Suzaku search for evidence of sterile neutrinos in the X-ray spectra of dwarf spheroidal galaxies Michael Loewenstein, Alexander Kusenko (UCLA), Peter.

Slides:



Advertisements
Similar presentations
Astronomical Solutions to Galactic Dark Matter Will Sutherland Institute of Astronomy, Cambridge.
Advertisements

The extremely high gas content of galaxy UGC8802 Chang Rui-xiang Hou Jin-liang Shen Shi-yin.
Ultra-faint dwarfs as fossils of the First Galaxies Mia S. Bovill Advisor: Massimo Ricotti University of Maryland Mia S. Bovill Advisor: Massimo Ricotti.
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)
Chapter 16 Dark Matter And The Fate Of The Universe.
L.S.Stark 1, M.Doro 2, H.Bartko 3, A.Biland 1, M.Gaug 2, S.Lombardi 2, M.Mariotti 2, F.Prada 4, M.Sanchez-Conde 4, F.Zandanel 2 (for the MAGIC Collaboration*)
The first stars formation in warm dark matter model Liang Gao National Observatories, China.
Ben Maughan (CfA)Chandra Fellows Symposium 2006 The cluster scaling relations observed by Chandra C. Jones, W. Forman, L. Van Speybroeck.
EGRET unidentified sources and gamma-ray pulsars I. CGRO mission and the instrument EGRET and it’s scientific goals II. Simple introduction of EGRET sources.
Annihilating Dark Matter Nicole Bell The University of Melbourne with John Beacom (Ohio State) Gianfranco Bertone (Paris, Inst. Astrophys.) and Gregory.
Theoretical work on Cosmology and Structure Formation Massimo Ricotti.
Star-Formation in Close Pairs Selected from the Sloan Digital Sky Survey Overview The effect of galaxy interactions on star formation has been investigated.
The Milky Way PHYS390 Astrophysics Professor Lee Carkner Lecture 19.
Andreas Ringwald, DESY 27 th DESY PRC Closed Session, DESY, Hamburg, 26 October 2011 Towards a comprehensive summary Physics Case for WISP Searches.
Growth of Structure Measurement from a Large Cluster Survey using Chandra and XMM-Newton John R. Peterson (Purdue), J. Garrett Jernigan (SSL, Berkeley),
The all-sky distribution of 511 keV electron-positron annihilation emission Kn ö dlseder, J., Jean, P., Lonjou, V., et al. 2005, A&A, 441, 513.
Chapter 23: Our Galaxy Our location in the galaxy Structure of the galaxy Dark matter Spiral arm formation Our own supermassive black hole.
1 Origin of Variability of X-ray and γ-ray Spectra on Daily Scale Radovan Milinčić Astrophysics 711 May 3 rd 2005.
The Milky Way Galaxy 19 April 2005 AST 2010: Chapter 24.
X-ray Polarization as a Probe of Strong Magnetic Fields in X-ray Binaries Shane Davis (IAS) Chandra Fellows Symposium, Oct. 17, 2008.
“ Testing the predictive power of semi-analytic models using the Sloan Digital Sky Survey” Juan Esteban González Birmingham, 24/06/08 Collaborators: Cedric.
MACRO Atmospheric Neutrinos Barry Barish 5 May 00 1.Neutrino oscillations 2.WIMPs 3.Astrophysical point sources.
Constraining Galactic Halos with the SZ-effect
Stellar Kinematics Astronomy 315 Professor Lee Carkner Lecture 18.
MATTEO VIEL THE LYMAN-  FOREST: A UNIQUE TOOL FOR COSMOLOGY Bernard’s cosmic stories – Valencia, 26 June 2006 Trieste Dark matter Gas.
1 TEV PA Meeting July 2009 Preliminary Fermi-LAT Limits on High Energy Gamma Lines from WIMP Annihilation Yvonne Edmonds representing the Fermi-LAT Collaboration.
Evolution of Galaxy groups Michael Balogh Department of Physics University of Waterloo.
In this talk we'll see that : We can only see about 1% of the Universe The dark side And ask: What is the Universe made of?
1 Arecibo Synergy with GLAST (and other gamma-ray telescopes) Frontiers of Astronomy with the World’s Largest Radio Telescope 12 September 2007 Dave Thompson.
The Dual Origin of a Simulated Milky Way Halo Adi Zolotov (N.Y.U.), Beth Willman (Haverford), Fabio Governato, Chris Brook (University of Washington, Seattle),
Potential Neutrino Signals from Galactic  -Ray Sources Alexander Kappes, Christian Stegmann University Erlangen-Nuremberg Felix Aharonian, Jim Hinton.
The Number of Light Neutrino Families ● Physics motivation for measurement ● Direct / indirect searches for ● Analysis methodology for ● Single photon.
Laue lenses for hard X-rays (> 60 keV) F. Frontera and A. Pisa on behalf of a Large Collaboration Rome, 18 March 2005.
