Dark Matter in the X-Ray Sky

Total Page:16

File Type:pdf, Size:1020Kb

Dark Matter in the X-Ray Sky Opening New Windows on Dark Matter in the X-ray Sky Kerstin Perez A Rainbow of Dark Sectors ACP Winter Workshop March 22, 2021 * Photo from 33 km up in the air! Prototype GAPS balloon flight, June 2012 See poster: Field Rogers “Low-energy Cosmic Antinuclei for Dark Matter” The sky from low to high-energy Optical, IR, UV: X-rays: Gamma-rays: FERMI HUBBLE NuSTAR + CHANDRA HESS CHANDRA HUBBLE + SPITZER Accreting black holes, Stars and gas white dwarfs, neutron stars; Pulsars, supernovae, supernovae, very hot gas, active galactic nuclei scattering by cosmic rays K. Perez - MIT 2 NuSTAR: first focusing high-energy X-ray telescope Launched June 2012 1. Two co-aligned, multilayer coated, grazing incidence focusing optics 3. CdZnTe pixel detector spectrometers 2. Deployable 10 m mast Harrison+ (2013) arxiv:1301.7307 3 NuSTAR: first focusing high-energy X-ray telescope • Energy Band: 3-79 keV • Angular Resolution: 58” (HPD), 18” (PSF) • Field-of-view: 12’ x 12’ • Energy resolution (FWHM): 0.4 keV at 6 keV, 0.9 keV at 60 keV • Temporal resolution: 0.1 ms • Maximum Flux Rate: 10k ct/s • ToO response: <24 hours Harrison+ (2013) arxiv:1301.7307 4 Focus on the Galactic Center • High density of both astrophysical X- rays and dark matter 2° INTEGRAL E = 20-40 keV E = 10-40 keV >2 Ms exposure 1.5° G. Belanger, et al. (2006) K. Mori+ (2015) arxiv:1510.04631 5 K. Mori+ (2015) arxiv:1510.04631 Massive, magnetically accreting population in the central ~10 pc 10-20 keV Perez+ Nature (2015) XMM Fe-Ka contours Echoes of X-ray, cosmic-ray Field Rogers injection in molecular clouds? (NSF grad fellow) F. Rogers et al. (in prep.) Constraining stellar remnant populations in galactic nuclei Hong+ (2016) arXiv:1605.03882 K. Perez - MIT 6 Adapting NuSTAR as a large-aperture DM telescope • “0-bounce” photons that bypass the optics are typically a major background 3.5 deg • Novel analysis exploits >10x increase in efficiency for slowly-varying, diffuse signal • Expands energy range up to 160 keV 0.2 0.4 0.6 0.8 • High-resolution, small field-of-view (0.05deg2), snapshots of the sky 7 X-rays from sterile neutrino dark matter Neutrino Minimal Standard Model 3 light SM neutrinos 3 sterile neutrinos: • only interact via neutrino oscillations • two heavy (>100 GeV) explain oscillations • one lighter (~keV) can account for DM Sterile neutrino decay can provide a clear X-ray line signature 8 The sterile neutrino landscape Only a narrow window remains in which sterile neutrinos (in the simplest models) can constitute all of dark matter Require *model- More mixing momentum independent with standard distribution not Abazajian, Fuller neutrinos & Patel 2001; underproduce KA 2005 small-scale structure Require correct dark matter Less mixing with abundance standard produced in the neutrinos early universe 9 …the “3.5 keV line”? 1. A faint line detected in XMM-Newton 2. Line consistent with observations using spectra of stacked galaxy clusters many instruments and astrophysical regions Bulbul+ (2014) 10 …the “3.5 keV line”? 1. A faint line detected in XMM-Newton 2. Line consistent with observations using spectra of stacked galaxy clusters many instruments and astrophysical regions Bulbul+ (2014) 3. Ruled out using full ~550Ms XMM-Newton data catalog? Foster+ (2021) Dessert+ Science (2020) 11 Perez, Ng, Beacom+ (2017) The Galactic Center/Bulge (+) Large dark matter density (+) Large sensitivity from unfocused FOV (–) Galactic ridge emission incl. bright Fe lines Perez, Ng, Beacom+ (2017) K. Ng, Roach, Perez+ (2019) M31 (Andromeda Galaxy) 105 FPMA FPMB 105 FPMA FPMB )] 1 − )] 1 − 104 M31 (Andromeda Galaxy) 104 (cts keV ⇥ Inst. + solar (cts keV Inst. + solar 103 ⇥ Inst. + solar 0-b CXB Inst. + solar 0-b CXB 3 [keV 10 0-b CXB 