CAN WE UNDERSTAND THE PAMELA POSITRON EXCESS AS WINOS? Gordy Kane January 2009 Ann Arbor arXiv 0812.4555, see also 0807.1509 Phill Grajek, Aaron Pierce,

Slides:



Advertisements
Similar presentations
Kiwoon Choi PQ-invariant multi-singlet NMSSM
Advertisements

Combined Energy Spectra of Flux and Anisotropy Identifying Anisotropic Source Populations of Gamma-rays or Neutrinos Sheldon Campbell The Ohio State University.
Dark Matter Annihilation in the Milky Way Halo Shunsaku Horiuchi (Tokyo) Hasan Yuksel (Ohio State) John Beacom (Ohio State) Shin’ichiro Ando (Caltech)
What mass are the smallest protohalos in thermal WIMP dark-matter models? Kris Sigurdson Institute for Advanced Study Space Telescope Science Institute.
MSSM in view of PAMELA and Fermi-LAT Ts. Enkhbat 2 nd workshop on LHC physics, CYCU, Chungli Based on: arXiv: B. BajcB. Bajc, Ts. E, D. K. Ghosh,
DARK MATTER – HOW CAN WE SEE IT AND UNDERSTAND IT? Gordy Kane Mitchell Symposium College Station May 2007.
Cosmology The Origin and Future of the Universe Part 2 From the Big Bang to Today.
Implication of recent cosmic ray data Qiang Yuan Institute of High Energy Physics Collaborated with Xiaojun Bi, Hong Li, Jie Liu, Bing Zhang & Xinmin Zhang.
Dark Matter Explanation For e^\pm Excesses In Cosmic Ray Xiao-Gang He CHEP, PKU and Physics, NTU.
Significant effects of second KK particles on LKP dark matter physics
Testing astrophysical models for the PAMELA positron excess with cosmic ray nuclei Philipp Mertsch Rudolf Peierls Centre for Theoretical Physics, University.
WIMPs and superWIMPs Jonathan Feng UC Irvine SUGRA20 18 March 2003.
SLAC, June 23 rd Dark Matter in Galactic Gamma Rays Marcus Ziegler Santa Cruz Institute for Particle Physics Gamma-ray Large Area Space Telescope.
Workshop on the interconnection between particle physics and cosmology Gordy Kane Texas A&M May 2007.
The positron excess and supersymmetric dark matter Joakim Edsjö Stockholm University
The LC and the Cosmos: Connections in Supersymmetry Jonathan Feng UC Irvine Arlington LC Workshop January 2003.
The LC and the Cosmos: Connections in Supersymmetry Jonathan Feng UC Irvine American Linear Collider Physics Group Seminar 20 February 2003.
Enhancement of Line Gamma Ray Signature from Bino-like Dark Matter Annihilation due to CP Violation Yoshio Sato (Saitama University/Technical University.
CMB constraints on WIMP annihilation: energy absorption during recombination Tracy Slatyer – Harvard University TeV Particle Astrophysics SLAC, 14 July.
Primordial BHs. 2 Main reviews and articles astro-ph/ Primordial Black Holes - Recent Developments astro-ph/ Gamma Rays from Primordial.
Significant enhancement of Bino-like dark matter annihilation cross section due to CP violation Yoshio Sato (Saitama University) Collaborated with Shigeki.
Antideuteron Searches for Dark Matter LR W/ Yanou Cui John Mason.
Quintessino model and neutralino annihilation to diffuse gamma rays X.J. Bi (IHEP)
Did Dark Matter Annihilations Reionize The Universe? Dan Hooper Fermilab Theoretical Astrophysics Group FNAL Particle Astrophysics Seminar June 1, 2009.
SUSY Dark Matter Collider – direct – indirect search bridge. Sabine Kraml Laboratoire de Physique Subatomique et de Cosmologie Grenoble, France ● 43. Rencontres.
The Dark Side of the Universe What is dark matter? Who cares?
Exploring the Early Universe Chapter Twenty-Nine.
High-energy electrons, pulsars, and dark matter Martin Pohl.
Singlet Dark Matter, Type II Seesaw and Cosmic Ray Signals Nobuchika Okada Miami Fort Fauderdale, Dec , 2009 University of Alabama, Tuscaloosa.
Overview of indirect dark matter detection Jae Ho HEO Theoretical High Energy group Yonsei University 2012 Jindo Workshop, Sep
