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GERDA General Meeting, Tübingen, 9.-11. November 2005 Nitrogen and argon radiopurity Grzegorz Zuzel for TG11 MPI-K Heidelberg MPI-K Heidelberg
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09.-11. Nov. 2005 Grzegorz ZuzelGERDA General Meeting, Tübingen 39 Ar, 42 Ar and 85 Kr - in argon - in nitrogen 222 Rn in nitrogen and argon - concentrations in different qualities - concentrations in different qualities - emanation from the storage tanks - emanation from the storage tanks - purification tests - purification tests Purification system for LN 2 /LAr (?) Conclusions and planned activity Outline
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09.-11. Nov. 2005 Grzegorz ZuzelGERDA General Meeting, Tübingen 39 Ar, 42 Ar and 85 Kr Q-value of 39 Ar and 85 Kr below 700 keV – relevant in case of dark matter detection Dead-time could be a problem when Ar scintillation is used (slow decay time: ~ 1 µ s) 42 Ar is naturally low Decay mode Source Concentration (STP) 222 Rn T 1/2 = 3.8 d , , Primordial 238 U 1 - ?00 Bq/m 3 air 85 Kr T 1/2 = 10.8 y (687 keV), 235 U fission (nuclear fuel reprocessing plants) 1.4 Bq/m 3 air 1.2 MBq/m 3 Kr 39 Ar T 1/2 = 269 y (565 keV) Cosmogenic 17 mBq/m 3 air 1.8 Bq/m 3 Ar 42 Ar T 1/2 = 32.9 y (600 keV) Cosmogenic 0.5 µ Bq/m 3 air 50 µ Bq/m 3 Ar
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09.-11. Nov. 2005 Grzegorz ZuzelGERDA General Meeting, Tübingen 39 Ar and 85 Kr in argon Dead time: Assume 10 m 3 active volume Assume 10 m 3 active volume – 39 Ar rate: 15 kHz 1.5 % Fine! – 85 Kr rate not higher ≤ 0.3 ppm Kr required Results from a 2.3 kg WARP test stand : ~ 0.6 ppm Other measurement possibilities: -mass spectrometry of Kr -direct counting of 85 Kr
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09.-11. Nov. 2005 Grzegorz ZuzelGERDA General Meeting, Tübingen 39 Ar in argon 39 Ar and dark matter detection (H. Simgen)
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09.-11. Nov. 2005 Grzegorz ZuzelGERDA General Meeting, Tübingen 39 Ar, 42 Ar and 85 Kr in argon 39 Ar gives a significant increase of background in the low energy region Ar scintillation used as a veto helps, however... background index stays at the level background index stays at the level of ~ 1 cts/keV rec /kg/y, which limits the ability for dark matter detection of ~ 1 cts/keV rec /kg/y, which limits the ability for dark matter detection Kr present in Ar at the ppm level would give similar contribution (through 85 Kr) Contribution from 42 Ar gives 4 10 -5 events/(kg y keV) at Q and is also negligible for dark matter
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09.-11. Nov. 2005 Grzegorz ZuzelGERDA General Meeting, Tübingen 39 Ar and 85 Kr in nitrogen Description Ar [ppm] Kr [ppt] MESSER RPN 2 (4.0, used in HD) 200 1 680 Air Liquide RPN 2 (4.0, used at GS) 1040 Air Liquide HPN 2 1030 Air Liquide 6.0 1413 Linde Worms (7.0) 0.0150.05 SOL Mantova (6.0) 0.0050.04 Westfalen AG Hörstel (6.0) 0.00050.06 1 ppt Kr = 1 µBq/m 3 (STP) 1 ppm Ar = 1.2 µBq/m 3 (STP) If LN 2 is used 39 Ar and 85 Kr should not affect detection of dark matter
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09.-11. Nov. 2005 Grzegorz ZuzelGERDA General Meeting, Tübingen 39 Ar, 42 Ar and 85 Kr - in argon - in nitrogen 222 Rn in nitrogen and argon - concentrations in different qualities - concentrations in different qualities - emanation from the storage tanks - emanation from the storage tanks - purification tests - purification tests Purification system for LN 2 /LAr (?) Conclusions and planned activity Outline
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09.-11. Nov. 2005 Grzegorz ZuzelGERDA General Meeting, Tübingen 222 Rn in nitrogen and argon According to the simulations: 222 Rn in LN 2 /LAr at the level of ~ 0.3 mBq/m 3 → B ~ 10 -4 cts/keV/kg/y 0.3 mBq/m 3 liquid → 0.5 µBq/m 3 gas (STP)
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09.-11. Nov. 2005 Grzegorz ZuzelGERDA General Meeting, Tübingen 222 Rn concentration in Ar of different qualities (Westfalen AG) Quality 222 Rn concentration [mBq/m 3 (STP)] Remarks 5.08.4 ± 0.2At the filling time 6.00.38 ± 0.03At the filling time Specification: 0.5 10 -3 mBq/m 3 gas (STP)
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09.-11. Nov. 2005 Grzegorz ZuzelGERDA General Meeting, Tübingen 222 Rn concentration in N 2 of different qualities Quality 222 Rn concentration [mBq/m 3 (STP)] 4.00.05 – 0.2 7.0~ 0.001 Conclusions: - initial 222 Rn content in nitrogen is lower than in argon of a similar class - however 222 Rn decays (T 1/2 =3.8 d) – emanation from the storage tank limits the final purity
