Spectra of Cosmic Rays

Similar documents
The positron and antiproton fluxes in Cosmic Rays

PHY326/426 Dark Matter and the Universe. Dr. Vitaly Kudryavtsev F9b, Tel.:

Dark matter in split extended supersymmetry

Propagation in the Galaxy 2: electrons, positrons, antiprotons

DARK MATTER. Martti Raidal NICPB & University of Helsinki Tvärminne summer school 1

M. Lattanzi. 12 th Marcel Grossmann Meeting Paris, 17 July 2009

PERSPECTIVES of HIGH ENERGY NEUTRINO ASTRONOMY. Paolo Lipari Vulcano 27 may 2006

Project Paper May 13, A Selection of Dark Matter Candidates

Lecture 14. Dark Matter. Part IV Indirect Detection Methods

Cosmic Ray Transport (in the Galaxy) Luke Drury. Dublin Institute for Advanced Studies Institiúid Ard-Léinn Bhaile Átha Cliath

Testing a DM explanation of the positron excess with the Inverse Compton scattering

Dennis Silverman UC Irvine Physics and Astronomy Talk to UC Irvine OLLI May 9, 2011

Fermi: Highlights of GeV Gamma-ray Astronomy

Antimatter and DM search in space with AMS Introduction. 2 Cosmology with Cosmic Rays

CMB constraints on dark matter annihilation

Gamma ray and antiparticles (e + and p) as tools to study the propagation of cosmic rays in the Galaxy

A New View of the High-Energy γ-ray Sky with the Fermi Telescope

99 Years from Discovery : What is our current picture on Cosmic Rays? #6 How cosmic rays travel to Earth? Presented by Nahee Park

Astrophysical issues in the cosmic ray e spectra: Have we seen dark matter annihilation?

The High-Energy Interstellar Medium

Neutrinos and DM (Galactic)

Structure of Dark Matter Halos

Indirect dark matter detection and the Galactic Center GeV Excess

The Mystery of Dark Matter

Week 3 - Part 2 Recombination and Dark Matter. Joel Primack

Dark matter annihilations and decays after the AMS-02 positron measurements

DIETRICH MÜLLER University of Chicago SLAC SUMMER INSTITUTE 2011

Cosmic ray electrons from here and there (the Galactic scale)

Dark Matter searches with astrophysics

A-Exam: e + e Cosmic Rays and the Fermi Large Array Telescope

Astro2020 Science White Paper Prospects for the detection of synchrotron halos around middle-age pulsars

Natural explanation for 130 GeV photon line within vector boson dark matter model

Measuring Dark Matter Properties with High-Energy Colliders

Our Galaxy. Milky Way Galaxy = Sun + ~100 billion other stars + gas and dust. Held together by gravity! The Milky Way with the Naked Eye

Whither WIMP Dark Matter Search? Pijushpani Bhattacharjee AstroParticle Physics & Cosmology Division Saha Institute of Nuclear Physics Kolkata

Implication of AMS-02 positron fraction measurement. Qiang Yuan

Interstellar gamma rays. New insights from Fermi. Andy Strong. on behalf of Fermi-LAT collaboration. COSPAR Scientific Assembly, Bremen, July 2010

Signals from Dark Matter Indirect Detection

Understanding High Energy Neutrinos

Astroparticle Anomalies

Dark Matter Decay and Cosmic Rays

Using the Fermi-LAT to Search for Indirect Signals from Dark Matter Annihilation

GALACTIC CENTER GEV GAMMA- RAY EXCESS FROM DARK MATTER WITH GAUGED LEPTON NUMBERS. Jongkuk Kim (SKKU) Based on Physics Letters B.

a cosmic- ray propagation and gamma-ray code

Dark Matter searches with radio observations

EGRET Excess of diffuse Galactic Gamma Rays as a Trace of the Dark Matter Halo

COSMOLOGY and DARK MATTER

New results from the AMS experiment on the International Space Station. Henning Gast RWTH Aachen

DARK MATTER SEARCHES WITH AMS-02 EXPERIMENT

Hunting for Dark Matter in Anisotropies of Gamma-ray Sky: Theory and First Observational Results from Fermi-LAT

Dark Matter in the Universe

Dark Matter. Evidence for Dark Matter Dark Matter Candidates How to search for DM particles? Recent puzzling observations (PAMELA, ATIC, EGRET)

