2005-2-18 Workshop for Underground experiments and astroparticle physics 1 Radon Environment of Underground Experiment and Detection of Radon Lee, Myeong.

Slides:



Advertisements
Similar presentations
Radiation is All around Us Sunlight is electromagnetic radiation High-energy wavelengths above ultraviolet are collectively called “ionizing radiation”
Advertisements

Purification of Liquid Scintillators for Low Radioactivity Frank Calaprice Princeton University Borexino Experiment 6/14/13 RENO Workshop June ,
outline introduction experimental setup & status
UNIVERSITA’ DEGLI STUDI DI PALERMO DIN DIPARTIMENTO DI INGEGNERIA NUCLEARE CHERNE th Workshop on European Collaboration for Higher Education and.
3/2003 Rev 1 I.4.1 – slide 1 of 33 Part I Review of Fundamentals Module 4Sources of Radiation Session 1Terrestrial Radionuclides Module I.4.1 IAEA Post.
Welcome to Chem 108! Brian Majestic Environmental Chemistry and Technology and Department of Chemistry.
Classify the following properties as Physical or Chemical:
M. Carson, University of Sheffield, UKDMC ILIAS-Valencia-April Gamma backgrounds, shielding and veto performance for dark matter detectors M. Carson,
Rn-222 Measurement Performance Criteria Melinda Ronca-Battista ANSI N42.51 Co-chair Phil Jenkins, Co-Chair Phil Jenkins Jim Burkhart Tom Voss Shawn Price.
Status of Ultra-low Energy HPGe Detector for low-mass WIMP search Li Xin (Tsinghua University) KIMS collaboration Oct.22nd, 2005.
Mass Analyzer of SuperHeavy Atoms Some recent results 2012 Student Practice in JINR Fields of Research 9.oct.2012 I. Sivacekflerovlab.jinr.ru.
ILIAS J1, 3rd General Meeting, Paris, 14th Feb Coordinated gamma measurements in the underground labs Jan Kisiel Institute of Physics, University.
How long will the test last?
Prospects for 7 Be Solar Neutrino Detection with KamLAND Stanford University Department of Physics Kazumi Ishii.
Krypton source for the Project 8 neutrino mass experiment Arman Ballado Advisor: Mike Miller.
IAEA Natural Terrestrial Radiation Day 3 – Lecture 7 Sources of Radiation 1.
By Sanaa Ahmed. Main Idea Physical and chemical properties are characteristics to describe, identify, and classify matter Matter is anything that has.
LAUNCH - Low-energy, Astroparticle Underground, Neutrino physics and Cosmology in Heidelberg, Low-level techniques applied in experiments.
INDOOR AIR POLLUTION: RADON In 1990 EPA placed indoor air pollution at the top of the list of 18 sources of cancer risk Indoor pollution is rated by risk.
Lesson 5 What devices do we use to measure radon?.
IDEA Meeting, LAL-Orsay, April 2005 Purification of nitrogen (argon) Grzegorz Zuzel MPI-K Heidelberg.
RADON MEASUREMENT OPERATORS PROFICIENCY COURSE
Measurement of Kr background in the XMASS experiment ICRR master’s course in physics Keisuke Hieda 1.
1 Alpha Emissions (How a Smoke Alarm Works). 2 Radioactive Emissions (Radiation) Penetrating Power SymbolEquivalentDescriptionType He Stopped by thick.
Lee, Myeong Jae DMRC, Seoul national university
Link to a set of 9 quick lessons about solutes and solubility: hapter5/lesson1
Radon. Introduction  Radon is a colorless and odorless gas produced by the decay of radium – 226  Radon after decay produces radioisotopes known as.
Developed by the Healthy Environments for Children Initiative at the University of Connecticut for the Connecticut Department of Public Health 2006 Measuring.
Transmutation Transmutation is the process of atoms of unstable nuclide A changing into atoms of nuclide B. This can occur naturally (by radioactive decay)
Colligative Properties Honors Chemistry Chapter 14.
A screening facility for next generation low-background experiments Tom Shutt Laura Cadonati Princeton University.
Lesson 1 What is radon?. Slide 1-1 Which characteristics apply to radon? Liquid Gas Solid Colorless Grayish-green Greenish-blue Smells like ozone Has.