0-b CXB [keV dE dN 2-b M31 2-b M31 E 2-b CXB 2-b CXB dE dN 2-b M31 2-b M31 2 E 2-b CXB 2-b CXB 10 1 2 102 10 10 1.2 101 102 1.0 1.2 0.8 1.0 0.8 Data / Model 0.6 1 2 1 2 10 Data / Model 0.6 10 10 10 1 2 1 2 10 E[keV] 10 10 10 E[keV] (+) No Fe emission lines (+) surveys dark matter from both core and halo (-) emission from M31 disk Perez, Ng, Beacom+ (2017) Ng, Roach, Perez+ (2019) M31 (Andromeda Galaxy) (+) minimal Galactic contamination (+) near center of the dark matter halo (-) seeing deviations from instrument background model B. Roach, Ng, Perez+ (2020) Off-plane Galactic Center Leading sensitivity across broad mass range • Combination of Galactic center, Andromeda (M31), and Galactic bulge give leading constraints for masses 10-50 keV • Improve on previous constraints by over an order of magnitude in some mass ranges Kenny Ng Brandon Roach (GRAPPA) (graduate student) Cora Hersh (Haverford undergrad à MIT EAPS Ph.D.) See also: Foster et al. A deep search for decaying dark matter with XMM-Newton arXiv:2102.02207 (2021) 15 Stars as factories for axion-like particles (ALPs) • Axions introduced to explain why the strong interactions preserve the CP symmetry (Peccei-Quinn mechanism) • Axion-like particles generic feature of many BSM models (e.g. string theory) Couples to fermions Couples to photons Compton Bremsstrahlung Primakoff Most relevant process for stars! photon axion photon* Image: Hubble Telescope 17 Galactic magnetic fields photon photon axion NuSTAR photon* photon* Image: Hubble Telescope Jaffe (2019) 18 Betelgeuse 1. Hot core à predicted signal in the hard X-ray range 2. No stable corona à essentially zero standard astrophysical X-ray background 3. Relatively nearby, well- studied region Dr. Mengjiao Xiao (postdoc researcher) M. Xiao, Perez, See also: Dessert, Foster, Safdi Gianotti+ X-ray searches for Axions from Super Star Clusters, PRL (2021) PRL (2021) Image credit: Sky & Telescope Magazine 19 Astro observations constrain light axion-like particles predicted axion spectra data (background subtracted) Astro observations constrain light axion-like particles predicted axion spectra data (background subtracted) Xiao, Perez, Gianotti+ PRL (2021) • No excess of events over the expected background • Limits at least ~3x deeper than CAST • Comparable to next- generation axion experiments ALPS-II and Baby-IAXO Astro observations constrain light axion-like particles • overlapping astrophysical constraints, with separate modeling assumptions and uncertainties • builds confidence in the exclusion of this corner of parameter space Xiao, Perez, Gianotti+ PRL (2021) See also: Dessert, Foster, Safdi X-ray searches for Axions from Super Star Clusters, PRL (2021) Novel X-ray Optics for the International Axion Observatory • The International Axion Observatory (IAXO) is the successor to the current leading axion solar telescope, CAST • Axions from Sun re-converted to photons in large laboratory magnetic field • The X-ray optics assembly expands the technology developed for NuSTAR, XRISM, XMM-Newton, etc. 8 X-ray optics focus signal onto low- background detectors JCAP 1906 (2019) 047 arXiv:1904.09155 23 • NuSTAR has delivered leading sensitivity to light dark matter and stellar backgrounds to new physics • Much of this sensitivity not foreseen before launch! • Looking forward to other new windows opening on our sky Backup 25 …Elephants in the Galactic center? Measured MWD ~ 0.9MO is much heavier than implied by low-energy X-ray surveys Higher temperature, All looking at the same elephant…that weighs ~0.9M proportional to MWD O Measured by hard X-rays ...and different animals altogether in the Galactic bulge: cooling material, Perez, Krivonos, Wik ApJ (2020) peak emissivity <10 keV Measured by soft X-rays Hailey, Mori, Perez+ ApJ (2016) Hong+ ApJ (2016) – Point sources in central 