Ingredients to this analysis

Constraining Dark Matter annihilation with the Fermi-LAT isotropic gamma-ray background

Monthly Proton Flux. Solar modulation with AMS. Veronica Bindi, AMS Collaboration

Indirect Dark Matter Detection

Gravitinos, Reheating and the Matter-Antimatter Asymmetry of the Universe

The Large Area Telescope on-board of the Fermi Gamma-Ray Space Telescope Mission

Dark Matter and Dark Energy components chapter 7

Fundamental Physics with GeV Gamma Rays

Searching for Dark Matter Annihilation from Milky Way Dwarf Spheroidal Galaxies. Present status and future prospects

UNVEILING THE ULTIMATE LAWS OF NATURE: DARK MATTER, SUPERSYMMETRY, AND THE LHC. Gordon Kane, Michigan Center for Theoretical Physics Warsaw, June 2009

Astrophysical issues in indirect DM detection

The Search for Dark Matter. Jim Musser

Physics 5I LECTURE 4 October 21, 2011

Searching for spectral features in the g-ray sky. Alejandro Ibarra Technische Universität München

LATE DECAYING TWO-COMPONENT DARK MATTER (LD2DM) CAN EXPLAIN THE AMS-02 POSITRON EXCESS

Introduction to Particle Physics

Signatures of clumpy dark matter in the global 21 cm background signal D.T. Cumberland, M. Lattanzi, and J.Silk arxiv:

THE MAGIC TELESCOPES. Major Atmospheric Gamma Imaging Cherenkov Telescopes

Dark Matter ASTR 2120 Sarazin. Bullet Cluster of Galaxies - Dark Matter Lab

The Egret Excess, an Example of Combining Tools

Cosmic Positron Signature from Dark Matter in the Littlest Higgs Model with T-parity

Dark Matter and Dark Energy components chapter 7

² The universe observed ² Relativistic world models ² Reconstructing the thermal history ² Big bang nucleosynthesis ² Dark matter: astrophysical

Search for exotic process with space experiments

Chapter 22 Back to the Beginning of Time

Dark Matter Models. Stephen West. and. Fellow\Lecturer. RHUL and RAL

PAMELA from Dark Matter Annihilations to Vector Leptons

An Auger Observatory View of Centaurus A

Search for Dark Matter from the Galactic Halo with the IceCube Neutrino Observatory Paper Review

Lecture 14 Cosmic Rays

A100H Exploring the Universe: Quasars, Dark Matter, Dark Energy. Martin D. Weinberg UMass Astronomy

LHC searches for dark matter.! Uli Haisch

Topics. 1. Towards a unified picture of CRs production and propagation: 2. AMS-02 good candidates for Dark Matter space search

Properties of Elementary Particle Fluxes in Cosmic Rays. TeVPA Aug. 7, Yuan-Hann Chang National Central University, Taiwan

Indirect Dark Matter constraints with radio observations

The Galactic diffuse gamma ray emission in the energy range 30 TeV 3 PeV

COSMIC RAYS DAY INTRODUCTION TO COSMIC RAYS WINDWARD COMMUNITY COLLEGE - SEPTEMBER 26, 2015 VERONICA BINDI - UNIVERSITY OH HAWAII

Astroparticle Physics with IceCube

Indirect detection of decaying dark matter

Dynamical Dark Matter and the Positron Excess in Light of AMS

The Inner Region of the Milky Way Galaxy in High Energy Gamma Rays

Searching for dark photon. Haipeng An Caltech Seminar at USTC

Neutrino Signals from Dark Matter Decay

Cosmic Rays - R. A. Mewaldt - California Institute of Technology

On the scientific motivation for a wide field-of-view TeV gamma-ray observatory in the Southern Hemisphere

The Inner Region of the Milky Way Galaxy in High Energy Gamma Rays

Sep. 13, JPS meeting

Elementary Particle Physics Glossary. Course organiser: Dr Marcella Bona February 9, 2016

Transcription:

Spectra of Cosmic Rays Flux of relativistic charged particles [nearly exactly isotropic] Particle density

Power-Law Energy spectra Exponent (p, Nuclei) : Why power laws? (constraint on the dynamics of the accelerators and propagation)

Electron flux is smaller and softer than the proton flux. Smaller contributions of positrons and antiprotons

Study of cosmic rays inside the Galaxy (at different positions) via Gamma Astronomy Main source of gamma rays Emission from point

Map of Fermi-LAT counts (200 MeV 100 GeV) Examples of angular distribution Cosmic rays near the disk of the Galaxy have a spectrum with a position independent shape (and only a small spatial gradient)

Cosmic Ray in the Milky Way: Injection : Sources release relativistic charged particles in interstellar space. Propagation : The charged particles are (temporarily) trapped by magnetic fields and can travel from the injection point to the Earth.

