Cumulative  Deviation of data & model scaled  to 0.3  99%  90%  95% HD 36861J (rp200200a01) 0.829 Probability of Variability A Large ROSAT Survey.

Slides:



Advertisements
Similar presentations
Probing Magnetic Reconnection with Active Region Transient Brightenings Martin Donachie Advisors: Adam Kobelski & Roger Scott.
Advertisements

Spatial and temporal relationships between UV continuum and hard x-ray emissions in solar flares Aaron J. Coyner and David Alexander Rice University June.
Chapter 8 The Sun – Our Star.
Copyright © 2010 Pearson Education, Inc. Chapter 16 Galaxies and Dark Matter.
X-ray Diagnostics and Their Relationship to Magnetic Fields David Cohen Swarthmore College.
Swift/BAT Hard X-ray Survey Preliminary results in Markwardt et al ' energy coded color.
X-ray Diagnostics and Their Relationship to Magnetic Fields David Cohen Swarthmore College.
X-ray Diagnostics and Their Relationship to Magnetic Fields David Cohen Swarthmore College.
Wind Signatures in the X-ray Emission Line Profiles of the O Supergiant  Orionis Kevin Grizzard 1, David Cohen 2, Maurice Leutenegger 3, Casey Reed 2,
GALEX UV Light-curves of M-Dwarf Flare Stars: “ THE FLARING UV SKY” Barry Welsh, Jonathan Wheatley & Stanley Browne (UC Berkeley) Richard Robinson (Catholic.
Coronal Boundaries of Active Regions Derived From Soft X-ray Images.
Spectral analysis of starlight can tell us about: composition (by matching spectra). temperature (compare to blackbody curve). (line-of-sight) velocity.
Growth of Structure Measurement from a Large Cluster Survey using Chandra and XMM-Newton John R. Peterson (Purdue), J. Garrett Jernigan (SSL, Berkeley),
X-ray occultation of Scorpius X-1 by small trans-neptunian objects Liang, Jau-shian Institute of Physics, NTHU 2006/04/27.
A Search for Point Sources of High Energy Neutrinos with AMANDA-B10 Scott Young, for the AMANDA collaboration UC-Irvine PhD Thesis:
Extra-Solar Planets Astronomy 311 Professor Lee Carkner Lecture 24.
The Application of Forbidden Line X-Ray Diagnostics to the Hot Star Tau Sco Author: Geneviève de Messières Swarthmore College ‘04 Advised by: David Cohen.
X-rays from Magnetically Channeled Winds of OB Stars David Cohen Swarthmore College with M. Gagné, S. St. Vincent, A. ud-Doula, S. Owocki, R. Townsend.
Stephen St. Vincent (Swarthmore, class of 2007) Advisor: Prof. David Cohen Visualizing Numerical Simulations of Magnetized Stellar Winds, and the Synthesis.
X-ray Polarization as a Probe of Strong Magnetic Fields in X-ray Binaries Shane Davis (IAS) Chandra Fellows Symposium, Oct. 17, 2008.
The spectral resolution of x-ray telescopes has improved many hundred-fold over the past decade, enabling us to detect and resolve emission lines in hot.
Analysis of Doppler-Broadened X-ray Emission Line Profiles from Hot Stars David Cohen - Swarthmore College with Roban Kramer - Swarthmore College Stanley.
Stephen St.Vincent (Swarthmore, class of 2007) Advisor: Prof. David Cohen Visualizing Numerical Simulations of Magnetized Stellar Winds and the Synthesis.
X-ray Emission from O Stars David Cohen Swarthmore College.
X-ray Emission from Massive Stars David Cohen Swarthmore College.
Layers of the Solar Atmosphere Corona Chromosphere Photosphere Details of solar activity can be seen more easily in the hotter outer layers, which are.
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.
 Galaxies with extremely violent energy release in their nuclei  Active Galactic Nuclei (AGN)  Up to many thousand times more luminous than the entire.
This is the Local Group of galaxies, about 45 galaxies within about 1 Mpc of the Milky Way. Most are dwarf-elliptical or iregular. A distance of one million.
V410 TAU T TAURI Pre Main Sequence – young, low mass stars that are contracting as they evolve toward their main sequence stage. Mostly made of Hydrogen,
NASSP Masters 5003F - Computational Astronomy Lecture 19 EPIC background Event lists and selection The RGA Calibration quantities Exposure calculations.
Chapter 3 concepts/objectives Define and describe density curves Measure position using percentiles Measure position using z-scores Describe Normal distributions.
Radio and X-Ray Properties of Magellanic Cloud Supernova Remnants John R. Dickel Univ. of Illinois with: D. Milne. R. Williams, V. McIntyre, J. Lazendic,
Wide Field Imagers in Space and the Cluster Forbidden Zone Megan Donahue Space Telescope Science Institute Acknowledgements to: Greg Aldering (LBL) and.
