Can dark matter annihilation account for the cosmic e+- excesses?

Slides:



Advertisements
Similar presentations
Combined Energy Spectra of Flux and Anisotropy Identifying Anisotropic Source Populations of Gamma-rays or Neutrinos Sheldon Campbell The Ohio State University.
Advertisements

Dark Matter Annihilation in the Milky Way Halo Shunsaku Horiuchi (Tokyo) Hasan Yuksel (Ohio State) John Beacom (Ohio State) Shin’ichiro Ando (Caltech)
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.
Annihilating Dark Matter Nicole Bell The University of Melbourne with John Beacom (Ohio State) Gianfranco Bertone (Paris, Inst. Astrophys.) and Gregory.
Testing astrophysical models for the PAMELA positron excess with cosmic ray nuclei Philipp Mertsch Rudolf Peierls Centre for Theoretical Physics, University.
CAN WE UNDERSTAND THE PAMELA POSITRON EXCESS AS WINOS? Gordy Kane January 2009 Ann Arbor arXiv , see also Phill Grajek, Aaron Pierce,
Constraints on large DM annihilation cross sections from the early Universe Fabio Iocco Institut de Physique Theorique, CEA/Saclay Institut d’Astrophysique.
The positron excess and supersymmetric dark matter Joakim Edsjö Stockholm University
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.
Constraining DM scenarios with CMB Fabio Iocco Institut d’Astrophysique de Paris Institut de Physique Theorique, CEA/Saclay In collaboration with: G. Bertone,
Significant enhancement of Bino-like dark matter annihilation cross section due to CP violation Yoshio Sato (Saitama University) Collaborated with Shigeki.
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.
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
Gamma rays annihilated from substructures of the Milky Way and Quintessino dark matter Bi Xiao-Jun Institute of High Energy Physics, Chinese Academy of.
Dark Matter: halo-shape and relic density constraints on dark matter theories with Sommerfeld enhancement Recent observations by PAMELA, etc. have been.
Reionizing the Universe with Dark Matter : constraints on self-annihilation cross sections Fabio Iocco Marie Curie fellow at Institut d’Astrophysique de.
1 Additional observable evidences of possible new physics Lecture from the course “Introduction to Cosmoparticle Physics”
中国科学院高能物理研究所 INSTITUTE OF HIGH ENERGY PHYSICS Constraints on the cross-section of dark matter annihilation from Fermi observation of M31 Zhengwei Li Payload.
The science objectives for CALET Kenji Yoshida (Shibaura Institute of Technology) for the CALET Collaboration.
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.
Collider searchIndirect Detection Direct Detection.
MARCH 11YPM 2015  ray from Galactic Center Tanmoy Mondal SRF PRL Dark Matter ?
Antimatter in our Galaxy unveiled by INTEGRAL
Propagation of CR electrons and the interpretation of diffuse  rays Andy Strong MPE, Garching GLAST Workshop, Rome, 17 Sept 2003 with Igor Moskalenko.
Yu-Feng Zhou KITPC/ITP-CAS
Cosmic Ray Excesses From Multi-Component Dark Matter Da Huang Physics Department, Fo Guang Shan Fo Guang Shan PRD89, (2014) [arXiv:
Multi-wavelength signals of dark matter annihilations in the Galactic diffuse emission (based on MR and P. Ullio, arXiv: )‏ Marco Regis University.
Direct measurements of cosmic rays in space ROBERTA SPARVOLI ROME “TOR VERGATA” UNIVERSITY AND INFN, ITALY Vulcano Workshop 2014 Vulcano Island (Italy),
Type II Seesaw Portal and PAMELA/Fermi LAT Signals Toshifumi Yamada Sokendai, KEK In collaboration with Ilia Gogoladze, Qaisar Shafi (Univ. of Delaware)
Dark matter search at HERD X.-J. Bi Institute of High Energy Physics 3 nd Workshop of Herd. Xi’an,
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.
Recent developments in Dark Matter Malcolm Fairbairn.
On the Galactic Center being the main source of Galactic Cosmic Rays as evidenced by recent cosmic ray and gamma ray observations Yiqing Guo, Zhaoyang.
Studies of Systematics for Dark Matter Observations John Carr 1.
Evidence for a dark matter particle Yukio Tomozawa University of Michigan March 2016.
Gamma-ray emission from warm WIMP annihilation Qiang Yuan Institute of High Energy Physics Collaborated with Xiaojun Bi, Yixian Cao, Jie Liu, Liang Gao,
Antiproton and Electron Measurements and Dark Matter Searches
Topics on Dark Matter Annihilation
CR Backgrounds for DM Searches
An interesting candidate?
Dark Matter at a LC Third JCL (Journées Collisionneur Linéaire) 1-3 December 2014 LPSC Grenoble François Richard LAL/Orsay F. Richard December 2014.
Observational Evidence for Extra Dimensions from Dark Matter
Dark Matter in Galactic Gamma Rays
Dark Matter Subhalos in the Fermi First Source Catalog
Implications of new physics from cosmic e+- excesses
Karl Mannheim – ITPA Würzburg
Cooperate with X-L. Chen , Q. Yuan, X-J. Bi, Z-Q. Shen
Primordial BHs.
DARK MATTER AND INDIRECT DETECTION IN COSMIC RAYS
High Energy emission from the Galactic Center
Particle Acceleration in the Universe
Cosmic rays, γ and ν in star-forming galaxies
Progress in the Indirect Detection of Dark Matter
Dark Matter Limits From The Galactic Halo With H.E.S.S.
Eiichiro Komatsu University of Texas at Austin A&M, May 18, 2007
Gamma-ray emission from warm WIMP annihilation
Dark matter annihilation and the Milky Way diffuse gamma
High Energy Astrophysics: problems and expectations
We-Fu Chang, Wei-Ping Pan
Leptophilic Dark Matter from ATIC and Pamela
Gravitons and Dark Matter in Universal Extra Dimensions
Dark Matter Explanation in Singlet Extension of MSSM
Two-zone diffusion of e-/e+ from Geminga explains the e+ anomaly
Kunihito Ioka & Mihoko M. Nojiri (KEK, Japan)
Presentation transcript:

Can dark matter annihilation account for the cosmic e+- excesses? Bi Xiao-Jun IHEP, CAS 2009-11-20 Dark matter, dark energy, matter-antimatter asymmetry, Tsinghua University, Taiwan

PAMELA results of antiparticles in cosmic rays Positron fraction Antiproton fraction PAMELA released data on the positron/electron ratio up to about 100 GeV, which show clear excess above ~10 GeV. The low energy data is affected by the solar environment and we do not need care it too much. Nature 458, 607 (2009) Phys.Rev.Lett.102:051101,2009 390 citations after submitted on 28th Oct. 2008, 1paper per day

The total electron+positron spectrum ATIC bump Fermi excess Chang et al. Nature456, 362 2008 Phys.Rev.Lett.102:181101,2009

Possible explanations Astrophysical sources Exotic sources Nearby SNRs, pulsars Propagation Early SN stage interaction of CRs Dark matter annihilation Dark matter decay

Possible origins of e+e-: pp interaction (Blasi, 0903.2794) Occur at the cosmic ray acceleration source: hard spectrum If we consider some new processes, we may first consider within cosmic rays physics Comment: nature for Fermi spectrum; antiprotons may set constraints on this picture

From CRs interaction There is knee in CR spectrum at ~10^15 eV (Hu, Bi et al., 0901.1520) There is knee in CR spectrum at ~10^15 eV It is proposed the knee is generated by interaction, with Eγ=1eV, the threshold energy is at ~10^15 eV 3% converted can explain the ATIC or Fermi Fermi excess Pamela is related with knee; the knee is at knee; knee is generated by the pair production. It should be noted that for 1ev the threshold energy is just at the knee. By simulation

Nearby pulsars

Astrophysical sources D. Hooper et al. S. Profumo …… Nearby pulsars:

Many possible astrophysical solutions to explain the excesses are proposed. However, these sources are easy to account for the Fermi spectrum, not easy for ATIC.