100 pc 26 Population changes in the Galactic bulge NuSTAR field-of-view (Module A) NuSTAR field-of-view (Module B) ~6° INTEGRAL image in 17-60 keV overlaid with stellar mass density distribution Perez, Krivonos, Wik. ApJ (2020) • First broad-band X-ray Galactic observations of the Galactic bulge bulge confirm spectrum dominated by non-magnetic white Cosmic X-ray Background dwarf binaries • No hard X-ray emission >20 keV • Supports conclusions from Fe emission line measurements Xu et al. 2016; Yamauchi et al. 2016; Koyama 2018; Nobukawa et al. 2016 27 Origins of Central Hard X-ray Emission? • Massive Intermediate Polars (IPs) …but <MWD> ≈ 0.9MO? • Quiescent black hole low-mass X-ray binaries …but previously undiscovered large population (~600-1200)? must have very faint or long-recurrence outburst? • Millisecond pulsars with non-thermal high-energy spectrum …but previously undiscovered large population (~3000) ? • Bremsstrahlung and inverse Compton from Sgr A* particle outflows interacting with dense molecular material (Dogiel et al. 2015) … but no correlation with radio or radiation density models? K. Perez - MIT 28 Point Sources in the inner 100 pc • 70 hard (3-79 keV) X-ray point sources in a 0.6 deg2 region around Sgr A* with a total exposure of 1.7 Ms • 7 sources in the Sgr B2 field with 300 ks • Sensitive to ~4x1032 erg s-1 in 3-10 keV and ~8x1032 erg s-1 in 10-40 keV NuSTAR 10-40 keV Trial Map J. Hong+ (2016) arxiv:1605.03882 NuSTAR point sources indicate heavy mCVs • The NuSTAR (10-40 keV) J. Hong+ (2016) arxiv:1605.03882 and Chandra (0.5-8 keV) distributions match if the average spectra are Γ~1.5- 2 or kT ~ 20-50 keV • High percentage with Fe lines (60%) and hard spectra support dominant mCV population • High plasma temperature translates to MWD > 0.8MO • Consistent with average white dwarf mass measured by SDSS K. Perez - MIT 30 Adapting NuSTAR as a large-aperture DM telescope • “0-bounce” photons that bypass the optics are typically a major background 3.5 deg • Novel analysis exploits >10x increase in efficiency for slowly-varying, diffuse signal 0.2 0.4 0.6 0.8 31 Population changes in the Galactic bulge? Xu (2016); Yamauchi+ (2016); Yuasa et al.
Recommended publications
  • X-Ray and Near-Infrared Spectroscopy of Dim X-Ray Point Sources Constituting the Galactic Ridge X-Ray Emission
    Acta Polytechnica CTU Proceedings 1(1): 222{226, 2014 doi: 10.14311/APP.2014.01.0222 222 222 X-Ray and Near-Infrared Spectroscopy of Dim X-Ray Point Sources Constituting the Galactic Ridge X-Ray Emission Kumiko Morihana1, Masahiro Tsujimoto2, Ken Ebisawa2 1Nishiharima Astronomical Observatory, Center for Astronomy, University of Hyogo, 407-2 Nishigaichi, Sayo-cho, Sayo- gun, Hyogo, 679-5313, Japan 2Japan Astrospace Exporation Agency, Institute of Space and Astronautical Science, 3-1-1 Yoshino-dai, Chuo-ku, Sagami- hara, Kanagawa 252-5210, Japan Corresponding author: [email protected] Abstract We present the results of X-ray and Near-Infrared observations of the Galactic Ridge X-ray Emission (GRXE). We extracted 2,002 X-ray point sources in the Chandra Bulge Field (l =0◦.113, b = 1◦.424) down to ∼10−14:8 ergs cm−2 s−1 in 2{8 keV band with the longest observation (∼900 ks) of the GRXE. Based on X-ray brightness and hardness, we classified the X-ray point sources into three groups: A (hard), B (soft and broad spectrum), and C (soft and peaked spectrum). In order to know populations of the X-ray point sources, we carried out NIR imaging and spectroscopy observation. We identified ∼11% of X-ray point sources with NIR and extracted NIR spectra for some of them. Based on X-ray and NIR properties, we concluded that non-thermal sources in the group A are mostly active galactic nuclei and the thermal sources are mostly white dwarf binaries such as cataclysmic variables (CVs) and Pre-CVs.
