highly reliable operation of thesystem in a over a useful range of cycle times.
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Summary and ConclusionsNext Steps
Attempt real physics measurements with current system.
Work toward vastly improved system utilizing X-Array.
Commission second deflector beamline. Design, build, commission another tape station for 16 mm
tape (faster). Design, build implant/detection chamber to house
detectors and bring tape into X-Array. X-Array development and move to CARIBU.
Decay spectroscopy with 500 mCi source.
CARIBU Tape Station
CARIBU System Results Conclusion Extras
A k l dg ts
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AcknowledgmentsCollaborators
B. DiGiovine (ANL/PHY)C. J. Lister (UMass-Lowell)A. Y. Deo (UMass-Lowell)P. Chowdhury (UMass-Lowell)
J. A. Clark (ANL/PHY)F. G. Kondev (ANL/NE)S. Lakshmi (UMass-Lowell)C. Nair (ANL/NE)J. Rohrer (ANL/PHY)
G. Savard (ANL/PHY)K. Teh (ANL/PHY)J. Van Schelt (UChicago)
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Leading Systematic Effect
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Leading Systematic EffectTime Dependent DAQ Dead-timeRun #1 - 142Cs Beam
0 2 4 6 8 10 12 14 16 18 20Time into Cycle (sec)
0.97
0.98
0.99
1
1.01
AverageLive-timeFraction
(%)
Growth Decay
TapeMov
e-DAQVeto
Background
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Time (sec)0 5 10 15 20 25
(keV)
E
940
945
950
955
960
965
970
975
980
= 967 keV
Ba, Run #2, E142Cs142 = 967 keV
Ba, Run #2, E142Cs142
Time (sec)0 5 10 15 20 25
Counts/1
00ms
0
10
20
30
40
50
60
70
= 967 keV
Ba, Run #2, E142Cs142
= 1.72(6) sec1/2T
/n= 1.02
= 967 keV
Ba, Run #2, E142Cs142
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Time (sec)0 5 10 15 20 25
(ke
V)
E
1140
1150
1160
1170
1180
1190
1200
= 1176 keV
Ba, Run #2, E142Cs142 = 1176 keV
Ba, Run #2, E142Cs142
Time (sec)0 5 10 15 20 25
Counts/1
00ms
0
5
10
15
20
25
30
= 1176 keV
Ba, Run #2, E142Cs142
= 1.7(1) sec1/2T
/n= 0.62
= 1176 keV
Ba, Run #2, E142Cs142
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Time (sec)0 5 10 15 20 25
(ke
V)
E
1300
1305
1310
1315
1320
1325
1330
1335
1340
= 1326 keV
Ba, Run #2, E142Cs142 = 1326 keV
Ba, Run #2, E142Cs142
Time (sec)0 5 10 15 20 25
Counts/1
00ms
0
10
20
30
40
50
60
70
= 1326 keV
Ba, Run #2, E142Cs142
= 1.64(6) sec1/2T
/n= 1.22
= 1326 keV
Ba, Run #2, E142Cs142
CARIBU Tape Station
CARIBU System Results Conclusion Extras
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Run #2 Cs BeamE= 0-800 keV
Ge1GM__1Entries310508
Mean 294.4
RMS 177.1
(keV)E0 100 200 300 400 500 600 700 800
Counts/keV
0
200
400
600
800
1000
1200
Ge1GM__1Entries310508
Mean 294.4
RMS 177.1 Cs Beam142
Run #2 -
La2
32keV(12%)
142
Ba
142
Ce
641keV(47
%)
142
La
142
La
425keV(6%)
142
Ba
142
La25
5keV(21%)
142
Ba
142
511keV
Ba35
9keV(27%)
142
Cs
142
Ba380,
382
keV
142
Cs
142
Ba475keV(0.1
%)
142
Cs
142
Time (sec)0 5 10 15 20 25
(keV)
E
200
300
400
500
600
700
gtmat1__1Entries 310450
Mean x 8.961
Mean y 368.7
RMSx 4.047
RMSy 130.4
gtmat1__1Entries 310450
Mean x 8.961
Mean y 368.7
RMSx 4.047
RMSy 130.4Cs Beam142Run #2 - La) = 10.6 min
142Ba142(1/2T
Ce) = 91.1 min142La142
(1/2T
232 keV
255 keV
425 keV
641 keV
CARIBU Tape Station
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Run #2 Cs BeamE= 800-1500 keV
Ge1GM__1
Entries310508
Mean 1096
RMS 187.4
(keV)E800 900 1000 1100 1200 1300 1400 1500
Coun
ts/ke
V
0
50
100
150
200
250
300
Ge1GM__1
Entries310508
Mean 1096
RMS 187.4 Cs Beam142Run #2 -
La
895ke
V(14%)
142
Ba
142
Ba
967keV(9%)
142
Cs
142
Ba1
326keV(13%)
142
Cs
142
B
a1176keV(4%)
142
Cs
142
Ba1280keV(2%)
142
Cs
142
Ba1064keV(1%)
142
Cs
142
Ba1423keV(1%)
142
Cs
142
Ba1243(0.5
%)
142
Cs
142
La1204keV(6%)
142
Ba
142
Ce1191ke
V(0.4
%)
142
La
142
***unlikely***
~1.6sec
1/2
???