Flux observed here (near the Sun) and now Injection of Cosmic Rays (of type a) Density of cosmic rays (of type a)

Injection of Cosmic Rays (of type a) Propagation Density of cosmic rays (of type a) [density and injection (after averaging over an appropriate time) are very likely stationary]

Galactic Cosmic Rays Different particles Dimensional analysis Injection of cosmic rays Containment time

Source of relativistic positrons p

Possible additional sources of relativistic positrons in the Milky Way 1. Dark Matter annihilation (or decay) 2. Astrophysical sources that accelerate positrons.

Possible additional sources of relativistic positrons in the Milky Way 1. Dark Matter annihilation (or decay) 2. Astrophysical sources that accelerate positrons. Observations:

Dynamical evidence for Dark Matter at different length-scales [Galaxies, Clusters of Galaxies, the entire universe] Cold Dark Matter Cornelia Parker. (Tate Gallery, London) What is the nature of the Dark Matter?

Dark Matter Halo in spiral Galaxies Spiral galaxy NGC 3198 overlaid with hydrogen column density [21 cm] [ApJ 295 (1995) 305 Extra invisible component Expected from luminous Matter in the disk (Keplerian 1/Sqrt[r] )

The thermal relic or WIMP paradigm for Dark Matter Hypothesis that the Dark Matter is formed by a (yet undiscovered) elementary particle This particle was in thermal equilibrium in the early universe when the temperature was The relic abundance of this particle is determined by (and is inversely proportional to) its (velocity averaged) annihilation cross section.

Concept of thermal relic [WIMP] : Annihilation cross section Determines the relic abundance

Relic abundance estimate in standard Cosmology (simplest treatment) Connection with Weak (Fermi) scale?! [and perhaps supersymmetry] The WIMP's Miracle?

the WIMP's miracle Killing two birds with a single stone Dark Matter Particle Direct observational puzzle New particles are predicted in beyond the Standard Model theories, (in particular Supersymmetry) that have the DM particle properties. Theoretical motivations (hierarchy problem)

Supersymmetry Fermionic degrees of freedom Bosonic degrees Of freedom All internal quantum numbers (charge, color,...) must be identical squark selectron gluino...

Standard Model fields New bosons (scalar) spin 0 S- fermions bosons New fermions spin 1/2 -ino 2 Higgs Weak (~100 GeV) Mass scale? Super-symmetric extension 1 stable New Particle (R-parity conserved)

Three roads to the discovery of DM in the form of thermal relics (WIMP's) Annihilation Creation Time reversal Elastic Crossing symmetry

Three roads to the discovery of DM in the form of thermal relics (WIMP's)

3 Roads to test the WIMP hypothesis Direct searches (elastic scattering) Accelerator Searches Indirect searches

Indirect searches for DARK MATTER Dark Matter Halo in our Galaxy.

In the WIMP paradigm Dark Matter is NOT really dark Self-annihilation of the DM particles that form the halo Number density of Dark Matter particles Number of annihilations per unit time and unit volume Luminosity per unit volume

What is the energy output of the Milky Way in DM annihilations? We know (at least approximately) from cosmology Astrophysical observations (rotation velocity) + Modeling of galaxy formation for the central part of the Galaxy

DM in the Milky Way sun Density distribution determined by Rotation velocity measurements Cusp at GC derived by N-body simulations

DM in the Milky Way sun Navarro,Frenk,White Density distribution determined by Rotation velocity measurements Cusp at GC derived by N-body simulations

Power generated by DM annihilations in the Milky Way halo [Majorana particle] For comparison: Power of the Cosmic Ray Accelerators in the Milky Way: small effect of Cusp on total luminosity

