Searching for Quantum Gravity with AMANDA-II and IceCube John Kelley November 11, 2008 PANIC’08, Eilat, Israel.

Slides:



Advertisements
Similar presentations
Teppei Katori, Indiana University1 PRD74(2006) Global 3 parameter Lorentz Violation model for neutrino oscillation with MiniBooNE Teppei Katori,
Advertisements

Searching for Quantum Gravity with High-energy Neutrinos John Kelley Radboud University Nijmegen ESQG Workshop Nordita, Stockholm, Sweden July 12, 2010.
The IceCube Neutrino Telescope Kyler Kuehn Center for Cosmology and AstroParticle Physics The Ohio State University Novel Searches for Dark Matter CCAPP.
Sean Grullon For the IceCube Collaboration Searching for High Energy Diffuse Astrophysical Neutrinos with IceCube TeV Particle Astrophysics 2009 Stanford.
The IceCube Neutrino Telescope Project overview and Status EHE Physics Example: Detection of GZK neutrinos TAUP2003 Shigeru Yoshida, Chiba University.
IceCube.
Recent Results Lutz Köpke University of Mainz, Germany July 31, 2003
Search for Extremely-high Energy Cosmic Neutrino with IceCube Chiba Univ. Mio Ono.
Optical Sensor and DAQ in IceCube Albrecht Karle University of Wisconsin-Madison Chiba July, 2003.
The IceCube High Energy Telesope The detector elements Expected Sensitivity Project Status Shigeru Yoshida Dept. of Physics CHIBA Univ. ICRC 2003.
Neutrino Astronomy at the South Pole David Boersma UW Madison “New Views of the Universe” Chicago, 10 December 2005.
IceCube a kilometer-scale deep-ice observatory in Antarctica Olga Botner Uppsala university, Sweden Neutrino 2004, June 14-19, icecube.wisc.edu.
1. Introduction 2. IceCube Detector 3. Neutrino Detection Principles 4. Status of the Construction and Performance 5. Summary IceCube neutrino
1 IceCube: A Neutrino Telescope at The South Pole Chihwa Song UW-Madison photographed by Mark Krasberg 4 th Korean Astrophysics Workshop May 17-19, 2006.
M. Giorgini University of Bologna, Italy, and INFN Limits on Lorentz invariance violation in atmospheric neutrino oscillations using MACRO data From Colliders.
Per Olof Hulth Stockholm university1 NSF Review March 25-27, 2003 Introductory remarks Per Olof Hulth Stockholm university.
A km 3 Neutrino Telescope: IceCube at the South Pole Howard Matis - LBNL for the IceCube Collaboration.
Alexander Kappes LTP/PSI Colloquium Paul Scherrer Institut, 30. Sept Neutrinos on the rocks – Astronomy at the South Pole with IceCube.
IceCube S Robbins University of Wuppertal Moriond - “Contents and Structures of the Universe” La Thuile, Italy, March 2006 Outlook for Neutrino Detection.
Frontiers in Contemporary Physics: May 23, 2005 Recent Results From AMANDA and IceCube Jessica Hodges University of Wisconsin – Madison for the IceCube.
Tyce DeYoung Penn State University for the IceCube Collaboration June 22, 2007 IceCube Recent Results and Prospects Rome International Conference on Astroparticle.
First Results from IceCube Physics Motivation Hardware Overview Deployment First Results Conclusions & Future Plans Spencer Klein, LBNL for the IceCube.
Neutrino Astronomy at the South Pole David Boersma UW Madison Lake Louise Winter Institute Chicago, 23 February 2006.
CIPANP 2006K. Filimonov, UC Berkeley From AMANDA to IceCube: Neutrino Astronomy at the South Pole Kirill Filimonov University of California, Berkeley.
The Status of IceCube Mark Krasberg University of Wisconsin-Madison RICH 2004 Conference, Playa del Carmen, Mexico Dec 3, 2004.
Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array.
News from the South Pole: Recent Results from the IceCube and AMANDA Neutrino Telescopes Alexander Kappes UW-Madison PANIC ‘08 November 2008, Eilat (Israel)
Neutrino Astronomy at the South Pole Searches for astrophysical high-energy neutrinos with IceCube Kurt Woschnagg UC Berkeley Miami 2012 Lago Mar, Ft Lauderdale,
COSMO/CosPA 2010 Searches for the Highest Energy Neutrino with IceCube Searches for the Highest Energy Neutrino with IceCube Aya Ishihara ( Fellow) (JSPS.
B.Baret Vrije Univertsiteit Brusse l Vrije Universiteit Brussel, Belgium The AMANDA – IceCube telescopes & Dark Matter searches B. Baret on behalf of the.
Sensitivity to New Physics using Atmospheric Neutrinos and AMANDA-II John Kelley UW-Madison Penn State Collaboration Meeting State College, PA June 2006.