    [Show full text]
  • Non-Thermal Galactic Background Radiation
    NON-THERMAL GALACTIC BACKGROUND RADIATION by H.V. Cane, B.Sc. (Hons.) submitted in fulfilment of the requirements for the degree of Doctor of Philosophy UNIVERSITY OF TASMANIA HOBART OCTOBER 1977 —I- 4e..) ;.j. This thesis contains no material which has been submitted or accepted for the award of any other degree or diploma in any university. To the best of my knowledge and belief, the thesis contains no copy or paraphrase of material previously published or written by another person, except where due acknowledgement is made in the text. ,(7/3 „. Kc . ABSTRACT This thesis presents the results and analysis of data obtained using the Llanherne low-frequency array. Surveys of the Galaxy at five frequencies in the range 2 to 20 MHz have been made and the data have been assembled into maps covering the area 320 0 < k < 30 ° and -25° < b < 22 ° . The data from these maps are combined with data from seven earlier continuum surveys to produce galactic radio spectra in various directions. A summary is made of most of the measurements, at frequencies less than approximately 400 MHz, 'of the galactic background radiation and their interpretation. Two new composite maps, at 10 and 30 MHz, are presented. These, combined with the 85 MHz all-sky map, are used to illustrate the variation of the galactic non-thermal radiation across the sky, and with frequency. The galactic spectra are interpreted in terms of a model of the Galaxy in which synchrotron emission, and absorption in HII regions predominate in spiral arms. However, it is proposed that the synchrotron emission arms and the arms defined by HII regions are not coincident.
    [Show full text]
  • The Nanograv 11 Yr Data Set: Limits on Supermassive Black Hole Binaries in Galaxies Within 500 Mpc
    The Astrophysical Journal, 914:121 (15pp), 2021 June 20 https://doi.org/10.3847/1538-4357/abfcd3 © 2021. The American Astronomical Society. All rights reserved. The NANOGrav 11 yr Data Set: Limits on Supermassive Black Hole Binaries in Galaxies within 500 Mpc Zaven Arzoumanian1, Paul T. Baker2 , Adam Brazier3, Paul R. Brook4,5 , Sarah Burke-Spolaor4,5 , Bence Becsy6 , Maria Charisi7,8,38 , Shami Chatterjee3 , James M. Cordes3 , Neil J. Cornish6 , Fronefield Crawford9 , H. Thankful Cromartie10 , Megan E. DeCesar11 , Paul B. Demorest12 , Timothy Dolch13,14 , Rodney D. Elliott15 , Justin A. Ellis16, Elizabeth C. Ferrara17 , Emmanuel Fonseca18 , Nathan Garver-Daniels4,5 , Peter A. Gentile4,5 , Deborah C. Good19 , Jeffrey S. Hazboun20 , Kristina Islo21, Ross J. Jennings3 , Megan L. Jones21 , Andrew R. Kaiser4,5 , David L. Kaplan21 , Luke Zoltan Kelley22 , Joey Shapiro Key20 , Michael T. Lam23,24 , T. Joseph W. Lazio7,25, Jing Luo26 , Ryan S. Lynch27 , Chung-Pei Ma28 , Dustin R. Madison4,5,39 , Maura A. McLaughlin4,5 , Chiara M. F. Mingarelli29,30 , Cherry Ng31 , David J. Nice11 , Timothy T. Pennucci32,33,40 , Nihan S. Pol4,5,8 , Scott M. Ransom32 , Paul S. Ray34 , Brent J. Shapiro-Albert4,5 , Xavier Siemens21,35 , Joseph Simon7,25 , Renée Spiewak36 , Ingrid H. Stairs19 , Daniel R. Stinebring37 , Kevin Stovall12 , Joseph K. Swiggum11,41 , Stephen R. Taylor8 , Michele Vallisneri7,25 , Sarah J. Vigeland21 , and Caitlin A. Witt4,5 The NANOGrav Collaboration 1 X-Ray Astrophysics Laboratory, NASA Goddard Space Flight Center, Code 662, Greenbelt, MD 20771, USA 2 Department of Physics and Astronomy, Widener University, One University Place, Chester, PA 19013, USA 3 Cornell Center for Astrophysics and Planetary Science and Department of Astronomy, Cornell University, Ithaca, NY 14853, USA 4 Department of Physics and Astronomy, West Virginia University, P.O.