Donna Kubik PHYS162 Fall, Because of its electric and magnetic properties, light is called electromagnetic radiation. It consists of perpendicular,
A Short Talk on… Gravitational Lensing Presented by: Anthony L, James J, and Vince V.
1 THE RELATION BETWEEN CORONAL EIT WAVE AND MAGNETIC CONFIGURATION Speakers: Xin Chen
Our Evolving Universe1 Vital Statistics of the Universe Today… l l Observational evidence for the Big Bang l l Vital statistics of the Universe   Hubble’s.
TYPES OF STATISTICAL METHODS USED IN PSYCHOLOGY Statistics.
X-ray Diagnostics and Their Relationship to Magnetic Fields David Cohen Swarthmore College.
Post Processing of ZEUS MHD Simulations of Young, Hot Stars Stephen V. St.Vincent and David H. Cohen Swarthmore College Department of Physics & Astronomy.
Can variability account for apparent age spreads in OB association colour-magnitude diagrams? Ben Burningham & Tim Naylor School of Physics, University.
Final Presentation By Matthew Lewis 17 th March 2006 “To Determine the Accuracy that GOES True Numbers can Reproduce the Full X-ray Spectrum of the Sun”
X-ray Diagnostics and Their Relationship to Magnetic Fields David Cohen Swarthmore College.
Chandra X-Ray Spectroscopy of DoAr 21: The Youngest PMS Star with a High-Resolution Grating Spectrum The High Energy Grating Spectrum of DoAr 21, binned.
Lecture Outlines Astronomy Today 7th Edition Chaisson/McMillan © 2011 Pearson Education, Inc. Chapter 23.
NoRH Observations of RHESSI Microflares M.R. Kundu, Dept. of Astronomy, University of Maryland, College Park, MD E.J.Schmahl, Dept. of Astronomy, University.
Galaxies with Active Nuclei Chapter 14:. Active Galaxies Galaxies with extremely violent energy release in their nuclei (pl. of nucleus).  “active galactic.
Warm Absorbers: Are They Disk Outflows? Daniel Proga UNLV.
Active Galaxies and Supermassive Black Holes Chapter 17.
Conclusions The prototype  Pup (O4 I) has X-ray emission line profiles consistent with a simple spherically symmetric wind shock model. What can lead.
Copyright © 2013, 2009, and 2007, Pearson Education, Inc. Chapter 11 Analyzing the Association Between Categorical Variables Section 11.2 Testing Categorical.
XMM-Newton observations of open clusters and star forming regions R. Pallavicini and E. Franciosini INAF- Osservatorio Astronomico di Palermo, Italy S.
The Power Spectra and Point Distribution Functions of Density Fields in Isothermal, HD Turbulent Flows Korea Astronomy and Space Science Institute Jongsoo.
Statistical Properties (PS, PDF) of Density Fields in Isothermal Hydrodynamic Turbulent Flows Jongsoo Kim Korea Astronomy and Space Science Institute Collaborators:
SEP Event Onsets: Far Backside Solar Sources and the East-West Hemispheric Asymmetry S. W. Kahler AFRL Space Vehicles Directorate, Kirtland AFB, New Mexico,
Exploring an evidence of supermassive black hole binaries in AGN with MAXI Naoki Isobe (RIKEN, ) and the MAXI
KASI Galaxy Evolution Journal Club A Massive Protocluster of Galaxies at a Redshift of z ~ P. L. Capak et al. 2011, Nature, in press (arXive: )
Hiroyasu Tajima Stanford Linear Accelerator Center Kavli Institute for Particle Astrophysics and Cosmology October 26, 2006 GLAST lunch Particle Acceleration.
Active Galaxies Galaxies with extremely violent energy release in their nuclei (pl. of nucleus). → “Active Galactic Nuclei” (= AGN) Up to many thousand.
Chapter 11: Categorical Data n Chi-square goodness of fit test allows us to examine a single distribution of a categorical variable in a population. n.
Class Seven Turn In: Chapter 18: 32, 34, 36 Chapter 19: 26, 34, 44 Quiz 3 For Class Eight: Chapter 20: 18, 20, 24 Chapter 22: 34, 36 Read Chapters 23 &
Chapter 20 Cosmology. Hubble Ultra Deep Field Galaxies and Cosmology A galaxy’s age, its distance, and the age of the universe are all closely related.
A smoothed hardness map of the hotspots of Cygnus A (right) reveals previously unknown structure around the hotspots in the form of outer and inner arcs.
goals  Observe distorted galaxies using advanced techmaun telescopes  Determine possible galaxy type  Determine possible causes for the distortions.
Tobias Jogler Max-Planck Institut für Physik IMPRS YSW Ringberg 2007 VHE emission from binary systems Outline Binary systems Microquasar Pulsar binaries.
P-values.
