Search for Strangelets in Lunar Soil Ke Han / May 26, 2016 ------------------------------------ Alexei Chikanian, Evan Finch, Ke Han, Richard Majka, Jack.

Slides:



Advertisements
Similar presentations
PID v2 and v4 from Au+Au Collisions at √sNN = 200 GeV at RHIC
Advertisements

Professor: Scott M. LaBrake Course: Physics 300 – Spring 2013 Office: NWSE N308, N008b Phone: & 6562 Office Hours: MWF.
Strangelets and nuclearites—an overview
Spontaneous Parity Violation in Strong Interactions Dhevan Gangadharan (UCLA) On behalf of the STAR Collaboration WWND
Search for nuclearites with the SLIM detector V. Popa, for the SLIM Collaboration From Colliders to Cosmic Rays 7 – 13 September 2005, Prague, Czech Republic.
Search for Strange Quark Matter and Q-Balls with the SLIM Experiment. Zouleikha Sahnoun Astrophys. Dept. CRAAG, Algiers & INFN Bologna, Italy.
Search for spontaneous muon emission from lead nuclei with OPERA bricks M. Giorgini, V. Popa Bologna Group OPERA Collaboration Meeting, LNGS, 19-22/05/2003.
March 13thXXXXth RENCONTRES DE MORIOND 1 The Alpha Magnetic Spectrometer on the International Space Station Carmen Palomares CIEMAT (Madrid) On behalf.
MAGNETIC MONOPOLES Andrey Shmakov Physics 129 Fall 2010 UC Berkeley.
24/04/2007ALICE – Masterclass Presentation1 ALICE Hannah Scott University of Birmingham.
Charged Particles. Nuclear Physics Charged particles can come from nuclear decay. Nuclear physics figures into particle detection. Use terminology from.
Christopher G. Hamaker, Illinois State University, Normal IL
Cross section measurements for analysis of D and T in thicker films Liqun Shi Institute of Modern Physics, Fudan University, Shanghai, , People’s.
30 Ge & Si Crystals Arranged in verticals stacks of 6 called “towers” Shielding composed of lead, poly, and a muon veto not described. 7.6 cm diameter.
Stopping Power The linear stopping power S for charged particles in a given absorber is simply defined as the differential energy loss for that particle.
Atomic Structure and Radiation REVIEW GAME
Atmospheric Neutrino Oscillations in Soudan 2
Sayfa 1 EP228 Particle Physics Department of Engineering Physics University of Gaziantep Dec 2014 Topic 5 Cosmic Connection Course web page
NUCLEAR UNIT A: Radiation, Energy and Atoms. RADIATION  Irradiation is the exposure of a sample of material to radiation.  There are many types of radiation.
Sevil Salur for STAR Collaboration, Yale University WHAT IS A PENTAQUARK? STAR at RHIC, BNL measures charged particles via Time Projection Chamber. Due.
SL Chemistry Tuesday September 22nd Agenda Begin Topic 2 - Atomic Structure.
ISOTOPES & AVERAGE ATOMIC MASS
W properties AT CDF J. E. Garcia INFN Pisa. Outline Corfu Summer Institute Corfu Summer Institute September 10 th 2 1.CDF detector 2.W cross section measurements.
Search for Strangelets with Solid State Nuclear Track Detectors ATANU MAULIK Center for Astroparticle Physics and Space Science Bose Institute Kolkata,
March 13thXXXXth RENCONTRES DE MORIOND 1 The Alpha Magnetic Spectrometer on the International Space Station Carmen Palomares CIEMAT (Madrid) On behalf.
Energy Distribution of Cosmic Ray Muons Paul Hinrichs With David Lee Advised by Phil Dudero.
Evaluation of the flux of CR nuclei inside the magnetosphere P. Bobik, G. Boella, M.J. Boschini, M. Gervasi, D. Grandi, K. Kudela, S. Pensotti, P.G. Rancoita.
Radioactivity and radioisotopes The nature of radiation Distinguishing Radiation Background Radiation.
Atomic Structure. Elements and Atoms Element- a pure substance made up of only one type of atom. Atom- smallest unit of an element that maintains the.
 -capture measurements with the Recoil-Separator ERNA Frank Strieder Institut für Physik mit Ionenstrahlen Ruhr-Universität Bochum HRIBF Workshop – Nuclear.
Mass spectrometry (Test) Mass spectrometry (MS) is an analytical technique that measures masses of particles and for determining the elemental composition.
Measurement of lifetime for muons captured inside nuclei
