“Other” UCN Physics Jeff Martin University of Winnipeg TRIUMF Townhall Meeting Ultracold Neutron Working Group Aug. 2007 Topics: 1. n-nbar oscillations.

Slides:



Advertisements
Similar presentations
TRIUMF UCN workshop, 2007 Solid state physics experiments with UCN E. Korobkina.
Advertisements

Bruce Kennedy, RAL PPD Particle Physics 2 Bruce Kennedy RAL PPD.
The electromagnetic (EM) field serves as a model for particle fields
IKON7, Instrument clip session, September 2014, ESS Headquarters and Medicon Village, Lund, Sweden A cold neutron beamline for Particle
Discrete Space-Time Symmetries Xiao-Gang He USTC, Nanakai, and NTU 1. Discrete Space-Time Symmetries 2. The Down Fall of Parity P Symmetry 3. The Down.
Bruce Kennedy, RAL PPD Particle Physics 2 Bruce Kennedy RAL PPD.
The electromagnetic (EM) field serves as a model for particle fields  = charge density, J = current density.
Neutrino Physics - Lecture 1 Steve Elliott LANL Staff Member UNM Adjunct Professor ,
Another Route to CP Violation Beyond the SM – Particle Dipole Moments Dave Wark Imperial/RAL WIN05 Delphi June 10, 2005.
TESTING EXTRA DIMENSIONS Jonathan Feng University of California, Irvine Kavli Frontiers of Science Symposium National Academy of Sciences 2-4 November.
November 2, 2006LIGO / pulsar workshop1 How LIGO searches are affected by theory & astronomical observations Ben Owen.
Concluding Comments For the Course Cosmology Fascinating Past Highly accomplished present (for example, the material covered in this course). Really exciting.
NNbar program: 3:30-5:30 R. N. Mohapatra: 3:30-4:00 (25+5) What physics from NNbar ? K. S. Babu: 4:00-4:25 (20+5) Origin of matter and NNbar R. Shrock:
Topological Insulators and Beyond
1 New Frontiers in Particle Physics Jeff Forshaw University of Manchester.
Dark Matter Masses of Galaxies Gravity and Light Black Holes What is Dark Matter?
Dark Matter Search with Direction sensitive Scintillator Ⅱ Department of Physics, School of Science The University of Tokyo Y. Shimizu, M. Minowa, Y. Inoue.
P WARNING: Exam 1 Week from Thursday. P Class 09: Outline Hour 1: Conductors & Insulators Expt. 4: Electrostatic Force Hour 2: Capacitors.
Fundamental Physics With Cold and Ultra-cold Neutrons Albert Young North Carolina State University.
Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 1 Chapter 30: Particle Physics Fundamental.
Yuri Kamyshkov/ University of Tennessee Mini-Workshop, WU St. Louis, February 11, 2011.
4-th SNOLAB Workshop, August 15-17, 2005 at Sudbury Yuri Kamyshkov Univ. of Tennessee TRIGA reactor.
Underground Laboratories and Low Background Experiments Pia Loaiza Laboratoire Souterrain de Modane Bordeaux, March 16 th, 2006.
Hadron Spectroscopy with high momentum beam line at J-PARC K. Ozawa (KEK) Contents Charmed baryon spectroscopy New experiment at J-PARC.
March 2005 Theme Group 2 What can N-N-bar Oscillation teach us about physics Beyond the standard model ? R. N. Mohapatra University of Maryland NANO workshop,
On behalf of NNbar Collaboration Yuri Kamyshkov University of Tennessee May 5, 2006 SUNY Stony Brook Search for neutron  antineutron transitions at DUSEL.
Neutron-Antineutron Oscillations With Cold Neutron Beams
Neutrino mass and DM direct detection Daijiro Suematsu (Kanazawa Univ.) Erice Sept., 2013 Based on the collaboration with S.Kashiwase PRD86 (2012)