Madison, May 20, 2009 Tom Gaisser1 IceCube Collaboration Overview & Response to 2008 SAC Report.
IceCube a new window on the Universe Muons & neutrinos Neutrino astronomy IceCube science Status & plans Tom Gaisser for the IceCube Collaboration Arequipa,
1 MACRO constraints on violation of Lorentz invariance M. Cozzi Bologna University - INFN Neutrino Oscillation Workshop Conca Specchiulla (Otranto) September.
AMANDA. Latest Results of AMANDA Wolfgang Rhode Universität Dortmund Universität Wuppertal for the AMANDA Collaboration.
IceCube and AMANDA: Neutrino Astronomy at the South Pole Brennan Hughey February 22nd, 2007.
1 Jan Conrad (CERN) GLAST Lunch, 09. Mar. 2006, Jan Conrad (KTH) The AMANDA neutrino telescope: Results from GRB and dark matter searches Jan Conrad (KTH,
Alexander Kappes Erlangen Centre for Astroparticle Physics for the ANTARES collaboration IAU GA, SpS 10, Rio de Janeiro, Aug Status of Neutrino.
KEK, Feb 27, 2006Tom Gaisser1 Cosmic-ray physics with IceCube IceTop the surface component of IceCube.
XIX European Cosmic Ray Symposium Firenze (Italy) Neutrino Astronomy and Cosmic Rays at the South Pole Latest.
Science Advisory Committee March 30, 2006 Jim Yeck IceCube Project Director IceCube Construction Progress.
Status and Results Elisa Bernardini DESY Zeuthen, Germany VLVnT Workshop Amsterdam, Oct (
IPPOG masterclass working group May 15, Building an IceCube Collaboration outreach activity Inspired by the International Masterclasses for hands-
IceCube: Status and Results
IceCube project Shigeru Yoshida Dept. of Physics, Chiba University.
Searching for Quantum Gravity with AMANDA-II and IceCube John Kelley IceCube Collaboration University of Wisconsin, Madison, U.S.A. October 27, 2008 KICP.
Icecube Neutrino Observatory at the South Pole Kirill Filimonov, University of California, Berkeley, for the IceCube Collaboration.
To Determine the Initial Flavor Composition of UHE Neutrino Fluxes with Neutrino Telescopes Shun Zhou ( IHEP, Beijing ) April 23-26, 2006 International.
Tests of Lorentz Invariance using Atmospheric Neutrinos and AMANDA-II John Kelley for the IceCube Collaboration University of Wisconsin, Madison Workshop.
I Taboada, GA Tech High-energy neutrino astronomy with IceCube Ignacio Taboada Georgia Institute of Technology for the IceCube collaboration Madison, NDM.
1 Particles and Nuclei International Conference (PANIC05) Santa Fe, NM (U.S.A.) October 24 th, from Quark n.36, 02/01/04 Neutrino.
08/2006Julia Becker, Universität Dortmund TeV particle astrophysics, Madison Julia Becker for the IceCube collaboration August 2006 by the AMANDA experiment.
1 slide Brennan Hughey University of Wisconsin – Madison for the AMANDA Collaboration Recent Results From the AMANDA Experiment Rencontres du Vietnam August.
Sensitivity to New Physics using Atmospheric Neutrinos and AMANDA-II John Kelley UW-Madison IceCube Collaboration Meeting Baton Rouge, LA April 10, 2006.
IceCube Neutrino Telescope Astroparticle Physics at the South Pole Brendan Fox Pennsylvania State University for the IceCube Collaboration VLVNT08 - Very.
Search for Ultra-High Energy Tau Neutrinos in IceCube Dawn Williams University of Alabama For the IceCube Collaboration The 12 th International Workshop.
High-energy Neutrino Astrophysics with IceCube Neutrino Observatory
Albrecht Karle University of Wisconsin - Madison for the IceCube Collaboration IceCube Current status, recent results and future prospects.
Dark Matter Searches with AMANDA and IceCube Catherine De Clercq for the IceCube Collaboration Vrije Universiteit Brussel Interuniversity Institute for.
1 IceCube Christian Spiering for the IceCube Collaboration EPSC, Cracow July 2009.
Measuring the total neutrino cross section using the IceCube detector
Searching for New Physics with Atmospheric Neutrinos and AMANDA-II
Julia Becker for the IceCube collaboration
Analysis of Atmospheric Neutrinos: AMANDA
Searching for Quantum Gravity with Atmospheric Neutrinos
IceCube Neutrino Telescope Astroparticle Physics at the South Pole
Status and prospects of the IceCube Neutrino Telescope
The IceCube Neutrino Telescope
Probing the Broken - Symmetry with Neutrino Telescopes
Presentation transcript:

Searching for Quantum Gravity with AMANDA-II and IceCube John Kelley November 11, 2008 PANIC’08, Eilat, Israel

AMANDA-II optical module The AMANDA-II neutrino telescope is buried in deep, clear ice, 1500m under the geographic South Pole 677 optical modules: photomultiplier tubes in glass pressure housings (~540 used in analysis) Muon direction can be reconstructed to within 2-3º

AMANDA-II skiway South Pole Station Geographic South Pole Amundsen-Scott South Pole Research Station

Current Experimental Status neutrino skymap, courtesy of J. Braun (publication in preparation; see his talk) Opportunity for particle physics with high-energy atmospheric No detection (yet) of –point sources or other anisotropies –diffuse astrophysical flux –transients (e.g. GRBs, AGN flares, SN) Astrophysically interesting limits set Large sample of atmospheric neutrinos –AMANDA-II: >5K events, TeV

New Physics with Neutrinos? Neutrinos are already post-Standard Model (massive) For E > 100 GeV and m Oscillations are a sensitive quantum-mechanical interferometer — small shifts in energy can lead to large changes in flavor content Eidelman et al.: “It would be surprising if further surprises were not in store…”

New Physics Effects Violation of Lorentz invariance (VLI) in string theory or loop quantum gravity* Violations of the equivalence principle (different gravitational coupling) † Interaction of particles with space-time foam  quantum decoherence of flavor states ‡ * see e.g. Carroll et al., PRL (2001), Colladay and Kosteleck ý, PRD (1998) † see e.g. Gasperini, PRD (1989) ‡ see e.g. Anchordoqui et al., hep-ph/ c -  1 c -  2

VLI Atmospheric  Survival Probability maximal mixing,  c/c = VLI oscillations from velocity eigenstates

QD Atmospheric  Survival Probability p=1/3 decoherence into superposition of flavors

Results: Observables Data consistent with atmospheric neutrinos + O(1%) background Confidence intervals constructed with F+C plus systematics zenith anglenumber of OMs hit

Results: Preliminary VLI limit SuperK+K2K limit*:  c/c < 1.9  (90%CL) This analysis:  c/c < 2.8  (90%CL) 90%, 95%, 99% allowed CL excluded *González-García & Maltoni, PRD (2004) maximal mixing

Results: Preliminary QD limit SuperK limit ‡ (2-flavor):  i < 0.9  GeV -1 (90% CL) ANTARES sensitivity* (2-flavor):  i ~ GeV -1 (3 years, 90% CL) This analysis:  i < 1.3  GeV -1 (90% CL) * Morgan et al., astro-ph/ ‡ Lisi, Marrone, and Montanino, PRL 85 6 (2000) E 2 model best fit excluded log 10  * 6,7 / GeV -1 log 10  * 3,8 / GeV -1