Nuclear Radiation R A D I O A C T I V ER A D I O A C T I V E ?
8 th Topical Seminar on “Innovative Particle and Radiation Detectors” Siena Oct CALIBRATION AND SEARCH FOR EXOTIC PARTICLES WITH CR39 AND MAKROFOL.
Hadron Spectroscopy with high momentum beam line at J-PARC K. Ozawa (KEK) Contents Charmed baryon spectroscopy New experiment at J-PARC.
Light nuclei production in heavy-ion collisions at RHIC Md. Rihan Haque, for the STAR Collaboration Abstract Light nuclei (anti-nuclei) can be produced.
CEBAF The Continuous Electron Beam Accelerating Facility (CEBAF) at JLab in Newport News, Virginia, is used to study the properties of quark matter. CEBAF.
KPS Chonbuk University 2005/10/22 HYUNSU LEE Status of the KIMS dark matter search experiment with CsI(Tl) crystals Hyun Su Lee Seoul National.
A. Bâ, S. Balestra, M. Cozzi, G. Giacomelli, R. Giacomelli, M. Giorgini, A. Kumar G. Mandrioli, S. Manzoor, A.R. Margiotta, E. Medinaceli, L. Patrizii,
Jet Physics at CDF Sally Seidel University of New Mexico APS’99 24 March 1999.
Nucleon Decay Search in the Detector on the Earth’s Surface. Background Estimation. J.Stepaniak Institute for Nuclear Studies Warsaw, Poland FLARE Workshop.
1 Experimental particle physics introduction. 2 What holds the world together?
Why Accelerator Mass spectrometry (AMS) The determination of the concentration of a given radionuclide in a sample can be done in 2 ways: a) measure the.
On Detecting Strange Quark Matter with GLAST-LAT 1 Department of Physics, Royal Institute of Technology (KTH), Stockholm, Sweden Contact:
Monday, Sept. 18, 2006PHYS 3446, Fall 2006 Jae Yu 1 PHYS 3446 – Lecture #5 Monday, Sept. 18, 2006 Dr. Jae Yu 1.Nuclear Phenomenology 2.Properties of Nuclei.
Nuclear Changes Objectives: Students will:
Radioactivity By the end of this chapter you should be able to: describe the properties of alpha, beta and gamma radiations; explain why some nuclei are.
2 protons 2 neutrons Energy of a nucleus The mass of a helium nucleus is slightly smaller (
 0 life time analysis updates, preliminary results from Primex experiment 08/13/2007 I.Larin, Hall-B meeting.
INTERACTIONS OF RADIATION WITH MATTER. twCshttp:// twCs
Methodology to Search for Massive Particle in Cosmic Rays Takeshi SAITO Institute for Advanced Studies, Shinjyuku , Shinjyuku, Tokyo, Japan.
Thomas Roser Snowmass 2001 June 30 - July 21, 2001 Proton Polarimetry Proton polarimeter reactions RHIC polarimeters.
Lecture 8 Radiometric Dating
Absolute Polarization Measurement at RHIC in the Coulomb Nuclear Interference Region September 30, 2006 RHIC Spin Collaboration Meeting RIKEN, Wako, Japan.
Elements, Compounds, Mixtures, Law of Definite Proportions, and an Introduction to the Periodic Table.
A New Upper Limit for the Tau-Neutrino Magnetic Moment Reinhard Schwienhorst      ee ee
重离子碰撞中的 ( 反 ) 超核研究 马余刚 中国科学院上海应用物理研究所 引言 RHIC-STAR 的超核测量 – 超氚核构建 – 寿命测量 – 奇异性因子 GSI 超核寿命测量实验简介 超核产生机制研究 关于 H 粒子寻找简介.
History of the Atom. Atoms and Elements Any material that is composed of only one type of atom is called an element. An atom is the smallest particle.
Fiducial Cuts for the CLAS E5 Data Set K. Greenholt (G.P. Gilfoyle) Department of Physics University of Richmond, Virginia INTRODUCTION The purpose of.
Nuclear Chemistry The alpha particle (  ) The beta particle (  ) Gamma radiation (γ)
High p T hadron production and its quantitative constraint to model parameters Takao Sakaguchi Brookhaven National Laboratory For the PHENIX Collaboration.
The NSCL is funded in part by the National Science Foundation and Michigan State University. Results: the neutron source was located 19.9 inches from the.
THE MASS SPECTROMETER WHAT IS A MASS SPECTROMETER
Fundamental Particles, Fundamental Questions
Department of Tandem Accelerators
The BLAIRR Irradiation Facility Hybrid Spallation Target Optimization
The Transition Radiation Detector for the PAMELA Experiment
of secondary light ion beams
Simulation study for Forward Calorimeter in LHC-ALICE experiment
Presentation transcript:

Search for Strangelets in Lunar Soil Ke Han / May 26, Alexei Chikanian, Evan Finch, Ke Han, Richard Majka, Jack Sandweiss 1 Jeffrey Ashenfelter, Andreas Heinz, Peter Parker 2 Peter Fisher, Benjamin Monreal 3 Jes Madsen 4 1. High Energy Physics Group, Yale University 2. Wright Nuclear Structure Laboratory, Yale University 3. Laboratory for Nuclear Science, MIT 4. Physics Department, University of Aarhus, Denmark

SQM2008, Oct 9, Beijing Lunar Soil Strangelet Search --- Ke Han / Yale2 Strange Quark Matter SQM with similar amounts of u, d and s quarks could be metastable or even stable. Strangelets: SQM with A<10 6 Normal Strange C. Greiner, arXiv:nucl-th/

SQM2008, Oct 9, Beijing Lunar Soil Strangelet Search --- Ke Han / Yale3 Energy per baryon number Madsen, arXiv:astro-ph/ v1 (1998) Original calculation: Farhi and Jaffe, Phys. Rev. D 30, 2379 (1984) Stable region Bulk property Bag Model calculation

SQM2008, Oct 9, Beijing Lunar Soil Strangelet Search --- Ke Han / Yale4 Cosmic strangelet flux (if bulk SQM is stable) Strangelets are ejected from strange star collisions. −Strangelets travel along with cosmic rays to the Earth and Moon The Moon is a better depository than Earth −No geological activity  25% of strangelets stop within 10cm beneath the moon surface, and remain there. −No geomagnetic cutoff, no atmosphere  Low energy strangelets are not rejected. Strange Oxygen concentration is ~10 −16 per normal atoms in the lunar soil sample −500M year exposure to cosmic ray

SQM2008, Oct 9, Beijing Lunar Soil Strangelet Search --- Ke Han / Yale5 Interesting events Two events from AMS He: Z = 2, A~16 in ~10 6 Z = 2 cosmic ray events 54 O: Z = 8, A = 54+8(−6) event in ~10 5 events with Z > 2. Balloon-borne detectors events 4 events from 3 different experiments All consistent with strangelet characteristics, but none can be seen as definite evidence.