E~1353keV,
TBa933keV(0.5
%)
142
Cs
142
La949keV(11%
)
142
Ba
142
Ba1101keV(0.3%
)
142
Cs
142
La1079keV(12%)
142
Ba
142
Ce1044keV(3%)
142
La
142
La1001keV(10%)
142
Ba
142
Cs984,9
96keV
142
Xe
142
Ce862keV(2%)
142
La
142
Time (sec)0 5 10 15 20 25
(keV)
E
800
900
1000
1100
1200
1300
1400
1500
gtmat1__1
Entries 310450Mean x 8.769Mean y 1096
RMSx 3.701RMSy 187.4
gtmat1__1
Entries 310450Mean x 8.769Mean y 1096
RMSx 3.701RMSy 187.4 Cs Beam
142Run #2 -
La) = 10.6 min142Ba142(1/2T
Ce) = 91.1 min142La142
(1/2T
895 keV
949 keV
1001 keV
1079 keV
1204 keV
1044 keV
CARIBU Tape Station
CARIBU System Results Conclusion Extras
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#E= 1500-2100 keV
Ge1GM__1__1
Entries310508
Mean 1783
RMS 172.5
(keV)E1500 1600 1700 1800 1900 2000 2100
Counts/keV
10
20
30
40
50
60
70
80
90
Ge1GM__1__1
Entries310508
Mean 1783
RMS 172.5 Cs Beam142
Run #2 -
B
a1768ke
V(0
.5%)
142
Cs
142
Ba1818
keV(0.3
%)
142
Cs
142
Ce
1901ke
V(7%)
142
La
142
***un
like
ly***
Ba1935keV(0.3
%)
142
Cs
142
B
a1982ke
V(1
.2%)
142
Cs
142
Ba
1957ke
V(0
.25%)
142
Cs
142
~1.6sec
1/2
???
E~1615keV,
T
Cs1711
keV
142
Xe
142
Time (sec)0 5 10 15 20 25
(keV)
E
1500
1600
1700
1800
1900
2000
2100
Cs Beam142Run #2 -
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#E= 2100-3000 keV
Ge1GM__1Entries310508
Mean 2457
RMS 229.7
(keV)E2100 2200 2300 2400 2500 2600 2700 2800 2900 3000
Counts/keV
0
10
20
30
40
50
60
70
Ge1GM__1Entries310508
Mean 2457
RMS 229.7 Cs Beam142Run #2 -
C
e2398keV(13%)
142
La
142
Ce
2543keV(10%)
142
La
142
Ba2
246keV(0.4
%)
142
Cs
142
~1.6sec
1/2
???
E~2723keV,T
~1.6s
ec
1/2
???
E~2754keV,
T
Time (sec)0 5 10 15 20 25
(keV)
E
2100
2200
2300
2400
2500
2600
2700
2800
2900
3000
gtmat1__1
Entries 310450
Mean x 8.745Mean y 2457
RMSx 3.669
RMSy 229.7
gtmat1__1
Entries 310450
Mean x 8.745Mean y 2457
RMSx 3.669
RMSy 229.7 Cs Beam142
Run #2 -Ce) = 91.1 min142La
142(1/2T
2398 keV
2543 keV
CARIBU Tape Station
CARIBU System Results Conclusion Extras
Run #3 - 144Cs Beam
-
7/25/2019 ANL Tape Station Commissioning
49/51
#E= 0-250 keV
(keV)E60 80 100 120 140 160 180 200 220 240
Counts/keV
0
10
20
30
40
50
60
70
80
90
100
Cs Beam144Run #3 -
Ba199keV
144
Cs
144
La228keV
144
Ba
144
???
La173keV
144
Ba
144
La153keV
144
Ba
144
La104keV
144
Ba
144
La109keV
144
B
a
144La
82keV
144
Ba
144
???
Ba116keV
144
Cs
144
Time (sec)0 2 4 6 8 10 12 14 16
(keV)
E
60
80
100
120
140
160
180
200
220
240
Cs Beam144Run #3 -
short-livedparent seems
parent seems
short-lived
Ba) = 0.994 sec144Cs144
(1/2T
La) = 11.5 sec144Ba144
(1/2T
104 keV
153 keV
173 keV
CARIBU Tape Station
CARIBU System Results Conclusion Extras
Run #3 - 144Cs Beam
-
7/25/2019 ANL Tape Station Commissioning
50/51
#E= 250-450 keV
(keV)E260 280 300 320 340 360 380 400 420 440
Counts/keV
5
10
15
20
25
30
Cs Beam144Run #3 -
Ba
301,3
02,3
08keV
144
Cs
144
Ba331keV
144
Cs
144
B
a348keV
144
Cs
144 L
a355ke
V
144
Ba
144
Ce372-374keV
144
La
144
Ba
144
Cs
144
La430keV
144
Ba
144
Ce397keV
144
La
144
La388keV
144
Ba
144
Cs
144
Ba 394 keV144Cs144
should be here
Ba418
keV
144
Cs
144
Cs405ke
V
144
Xe
144
Time (sec)0 2 4 6 8 10 12 14 16
(keV)
E
260
280
300
320
340
360
380
400
420
440
Cs Beam144Run #3 - Ba) = 0.994 sec144Cs144(1/2T
La) = 11.5 sec144Ba144
(1/2TCe) = 40.8 sec144La
144(1/2T
430 keV
397 keV
388 keV
331 keV
302 keV
CARIBU Tape Station
CARIBU System Results Conclusion Extras
Run #3 - 144Cs Beam
-
7/25/2019 ANL Tape Station Commissioning
51/51
E= 450-800 keV
(keV)E450 500 550 600 650 700 750 800
Counts/keV
0
5
10
15
20
25
30
Cs Beam144Run #3 -
Ba560keV
144
Cs
144
Ba639keV
144
Cs
144
Ba671keV
144
Cs
144
Ba759keV
144
Cs
144
Ce541keV
144
La
144
Ba
144
Cs
144
Time (sec)0 2 4 6 8 10 12 14 16
(keV)
E
450
500
550
600
650
700
750
800
Cs Beam144Run #3 -
759 keV
639 keV
560 keV
Ba) = 0.994 sec144Cs144
(1/2T
CARIBU Tape Station