Relic Neutrinos, thermal axions and cosmology in early 2014 Elena Giusarma arXiv: Based on work in collaboration with: E. Di Valentino, M. Lattanzi,
The Evolution of Quasars and Massive Black Holes “Quasar Hosts and the Black Hole-Spheroid Connection”: Dunlop 2004 “The Evolution of Quasars”: Osmer 2004.
Complementarity of weak lensing with other probes Lindsay King, Institute of Astronomy, Cambridge University UK.
Scientific objectives for XEUS: Galaxies Groups and Clusters at z~2 Study of the Evolution of clusters in the mass range kT > 2 keV up to z=2. Dynamics,
Suzaku, XMM-Newton and Chandra Observations of the Central Region of M 31 Hiromitsu Takahashi (Hiroshima University, Japan) M. Kokubun, K. Makishima, A.
Lecture Outlines Astronomy Today 8th Edition Chaisson/McMillan © 2014 Pearson Education, Inc. Chapter 25.
Summary(3) -- Dynamics in the universe -- T. Ohashi (Tokyo Metropolitan U) 1.Instrumentation for dynamics 2.Cluster hard X-rays 3.X-ray cavities 4.Dark.
Searching for Brown Dwarf Companions to Nearby Stars Michael W. McElwain, James E. Larkin & Adam J. Burgasser (UC Los Angeles) Background on Brown Dwarfs.
Clustering in the Sloan Digital Sky Survey Bob Nichol (ICG, Portsmouth) Many SDSS Colleagues.
Hot gas in galaxy pairs Olga Melnyk. It is known that the dark matter is concentrated in individual haloes of galaxies and is located in the volume of.
Dark Matter Particle Physics View Dmitri Kazakov JINR/ITEP Outline DM candidates Direct DM Search Indirect DM Search Possible Manifestations DM Profile.
The Detection of an Unexplained Emission Line at 3.56 keV Esra Bulbul Harvard-Smithsonian Center for Astrophysics Maxim Markevitch (NASA/GSFC), Adam Foster.
The X-ray Universe Sarah Bank Presented July 22, 2004.
Gamma-rays from Dark Matter Annihilation in Milky Way Satellites Louie Strigari UC Irvine, Center for Cosmology Getting Prepared for GLAST UCLA,
Lecture Outlines Astronomy Today 7th Edition Chaisson/McMillan © 2011 Pearson Education, Inc. Chapter 23.
Primordial black holes B. Czerny Copernicus Astronomical Center, Warsaw on behalf of collaboration: D. Cline, B. Czerny, A. Dobrzycki, A. Janiuk, C. Matthey,
Neutrino mass and DM direct detection Daijiro Suematsu (Kanazawa Univ.) Erice Sept., 2013 Based on the collaboration with S.Kashiwase PRD86 (2012)
21 Sept The MSM -- Neutrino Masses and Dark matter -- Takehiko Asaka (Tohoku University) TA, S.Blanchet, M.Shaposhnikov [hep-ph/ ] TA, M.Shaposhnikov.
X-ray Astronomy School 2002 Clusters of Galaxies (and some Cosmology) Scientific and Data Analysis Issues Keith Arnaud NASA/GSFC and UMCP.
Galactic structure and star counts Du cuihua BATC meeting, NAOC.
Potential Neutrino Signals from Galactic  -Ray Sources Alexander Kappes, Christian Stegmann University Erlangen-Nuremberg Felix Aharonian, Jim Hinton.
The High Redshift Universe Next Door
The Formation and Evolution of Galaxies Michael Balogh University of Waterloo.
Exploring an evidence of supermassive black hole binaries in AGN with MAXI Naoki Isobe (RIKEN, ) and the MAXI
The XMM Distant Cluster Project: Survey limits and Pilot Survey Georg Lamer A. Schwope, V. Hambaryan, M. Godolt (AIP) H. Böhringer, R. Fassbender, P. Schücker,
Competitive Science with the WHT for Nearby Unresolved Galaxies Reynier Peletier Kapteyn Astronomical Institute Groningen.
Chapter 25 Galaxies and Dark Matter. 25.1Dark Matter in the Universe 25.2Galaxy Collisions 25.3Galaxy Formation and Evolution 25.4Black Holes in Galaxies.
Science Drivers for Small Missions in High Energy Astrophysics Luigi PiroCAS-ESA Workshop – Chengdu Feb. 25, 2014 Science Drivers for Small Missions in.
1 ASTRON is part of the Netherlands Organisation for Scientific Research (NWO) Netherlands Institute for Radio Astronomy Astronomy at ASTRON George Heald.
Scattered Radiation and Unified Model of Active Galactic Nuclei
Studies of Systematics for Dark Matter Observations John Carr 1.
Bayesian analysis of joint strong gravitational lensing and dynamic galactic mass in SLACS: evidence of line-of-sight contamination Antonio C. C. Guimarães.
An interesting candidate?
Sterile Neutrinos and WDM
Dark Matter Subhalos in the Fermi First Source Catalog
Ultra-Faint, Ultra-Dark, and Ultra-Handsome
Presentation transcript:

Suzaku search for evidence of sterile neutrinos in the X-ray spectra of dwarf spheroidal galaxies Michael Loewenstein, Alexander Kusenko (UCLA), Peter Biermann (MPIfr, UAla)

Meet the Sterile Neutrino Right-handed (sterile) neutrinos may be introduced in extensions of the Standard Model that account for neutrino masses.  mix Sterile ’s may be thermally produced via neutrino oscillations in the early universe at a rate that depends on the active-sterile mixing angle,  mix. m ster- Dodelson & Widrow (1994) showed that sterile ’s could be produced in this manner in sufficient numbers to account for dark matter if m ster- ~1 keV.  mix. There are alternative production scenarios that decouple or alter the dependence of the rate on  mix.

Astrophysical Context (Warm) dark matter in the form of the keV sterile neutrino could resolve discrepancies between CDM and small scale structure. Sterile ’s can explain pulsar kicks: magnetic field  polarization- dependent scattering  asymmetric momentum distribution  They may also facilitate primordial star formation. They must not wipe out small scale structure seen in the Ly  forest.

Motivation for this project  Sterile neutrinos decay into an active neutrino and an X-ray photon (e=m/2) -- producing an emission line amenable to X-ray spectroscopic investigation.  Detection and measurement of such a feature would point the way to physics beyond the standard model, and enable one to map out the distribution of dark matter using X-ray spectroscopy.  There’s an interesting regime in which sterile neutrino radiative decay may be detectable by X-ray instruments presently in orbit.

Motivation for this project

Where to look, What to look with Target selection: maximize dark matter surface density and minimize other X-ray emitting components. Local group dwarf spheroidals are ideal: X-ray dark, (no hot gas, AGN, X-ray binaries) nearby concentrations of dark matter with just enough stars to measure their distance and total mass.

