Topical Workshop in Low Radioactivity Techniques, Sudbury, Canada, August 28-29, 2010 Surface cleaning techniques B. Majorowits a, M. Wójcik b, G. Zuzel.

Slides:



Advertisements
Similar presentations
Surface Sensitive Bolometers (SSB): last development MARISA PEDRETTI INFN - Milano.
Advertisements

Stefano Pirro, IDEA Meeting –Milano November Status of the scintillating bolometer program Scintillating Bolometers Background rejection capabilities.
# Neutrons. Radioactive Isotopes Only certain isotopes of some elements are radioactive. If an atom is radioactive the proton to neutron ratio is not.
M. Carson, University of Sheffield, UKDMC ILIAS-Valencia-April Gamma backgrounds, shielding and veto performance for dark matter detectors M. Carson,
Progress of TG-1 activities (refurbishment of Phase-I detectors) Stefan Schönert on behalf of TG 1 GERDA general meeting Tuebingen, Nov. 9-11, 2005.
ILIAS J1, 3rd General Meeting, Paris, 14th Feb Coordinated gamma measurements in the underground labs Jan Kisiel Institute of Physics, University.
TG 11 overview - Material screening - Hardy Simgen MPI für Kernphysik Heidelberg.
Measurement and Survey Protocols Defining and Identifying Radioactive Materials.
LAUNCH - Low-energy, Astroparticle Underground, Neutrino physics and Cosmology in Heidelberg, Low-level techniques applied in experiments.
GERDA General meeting, Krakow, Poland 222 Rn measurements H. Richter, H. Simgen, G. Zuzel Max-Planck-Institut für Kernphysik, Heidelberg.
IDEA Meeting, MPI-K Heidelberg, October 2004 Techniques for analysis and purification of nitrogen and argon Grzegorz Zuzel MPI-K Heidelberg.
IDEA Meeting, LAL-Orsay, April 2005 Purification of nitrogen (argon) Grzegorz Zuzel MPI-K Heidelberg.
Proposal for high sensitive measurements of 238 U and 232 Th with NAA Ezio Previtali INFN Sez. Milano Milano-Bicocca University ILIAS: JRA1 3rd General.
Stefano Pirro LRT-2004 Sudbury December 13, 2004 Cleanliness backgrounds and surface contaminations in Cuore Stefano Pirro INFN-Milano.
CUORICINO and CUORE Chiara Brofferio Università di Milano – Bicocca and INFN, Sez. di Milano NOW 2004 – Otranto 12 – 17 September 2004 On behalf of the.
Lee, Myeong Jae DMRC, Seoul national university
Sudbury, Canada Workshop in Low Radioactivity Techniques December 2004 Highly sensitive measurements of 222 Rn emanation and diffusion Grzegorz.
A screening facility for next generation low-background experiments Tom Shutt Laura Cadonati Princeton University.
Preparation of crystals for channeling University of Ferrara V. Guidi Department of Physics and INFN, Via Paradiso 12, I Ferrara, Italy A. Vomiero.
238 U (4.47  10 9 years) 226 Ra (1600 years) 222 Rn (3.82 days) 218 Po (3.10 mins) 214 Pb (26.8 mins) 214 Bi (19.9 mins) 210 Tl (1.30 mins) 214 Po (164.
th KPS meeting 1 Development of Radon Monitoring Detector for the KIMS Experiment Lee, Myoung Jae DMRC, Seoul national university.
Workshop for Underground experiments and astroparticle physics 1 Radon Environment of Underground Experiment and Detection of Radon Lee, Myeong.
Radioisotopes, and their use in “dating” rocks. Radioactive Decay Certain isotopes of some elements are not stable. They naturally change (decay) over.
Surface events suppression in the germanium bolometers EDELWEISS experiment Xavier-François Navick (CEA Dapnia) TAUP Sendai September 07.
Warszawa, July 3rd Measurements of natural radioactivity in European underground labs within the ILIAS project Jan Kisiel Institute of Physics, University.
Isotopic and Nuclear Analytical Techniques for Health and Environment
May 6, 2006Henderson Dusel Capstone Meeting Low Background Counting A Facility Wish List for the New Underground Laboratory F. Calaprice.
M. Wójcik for the GERDA Collaboration Institute of Physics, Jagellonian University Epiphany 2006, Kraków, Poland, 6-7 January 2006.
ILIAS-JRA2 Production of enriched Selenium -2 kilos « ITEP-Kurchatov » -New contacts with ECP-Krasnoyarsk -New production from Tomsk -What’s next ? Integrated.
Half Day IoP Meeting: Neutrinoless Double Beta Decay, University College London, Great Britain The GERDA Experiment at Gran Sasso Grzegorz Zuzel.
Application of Nuclear Chemistry Cancer Treatment – Cancer cells are more susceptible to radiation bc they are fast growing. Thyroid cancer can be treated.