    [Show full text]
  • Annual Report ESO Staff Papers 2018
    ESO Staff Publications (2018) Peer-reviewed publications by ESO scientists The ESO Library maintains the ESO Telescope Bibliography (telbib) and is responsible for providing paper-based statistics. Publications in refereed journals based on ESO data (2018) can be retrieved through telbib: ESO data papers 2018. Access to the database for the years 1996 to present as well as an overview of publication statistics are available via http://telbib.eso.org and from the "Basic ESO Publication Statistics" document. Papers that use data from non-ESO telescopes or observations obtained with hosted telescopes are not included. The list below includes papers that are (co-)authored by ESO authors, with or without use of ESO data. It is ordered alphabetically by first ESO-affiliated author. Gravity Collaboration, Abuter, R., Amorim, A., Bauböck, M., Shajib, A.J., Treu, T. & Agnello, A., 2018, Improving time- Berger, J.P., Bonnet, H., Brandner, W., Clénet, Y., delay cosmography with spatially resolved kinematics, Coudé Du Foresto, V., de Zeeuw, P.T., et al. , 2018, MNRAS, 473, 210 [ADS] Detection of orbital motions near the last stable circular Treu, T., Agnello, A., Baumer, M.A., Birrer, S., Buckley-Geer, orbit of the massive black hole SgrA*, A&A, 618, L10 E.J., Courbin, F., Kim, Y.J., Lin, H., Marshall, P.J., Nord, [ADS] B., et al. , 2018, The STRong lensing Insights into the Gravity Collaboration, Abuter, R., Amorim, A., Anugu, N., Dark Energy Survey (STRIDES) 2016 follow-up Bauböck, M., Benisty, M., Berger, J.P., Blind, N., campaign - I. Overview and classification of candidates Bonnet, H., Brandner, W., et al.
    [Show full text]
  • Origin of the Galactic Ridge X-Ray Emission
    A&A 452, 169–178 (2006) Astronomy DOI: 10.1051/0004-6361:20054268 & c ESO 2006 Astrophysics Origin of the Galactic ridge X-ray emission M. Revnivtsev1,2, S. Sazonov1,2, M. Gilfanov1,2,E.Churazov1,2,andR.Sunyaev1,2 1 Max-Planck-Institute für Astrophysik, Karl-Schwarzschild-Str. 1, 85740 Garching bei München, Germany e-mail: [email protected] 2 Space Research Institute, Russian Academy of Sciences, Profsoyuznaya 84/32, 117997 Moscow, Russia Received 28 September 2005 / Accepted 31 January 2006 ABSTRACT We analyze a map of the Galactic ridge X-ray emission (GRXE) constructed in the 3–20 keV energy band from RXTE/PCA scan and slew observations. We show that the GRXE intensity follows the Galactic near-infrared surface brightness closely and thus traces the Galactic stellar mass distribution. The GRXE consists of two spatial components that can be identified with the bulge/bar and the disk of the Galaxy. The parameters of these components determined from X-ray data are compatible with those derived from near-infrared −11 −1 −2 −2 data. The inferred ratio of X-ray to near-infrared surface brightness I3−20 keV(10 erg s cm deg )/I3.5 µm(MJy/sr) = 0.26 ± 0.05, −5 and the ratio of X-ray to near-infrared luminosity L3−20 keV/L3−4 µm = (4.1 ± 0.3) × 10 . The corresponding ratio of the 3–20 keV 27 −1 −1 luminosity to the stellar mass is Lx/M = (3.5 ± 0.5) × 10 erg s M , which agrees within the uncertainties with the cumulative emissivity per unit stellar mass of point X-ray sources in the Solar neighborhood, determined in an accompanying paper (Sazonov et al.).
