Pleasantness Review* Department of Physics, Technion, Israel. Noam Soker

Similar documents
Pleasantness Review*

The Core-Degenerate (CD) Scenario Noam Soker Department of Physics, Technion

The Evolution of Close Binaries

Follow the Angular Momentum! Pleasantness Review

FORMATION AND EVOLUTION OF COMPACT BINARY SYSTEMS

Mass Transfer in Binaries

The Deaths of Stars. The Southern Crab Nebula (He2-104), a planetary nebula (left), and the Crab Nebula (M1; right), a supernova remnant.

Post Common Envelope Binary Stars. Prof. Todd Hillwig Summer 2017

This class: Life cycle of high mass stars Supernovae Neutron stars, pulsars, pulsar wind nebulae, magnetars Quark-nova stars Gamma-ray bursts (GRBs)

Cassiopeia A: Supernova Remnant

Introductory Astrophysics A113. Death of Stars. Relation between the mass of a star and its death White dwarfs and supernovae Enrichment of the ISM

Ch. 16 & 17: Stellar Evolution and Death

arxiv:astro-ph/ v1 10 Nov 1998

arxiv: v1 [astro-ph.sr] 25 Oct 2018

Special Relativity. Principles of Special Relativity: 1. The laws of physics are the same for all inertial observers.

Einführung in die Astronomie II

Lecture 8: Stellar evolution II: Massive stars

The structure and evolution of stars. Learning Outcomes

Supernovae, Neutron Stars, Pulsars, and Black Holes

Billions and billions of stars

Astronomy 113. Dr. Joseph E. Pesce, Ph.D. Dr. Joseph E. Pesce, Ph.D.

Stars with Mⵙ go through two Red Giant Stages

Astro 1050 Fri. Apr. 10, 2015

Star Formation. Stellar Birth

Supernovae. Supernova basics Supernova types Light Curves SN Spectra after explosion Supernova Remnants (SNRs) Collisional Ionization

Phys 100 Astronomy (Dr. Ilias Fernini) Review Questions for Chapter 9

Neutron Stars. We now know that SN 1054 was a Type II supernova that ended the life of a massive star and left behind a neutron star.

Black Holes ASTR 2110 Sarazin. Calculation of Curved Spacetime near Merging Black Holes

Guiding Questions. The Deaths of Stars. Pathways of Stellar Evolution GOOD TO KNOW. Low-mass stars go through two distinct red-giant stages

The Deaths of Stars 1

The Bizarre Stellar Graveyard

Guiding Questions. The Deaths of Stars. Pathways of Stellar Evolution GOOD TO KNOW. Low-mass stars go through two distinct red-giant stages

Stellar Evolution: The Deaths of Stars. Guiding Questions. Pathways of Stellar Evolution. Chapter Twenty-Two

Stellar Evolution: Outline

Astronomy 110: SURVEY OF ASTRONOMY. 11. Dead Stars. 1. White Dwarfs and Supernovae. 2. Neutron Stars & Black Holes

The Stellar Graveyard

Friday, March 21, 2014 Reading for Exam 3: End of Section 6.6 (Type Ia binary evolution), 6.7 (radioactive decay), Chapter 7 (SN 1987A), NOT Chapter

Astronomy. Chapter 15 Stellar Remnants: White Dwarfs, Neutron Stars, and Black Holes

Stellar Evolution. Eta Carinae

Stars and their properties: (Chapters 11 and 12)

The Stellar Graveyard Neutron Stars & White Dwarfs

Lecture 9: Supernovae

Supernova events and neutron stars

AST 101 Introduction to Astronomy: Stars & Galaxies

Supernovae. Supernova basics Supernova types Light Curves SN Spectra after explosion Supernova Remnants (SNRs) Collisional Ionization

Lecture 13: Binary evolution

Comparing a Supergiant to the Sun

Neutron Stars. Neutron Stars and Black Holes. The Crab Pulsar. Discovery of Pulsars. The Crab Pulsar. Light curves of the Crab Pulsar.