Possible explanations Astrophysical sources Exotic sources Nearby SNRs, pulsars Propagation Early stage interaction of CRs Dark matter annihilation Dark matter decay ATIC ?? Fermi ATIC OK

Primary positron/electrons from dark matter – implication from new data DM annihilation/decay produce leptons mainly in order not to produce too much antiprotons. Very hard electron spectrum -> dark matter annihilates/decay into leptons. Very large annihilation cross section, much larger (~1000) than the requirement by relic density. 1) nonthermal production, 2) Sommerfeld enhancement 3) Breit-Wigner enhancement 4) dark matter decay.

positron ratio from DM annihilation Yin, et al. arXiv:0811.0176

Global fit to the ATIC or Fermi and PAMELA data Liu, Yuan, Bi, Li, Zhang, Astro-ph/0906.3858

Possible explanations Astrophysical sources Exotic sources Nearby SNRs, pulsars Propagation Early stage interaction of CRs Dark matter annihilation Dark matter decay ATIC ?? Fermi ATIC OK OK OK

How to have so large flux Very large annihilation cross section, much larger (~1000) than the requirement by relic density. 1) nonthermal production, ,suppress gamma 2) Sommerfeld enhancement 3) Breit-Wigner enhancement 4) dark matter decay.

Sommerfeld enhancement Kinematically suppression Mass of φis about 1GeV, is Kinematically suppressed to antiprotons; At the same time attractive interaction can enhance the annihilation rate, Sommerfeld enhancement. (Arkani-Hamed et al. 0810.0713  ) For Coulomb potential we have To enhance the dark matter annihilation we have long range attractive force

Fine tunning of Sommerfeld enhancement Yuan, Bi, Liu, Yin, Zhang and Zhu, Astro-ph/0905.2736

J. Zavala, M. Vogelsberger, and S. White, Astro-ph/0910.5221

Breit-Wigner enhancement and fine tunning Bi, He, Yuan, Astro-ph/0903.0122 We require delta, gamma ~ 10-4 to boost ~1000.

Constraints on the dark matter annihilation scenario Since the DM annihilation rate is very large, they imply the existence of an abundant population of e+- in the galactic halo, dwarf galaxies, galaxy clusters, galactic center, or at the early Universe. The abundance of e+- may induce observables that can be constrained by the present experiments.

Constraints from CMB DM annihilation heats and ionizes the photon-baryon plasma at z~1000, constrained by WMAP and Planck T.R. Slatyer et al., 0906.1197

Constraints on the minimal subhalos by observations of clusters A. Pinzke et al., 0905.1948 Standard CDM predicts the minimal subhalos Observation constrains Fermi limit to DM is warm

Constraints from extragalactic diffuse gamma rays S. Profumo et al., 0906.0001

Constraint by Galactic diffuse gamma rays M. Cirelli et al., 0904.3830

Emission from the GC Constraint on the central density of DM Tension Bi et al., 0905.1253 Constraint on the central density of DM Tension Exist for the annihilating DM scenario, but consistent with decay scenario annihilation decay Liu, Yuan, Bi, Li, Zhang, 0906.3858

Constraints from the diffuse gamma ray emission Zhang, Yuan, Bi, 0908.1236

Possible explanations Astrophysical sources Exotic sources Nearby SNRs, pulsars Propagation Early stage interaction of CRs Dark matter annihilation ? Dark matter decay ATIC ?? Fermi ATIC OK OK OK

Summary ATIC DM Fermi Annihilation: how to boost? Strong constraints! Decay: how to get such long life time, ~1026s Astrophysical sources: difficult to test; (century problems: origin of CRs, knee of CRs