    [Show full text]
  • Hard X-Ray Emission from the Galactic Ridge
    HARD X-RAY EMISSION FROM THE GALACTIC RIDGE R. Krivonos1;2, M. Revnivtsev1;2, E. Churazov1;2, S. Sazonov1;2, S. Grebenev1, and R. Sunyaev1;2 1Space Research Institute, Russian Academy of Sciences, Profsoyuznaya 84/32, 117997 Moscow, Russia 2Max-Planck-Institute fur¨ Astrophysik, Karl-Schwarzschild-Str. 1, D-85740 Garching bei Munc¨ hen,Germany ABSTRACT emission is likely a result of interactions of cosmic rays with interstellar matter [e.g. 21, 35, 36, 18, 16]. We present results1 of a study of the Galactic ridge X- From the first all sky surveys in X-rays (∼ 2-10 keV) it ray emission (GRXE) in hard X-rays performed with the became clear that in this energy band the emission of the IBIS telescope aboard INTEGRAL. The imaging capa- Galaxy as a whole is dominated by the contribution from bilities of this coding aperture telescope make it possi- bright point sources, mainly accreting black holes and ble to account for the flux from bright Galactic point neutron star binaries. However, there was also discov- sources whereas the wide field of view permits to collect ered emission that was not resolved into separate point large flux from the underlying GRXE. Extensive study of sources – the Galactic ridge X-ray emission (GRXE, e.g. the IBIS/ISGRI detector background allowed us to con- Worrall et al. 44). Even the significant increase of the struct a model that predicts the detector count rate with sensitivity of X-ray instruments over the last decades has ∼ 1 − 2% accuracy in the energy band 17-60 keV.
    [Show full text]
  • Dark Matter Annihilation at the Galactic Center
    Electronic Theses and Dissertations UC Santa Cruz Peer Reviewed Title: Dark Matter Annihilation at the Galactic Center Author: Linden, Timothy Ryan Acceptance Date: 2013 Series: UC Santa Cruz Electronic Theses and Dissertations Degree: Ph.D., PhysicsUC Santa Cruz Advisor: Profumo, Stefano Committee: Jeltema, Tesla, Ritz, Steve Permalink: http://escholarship.org/uc/item/41d7v3qd Abstract: Copyright Information: All rights reserved unless otherwise indicated. Contact the author or original publisher for any necessary permissions. eScholarship is not the copyright owner for deposited works. Learn more at http://www.escholarship.org/help_copyright.html#reuse eScholarship provides open access, scholarly publishing services to the University of California and delivers a dynamic research platform to scholars worldwide. UNIVERSITY OF CALIFORNIA SANTA CRUZ DARK MATTER ANNIHILATION AT THE GALACTIC CENTER A dissertation submitted in partial satisfaction of the requirements for the degree of DOCTOR OF PHILOSOPHY in PHYSICS by Tim Linden June 2013 The Dissertation of Tim Linden is approved: Professor Stefano Profumo, Chair Professor Tesla Jeltema Professor Steve Ritz Dean Tyrus Miller Vice Provost and Dean of Graduate Studies Copyright c by Tim Linden 2013 Table of Contents List of Figures v List of Tables vi Abstract vii Acknowledgments ix 1 Introduction 1 1.1 Gravitational Signatures of Dark Matter . 1 1.2 Particle Properties of Dark Matter . 6 1.3 The Indirect Detection of Particle Dark Matter . 9 1.4 Astrophysical Backgrounds . 12 1.5 Telescopes and Relevant Search Techniques . 13 1.6 Outline . 15 2 On the Origin of Gamma Rays from the Galactic Center 18 2.1 Analysis Procedure . 20 2.2 Properties of the Inner Emission .