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09.-11. Nov. 2005 Grzegorz ZuzelGERDA General Meeting, Tübingen 222 Rn emanation from storage tanks Tank description Volume [m 3 ] 222 Rn emanation rate [mBq] Storage tank for argon 5.0 (Westfalen) 2.9 177 ± 7 Storage tank for argon 6.0 (Westfalen) 0.66 42 ± 2 Special storage tank for ultra-pure gases (Linde) 3 2.7 ± 0.3 2.7 ± 0.3 C Rn 1µBq/m 3 Ar (STP) It should be possible to have argon with low enough 222 Rn concentration without purification
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09.-11. Nov. 2005 Grzegorz ZuzelGERDA General Meeting, Tübingen Outline 39 Ar, 42 Ar and 85 Kr - in argon - in nitrogen 222 Rn in nitrogen and argon - concentrations in different qualities - concentrations in different qualities - emanation from the storage tanks - emanation from the storage tanks - purification tests - purification tests Purification system for LN 2 /LAr (?) Conclusions and planned activity
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09.-11. Nov. 2005 Grzegorz ZuzelGERDA General Meeting, Tübingen Nitrogen purification from 222 Rn Liquid nitrogen purification plant works at GS for Borexino 222 Rn in N 2 before purif. ~50 μBq/m 3 222 Rn in N 2 after purif. < 0.3 μBq/m 3 Red. factor: > 100 Ads. mass: ~2 kg
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09.-11. Nov. 2005 Grzegorz ZuzelGERDA General Meeting, Tübingen Argon purification from 222 Rn 222 Rn in Ar before purif. ~200 μBq/m 3 222 Rn in Ar after purif. < 0.5 μBq/m 3 Red. factor: > 400 Ads. mass: ~0.15 kg MoREx: Mobile Radon Extraction Unit
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09.-11. Nov. 2005 Grzegorz ZuzelGERDA General Meeting, Tübingen Ar purification from 222 Rn Init. C Rn [mBq/m 3 ] Final C Rn [mBq/m 3 ] Red. factor R M Ads R/M Ads[1/kg] 0.20 ± 0.02 < 0.0005 (90% CL) > 400 > 2700 Purification in gas phase Purification in liquid phase Init. C Rn [mBq/m 3 ] Final C Rn [mBq/m 3 ] Red. factor R M Ads R/M Ads[1/kg] 5.4 ± 0.10.60 ± 0.029300 0.10 ± 0.010.006 ± 0.00117570 Average: 13 13 ~ 400
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09.-11. Nov. 2005 Grzegorz ZuzelGERDA General Meeting, Tübingen LN 2 /LAr purification from 222 Rn It is possible to effectively remove radon from argon / nitrogen Removal of 222 Rn from liquid phase is somewhat less effective than from gas phase
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09.-11. Nov. 2005 Grzegorz ZuzelGERDA General Meeting, Tübingen Outline 39 Ar, 42 Ar and 85 Kr - in argon - in nitrogen 222 Rn in nitrogen and argon - concentrations in different qualities - concentrations in different qualities - emanation from the storage tanks - emanation from the storage tanks - purification tests - purification tests Purification system for LN 2 /LAr (?) Conclusions and planned activity
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09.-11. Nov. 2005 Grzegorz ZuzelGERDA General Meeting, Tübingen Purification system for LN 2 /LAr (?) Having clean storage tanks we do not need a purification system, but it has several advantages: Having clean storage tanks we do not need a purification system, but it has several advantages: Operational conditions for the cryo-plant are more relaxed (safety, shorter “access” time) The same system can be used for LN 2 and LAr purification We know how to build such a plant (Borexino plant) Optimal column size ~200 g (LArGe) / ~1 kg (GERDA) of CarboAct (need some further tests)
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09.-11. Nov. 2005 Grzegorz ZuzelGERDA General Meeting, Tübingen Purification system for LAr
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09.-11. Nov. 2005 Grzegorz ZuzelGERDA General Meeting, Tübingen Conclusions LN 2 allows investigation of 0 2 (and dark matter) 39 Ar limits ability to detect dark matter if LAr is used It is possible to buy „ 222 Rn-free“ LN 2 (proven in frame of Borexino) 222 Rn content in fresh argon is higher than in nitrogen of similar quality It should be also possible to have „ 222 Rn-free“ LAr without purification – still to be confirmed 222 Rn removal from argon as effective as from nitrogen From the radiopurity point of view for GERDA 0 2 experiment LAr and LN 2 can be used
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09.-11. Nov. 2005 Grzegorz ZuzelGERDA General Meeting, Tübingen Planned activity Measure 222 Rn content in argon after long storage in the tank of known emanation 85 Kr/Kr measurement in argon Test of a purification system for LArGe (design for GERDA) Full supply chain test of ultra-pure nitrogen for Borexino – results interesting also for GERDA
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