Conventional Analysis Parameters of interest: normalization, spectral slope change  relative to Barr et al. Result: determine atmospheric muon neutrino flux (“forward-folding” approach) 90%, 95%, 99% allowed best fit normalization change in spectral slope

Result Spectrum Blue band: SuperK data, González-García, Maltoni, & Rojo, JHEP 0610 (2006) 075 this work

AMANDA-II IceCube skiway South Pole Station Geographic South Pole Update on IceCube

Installation Status & Plans AMANDA IceCube string deployed 12/05 – 01/06 IceCube string deployed 01/05 IceCube string and IceTop station deployed 12/06 – 01/ IceCube Lab commissioned 40 strings taking physics data Planning for at least 16 strings in 2008/09 IceCube string deployed 12/07 – 01/ m deep hole!

IceCube VLI Sensitivity IceCube: sensitivity of  c/c ~ Up to 700K atmospheric  in 10 years (González-García, Halzen, and Maltoni, hep-ph/ ) IceCube 10 year

Other Possibilities Extraterrestrial neutrino sources would provide even more powerful probes of QG –GRB neutrino time delay ( see, e.g. Amelino-Camelia, gr-qc/ ) –Electron antineutrino decoherence from, say, Cygnus OB2 (see Anchordoqui et al., hep- ph/ ) Hybrid techniques (radio, acoustic) will extend energy reach — GZK neutrinos

USA: Bartol Research Institute, Delaware Pennsylvania State University UC Berkeley UC Irvine Clark-Atlanta University University of Alabama Ohio State University Georgia Institute of Technology University of Maryland University of Wisconsin-Madison University of Wisconsin-River Falls Lawrence Berkeley National Lab. University of Kansas Southern University and A&M College, Baton Rouge University of Alaska, Anchorage Sweden: Uppsala Universitet Stockholm Universitet UK: Oxford University Belgium: Université Libre de Bruxelles Vrije Universiteit Brussel Universiteit Gent Université de Mons-Hainaut Germany: Universität Mainz DESY-Zeuthen Universität Dortmund Universität Wuppertal Humboldt Universität MPI Heidelberg RWTH Aachen Japan: Chiba University New Zealand: University of Canterbury THE ICECUBE COLLABORATION Netherlands: Utrecht University Switzerland: EPFL Thank you!

Backup Slides

Violation of Lorentz Invariance (VLI) Lorentz and/or CPT violation is appealing as a (relatively) low-energy probe of QG Effective field-theoretic approach by Kostelecký et al. (SME: hep-ph/ , hep-ph/ ) Addition of renormalizable VLI and CPTV+VLI terms; encompasses a number of interesting specific scenarios

Rotationally Invariant VLI Only c AB 00 ≠ 0; equivalent to modified dispersion relation * : Different maximum attainable velocities c a (MAVs) for different particles:  E ~ (  c/c)E For neutrinos: MAV eigenstates not necessarily flavor or mass eigenstates  mixing  VLI oscillations * see Glashow and Coleman, PRD (1999)

VLI Phenomenology Effective Hamiltonian (seesaw + leading order VLI+CPTV): To narrow possibilities we consider: –rotationally invariant terms (only time component) –only c AB 00 ≠ 0 (leads to interesting energy dependence…)

VLI + Atmospheric Oscillations For atmospheric, conventional oscillations turn off above ~50 GeV (L/E dependence) VLI oscillations turn on at high energy (L E dependence), depending on size of  c/c, and distort the zenith angle / energy spectrum (other parameters: mixing angle , phase  ) González-García, Halzen, and Maltoni, hep-ph/

Decoherence + Atmospheric Oscillations Energy dependence depends on phenomenology: n = -1 preserves Lorentz invariance n = 0 simplest n = 2 recoiling D-branes* n = 3 Planck-suppressed operators ‡ *Ellis et al., hep-th/ ‡ Anchordoqui et al., hep-ph/ characteristic exponential behavior 1:1:1 ratio after decoherence derived from Barenboim, Mavromatos et al. (hep-ph/ )