Dwarf spheroidals are… old and metal-poor... …and DM-dominated

Where to look, What to look with Need imaging (in case there are other sources in the field) X-ray spectroscopy with the best possible spectral resolution and lowest background to optimize sensitivity to weak emission lines. Because Suzaku XIS has the lowest background (orbit, design), and the sharpest spectral resolution among X-ray CCD detectors (dispersive spectrometers optimized for point sources) currently in orbit, it is the observatory of choice to search for weak lines from extended sources. Suzaku has three operational co-aligned detector/telescope pairs…

Where to look, What to look with Of the LG dSphs, the Ursa Minor and Draco systems are optimal based on their distances and large dark matter densities derived from stellar kinematics. In our pilot Suzaku Cycle 2 program, we observe the Ursa Minor and Draco dwarf spheroidal galaxies for ~ 67 ksec each (200 ksec of data). M/L L  

Ursa Minor (DSS)

How to look -- spectral analysis Extract spectra from cleaned photon event file in source-free region of all three active chips Generate spectral response matrices, efficiency curves

How to look -- spectral analysis Subtract NXB derived from night-earth data

How to look -- spectral analysis Fit to GXB+CXB with constraints from RASS  Derive upper limits to line fluxes when an extra emission line component is added to the spectral model, using Monte Carlo simulations to identify confidence levels

What we’ve found

Limits and what to do with them Using the Ursa Minor mass profile (Strigari et al.), convert flux limit to decay rate limit at each X-ray energy (=m ster- /2)… Using the Ursa Minor mass profile (Strigari et al.), convert flux limit to decay rate limit at each X-ray energy (=m ster- /2)… … which maps onto an excluded region in m ster- -  (mixing angle) plane -- that is more restrictive than previous limits… … which maps onto an excluded region in m ster- -  (mixing angle) plane -- that is more restrictive than previous limits…

Improved constraints The solid excluded region applies even if sterile neutrinos constitute a fraction of dark matter. The preliminary Suzaku Ursa Minor constraints shift this limit to the solid thick red line, thus eliminating a substantial portion of the (hatched) pulsar kick region. The thin dashed line shows the pre-Suzaku X-ray bound assuming that sterile neutrinos make up all the dark matter; this shifts to the broken red line.

What’s New, What’s NeXT Draco: a different approach (using maximum likelihood on the unsubtracted, unbinned data) yields preliminary results comparable to those for Ursa Minor (out to higher energies) … Draco: a different approach (using maximum likelihood on the unsubtracted, unbinned data) yields preliminary results comparable to those for Ursa Minor (out to higher energies) …

What’s New, What’s NeXT The Sloan Digital Sky Survey (SDSS) has doubled the number of know dwarf spheroidal galaxies by discovering ultra faint dwarfs, and implies that there may be ~1000 within the Milky Way halo (Tollerud et al., Bovill and Ricotti). The Sloan Digital Sky Survey (SDSS) has doubled the number of know dwarf spheroidal galaxies by discovering ultra faint dwarfs, and implies that there may be ~1000 within the Milky Way halo (Tollerud et al., Bovill and Ricotti). These are promising future targets. These are promising future targets.

What’s New, What’s NeXT

Summary  Our preliminary results for Ursa Minor (and Draco) demonstrate that, with Suzaku, we can extend the explored region of sterile neutrino parameter space into a new regime that will test some theories for pulsar kicks.  We are in the final analysis stage, and applying new statistical techniques. We expect to rule out some production mechanisms under the assumption that sterile neutrinos are the dominant constituent of dark matter (or discover evidence for their existence!).

Coda   Future observations with X-ray calorimeters (e.g., SXS on NeXT) will either detect emission lines from sterile neutrino radiative decay, or definitively imply a low abundance and/or mixing angle.   Sterile neutrinos are a well-motivated dark matter candidate, but one with mass and relic abundance poorly determined a priori. As long as dark matter remains unidentified, we intend to continue searching the X-ray sky…