Orbital Period Analyses for the CVs Inside the Period Gap

Similar documents
Orbital period analyses for the CVs inside the period gap

Orbital period analysis of eclipsing Z Cam-type Dwarf Nova EM Cygni: Evidence of magnetic braking and a third body

PoS(SSC2015)051. Multi-tomography of polars from SALT spectroscopy

WANTED THE TRUE BOUNCE -BACK SYSTEMS

Extrasolar Planets. Methods of detection Characterization Theoretical ideas Future prospects

FORMATION AND EVOLUTION OF COMPACT BINARY SYSTEMS

Searching for Other Worlds

GR VIRGINIS: A DEEP OVERCONTACT BINARY

Ay123 Set 1 solutions

CATACLYSMIC VARIABLES. AND THE TYPE Ia PROGENITOR PROBLEM PROGENITOR PROBLEM

arxiv: v2 [astro-ph] 18 Dec 2008

Reanalysis of the Orbital Period Variations of Two DLMR Overcontact Binaries: FG Hya and GR Vir

Star-planet interaction and planetary characterization methods

Monitoring orbital period variations in eclipsing white dwarf binaries

arxiv: v1 [astro-ph.sr] 21 Nov 2018

Mean-Motion Resonance and Formation of Kirkwood Gaps

Thermal-timescale mass transfer and magnetic CVs

AP Physics C Textbook Problems

Name Period Date Earth and Space Science. Solar System Review

Binary Stars (continued) ASTR 2120 Sarazin. γ Caeli - Binary Star System

Distribution of X-ray binary stars in the Galaxy (RXTE) High-Energy Astrophysics Lecture 8: Accretion and jets in binary stars

University of Central Florida Department of Physics, PSB 132, 4000 University Blvd., Orlando, FL, USA

Planets around evolved stellar systems. Tom Marsh, Department of Physics, University of Warwick

Starspot Magnetic Fields

DEPARTMENT OF PHYSICS AND ASTRONOMY. Planets around white dwarfs Matt Burleigh

Fundamental (Sub)stellar Parameters: Surface Gravity. PHY 688, Lecture 11

6 th lecture of Compact Object and Accretion, Master Programme at Leiden Observatory

A period investigation of the overcontact binary system V417 Aquilae. Qian Shengbang 1,2. Min.I = ḍ E (1)

arxiv:astro-ph/ v1 10 May 2006

Thermal pressure vs. magnetic pressure

The role of SW Sex stars in the evolution of CVs

Exoplanet Search Techniques: Overview. PHY 688, Lecture 28 April 3, 2009

Variable Stars South. Who we are What we do. 2

10/16/ Detecting Planets Around Other Stars. Chapter 10: Other Planetary Systems The New Science of Distant Worlds

Cataclysmic variables

Names: Team: Team Number:

Components of Galaxies Stars What Properties of Stars are Important for Understanding Galaxies?

10/25/2010. Stars, Galaxies & the Universe Announcements. Stars, Galaxies & the Universe Lecture Outline. Reading Quiz #9 Wednesday (10/27)

7. BINARY STARS (ZG: 12; CO: 7, 17)

Observed Properties of Stars - 2 ASTR 2110 Sarazin

Exoplanetary Atmospheres: Atmospheric Dynamics of Irradiated Planets. PHY 688, Lecture 24 Mar 23, 2009

Ay101 Set 1 solutions

Surface and Circumstellar Structures in Early-Type Interacting Binaries

Lecture 13: Binary evolution

Origins of Gas Giant Planets

arxiv:astro-ph/ v1 23 Oct 2002

The Hertzprung-Russell Diagram. The Hertzprung-Russell Diagram. Question

Space Science Jeopardy!

Lines of Hydrogen. Most prominent lines in many astronomical objects: Balmer lines of hydrogen

Two projects without apparent connection?