SQM2008, Oct 9, Beijing Lunar Soil Strangelet Search --- Ke Han / Yale6 Previous searches E. Finch, Strangelets: who is looking and how? J. Phys. G: Nucl. Part. Phys. 32 (2006) S251 Predicted strangelet flux from strange star collisions (J. Madsen) AMS-01 strange oxygen event

Our project Search for strangelets at 2σ range of the AMS-01 event. Confirm or rule out AMS-01 event: this requires a lunar soil search with sensitivity. SQM2008, Oct 9, Beijing Lunar Soil Strangelet Search --- Ke Han / Yale7

SQM2008, Oct 9, Beijing Lunar Soil Strangelet Search --- Ke Han / Yale8 Strangelet detection Smaller Z/A  longer stopping range  Strangelets are isolated on the E−dE plot. Without foil With foil

SQM2008, Oct 9, Beijing Lunar Soil Strangelet Search --- Ke Han / Yale9 Strangelet detection Smaller Z/A  longer stopping range  Strangelets are isolated on the E−dE plot. 56 Fe Without Foil With Foil

SQM2008, Oct 9, Beijing Lunar Soil Strangelet Search --- Ke Han / Yale10 Experiment setup Yale tandem Van-de-Graaff accelerator at WNSL. Inflector Magnet ‒ Mass acceptance 0.3amu ‒ Step size 0.25amu Analyzing Magnet V T =17MV, charge +5 E total =102MeV

SQM2008, Oct 9, Beijing Lunar Soil Strangelet Search --- Ke Han / Yale11 ZnS flag and Argon scint counter BeamZnS flag

SQM2008, Oct 9, Beijing Lunar Soil Strangelet Search --- Ke Han / Yale12 A typical run at 58.5 amu Calibrate the accelerator using 58 Ni beam at charge +11 and charge +5 Tune the accelerator according to the calibration and calculation to “transmit” mass 58.5 amu and charge +5 ions. Run for two hours. Check oxygen current out of the Inflector Magnet.

SQM2008, Oct 9, Beijing Lunar Soil Strangelet Search --- Ke Han / Yale13 Run the accelerator with no beam Accelerator Upgrade: –Generating Voltmeter (GVM) control module to regulate the V T without any beam feedback. –Hall Probe Teslameter inside the Inflector Magnet. “Calibration points”: –Doping the lunar soil sample with V, Co, Fe, Ni, or Cu. Strict run protocol

SQM2008, Oct 9, Beijing Lunar Soil Strangelet Search --- Ke Han / Yale14 Search sensitivity Single event sensitivity (SES) with respect to oxygen atom is determined by transmission efficiency. About 8% particles out of ion source per unit time We get as high as per second (16 uA). strangelet stripping prob. to charge +n. For n=5 ( 54 O), P n =0.4±0.1 run time per mass setting We run 2 hours

SQM2008, Oct 9, Beijing Lunar Soil Strangelet Search --- Ke Han / Yale15 Limits

Limits – Carbon and Fluorine SQM2008, Oct 9, Beijing Lunar Soil Strangelet Search --- Ke Han / Yale16

SQM2008, Oct 9, Beijing Lunar Soil Strangelet Search --- Ke Han / Yale17 Summary We searched for strangelet event with mass range 42 to 70 amu at about SES level. No strangelet signal was found. This may rule out the AMS-01 event pending evaluation of our full systematic errors. AMS-02 experiment will be 100 times more sensitive, and it covers the whole mass range.

SQM2008, Oct 9, Beijing Lunar Soil Strangelet Search --- Ke Han / Yale18

SQM2008, Oct 9, Beijing Lunar Soil Strangelet Search --- Ke Han / Yale19

Strangelet with Z≠8 The search is also sensitive to strangelets with Z≠8, like carbon and fluorine. SES (w.r.t. all atoms in lunar soil) for strange carbon and fluorine is proportional to SES of oxygen search The correlation coefficient is relative negative ion forming efficiency in the negative ion cone. SES fluorine =SES oxygen SES carbon =6 SES oxygen Nitrogen does not form negative ions. SQM2008, Oct 9, Beijing Lunar Soil Strangelet Search --- Ke Han / Yale20