What is the final state of DM annihilations? well we do not know, we have to build a model (for example supersymmetry). But it is plausible that the Dark Matter particle will (or could) produce all particles (and anti-particles) that we know. Most promising for detection: photons Charged (anti)particles Neutrinos

Charged particles: positrons and anti-protons Trapped by the Galactic magnetic field Extra contribution to the cosmic ray fluxes

Standard source of Positrons : Main expected contribution: Interaction of cosmic rays propagating in the interstellar medium:

Standard source of Positrons : Main expected contribution: Interaction of cosmic rays propagating in the interstellar medium:

Injection of positrons by the standard mechanism 2.9, 5.5, 8.9

Positron energy spectra are approximately scaling in the projectile fragmentation region (reflection of approximate validity of Feynman scaling) positron spectra as function of

(of same exponent) Positron injection (in the standard mechanism) is in good approximation a power law with the same exponent as the proton flux

Relation between: Injection spectrum Observed spectrum Study of Secondary Nuclei (Li, Be, B), (sub-iron group)

Nuclear Fragmentation (collisions with the Inter Stellar Medium) v proton at rest v v Solar system

Layer of material column density X The Boron/Carbon ratio allows to estimate the average column density crossed by cosmic rays.

From CREAM Lines of form: =rigidity

Interpretation of the result: Column density corresponds to the confinement time of cosmic rays in the Galaxy Observed Spectrum of cosmic rays is softer than the injection spectrum

Propagation of electrons (+positrons): Energy Losses [Synchrotron + Compton scattering (on the radiation fields present in Galaxy)] CMBR + stellar light

Combine the effects of Escape and Energy loss. Propagation effects softens the e+spectrum more than for protons and nuclei

Electron flux [same shape of injection as protons and nuclei] Positron flux Prediction : softer

Positron Fraction

Positron Fraction Flattening of the ratio

Has the existence of an extra-component In the positron flux established beyond doubt? (or it is somewhat model dependent?)

Has the existence of an extra-component In the positron flux established beyond doubt? (or it is somewhat model dependent?) The result of the existence of an extra-component (a new source of relativistic positrons has follows from some simple and robust ideas about the propagation of cosmic rays in our Galaxy, and can be considered as quite robust. Models that give good descriptions of all CR data (protons, nuclei, electrons, fail completely with positrons).

Has the existence of an extra-component In the positron flux established beyond doubt? (or it is somewhat model dependent?) The result of the existence of an extra-component (a new source of relativistic positrons has follows from some simple and robust ideas about the propagation of cosmic rays in our Galaxy, and can be considered as quite robust. Models that give good descriptions of all CR data (protons, nuclei, electrons, fail completely with positrons).. but there is no universal agreement on the need of an extra positron component

First (clear) indication of the positron excess by PAMELA (september 2009) > 1300 references First paper of AMS on the positron fraction (march 2013)

Some authors (3 groups) claim that the positron data are compatible with the standard mechanism of positrons production in cosmic ray collisions. [At the price of an important modification of the properties of Cosmic Ray propagation in the Galaxy.]

Dark Matter interpretation Marco Cirelli (Ricap-2014).

Dark Matter interpretation Marco Cirelli (Ricap-2014).

A Dark Matter interpretation of the positron excess can be tested with gamma-ray astronomy. [and is is possible tension with existing data From FERMI (and Cherenkov telescopes)]

Alternative Astrophysical explanation: Existence of a new class of astrophysical sources that accelerate positrons Injecting a very hard spectrum in interstellar space: and sufficient power -

FERMI satellite measurement of pulsars.

2nd FERMI pulsar catalog If pulsars are the sources of the positrons, then possible signal of directionality (anisotropy)

Conclusions : 1. The AMS detector has obtained new measurements of the electron and positron fluxes of unprecedented quality and precision. 2. There are strong indications for the existence of an extra-source of positrons. (confirming the indications of Pamela, Fermi,.) 3. A Dark Matter interpretation is consistent with the Observations, but requires: [a] A strong suppression of annihilation into p-pbar [or a revision of the present production estimates]. [b] A large enhancement of the expected annihilation rate 4. Astrophysical solutions (such as emission from young pulsars) are a possibility. 5. New data soon [anti-protons], Protons, nuclei (for more stringent constraints on propagation).