    [Show full text]
  • A Statistical Approach to Recognizing Source Classes for Unassociated Sources
    1 A Statistical Approach to Recognizing Source Classes for Unassociated Sources 2 in the First Fermi-LAT Catalog 2 3 3 4;5 6 7 8;9 3 M. Ackermann , M. Ajello , A. Allafort , E. Antolini , L. Baldini , J. Ballet , G. Barbiellini , 10;11 6 3 3 3 4;5 4 D. Bastieri , R. Bellazzini , B. Berenji , R. D. Blandford , E. D. Bloom , E. Bonamente , 3 12 13;14 6 15;16 17 5 A. W. Borgland , A. Bouvier , T. J. Brandt , J. Bregeon , M. Brigida , P. Bruel , 3 18 10;11 19 3 20 6 R. Buehler , T. H. Burnett , S. Buson , G. A. Caliandro , R. A. Cameron , P. A. Caraveo , 7 21 4;5 22;23;24 3 25 7 J. M. Casandjian , E. Cavazzuti , C. Cecchi , O.¨ C¸elik , E. Charles , A. Chekhtman , 20 26 3 27;5 3 28 8 A. W. Chen , C. C. Cheung , J. Chiang , S. Ciprini , R. Claus , J. Cohen-Tanugi , 29;30;31 21 32 22;33 34 9 J. Conrad , S. Cutini , A. de Angelis , M. E. DeCesar , A. De Luca , 15;16 35 3 3 3 10 F. de Palma , C. D. Dermer , E. do Couto e Silva , P. S. Drell , A. Drlica-Wagner , 3 3 15;16 17 22;1 3 17 11 R. Dubois , T. Enoto , C. Favuzzi , S. J. Fegan , E. C. Ferrara , W. B. Focke , P. Fortin , 36 3 15;16 16 21 22 12 Y. Fukazawa , S. Funk , P. Fusco , F. Gargano , D. Gasparrini , N. Gehrels , 4;5 15;16 15;16 37 3 3 13 S.
    [Show full text]
  • The Full Appendices with All References
    Breakthrough Listen Exotica Catalog References 1 APPENDIX A. THE PROTOTYPE SAMPLE A.1. Minor bodies We classify Solar System minor bodies according to both orbital family and composition, with a small number of additional subtypes. Minor bodies of specific compositions might be selected by ETIs for mining (c.f., Papagiannis 1978). From a SETI perspective, orbital families might be targeted by ETI probes to provide a unique vantage point over bodies like the Earth, or because they are dynamically stable for long periods of time and could accumulate a large number of artifacts (e.g., Benford 2019). There is a large overlap in some cases between spectral and orbital groups (as in DeMeo & Carry 2014), as with the E-belt and E-type asteroids, for which we use the same Prototype. For asteroids, our spectral-type system is largely taken from Tholen(1984) (see also Tedesco et al. 1989). We selected those types considered the most significant by Tholen(1984), adding those unique to one or a few members. Some intermediate classes that blend into larger \complexes" in the more recent Bus & Binzel(2002) taxonomy were omitted. In choosing the Prototypes, we were guided by the classifications of Tholen(1984), Tedesco et al.(1989), and Bus & Binzel(2002). The comet orbital classifications were informed by Levison(1996). \Distant minor bodies", adapting the \distant objects" term used by the Minor Planet Center,1 refer to outer Solar System bodies beyond the Jupiter Trojans that are not comets. The spectral type system is that of Barucci et al. (2005) and Fulchignoni et al.(2008), with the latter guiding our Prototype selection.
    [Show full text]
  • (Diffuse Emission in Galaxies) K.D.Kuntz the Henry A
    The ISM (Diffuse Emission in Galaxies) K.D.Kuntz The Henry A. Rowland Department of Physics and Astronomy The Johns Hopkins University KU-4/2007 Introduction Xray Emission from Galaxies Point Sources LMXB HMXB Population Studies{ Diffuse Emission SNR SFR Bubbles Super-Bubbles Un ID’d Multiple SW & SNE Due to single stars Large Scale Emission (multiple degrees or larger) XAS-7/2007 Introduction Outline • Diffuse Emission in the Milky Way – Large Scale Emission (LHB, Galactic Halo, Etc.) – Super Bubbles – Star-Forming Regions • Diffuse Emission in Other Galaxies – Global Correlations XAS-7/2007 Introduction Fundamentals of X-ray Astronomy • X-ray Absorption Cross-Section is E-2/3 – Lower energy photons more readily absorbed – One can see further at higher energies XAS-7/2007 Introduction Fundamentals of X-ray Astronomy • Typical hot ISM T~106K _emission below 0.7 keV – Most parts of the hot ISM hidden from us • Most of what we see at low E is local! XAS-7/2007 Introduction Diversion I • A high Galactic latitude, bulk of sources are AGN • Deep exposures reveal more & fainter sources XAS-7/2007 LHB Diversion I • Does _AGN=total X-ray surface brightness? Yes, but…answer depends upon the energy. XAS-7/2007 LHB A Model of the Sky • Consider a map of the absorbing column due to neutral and molecular gas in the Milky Way. • If all of the emission is due to AGN, what does the sky look like? XAS-7/2007 LHB A Model of the Sky Absorption _ keV em. XAS-7/2007 LHB A Model of the Sky Model Observed R12= _ keV XAS-7/2007 LHB The Observed Sky _ keV _ keV XAS-7/2007 LHB The Observed Sky 1/4 keV 100µm XAS-7/2007 LHB The Observed Sky • At _ keV and _ keV there is diffuse local emission – Not identifiable with any single SN, SNR, or SFR • Distribution in _ keV and _ keV bands is different – (not just an effect of absorption) • Distance to emission (and thus its mass) is unknown.