th KPS meeting 1 Development of Radon Monitoring Detector for the KIMS Experiment Lee, Myoung Jae DMRC, Seoul national university.
Topical Workshop in Low Radioactivity Techniques, Sudbury, Canada, August 28-29, 2010 Surface cleaning techniques B. Majorowits a, M. Wójcik b, G. Zuzel.
Neutron Monitoring Detector in KIMS Jungwon Kwak Seoul National University 2003 October 25 th KPS meeting.
Aging Studies for the ATLAS MDTs Dimos Sampsonidis for the ATLAS group of Thessaloniki.
Yasuhiro Kishimoto for KamLAND collaboration RCNS, Tohoku Univ. September 12, 2007 TAUP 2007 in Sendai.
Developments in Environmental Radiochemistry* Environmental Radioactivity Measurement Facility Department of Oceanography Florida State University Tallahassee,
Ultra-low background HPGe detector at ChyeongPyung Underground Laboratory TaeYeon Kim and KIMS(Korea Invisible Mass Search) Collaboration. * Contents *
Radioactivity.  Total mass of nucleus is always less than the sum of its protons and neutrons  Compare the mass of He-4 to that of its nucleus - mass.
The nucleus consists of protons and neutrons, collectively called nucleons. The number of protons is the atomic number. Protons plus neutrons is the atomic.
CTF and low background facility at Gran Sasso A. Ianni a, M. Laubenstein a and Y. Suvorov a a INFN, Gran Sasso Laboratory, Assergi (AQ), Italy The Counting.
Warszawa, July 3rd Measurements of natural radioactivity in European underground labs within the ILIAS project Jan Kisiel Institute of Physics, University.
May 6, 2006Henderson Dusel Capstone Meeting Low Background Counting A Facility Wish List for the New Underground Laboratory F. Calaprice.
Ultra-low background gamma spectrometry 2 nd LSM-Extension Workshop, Valfréjus, 16 October 2009 Pia Loaiza Laboratoire Souterrain de Modane.
10.1 Radioactivity Understand Radioactivity and distinguish between the types of decay.
CTF at Gran Sasso (overview of the hardware) Richard Ford (SNOLAB) (who has not been in the collaboration since 2004) March 19 th 2010.
Muon and Neutron Backgrounds at Yangyang underground lab Muju Workshop Kwak, Jungwon Seoul National University 1.External Backgrounds 2.Muon.
Activities on double beta decay search experiments in Korea 1.Yangyang Underground laboratory 2.Double beta decay search with HPGe & CsI(Tl) 3.Metal Loaded.
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.
HP SURVEY INSTRUMENT CALIBRATION AND SELECTION PRINCIPLES OF RADIATION DETECTION AND QUANTIFICATION CHAPTER 5 – REVIEW AND SUMMARY January 13 – 15, 2016.
08/06/2016 GCSE Radiation W Richards Worthing High School.
Sep. 22, 2011 Seoul National University Jae Keum Lee KIMS Background 1 China-Korea Workshop 2011 September 22-23, 2011.
** Radon is estimated to cause about 21,000 lung cancer deaths per year, according to EPA's 2003 Assessment of Risks from Radon in Homes (EPA 402-R ).EPA's.
RADON: What is it anyway? Hennepin County Community Health Department Health Protection, Epidemiology and Environmental Health.
Neutrinoless double beta decay (0  ) CdTe Semico nductor Band gap (eV) Electron mobility (cm 2 /V/s) Hole mobility (cm 2 /V/s) Density (g/cm 3.
09/04/2006NDM061 CANDLES for the study of 48 Ca double beta decay OGAWA Izumi ( 小川 泉 ) Osaka Univ. ( 大阪大学 )
Radon Reduced Air and SNOLAB Aksel Hallin Queen’s University August, 2006.
Radon Background of Y2L MyeongJae Lee (SNU) 2 nd workshop on Double beta decay Oct 6, 2010, KRISS.
Current status of R&D on MMC and TES and a full size crystal test setup Sang-jun Lee Seoul National University.
g a b α,  and  RADIATION gamma alpha beta e- Marie Curie
Measuring Radon in Residential Properties What is radon?
Muon and Neutron detector of KIMS experiment
2nd International Workshop on Double Beta Decay
Sr-84 0n EC/b+ decay search with SrCl2 crystal
Status of Neutron flux Analysis in KIMS experiment
g a b α,  and  RADIATION gamma alpha beta e- Marie Curie
Gas Transfer and Dissolved Oxygen Probe
Presentation transcript:

Workshop for Underground experiments and astroparticle physics 1 Radon Environment of Underground Experiment and Detection of Radon Lee, Myeong Jae DMRC, Seoul national university For the KIMS collaboration

Workshop for Underground experiments and astroparticle physics 2 Contents  Property of Radon  Radioactivity of the rock for other experiments  Radon detection for the KIMS experiments  Radon-Free techniques  Conclusion

Workshop for Underground experiments and astroparticle physics 3 Radon  Odorless, tasteless, invisible gas  Chemically inert and essentially non-reactive  Heaviest noble gas with highest melting and boiling point  Highly soluble in non-polar solvents  Moderately soluble in cold water  Able to diffuse through rock and soil  Decays by alpha particle emission (T 1/2 = 3.8 days)  Exists in the typical atmosphere and specially in the underground environment  outside : 0.2 ~ 0.7 pCi/L  inside : ~ 1.25 pCi/L  residential recommendation : 4 pCi/L

Workshop for Underground experiments and astroparticle physics 4 Decay chain of Radon232Th1.4e10yr238U3.5e9yr Ra5.75yr234Th24.10d 228Ac6.15h234Pa6.7h 228Th1.9yr234U2.5e5yr Ra3.65d230Th7.5e4yr Rn55.6s226Ra1600yr Po0.145s222Rn3.82d Pb10.6h218Po3.05m (~36%)212Bi60.6m(~64%) Po60.3us214Pb26.8m 208Tl3.05m Bi19.7m 208PbStable214Po164us Pb22.3yr 210Bi5.01d 210Po138.4d PbStable

Workshop for Underground experiments and astroparticle physics 5 Why Radon is Important? (From “Univ. of Minesota”) Can cause lung cancer !!

Workshop for Underground experiments and astroparticle physics 6 Why Radon is Important?(2)  Radioactive contamination of experimental setup  Radon dissolves in water and contaminates all other material  Po ion easily attaches to other material  Can cause b.g. event  For the neutrino experiment radon daughter beta decay is significant bg source

Workshop for Underground experiments and astroparticle physics 7 Radioactivity data for other experiment (From UKDMC Homepage)

Workshop for Underground experiments and astroparticle physics 8 Radioactive environment of Y2L U 3.46<0.5 Th Element(ppm) ABCD Sample < Avg. Y2L 호상편마암 (~2Gyr) 중생대 화성암 (~200Myr)

Workshop for Underground experiments and astroparticle physics 9 Radon Detection Method  No way to detect radon directly : Noble gas  Decay is detectable  alpha and its emitter detection  Lucas cell, SSNTD, electrostatic alpha spectroscopy, filter method, ionization detector  beta and its emitter detection  Liquid scintillator, beta spectroscopy, gamma counting

Workshop for Underground experiments and astroparticle physics 10 Radon Detection Scheme (electrostatic alpha spectroscopy) 222 Rn 218 Po (115keV) α (5.49MeV) Stripping effect 218 Po +,+2 Electrostatic collection near photodiode Decay α (6.00MeV) Detect Attach to water, aerosol, oxygen (chemically stable) Decay 214 Pb Decay 214 Bi 214 Po α (7.69MeV) Electrostatic collection near photodiode Decay