Lecture 23: Applications of the Shell Model 27/11/ Generic pattern of single particle states solved in a Woods-Saxon (rounded square well)
The Higgs Boson Observation (probably) Not just another fundamental particle… July 27, 2012Purdue QuarkNet Summer Workshop1 Matthew Jones Purdue University.
M. Deveaux, CBM-Collaboration-Meeting, 25 – 28. Feb 2008, GSI-Darmstadt Considerations on the material budget of the CBM Micro Vertex Detector. Outline:
Brian Plimley Physics 129 November Outline  What is the anomalous magnetic moment?  Why does it matter?  Measurements of a µ  : CERN.
7 April 2006 Determining Optical Constants for ThO 2 Thin Films Sputtered Under Different Bias Voltages from 1.2 to 6.5 eV by Spectroscopic Ellipsometry.
Contents Introduction (motivation of precise measurements of neutron lifetime, history of experimental accuracy improvement). a. Result of neutron lifetime.
1 Nuclear Fusion Class : Nuclear Physics K.-U.Choi.
International Workshop “Search for Baryon and Lepton Number Violations”, LBLN Berkeley, September Yuri Kamyshkov / University of Tennessee.
Backup slides Z 0 Z 0 production Once  s > 2M Z ~ GeV ÞPair production of Z 0 Z 0 via t-channel electron exchange. e+e+ e-e- e Z0Z0 Z0Z0 Other.
ANTIHYDROGEN Gravitational States above material surface A. Voronin P.Froelich V.Nesvizhevsky.
Ultra-Cold Neutron Group in Kellogg Lab - Neutron Electric Dipole Moment (EDM) Experiment - Search for new CP violation - Neutron Decay - Precision measurements.
Mike Cruise University of Birmingham Searches for very high frequency gravitational waves.
Chris Parkes University of Manchester Part VI Concluding Remarks 1)Other flavour physics / CPV searches 2)Overall Constraints on CKM Triangle.
An Ultracold Neutron Source for TRIUMF 1. UCN interactions 2. UCN physics experiments 3. Source work at RCNP and TRIUMF 4. CFI, relationship, collaboration,
Electric Dipole Response, Neutron Skin, and Symmetry Energy
qBOUNCE: a quantum bouncing ball gravity spectrometer
Standard Model of Particle Physics
Solar Neutrinos on the beginning of 2017
UCN transport and NN experiments
Latest results from the superfluid-helium UCN source SUN2 at ILL
Experiments on Fast Ion Instability at PLS
HOW TO TELL DIFFERENCE OF MAJORANA/DIRAC NEUTRINOS
The Dark Universe Susan Cartwright.
Using ultracold neutrons to constrain the neutron electric dipole moment Tamas Budner.
An interesting candidate?
University of Manchester
R. Young, M. Makela, G. Muhrer, C. Morris, A. Saunders
Gravitational Quantum States of Antihydrogen
Wakefield Accelerator
Light as a Wave                                            SPH4U Young Star Cluster NGC 7129.
Ron Settles MPI-Munich
Building ICECUBE A Neutrino Telescope at the South Pole
Building ICECUBE A Neutrino Telescope at the South Pole
dark matter and the Fate of the Universe
Radiation Shield Design by UA
neutron lifetime experiments
Modern observation and simulation of the physics of kinetic cascade leading to production of internal energy Organizers: William H Matthaeus, Tulasi N.
Frontiers of fundamental physics
Analysis of proximity effects in S/N/F and F/S/F junctions
The idea behind particle accelerators (atom smashers):
Cosmology.
Technician’s Notes Activity 10S Software Based 'Bubble chamber photographs'
Presentation transcript:

“Other” UCN Physics Jeff Martin University of Winnipeg TRIUMF Townhall Meeting Ultracold Neutron Working Group Aug Topics: 1. n-nbar oscillations (Kamyshkov, Young, Snow) 2. n to “mirror neutron” oscillations (Pokotilovski, Ban et al, Serebrov et al) 3. surface physics (Steyerl, Korobkina, et al) physics – experiment - TRIUMF

1. n-nbar oscillations ● A search for baryon number violation ● predictions in various models show possibilities just beyond current limit – supersymmetry (Mohapatra) – extra dimensions (Shrock) ● baryon number violation required to explain BAU (but doesn't necessitate nnbar oscillations) ● current limit for free neutrons (CN beam) – tau > 8.6e7 seconds

Vertical Cold Beam

Snow, 2003.

UCN-nbar oscillation experiment ● create a bunch of UCN ● put them in a bottle ● search for 5 pions appearing from the edge of your bottle, signifying annihilation of an nbar. ● magnetic shielding (magnetic moment of nbar is opposite that of n) ● previous best experiment was done with cold neutrons on a long beamline at ILL.

~few metres

UCN-UCNbar experiment issues: big detector B = 0 “resetting” of UCN wavefunction at surfaces => discovery potential linear w/ meas't time if there were no walls (or infinitely large vessel) would go as t^2. need lots of UCN

UCN-UCNbar history ● discussed extensively in recent workshops – IU, 2002 – Berkeley, 2007 (the week after our UCN workshop) ● considered in great detail in a set of two long papers by Yoshiki and Golub. – magnetic field tricks might maintain coherence at walls, partially, if UCNbar-nucleus interaction well known

Comments on nnbar for TRIUMF ● Very high physics rating. ● Requires high production and high density, which has never been created, anywhere, yet. ● Experiment alone would cost $10M. ● A good future goal to shoot for as UCN production increases.

2. n-n' oscillations: “mirror neutrons” ● Maybe there is a mirror universe with identical particle content to our own. ● A way to restore global parity symmetry. (Kobrzarev, Okun, Pomeranchuk, 1966) ● Recently: interesting implications for cosmology and particle physics – mirror universe as dark matter candidate – in 2005, no experimental limit on n-n' oscillations. Fast oscillations (tau << nlife) could erase GZK cutoff (PRL 2006, Berezhiani, Bento) – relationship to supersymmetry (Mohapatra, 2005)

Experiments ● Berezhiani, Bento derived tau > 1 s based on the old ILL nnbar experiment. ● So, any lab that had any UCN (ILL) and some magnets went searching... – Pokotilovski suggested a bunch of experiments (2006) – Ban et al (2007) tau > 103 s – Serebrov et al (2007) tau > 414 s

Basic experimental setup (Serebrov paper) ● Put in UCN ● See how many come out ● Compare experiments – B = 0 – B ≠ 0 B = 0 => degenerate => oscillations, B ≠ 0 => nondegenerate => no oscillations

Comments on Mirror Neutrons for TRIUMF ● Physics interest originally centered around short oscillation times. ● The easiest experiments have already been done. ● Possibly there would still be interest in several years time. ● Seems risky to bank our program on it.

3. Surface and Materials Physics with UCN ● Are mentioned in the UCN book (Golub, Richardson, Lamoreaux, 1991) – limited by flux – clever pioneering experiments by Steyerl ● Most modern work seems focused on interactions of UCN with surfaces, usually in relation to understanding the interaction so that better UCN- lifetime measurements can be made – Steyerl et al, EPJB 28, 299 (2002) – Korobkina et al, PRB 70, (2004)

E.g. Korobkina et al PRB article ● Most losses of UCN on surfaces are due to hydrogen on the surface – but what kind of hydrogen (tightly, weakly bound? 2D gas?) and how? ● Studied low-temperature (<77K) dependence of UCN loss rates on Cu surface with different surface qualities in oil-free vacuum. ● Discovered loss rate decreases with temperature

Interpretation ● Cu-H bond model disagees with data ● H2O ice in surface clusters agrees with date (or “hydrogenated surface clusters” C-H and/or O-H bonds) ● model based on previous measurements of theirs on (n,gamma) on surfaces, also done using UCN, and on measurements of surface contamination in first 10 nm of surface (showed 8% hydrogen contamination)

Relevance for surface physics ● Korobkina et al comment that – UCN very sensitive to hydrogenated films – can be used to monitor low frequency excitations in ~nm thick films with V_F < E_UCN (e.g. polymers, ice,...) – two methods: ● (n,gamma) using UCN ● UCN losses – sensitivity complementary to ● NIS (neutron inel. scatt.) (sensitive to bulk and higher energy excitations) ● electrons (thin films, but not H)

Comments on surface physics for TRIUMF ● Need more UCN to be useful (even Korobkina says that) ● Details of this type of surface physics have not been understood for 30 yrs – “anomalous losses” of UCN ● Possible to draw parallels with success of CN case, where instruments have been developed over time. ● A good goal to have, but nothing terribly concrete.

Summary and relevance to white paper 1. n-nbar oscillations ● good future goal 2. n to “mirror neutron” oscillations ● might be interesting if we had a source right now 3. surface physics ● interesting now, but need good ideas - in all three cases, if you have any UCN, people will be interested. - Personally, I do not see a (fast, initial) flagship experiment, here.