Names: Team: Team Number:

Quick Clicker Survey: What do like best about the class so far?

Dr. Reed L. Riddle. Close binaries, stellar interactions and novae. Guest lecture Astronomy 20 November 2, 2004

Chapter 18 The Bizarre Stellar Graveyard

The Life Cycles of Stars. Modified from Information provided by: Dr. Jim Lochner, NASA/GSFC

RESUME. Name: NOAM SOKER Date: January 2017 PERSONAL DETAILS. Place and Date of Birth: Israel, Marital Status: Married + 3

Neutron Stars. Chapter 14: Neutron Stars and Black Holes. Neutron Stars. What s holding it up? The Lighthouse Model of Pulsars

The electrons then interact with the surrounding medium, heat it up, and power the light curve. 56 Ni 56 Co + e (1.72 MeV) half life 6.

Astronomy Ch. 20 Stellar Evolution. MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.

Astronomy Ch. 20 Stellar Evolution. MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.

Dr G. I. Ogilvie Lent Term 2005 INTRODUCTION

Chapter 18 The Bizarre Stellar Graveyard. White Dwarfs. What is a white dwarf? Size of a White Dwarf White Dwarfs

Stellar Astronomy Sample Questions for Exam 4

Clicker Question: Clicker Question: Clicker Question: Clicker Question: What is the remnant left over from a Type Ia (carbon detonation) supernova:

Chapter 14: The Bizarre Stellar Graveyard. Copyright 2010 Pearson Education, Inc.

Termination of Stars

Chapter 14: The Bizarre Stellar Graveyard

Compton Lecture #4: Massive Stars and. Supernovae. Welcome! On the back table:

An Interacting Binary System Powers Precessing Outflows of an Evolved Star

3/13/18. Things to do. Synchrotron Radiation. Today on Stellar Explosions

Death of stars is based on. one thing mass.

Number of Stars: 100 billion (10 11 ) Mass : 5 x Solar masses. Size of Disk: 100,000 Light Years (30 kpc)

Astronomy Ch. 21 Stellar Explosions. MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.

Goal - to understand what makes supernovae shine (Section 6.7).

The Death of Stars. Today s Lecture: Post main-sequence (Chapter 13, pages ) How stars explode: supernovae! White dwarfs Neutron stars

Boris Gänsicke. Type Ia supernovae and their progenitors

Chapter 11 The Formation and Structure of Stars

The Formation of Stars

Brock University. Test 1, February, 2017 Number of pages: 9 Course: ASTR 1P02 Number of Students: 480 Date of Examination: February 6, 2017

Supernova from the smashing collision of a binary star

From AGB Stars to Planetary Nebula. Cats Eye Planetary Nebula: HST

Stellar Evolution. Stars are chemical factories The Earth and all life on the Earth are made of elements forged in stars

THIRD-YEAR ASTROPHYSICS

Protostars on the HR Diagram. Lifetimes of Stars. Lifetimes of Stars: Example. Pressure-Temperature Thermostat. Hydrostatic Equilibrium

STELLAR DEATH, AND OTHER THINGS THAT GO BOOM IN THE NIGHT. Kevin Moore - UCSB

Fate of Stars. relative to Sun s mass

Protostars evolve into main-sequence stars

A1199 Are We Alone? " The Search for Life in the Universe

arxiv:astro-ph/ v1 14 Sep 2004

Brock University. Test 1, January, 2015 Number of pages: 9 Course: ASTR 1P02 Number of Students: 500 Date of Examination: January 29, 2015

Accretion Disks. Review: Stellar Remnats. Lecture 12: Black Holes & the Milky Way A2020 Prof. Tom Megeath 2/25/10. Review: Creating Stellar Remnants

Chapter 13 Notes The Deaths of Stars Astronomy Name: Date:

Today in Bizarre-Land. Binary Systems: The Algol Paradox

Life of stars, formation of elements

Star Death ( ) High Mass Star. Red Supergiant. Supernova + Remnant. Neutron Star

5) What spectral type of star that is still around formed longest ago? 5) A) F B) A C) M D) K E) O

Today. Logistics. Visible vs. X-ray X. Synchrotron Radiation. Pulsars and Neutron Stars. ASTR 1040 Accel Astro: Stars & Galaxies

Stellar Birth. Stellar Formation. A. Interstellar Clouds. 1b. What is the stuff. Astrophysics: Stellar Evolution. A. Interstellar Clouds (Nebulae)

Chapter 19 Reading Quiz Clickers. The Cosmic Perspective Seventh Edition. Our Galaxy Pearson Education, Inc.

Supernova Explosions. Novae

Planetary Nebulae evolve to White Dwarf Stars

PHYS 1401: Descriptive Astronomy Notes: Chapter 12

Transcription:

Pleasantness Review* Department of Physics, Technion, Israel The role of jets: from common envelope to nebulae Nice 2015 Noam Soker Essential collaborators (Technion): Amit Kashi, Muhammad Akashi, Ealeal Bear, Oded Papish, Danny Tsebrenko, Avishai Gilkis, Efrat Sabach, Sagiv Shiber, Ron Schreier Dictionary translation of my name from Hebrew to English (real!): Noam = Pleasantness Soker = Review

Short Summary JETS This research was not supported by any grant

Summary: Issues in dispute Issue / Process Common envelope parameter α CE Most others Parameter commonly used My view which is Grazing envelope evolution (GEE) Supernova Ia Remnants Never heard about this Four different other scenarios T Core-collapse supernovae By neutrinos

Summary: Issues in dispute Issue / Process Common envelope parameter Grazing envelope evolution (GEE) Supernova Ia Remnants Core-collapse supernovae α CE Most others Parameter commonly used Never heard about this Four different other scenarios By neutrinos My view which is strongly supported by Problematic. Instead use Jets and migration (but no jets for WDs!!) Takes place in many cases The core degenerate scenario: SNIP (Danny Tsebrenko) Neutrino mechanisms have a generic problem. Explosion by jets

Summary: Issues in dispute Issue / Process Common envelope parameter Grazing envelope evolution (GEE) Supernova Ia Remnants Core-collapse supernovae α CE Most others Parameter commonly used Never heard about this Four different other scenarios By neutrinos My view which is strongly supported by Problematic. Instead use Jets and migration (but no jets for WDs!!) Takes place in many cases The core degenerate scenario: SNIP (Danny Tsebrenko) Neutrino mechanisms have a generic problem. Explosion by jets my wife and three kids Orsola de Marco (but she doesn t know it yet) my psychiatrist The clerk in charge of early retirement in the Technion.

Pleasantness Review: The role of jets: from common envelope to nebulae (1) What we see (2) What we see and simulate (3) What we simulate but don t see (4) What we don t see and did not simulate yet.

Red: X-ray Blue: radio implying jets. Low density Bubbles (cavities) (McNamara, B. and collaborators)

Planetary Nebula Hb 5: High resolution Low resolution Shaping by jets MS 0735.6+7421 A cluster of galaxies

Pleasantness Review: The role of jets: from common envelope to nebulae (1) What we see (2) What we see and simulate (3) What we simulate but don t see (4) What we don t see and did not simulate yet.