Experiment TGV II Multi-detector HPGe telescopic spectrometer for the study of double beta processes of 106 Cd and 48 Ca For TGV collaboration: JINR Dubna,
Different potential systematic uncertainties involved in 210 Pb dating method Begy R.-Cs. 1,2, Reizer E. 1, Forray F.-L. 3, Simon H. 1, Gabor A.-I. 1,2,
VIeme rencontres du Vietnam
Tracking (wire chamber) Shield radon, neutron,  Source foil (40 mg/cm 2 ) Scintillator + PMT 2 modules 2  3 m 2 → 12 m 2 Background < 1 event / month.
Ultra-low background gamma spectrometry 2 nd LSM-Extension Workshop, Valfréjus, 16 October 2009 Pia Loaiza Laboratoire Souterrain de Modane.
M. Wójcik Instytut Fizyki, Uniwersytet Jagielloński Instytut Fizyki Doświadczalnej, Uniwersytet Warszawski Warszawa, 10 Marca 2006.
The EDELWEISS-II experiment Silvia SCORZA Université Claude Bernard- Institut de Physique nucléaire de Lyon CEA-Saclay DAPNIA/DRECAM (FRANCE), CNRS/CRTBT.
GERDA general meeting, Padova Italy, Update on 222 Rn emanation measurements S. Lindemann, H. Richter, H. Simgen, G. Zuzel MPI für Kernphysik,
MaGe framework for Monte Carlo simulations MaGe is a Geant4-based Monte Carlo simulation package dedicated to experiments searching for 0 2  decay of.
Muon and Neutron Backgrounds at Yangyang underground lab Muju Workshop Kwak, Jungwon Seoul National University 1.External Backgrounds 2.Muon.
Cracow Epiphany Conference on Physics in Underground Laboratories and its Connection with LHC Cracow, Poland The GERDA Experiment at Gran.
BACKGROUND REJECTION AND SENSITIVITY FOR NEW GENERATION Ge DETECTORS EXPERIMENTS. Héctor Gómez Maluenda University of Zaragoza (SPAIN)
TG 11 overview / Material screening Hardy Simgen MPI für Kernphysik for Task Group 11.
Results of the NEMO-3 experiment (Summer 2009) Outline   The  decay  The NEMO-3 experiment  Measurement of the backgrounds   and  results.
TEXONO-KIMS Joint Workshop1 Radon level monitoring in Y2L and Radon reduction strategy Lee, Myoung Jae Seoul National University.
A screening facility for next generation low-background experiments Tom Shutt Case Western Reserve University.
Pia Loaiza AARM-Berkeley March 2010
ICP 9/25/12 Nuclear Decay Equations. Warmup 1)What composes an alpha particle? 2)What composes a beta particle? 3)What is gamma radiation?
PMN07 Blaubeuren Segmented germanium detectors in 0νββ-decay experiments Kevin Kröninger (Max-Planck-Institut für Physik, München)
Nasim Fatemi-Ghomi, Group Christmass Meeting December Nasim Fatemi-Ghomi Double Beta Decay Study of 150 Nd at NEMO3 (The magic isotope!!)
Sep. 22, 2011 Seoul National University Jae Keum Lee KIMS Background 1 China-Korea Workshop 2011 September 22-23, 2011.
Recent progress in ultra-low noise, ultra-low background detectors V. Marian, M.O. Lampert, B. Pirard, P. Quirin CANBERRA France (Lingolsheim) Workshop.
Surface Contamination Simulations with MaGe Rob Johnson Center for Experimental Nuclear Physics and Astrophysics University of Washington 15 February,
P. CermakRez near Prague, December 2005 EC/EC process measurement in TGV experiment For TGV collaboration: JINR Dubna, Russia CTU Prague, Czech Republic.
Ch 19 Nuclear Chemistry.  Know how nuclear equations are balanced: The same sums of both mass and atomic numbers appear on both sides of the equation.
ILIAS, Jaca, Spain 5 of December 2006 Se-82 purification: how to control the procedure (Bi-214)? Kornoukhov Vasily INR RAS Moscow.
Radon Background of Y2L MyeongJae Lee (SNU) 2 nd workshop on Double beta decay Oct 6, 2010, KRISS.
VALIDATION OF THE FLUKA MONTE CARLO CODE FOR RESIDUAL PRODUCTION WITH 500 MeV/u AND 950 MeV/u URANIUM BEAM ON COPPER AND STAINLESS STEEL TARGET E. Kozlova.
SuperCDMS & Radon Ray Bunker
Condition of electron beam welding toward a high gradient application
Overview of GERDA simulation activities with MaGe
On measurability of mBq/kg levels of alpha activity
Measurement of surface radioactivity by Alpha/Beta detection
Fabrication Steps of Detectors
Very preliminary study of the random background for the BiPo detector (PhoSwich configuration) Work done by Jonathan Ferracci.
WP 15.2 Progress and critical aspects
H. Simgen, MPI for Nuclear Physics / Heidelberg
Particulate and Dissolved 210Po and 210Pb in Water Columns from the
Munich GERDA/Majorana MC Meeting
Presentation transcript:

Topical Workshop in Low Radioactivity Techniques, Sudbury, Canada, August 28-29, 2010 Surface cleaning techniques B. Majorowits a, M. Wójcik b, G. Zuzel b,c a) Max Planck Institute for Physics, Munich, Germany b) Institute of Physics, Jagielonian University, Kraków, Poland c) Max Planck Institute for Nuclear Physics, Heidelberg, Germany

Topical Workshop in Low Radioactivity Techniques, Sudbury, Canada, August 28-29, 2010 Outlook  Motivation  Technique applied to tests of surface cleaning - Loading samples with the Rn daughters - Measurement of 210 Pb, 210 Bi and 210 Po  Copper, Steel and Germanium surface treatment - Etching and electropolishing of Copper - Etching of Steel - Etching of Germanium (optical quality)  Obtained results  Conclusions

Topical Workshop in Low Radioactivity Techniques, Sudbury, Canada, August 28-29, 2010 Motivation  Equilibrium in the 226 Ra decay chain is usually broken at the 210 Pb level  210 Pb may stay as main residual surface contamination after cleaning (will appear after some years as e.g. 210 Po)  Radio-chemistry of 210 Po not well understood, most probably quite different than chemistry of Pb and Bi  Long-lived 222 Rn/ 210 Pb daughters deposited on surfaces (or implanted into a sub-surface layer) may significantly contribute to the background of many experiments

Topical Workshop in Low Radioactivity Techniques, Sudbury, Canada, August 28-29, 2010 Technique applied to tests of surfaces cleaning  Removal of long-lived 222 Rn daughters form different surfaces, like Copper, Steel and Germanium was investigated  Samples in a form of discs with 50 mm diameter were used  To increase the sensitivity sample surfaces were artificially loaded with 210 Pb, 210 Bi and 210 Po  Activities of 210 Pb, 210 Bi and 210 Po were measured before and after cleaning using appropriate detectors

Topical Workshop in Low Radioactivity Techniques, Sudbury, Canada, August 28-29, Ra decay chain 222 Rn 226 Ra 218 Po 214 Pb 214 Bi 214 Po 210 Pb     210 Bi 210 Po 206 Pb   T 1/2 = 1622 y E = 4.8 MeV Br = 94 % T 1/2 = 3.8 d E = 5.5 MeV T 1/2 = 3.1 m E = 6.0 MeV T 1/2 = 26.8 m E m = 0.7 MeV Br = 48 %  T 1/2 = 19.8 m E m = 1.5 MeV Br = 40 % T 1/2 = 164  s E = 7.7 MeV T 1/2 = 22.3 y E m = 0.06 MeV Br = 81 % T 1/2 = 5.0 d E m = 1.2 MeV T 1/2 = d E = 5.3 MeV Stable

Topical Workshop in Low Radioactivity Techniques, Sudbury, Canada, August 28-29, 2010 Loading the samples Exposure time 6 – 8 months

Topical Workshop in Low Radioactivity Techniques, Sudbury, Canada, August 28-29, 2010 Measuring 210 Pb/ 210 Bi/ 210 Po  Screening of 210 Po with an alpha spectrometer 50 mm Si-detector, bcg ~ 2 /d (1-10 MeV) sensitivity ~ 20 mBq/m 2 (100 mBq/kg, 210 Po)  Screening of 210 Bi with a beta spectrometer 250 mm Si(Li)-detectors, bcg ~ 0.18/0.40 cpm sensitivity ~ 10 Bq/kg ( 210 Bi)  Screening of 210 Pb (46.6 keV line) with a gamma spectrometer 16 % - HPGe detector with an active and a passiveshield

Topical Workshop in Low Radioactivity Techniques, Sudbury, Canada, August 28-29, 2010 Copper  Electrolytic copper used to fabricate sample discs (50 mm in diameter, 1 mm thick)  Etching procedure: - 5 min in 1% H 2 SO 4 + 3% H 2 O min in 1% citric acid - rinsing with distilled water  Electropolishing procedure: - electrolyte: 85 % H 3 PO % 1-butanol (C 4 H 10 O) - drying in a nitrogen stream  Weighing the discs before and after cleaning to measure the thickness of a removed surface layer  Both discs surfaces investigated