Workshop for Underground experiments and astroparticle physics 11 Voltage Divider, Preamp Photodiode Radon Monitoring Detector  Electrostatic alpha spectroscopy  Use Si(Li) photodiode  30mm X 30mm  Photodiode – chassis potential difference : - 500V  Photodiode bias : -70V  Photodiode calibration : 210 Po, 241 Am  Neutralization of 218 Po : Humidity control is necessary  Volume : ~ 70 liter

Workshop for Underground experiments and astroparticle physics 12 Radon Detector Operation Radon detector Moisture trap Vacuum pump Voltage Divider Preamplifier Shaping amplifier ADC DAQ & Control computer HV Supply Humidity, Temperature, Pressure, HV monitor Controller HV Air Signal Control

Workshop for Underground experiments and astroparticle physics 13 Calibration data analysis Typical Event Shape Data Before Cut Mean time ADC Data After Cut Mean time ADC Data Histogram ADC  Energy resolution is not good,  But we can distinguish two alpha particle.

Workshop for Underground experiments and astroparticle physics 14 Typical signal and Background Air, ~0.74 Hz N 2, ~ Hz 12h DAQ for typical air 6h DAQ for typical air and nitrogen 6.00MeV ( 218 Po) 7.69MeV ( 214 Po) Recent BG measurement = ~0.037Hz

Workshop for Underground experiments and astroparticle physics 15 Standard Radon Source / Calibration Setup  226Ra in 5% HNO 3 50g  Max. Activity : Bq (at ~65days) = ~3500pCi = 50pCi/L * 70L  Made at at KRISS  Used at (34days after) : ~130.03Bq

Workshop for Underground experiments and astroparticle physics 16 Calibration data analysis Total EventPo214 Decay EventPo218 Decay Event Calibration factor = (activity)/(event rate) [pCi/liter/Hz] Radon detector Pump X Flow meter Filter Temp. Humidity Sensor X 300cc/min Silicagel 280g, 452cc Grain size : Φ3mm 11.5 liter/min 222Rn 130.3Bq ~1.8pCi/L/Hz = ~ 47Bq/Hz

Workshop for Underground experiments and astroparticle physics 17 Humidity Dependence Test Setup  Po positive ion easily attach to water molecule ⇒ “Neutralize” Po ion ⇒ Cannot detect alpha decay Always ~74% at 25 ℃ Saturated solution Salt (ex. NaCl) Radon detector (With know radon activity) Pump X Flow meter Temp. Humidity Sensor X 11.5 liter/min NaCl saturated water X X ~74% at 25 ℃

Workshop for Underground experiments and astroparticle physics 18 Humidity Dependence of Efficiency Humidity factor = (real event rate) / (expected event rate) Somewhat different with other experiment measurement Absolute humidity [kg/m 3 ] Humidity factor

Workshop for Underground experiments and astroparticle physics 19 Y2L Radon Level Days elapsed since (pCi/Liter)

Workshop for Underground experiments and astroparticle physics 20 Radioactivity data for other experiment Mine air~ SNOSudbury ~10UKDMCBoulby 80~100CDMSSoudan ~1~ 500KIMSYYL DAMA detector Mine air. Ventilation dependence ~670DAMA, CRESST, Borexino GranSasso Mine air. Seasonal dependence Control room S-K, KamLand Kamioka Rn222 contents(pCi/L) U contents (ppb) Exp.Location

Workshop for Underground experiments and astroparticle physics 21 Radon-Free techniques  Blocking  Filtering  Ventilation

Workshop for Underground experiments and astroparticle physics 22 Radon Blocking capability for various material

Workshop for Underground experiments and astroparticle physics 23 Radon Blocking material :Example of KamLand

Workshop for Underground experiments and astroparticle physics 24 Ventilation dependence of Radon

Workshop for Underground experiments and astroparticle physics 25 Summary  Radon monitoring detector setup completed in Y2L  Radon contamination level monitoring in the air of Y2L is ongoing  Radioactivity in the rock is similar and radon activity is much lower than other experiment  Gamma background reduction from radon daughter elements in KIMS experiments is possible