Dark Matter Particle Physics View Dmitri Kazakov JINR/ITEP Outline DM candidates Direct DM Search Indirect DM Search Possible Manifestations DM Profile.
DARK MATTER CANDIDATES Cody Carr, Minh Nguyen December 9 th, 2014.
Dark matter in split extended supersymmetry in collaboration with M. Quiros (IFAE) and P. Ullio (SISSA/ISAS) Alessio Provenza (SISSA/ISAS) Newport Beach.
Dark Matter, LSP wino dark matter, satellite data, moduli and non- thermal cosmological history, string theory, LHC, and CPV Gordy Kane String Phenomenology.
Dark Matter, LSP wino dark matter, satellite data, moduli and non- thermal cosmological history, and LHC Gordy Kane May 2009 PAMELA Physics Workshop.
Summary of indirect detection of neutralino dark matter Joakim Edsjö Stockholm University
Dark Matter: halo-shape and relic density constraints on dark matter theories with Sommerfeld enhancement Recent observations by PAMELA, etc. have been.
1 Additional observable evidences of possible new physics Lecture from the course “Introduction to Cosmoparticle Physics”
Analysis methods for Milky Way dark matter halo detection Aaron Sander 1, Larry Wai 2, Brian Winer 1, Richard Hughes 1, and Igor Moskalenko 2 1 Department.
The LHC – a “why” machine Gordy Kane Fermilab, January 2008.
SUSY in the sky: supersymmetric dark matter David G. Cerdeño Institute for Particle Physics Phenomenology Based on works with S.Baek, K.Y.Choi, C.Hugonie,
KIAA-WAP, Peking U 2015/9/28 Implications on CRs and DM from the AMS-02 results Xiao-Jun Bi ( 毕效军 ) Center for Particle and Astrophysics IHEP, Beijing.
Neutrino mass and DM direct detection Daijiro Suematsu (Kanazawa Univ.) Erice Sept., 2013 Based on the collaboration with S.Kashiwase PRD86 (2012)
Collider searchIndirect Detection Direct Detection.
MARCH 11YPM 2015  ray from Galactic Center Tanmoy Mondal SRF PRL Dark Matter ?
Indirect Detection Of Dark Matter
Propagation of CR electrons and the interpretation of diffuse  rays Andy Strong MPE, Garching GLAST Workshop, Rome, 17 Sept 2003 with Igor Moskalenko.
Cosmic Ray Excesses From Multi-Component Dark Matter Da Huang Physics Department, Fo Guang Shan Fo Guang Shan PRD89, (2014) [arXiv:
Supersymmetry Basics: Lecture II J. HewettSSI 2012 J. Hewett.
Fermi/LAT observations of Dwarf Galaxies highly constrain a Dark Matter interpretation of Excess Positrons seen in AMS-02, HEAT, and PAMELA DPF 2015 –
Type II Seesaw Portal and PAMELA/Fermi LAT Signals Toshifumi Yamada Sokendai, KEK In collaboration with Ilia Gogoladze, Qaisar Shafi (Univ. of Delaware)
Keegan Stoner Columbia High School. dark matter Obeying Inverse Square Law Outer stars orbit too fast what we should seewhat we actually see.
DARK MATTER Fisica delle Astroparticelle Piergiorgio Picozza a.a
The 2nd workshop of air shower detection at high LHAASO detection of dark matter and astrophysical gamma ray sources Xiao-Jun Bi IHEP, CAS.
Lisa Randall Harvard  It has gravitational interactions—of matter!  Gravitational lensing  Rotation curves in galaxies  Detailed.
Recent developments in Dark Matter Malcolm Fairbairn.
Topics on Dark Matter Annihilation
Indirect dark matter search with the balloon-borne PEBS detector
An interesting candidate?
Dark Matter in Galactic Gamma Rays
Dark Matter Subhalos in the Fermi First Source Catalog
Can dark matter annihilation account for the cosmic e+- excesses?
Implications of new physics from cosmic e+- excesses
MSSM4G: MOTIVATIONS AND ALLOWED REGIONS
Primordial BHs.
DARK MATTER AND INDIRECT DETECTION IN COSMIC RAYS
SUSY Dark Matter in light of CDMS/XENON Results
非最小超对称唯象研究: 工作汇报 杨 金 民 中科院 理论物理所 南开大学.
Leptophilic Dark Matter from ATIC and Pamela
Dark Matter Explanation in Singlet Extension of MSSM
Presentation transcript:

CAN WE UNDERSTAND THE PAMELA POSITRON EXCESS AS WINOS? Gordy Kane January 2009 Ann Arbor arXiv , see also Phill Grajek, Aaron Pierce, Dan Phalen, Scott Watson

LSP, WINO LSP, VERY WELL MOTIVATED FOR DARK MATTER -- over two decades -- anomaly mediated supersymmetry breaking -- “split” supersymmetry -- M theory compactified on G 2 manifold -- MSSM scan – Hewett, Rizzo et al EXCESS GALACTIC POSITRONS LONG AGO PREDICTED AS SIGNAL OF LSP DARK MATTER NAIVELY, CURRENT SIGNAL + CONSTRAINTS DO NOT SEEM TO DESCRIBE DATA WELL BUT SHOULD NOT QUICKLY DISCARD SUCH AN ATTRACTIVE EXPLANATION

CAN A WINO LSP DESCRIBE THE PAMELA DATA? Rate – too small with thermal equilibrium cosmology and standard propagation parameters, even though wino annihilates well into e + – normalize to local relic density – right procedure if most LSPs of non-thermal origin, e.g. moduli decay – we use no “boost factors” – small, energy dependent boost factors may actually be appropriate, and would help noticeably Antiprotons – no apparent signal – with somewhat different propagation parameters, factor 1.5 large -- OK simultaneously with rate? Note positrons and antiprotons have different energy loss mechanisms and come from different parts of the galaxy Gammas? Egret – probably OK? Fermi/GLAST – strong signal expected Synchrotron radiation – OK with somewhat different magnetic field parameters SO, MAYBE

OTHER ISSUES ATIC? – we do not describe this Pulsars – Profumo; Hooper et al Profile of galaxy dark matter – we use NFW in all calculations – results a little better if profile a little softer

NOTE TURNOVER 200 e + /(e -- + e + ) τ eff =5 τ eff =1 Note NYTimes – local density larger  1.5, v larger

Note -- τ eff =5, vary propagation (1) factor  5 degeneracy (2) Wino + background ≈1.5 PAMELA (3) Conventional background Conclude within astrophysical uncertainties antiproton data does not exclude 200 GeV wino 200 GeV wino + background Donato et al,  =0.85,K 0 =0.0016, L=1, V c =13.5, V A =22.4

Variation of antiproton flux with height of diffusion cylinder

Same parameters as best antiproton description

Expect clear excess below  200 GeV

Energy and particle dependent “boost factors” Bergstrom, Edjso et al Lavalle et al Cosmic ray propagation depends on particle, energy Positrons – nearby Antiprotons – distance increases with energy Lavalle et al consider distribution of clumps semi-analytically and with simulations arXiv:

J. Lavalle et al Positron “boost factors” Antiproton “boost factors”

Allowed for masses with wino line below limit, e.g. green line Synchrotron radiation constraint [U B /(U rad + U B )=0.1]

If wino LSP describes data, then probably need wino mass about 200 GeV – constraints worse for lower mass, rate smaller for larger mass Can get satisfactory agreement with all positron, antiproton, gamma data separately Showing can get good simultaneous agreement with all data and constraints is major computing problem – work underway

Dark matter at LHC Is what is seen at LHC same as in indirect data? Can we calculate the relic density?

LHC phenomenology of wino LSP well known Early  1999, 2000 Moroi-Randall Feng Moroi Randall Strassler Ghergetta, Giudice, Wells Recent Yanagida et al ph/ Acharya et al Chargino, LSP nearly degenerate, so hard to see Find via gluino, its decays as trigger – M gluino ranges from about 2 to about 9 M wino in models

CONCLUDE: premature to exclude wino LSP DM – still a promising candidate to describe PAMELA data including constraints IMPROVED EXPERIMENTAL TESTS VERY SOON: PAMELA larger energy positrons GeV – must see “turnover” (or flattening if one bin) PAMELA higher energy electrons Fermi/GLAST Pulsar data SOON LHC AMS-02

THEORY ISSUES: Non-thermal cosmology – any string theory, any supersymmetric theory? – seems to be so for supersymmetric theories that address EWSB, baryogenesis, inflation, etc -- dark matter still annihilates after scalar, moduli decays, to equilbrium, so result characterized by decay temperature rather than freeze-out temperature – relic density still determined by  ann, M pl, T  “wimp miracle” -- existence proof: M-theory compactified on G2 manifold  wino LSP, relic density about right. most LSP’s from moduli decay Energy dependent boost factors – increase for positrons, decrease for antiprotons Galactic propagation for signals, backgrounds – understand degeneracies, produce detailed comprehensive model

If the PAMELA excess is indeed due to a wino LSP the implications are remarkable Would have learned that the dark matter, about a fifth of the universe, is the W superpartner, and it approximate mass Discovery of supersymmetry – guarantees can study superpartners at LHC Would have learned that the universe had a non-thermal cosmological history, one we can probe Conservative interpretation: Keep LSP DM until clearly fails – not there yet – maybe successful Comprehensive underlying theory generically suggests non-thermal origin of DM

Rate “normalized” to local relic density, no “boost factor” Grajek, Kane, Pierce, Phalen, Watson signal Including solar wind effect from Clem et al 1996

Calculate DM thermal relic density, as universe cools and expands Leads to few percent of observed relic density for wino LSP

But moduli also give LSPs [ In G 2 moduli have vacuum value of order 20 in Planck scale units, mass (size of oscillation around minimum of potential) ≈ 50 TeV, decay BR (moduli  superpartners) ≈ 25%

Finally moduli decays give most of relic density