Topical Workshop in Low Radioactivity Techniques, Sudbury, Canada, August 28-29, 2010 Steel  Stainless steel from the GERDA cryostat used to fabricate sample discs (50 mm in diameter, 1 mm thick)  Etching procedure: - etching in 20 % HNO % HF - passivation in 15 % HNO 3 - rinsing with distilled water  Weighing the discs before and after cleaning to measure the thickness of a removed surface layer  Both discs surfaces investigated

Topical Workshop in Low Radioactivity Techniques, Sudbury, Canada, August 28-29, 2010 Germanium of optical quality  Optical quality Germanium used for a “test run” before using HPGe  Samples cut out from bigger Ge pieces, no special surface treatment after cutting  2 discs 50 mm in diameter and 3 mm thick were prepared  Discs etched by Canberra according to their standard procedure applied to HPGe crystals  Amount of removed material not measured

Topical Workshop in Low Radioactivity Techniques, Sudbury, Canada, August 28-29, 2010 Selected results for Copper Isotope Original activity [cpm] Activity after cleaning [cpm] Reduction factor R Amount of removed Cu Remarks 210 Pb 1.49  0.04 < 0.022> mg/cm µm Only side a was investigated 210 Bi   Only side a was investigated 210 Po 2.55   Only side a was investigated Etching: Disc side Original 210 Po activity [cpm] 210 Po activity after pol. [cpm] 210 Po reduction factor R Amount of removed Cu Remarks a 2.18   mg/cm µm Facing the cathode 3 times, each time for 30 min b 2.45   Facing the cathode 3 times, each time for 30 min Electropolishing (only results for 210 Po are shown):

Topical Workshop in Low Radioactivity Techniques, Sudbury, Canada, August 28-29, 2010 Selected results for Steel Isotope Original activity [cpm] After 1 st cleaning [cpm] Reduction factor R Amount of removed Cu Remarks 210 Pb 6.87     mg/cm m Etching time = 50 min 210 Bi 147     Po 16.5     Disc No. 1 Isotope Original activity [cpm] After cleaning [cpm] Reduction factor R Amount of removed Cu Remarks 210 Pb 6.34     mg/cm m Etching time = 120 min Solution stirred during etching 210 Bi 138     Po 24.7     Disc No. 2

Topical Workshop in Low Radioactivity Techniques, Sudbury, Canada, August 28-29, 2010 Selected results for Ge of optical quality Isotope Disc side Initial activity [cpm] Activity after cleaning [cpm] Reduction factor R Average reduction factor R av Remarks 210 Pb a2.08< 0.02> 104 Amount of removed Ge not measured. After etching side b not measured for 210 Pb. b Bi a42.7< 0.18> 237 > 427 b67.9< 0.11> Po a b Disc No. 1 Isotope Disc Side Initial activity [cpm] Activity after cleaning [cpm] Reduction factor R Average reduction factor R av Remarks 210 Pb A > 106Amount of removed Ge not measured. After etching side a not measured for 210 Pb. 210 Bi not measured because it has decayed. b2.12< 0.02> Bi a b Po a b Disc No. 2

Topical Workshop in Low Radioactivity Techniques, Sudbury, Canada, August 28-29, 2010 Comparison between Cu/Steel/Ge Isotope Average reduction factors for etching CopperSteelGe (Optical) 210 Pb~ 50~ Bi~ 50~ 100~ Po~ 1~ 20~ 1000

Topical Workshop in Low Radioactivity Techniques, Sudbury, Canada, August 28-29, 2010 Conclusions  Etching/electropolishing removes some m of treated material (depending on the treatement time)  210 Po deposited on- or just below the surface (relatively narrow α-peaks observed)  Etching does not remove 210 Po from Copper, it is re-deposited ( 209 Po added to the solution was found after etching on the surface)  Long electropolishing of Copper reduces 210 Po activity by a factor of ~200 – much more effective than etching  Etching of Copper removes most of 210 Pb and 210 Bi (> 98 %)  Electropolishing of Copper removes 210 Pb and 210 Bi more effective than etching (99.5 % of 210 Bi and > 99.9 % of 210 Pb removed)  Etching of Steel works fine for all isotopes and it is more efficient than etching of Copper  In a multi-stage etching process of Steel removal of all isotopes successively drops (passivation makes the process less effective)  Removal efficiency of all long-lived 222 Rn daughters from Ge is very high  Etching of Germanium seems to be more efficient than etching of Copper and Steel (especially for 210 Po)  Etching tests of HPGe discs ongoing