Dr G. I. Ogilvie Lent Term 2005 INTRODUCTION

Symbiotic stars: challenges to binary evolution theory. Joanna Mikołajewska Copernicus Astronomical Center, Warsaw

Revision: Sun, Stars (and Planets) See web slides of Dr Clements for Planets revision. Juliet Pickering Office: Huxley 706

UV Observations of Cataclysmic Variables and their role in multiband studies

Exoplanets: a dynamic field

Extrasolar Planets: Ushering in the Era of Comparative Exoplanetology

Actuality of Exoplanets Search. François Bouchy OHP - IAP

A Survey of Stellar Families Multiplicity of Solar-type Stars

Spectroscopy, the Doppler Shift and Masses of Binary Stars

arxiv:astro-ph/ v1 8 May 2002

Chapter 12 Stellar Evolution

Optical Photometry of Dwarf Nova QZ Serpentis in Quiescence

Lecture 20: Planet formation II. Clues from Exoplanets

Fundamental (Sub)stellar Parameters: Masses and Radii. PHY 688, Lecture 10

Analyzing X-Ray Pulses from Stellar Cores Pencil & Paper Version

Science Olympiad Astronomy C Division Event National Exam

Stellar Astronomy Sample Questions for Exam 3

Stellar Models ASTR 2110 Sarazin

Evolution of binary stars

EART164: PLANETARY ATMOSPHERES

Extrasolar Transiting Planets: Detection and False Positive Rejection

10/26/ Star Birth. Chapter 13: Star Stuff. How do stars form? Star-Forming Clouds. Mass of a Star-Forming Cloud. Gravity Versus Pressure

Long-time behavior of orbital periods of some Algol-type eclipsing binaries

Searching For Planets Like Earth around stars like the Sun

AST Section 2: Test 2

The observations of deeply eclipsing polars FL Ceti and CSS :

READ: Chapter 11.1, 11.2 (11.2.1, only), 11.3(

Microlensing Parallax with Spitzer

Formation Mechanisms of Brown Dwarfs: Observations & Theories. Dan Li April 2009

MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.

Several Methods of Estimating Times of Minima in Cataclysmic Variables And Some Fesults for EX Dra

Pulsations and planets at late stages of stellar evolution

HR Diagram, Star Clusters, and Stellar Evolution

Tidal Dissipation in Binaries

Habitable exoplanets: modeling & characterization

Lecture Outlines. Chapter 20. Astronomy Today 8th Edition Chaisson/McMillan Pearson Education, Inc.

The Evolution of Low Mass Stars

Boris Gänsicke. Eclipsing binaries, something different. York 2014 To commemorate the 250th anniversary of the birth of John Goodricke

Importance of the study of extrasolar planets. Exoplanets Introduction. Importance of the study of extrasolar planets

The Stars. Chapter 14

Observed Properties of Stars - 2 ASTR 2120 Sarazin

Globular Clusters. This list contains 135 of the brightest and largest globular clusters from the Astroleague's observing program/list.

Extrasolar Planets. Today. Dwarf Planets. Extrasolar Planets. Next week. Review Tuesday. Exam Thursday. also, Homework 6 Due

Based on the reduction of the intensity of the light from a star with distance. It drops off with the inverse square of the distance.

Heading for death. q q

THE AGE OF THE KIC SYSTEM. James MacDonald and D. J. Mullan Department of Physics and Astronomy, DE 19716, USA

Relativity and Astrophysics Lecture 15 Terry Herter. RR Lyrae Variables Cepheids Variables Period-Luminosity Relation. A Stellar Properties 2

Kozai-Lidov oscillations

Friday, September 23, 2011

Physical Parameters of KID , a Low-Mass, Double- Lined Eclipsing Binary

Transcription:

Orbital Period Analyses for the CVs Inside the Period Gap YNAO Dai Zhibin zhibin_dai@ynao.ac.cn Yunnan Astronomical Observatory, Chinese Academy of Sciences

OUTLINE What is the Period Gap? New orbital period distributions of CVs Orbital period analyses Summary

Part I. Period Gap

What is the Period Gap? Katysheva & Pavlenko (2003)

Why is there a gap? " Selection effect for observation (Rappaport et al., 1983) " CV Evolution A. The corresponding gap in white dwarf mass distribution (de Kool, 1992) M wd 0.46M Θ M wd 0. 56M Θ for the CVs below gap for the CVs above gap B. The similar gap has already been shown in the distribution of progenitors of CVs (Vojkhanskaja., 2007) Progenitors of CVs: White dwarf + red dwarf binary system / PCEBs C. Disrupted Magnetic Braking hypothesis (Robinson et al., 1981; McDermott & E. Taam, 1989) Sharp reduction in AML rate when secondary becomes fully convective

Standard paradigm of CV evolution A default argument: CVs evolution will shorten its Orbital period Evolution Above Gap Magnetic Wind With radiation core Below Gap Gravitational Radiation Full Convective

Part II. Investigation

Details of Orbital period distribution The distributions for different subtype of CVs a) Bimodality caused by DN and NL b) The shallower gap in MCV and DN c) No gap in NL and N&RN The pie diagram for the CVs inside below period gap a) MCV DN becomes is a significant a significant subtype subtype inside period below period gap gap b) The Over other 75% subtypes CVs below are gap nearly are DN equal and MCV New N&RN MCV DN NL!