Spectral analysis of starlight can tell us about:
Analyzing the Association Between Categorical Variables
Presentation transcript:

Cumulative  Deviation of data & model scaled  to 0.3  99%  90%  95% HD 36861J (rp200200a01) Probability of Variability A Large ROSAT Survey of X-Ray Time Variability in O Stars Allison S. Adelman 1, David H. Cohen 2 (1) Bryn Mawr College, (2) Swarthmore College THEORY O star X-ray emission comes from shock-heated gas present in their stellar winds; for B stars, the situation is more uncertain, and their X- rays may be related to magnetic fields, at least in some cases. The same may be true for certain O stars too. Unstable mass flow driven by the radiation field of the star produces strong shocks as faster wind material impacts on slower material (Owocki, Castor, & Rybicki 1988). Shocks occur stochastically, so X-ray output should be time variable. X-ray variability should be due to evolution of individual shock structures and due to time variability in the number of individual shock zones in the wind.  The X-ray variability properties (timescales and spectral properties, as well as amplitude of variability) should tell us about the properties and underlying physics of wind shocks. At the simplest level, the amplitude of X-ray variability is proportional to the square root of the number of individual shocks. Two Sample Images of ROSAT fields Analysis Procedure Data A pointed observation of O star HD57060 O star HD57061 is also present, but overlapping another point source, smeared out near the edge of the image The support structure of the telescope is clearly visible ObsID rp200066a02 HD HD HD A pointed observation of a young open cluster of O stars (NGC 6231) 3 O stars are present in the central cluster; however many were too indistinguishable to extract data 2 other O stars with good data are present in the field, as well as 1 more that is smeared out at the edge of the image Sample Light Curves of O Stars HD A Representative Non-Variable Star HD A Representative Variable O Star Background O Star X-Rays Project We searched the ROSAT PSPC archives of pointed observations for O stars, observed both intentionally and serendipitously Our sample includes 60 O stars in 86 separate observations, including many O stars not previously reported on in the X-ray literature. We extracted source counts for each O star, and performed several types of time variability analyses on each object HD mean = bins = 12 Reduced  2 = 0.80 P= 36% st. dev. = K-S Probability = HD36861J mean = bins = 20 Reduced  2 = 0.93 P = 45% st. dev. = K-S Probability = Examples of K-S Test Results  Cumulative  Deviation of data & model scaled to 0.3  99%  90%  95% HD (rp200199a00) Probability of Variability We ran  2 tests of the null hypothesis (of a constant count rate). And we also calculated the one-sided K-S statistic. For longer pointings, which were broken up into several observations, we calculated the K-S statistic for each observation. If the K-S test gave a positive result (>90% probability of variability) we tested the hard (E>0.5keV) and soft (E<0.5keV) spectral ranges separately. OBSERVATIONS Very few large, systematic studies of X-ray variability among O stars. It is generally accepted that O star X-ray emission is not variable, but this has not been thoroughly quantified. A few individual cases of X-ray variability have been detected:  1 Ori C: periodic modulation: a young magnetic rotator.   Pup: Very long observations have turned up very low level (~2%) periodic (P=18h) variability correlated with H  variability.  Ori: one-time brightening of ~15%: possibly also magnetic in origin.  Ori and Cyg OB2-8 detected with Einstein; also some interacting binaries.  No systematic survey of O star X-ray variability has been carried out using the largest, high-sensitivity database of X-ray observations: The ROSAT archive. There are numerous sites of X- ray emission on the sun. Each one evolves in time, as does the overall distribution, leading to significant X-ray variability. UV observations of O star winds show small- and large-scale variability; often periodic but also stochastic. ObsID rp200112n00 HD57061 HD57060 Linear Fits to Variable Stars O StarK-S Probability K-S Prob. for Soft Energy Channels K-S Prob. for Hard Energy Channels HD HD HD HD HD HD HD HD37742J (rp200198a00) HD37742J (rp900386n00) HD HD Hard and Soft Energy Channel K-S Probability Results Bright stars in the spectral range earlier than about B3 are soft X-ray sources, with L X ~ L Bol Note: K-S test is generally more sensitive than  2 (can see in lightcurve at the bottom of the previous column too) refers to linear fits 11 of the 17 observations showing variability have non-zero slope of their count rates Conclusions Nearly 30% of the O stars in the sample are variable No dramatic variability (e.g. no flares) Much of it is ‘long’ timescale variability (  > few ksec) Significant amount of hard variability wavelength - velocity Time (days) Numerical radiation hydrodynamic simulations (snapshot at left) show highly time-dependent structure, with shock waves advecting through the wind. Flow timescales and cooling timescales are of order 1000s of seconds. The ROSAT PSPC is a gas proportional counter with a two- degree field of view and some very modest energy resolution (each photon is tagged with an approximate energy, as well as a position and arrival time in the detector) Note: the spatial resolution (FWHM~5”) degrades rapidly off-axis.