    [Show full text]
  • The Contribution of Cosmic Rays Interacting with Molecular Clouds to the Galactic Center Gamma-Ray Excess
    The Contribution of Cosmic Rays Interacting With Molecular Clouds to the Galactic Center Gamma-Ray Excess Oscar Macias and Chris Gordon Department of Physics and Astronomy, Rutherford Building, University of Canterbury, Private Bag 4800, Christchurch 8140, New Zealand The Fermi-LAT data appear to have an excess of gamma rays from the inner 150 pc of the Galactic Center. The main explanations proposed for this are: an unresolved population of millisecond pulsars (MSPs), dark matter (DM) annihilation, and nonthermal bremsstrahlung produced by a population of electrons interacting with neutral gas in molecular clouds. The first two options have spatial templates well fitted by the square of a generalized Navarro-Frenk-White (NFW) profile with inner slope γ = 1:2. We model the third option with a 20-cm continuum emission Galactic Ridge template. A template based on the HESS residuals is shown to give similar results. The gamma-ray excess is found to be best fit by a combination of the generalized NFW squared template and a Galactic Ridge template. We also find the spectra of each template is not significantly affected in the combined fit and is consistent with previous single template fits. That is the generalized NFW squared spectrum can be fit by either of order 1000 unresolved MSPs or DM with mass around 30 GeV, a thermal cross section, and mainly annihilating to b¯b quarks. While the Galactic Ridge continues to have a spectrum consistent with a population of nonthermal electrons whose spectrum also provides a good fit to synchrotron emission measurements. We also show that the current DM fit may be hard to test, even with 10 years of Fermi-LAT data, especially if there is a mixture of DM and MSPs contributing to the signal, in which case the implied DM cross section will be suppressed.
    [Show full text]
  • Discrete Sources As the Origin of the Galactic X-Ray Ridge Emission
    Discrete sources as the origin of the Galactic X-ray ridge emission Revnivtsev M.1,2, Sazonov S.2,3, Churazov E. 3,2, Forman W. 4, Vikhlinin A.4,2, Sunyaev R.3,2 1Excellence Cluster Universe, Technische Universit¨at M¨unchen, Garching, Germany 2Space Research Institute, Moscow, Russia 3Max-Planck-Instutut fuer Astrophysik, Garching, Germany 4Harvard-Smithsonian Center for Astrophysics, Cambridge, USA An unresolved X-ray glow (at energies above a few kiloelectronvolts) was discovered about 25 years ago and found to be coincident with the Galactic diskthe Galactic ridge X-ray emission1, 2. This emission 3–10 has a spectrum characteristic of a 108K optically thin thermal plasma, with a prominent iron emission line at 6.7 keV.The gravitational well of the Galactic disk, however, is far too shallow to confine such a hot interstellar medium; instead, it would flow away at a velocity of a few thousand kilometres per second, exceeding the speed of sound in gas. To replenish the energy losses requires a source of 1043 erg s−1, exceeding by orders of magnitude all plausible energy sources in the Milky Way11. An alternative is that the hot plasma is bound to a multitude of faint sources12, which is supported by the recently observed arXiv:0904.4649v1 [astro-ph.GA] 29 Apr 2009 similarities in the X-ray and near-infrared surface brightness distributions13, 14 (the latter traces the Galactic stellar distribution). Here we report that at energies of 6-7 keV, more than 80 per cent of the seemingly diffuse X-ray emission is resolved into discrete sources, probably accreting white dwarfs and coronally active stars.
    [Show full text]