A gradual rise branch near 2hr -- is it a result the whole caused gap by gravitational radiation? CVs have spread over The real minimum of gap is near 3hr-- is longer period it a possible evidence for the sudden decline of stellar wind? A small shift towards Smaller interval 10mins for histogram of orbital period distribution

Part III. Analyses

Eclipsing CVs inside gap Subtype MCV DN N & RN Eclipse CVs Orbital Period (hr) *HU Aqr (~15mag) 0.086820459(2.08h)!DD Cir (~20mag) 0.09746 (2.34h) *UZ For (~18mag) 0.087865446(2.11h) *V348 Pup (~15mag) 0.101838933(2.44h)!V597 Pup (>18mag) 0.119583333(2.6687h) *DV Uma (~19mag) 0.085852633(2.06h) *IR Com (~15mag) 0.087038644(2.09h)!SDSS J170213 (~18mag) 0.100082090(2.40h)!CTCV J1300-3052 (~16mag) 0.088850000(2.13h)?TY Psa (~14mag) 0.084100000(2.02h)!V Per (~18mag) 1887 0.107123474(2.57h)!DD Cir (~20mag) 1999 0.097460000(2.34h)!V630 Sgr (~18mag) 1936 0.118000000(2.83h)!QU Vul (~19mag) 1984 0.111764700(2.68h)!V597 Pup (>18mag) 2007 0.119583333(2.6687h)

Photometries for AM Her (Dai et al., 2012, in preparation) It locates at the upper edge of period gap. Its secular evolution state is a key factor to test the current evolution theory. Collected from AAVSO and our photometries

New O-C diagram of AM Her A typical period decrease rate ~10-10.15 Low-state data just add the large scatters

The orbital period variations Cyclical Secular Log(P mod ) = -0.36(±0.10)Log(Ω) + 0.018 ² A combined masses of 0.78M sun (WD) + 0.26M sun (RD) means that mass transfer E0/Emin<<1 in AM Her with an average mass transfer rate 10-10 M sun yr -1 only induces the orbital period increase(gänsicke et al., 2001). ² This increase can be counteracted by the gravitational radiation. ² R 3 /a ~ 10 3 ² The magnetic braking may be suppressed ² in Mpolars 3 (min)/m (Cumming, 2 ~ 0.8 2002). Including Algol, RS CVn,WUMa and CVs (Lanza & Rodonò,1999)

Decreasing orbital period (Qian et al., MNRASL, 2011) (Qian et al., ApJL, 2008) HU Aqr(b) HU Aqr (c) Amplitude (d) 0.000 107(17) 0.000 122(14) Eccentricity 0.0 0.51(±0.15) Period (yr) 6.54(±0.01) 11.96(±1.41) Solar Titus-Bode relation Distance (au) 3.6(±0.8) 5.4(±0.9) Masses (Jup) 5.9(±0.6) HU Aqr 4.5(±0.5) HW Vir P cycle =15.7 yr A cycle = 0.000879d A planetary system with three giant planets

Can we find the orbital period increase? λ( q) Rcr Porb q 1 In conservative case Normal CVs cannot sustain conservative mass transfer. It obviously conflicts with hypothesis of CV evolution We need to pay more attention to the increasing O-C diagrams

Possible increasing orbital period (Dai et al., in preparation) E0/Emin~4 (Dai et al., MNRAS, 2010) V348 Pup UZ For UZ For The more increase observations in a decrease long base It Different line should are necessary be model a substellar can for result checking object out for both this totally models increasing opposite (>90% trend variation probability) trend

Summary The orbital period distribution for different subtype exhibits the complication of gap. Part of the eclipsing CVs inside gap never give us definite secular evolutional information Most of modulations in O-Cs can be explained by light travel-time effect

Thanks for your attention!