SAUNA III – a major upgradeSAUNA III main specifications SAUNA II SAUNA III Carrier gas Helium...
Transcript of SAUNA III – a major upgradeSAUNA III main specifications SAUNA II SAUNA III Carrier gas Helium...
Anders Ringbom, Anders Axelsson, Mattias Aldener, Tomas Fritioff, Johan Kastlander, Anders Mörtsell
Swedish Defence Research Agency (FOI)
SAUNA III – a major upgrade
Outline
• Scientific reasons to develop the noble gas systems in IMS.
• SAUNA III development:
• Collection and processing
• Detector
• Software
• Summary and Conclusions
Why do we need to develop the NG systems further?
Practical/economic reasons:
● Improve reliability, maintainability and user friendliness
Scientific reasons:
● The PrepCom requirements, set 20 years ago, need an update● Based on the technology available at the time● Background not known at the time● Only based on detection capability
● Need to approach the problem with respect to network verification capability● What is the unique NG signal, and how do we increase our capability to
detect it using the current 40 station network?
Better sensitivity is not the whole story
Current systems, 1kt , 100% release
Maximum achievable with current site configuration. 60% of explosions detected within one week (background not included).Will not improve with more sensitive systems*.
*FOI talk in session T4.1: “A novel approach to assess the verification capability of the network”
The signals we are looking for...
Isotope combination Network background* (95% conf. level)
Network background* (99% conf. level)
133Xe, 133mXe, and 135Xe 0.27% 0.07%133Xe and 135Xe 3.2% 0.98%133Xe and 133mXe 2.7% 0.67%133Xe 35% 28%133Xe and 131mXe 4.4% 1.9%
● Ratios and ATM compatible with time zero given by seismic signal● Other sources excluded
* Based on > 80 000 samples. See FOI poster:“The global radioxenon background – an update” (T2.4).
DPRK1 SAUNA measurement 2006DPRK1 IMS measurement 2006DPRK3 IMS measurement 2013
Potential improvements
Detection capability:
Relevant for all isotopes at remote stations with low background. Important to increase detection capability for 133mXe everywhere.
Measurement uncertainty:
Important for ratio interpretation. Small uncertainties increase ability to exclude scenarios. Ratio quantification increasingly risky close to detection limit
Time resolution:
Higher time resolution improves source location. Increases ability to distinguish explosion signal from background.
Measurement precision is crucial for discrimination
1h24h
~6 years of data (USX75), 4228 samples, 99% conf. level, 30/4228 = 0.7% remaining
Containment time:
Kalinowski 2010 line
SAUNA: 1999 - 2015 SAUNA-OSI-2014
1990-1999: “pre-SAUNA” NG network in Sweden
1999-2000: The Freiburg INGE experiment
SAUNA I - 1999
SAUNA I atSpitsbergen2000-2004
SAUNA II - 2004
Mobile sampling -2006
SAUNA III - 2018
SAUNA III main specifications
SAUNA II SAUNA III
Carrier gas Helium Nitrogen
Air volume/sample 16 m3 36 m3
Stable Xe volume in cell 1.2 ml 3.0 ml
Collection time 12 h 6 h
Air flow 22 SLM 100 SLM
MDC 133Xe / sample, 2 cells 0.3 mBq/m3 ~0.2 mBq/m3
MDC 133Xe / sample, 4 cells - ~0.15 mBq/m3
Sampling oven
Sampling oven
Pump
PLC
XPU
Process ovens
GC
SoH
Archive
PCPC
UPS
SAUNA II
He Detectors
Pumpand PSA
PLC
XPU
POV
GC
SoH
Archive
PCPC
UPS
SAUNA III
Sampling oven
Sampling oven
N Detectors
Sampling and processing*
Pump PSA Sampling
ovenProcess
oven GC
Goal: x10 sXe enrichment, 95% yield
See FOI poster: “Studies of increased air collection capability for SAUNA III”
Sampling and processing
One oven removed
New GC(OSI-type)Sample re-quantifiedafter activity measurement
Pump PSA Sampling
ovenProcess
oven GC
OSI-typesamplingoven :
Beta detector*
● Nitrogen as carrier gas + larger sXe volume => straggling● GEANT calculations to optimize design● Refinement of polishing and coating technique● Goal: all produced cells should have an energy resolution
< 35 keV @ 129 keV electron energy● Four different designs will be tested. First cells produced.
“polished”ΔE=31 keV
“rough”ΔE=54 keV
* See FOI poster “SAUNA III detector development”
electron energy (keV)
Beta detector
Teflon reflectorΔE=35 keV
New reflectormaterialΔE=28 keV
Example of test resultswith in-house manufacturedcells (SAUNA II geometry).
Achieved memory effect < 0.1 %.
Active energy drift control
● Energy scale drift ~1% / °C for NaI● Other sources for energy drift: PM-tubes, HV supply, …● Studies of drift performed● Solution using active compensation will be designed -
most likely the QC source will be used for this purpose.
New operational software
● All user functionality in one software with one GUI
● The system operated as a state machine with different modes
● Diagnostic mode● Calibration mode● Manual mode● Routine mode
Summary and conclusions
● In order to achieve better verification capability using the 40-station IMS NG network, increased measurement precision and time resolution is needed.
● The SAUNA III project address both issues.● The capacity of the sampling system will increase four-fold compared
to SAUNA II.● Nitrogen will be used as carrier gas.● The beta detector will be further developed to improve energy resolution.● Active adjustment of detector energy drift● New operator software is developed, including one single GUI and new
operational modes.● The design is handed over from FOI to manufacturer in December 2016.● According to manufacturer, production can start in 2018.
● The SAUNA concept - operation at ambient temperature - remains.