Observed (X-ray) bubbles in the Perseus cluster of galaxies Simulating a wide jet in a cluster Simulating bubble formation in planetary nebulae (Akashi & Soker 2012) Observed (visible [N II]) bubbles in NGC 3587 6 orders of magnitude difference in size 12-15 orders of magnitude difference in mass an energy

The Necklace planetary nebula (Form Romano Corradi et al. 2011): A binary central star with P=1.16 days. Clumpy ring JET JET

An equatorial dense and clumpy ring Necklace Planetary nebula SN 1987A Supernova remnant MyCn 18 Planetary nebula

Supernova 1987A evolution (Philipp Podsiadlowski et al.) and the rings (Soker et al.) require binary merger. Inner ring in 2004 (HST) The 3 rings in 1994 (HST)

The 3 rings in 1994 Eta Carinae Inner ring in 2004 The Necklace planetary nebula A binary central star with P=1.16 days planetary nebulae

MyCn18 planetary nebula (Form Sahai et al and O Connor et al.). JET JET

(Form David Jones et al. 2015, Last Friday) Fig. 2. HST images of Hen 2-161 (left, see also Sahai et al. 2011) and The Necklace (right; Corradi et al. 2011) highlighting their remarkably similar appearances (elongated with knotty waists).

* The outer rings of 1987A and Eta Carinae were shaped by jets. * Inner ring: Our proposal: Such A main rings sequence are formed companion in a synchronized accretes mass and systems launches opposite jets (in some planetary (companion outside the envelope), the companion but is during a WD) a Darwin unstable phase. nebulae and in symbiotic nebulae

* The outer rings of 1987A and Eta Carinae were shaped by jets. * Inner ring: Our proposal: Such rings are formed in a synchronized systems (companion outside the envelope), but during a Darwin unstable phase.

New results of Full 3D simulations of jets. (Muhammad Akashi et al., 2015). Spherical slow wind + wide jets (half opening angle of 50 degrees). Jet speed 1000 km/s. The interaction takes place very close to the binary system, when photons have no time to diffuse out. It is not the regular momentum or energy conserving cases. Distance in cm

Instabilities in the plane will lead to the formation of clumps

Instabilities in the plane will lead to the formation of clumps

Total (Kinetic +radiation) log(e/erg) Rapid mass accretion 1: See poster by Kashi & Soker 0 1 Log(time/day) Suggestion (Soker & Kashi 2012): Some bipolar planetary nebulae and pre-pne were formed by ILOTs. 3 4

Rapid mass accretion 2: Jones, Boffin, Rodriguez-Gil, Wesson, Corradi, Miszalski, & Mohamed (June 2015) support the claim of rapid accretion as suggested by the jet-feedback mechanism: "... all main-sequence companions, of planetary nebulae... display this [envelope] inflation.... Probably related to rapid accretion, immediately before the recent common-envelope phase,.. "

Other Objects shaped by jets. Note Type Ia Supernova Remnants NGC 6302 MyCn 18 IC 418 Kepler SN remnant (Type Ia) SN 1987A G299-2.9 SN remnant M&MS 0.01M e yr -1 Young star S106 IR in star forming region Hb 5 Eta Carinae Accretion rate onto a main sequence companion (via a disk with jets) M&MS 1M e yr -1

Planetary nebulae Remnants of supernovae Ia Jets might be common in pre - SN Ia, (Tsebrenko & Soker 2013, 2015a) SNIP: Supernovae Inside Planetary nebulae See poster by Danny Tsebrenko & Soker

Pleasantness Review: The role of jets: from common envelope to nebulae (1) What we see (2) What we see and simulate (3) What we simulate but don t see (4) What we don t see and did not simulate yet.

We suggest that core collapse supernovae are exploded by jets launched from the newly formed neutron star (or black hole). This is the jittering-jets model.

We suggest that core collapse supernovae are exploded by jets launched from the newly formed neutron star (or black hole). This is the jittering-jets model. A 2D axi-symmetric simulation with 2 jetslaunching episodes. PhD project of Oded Papish

We suggest that core collapse supernovae are exploded by jets launched from the newly formed neutron star (or black hole). This is the jittering-jets model. A 2D axi-symmetric simulation with 2 jetslaunching episodes. PhD project of Oded Papish Main challenge: To supply angular momentum to form accretion disks. PhD of Avishai Gilkis: Convection in pre-collapse core and instabilities lead to stochastic accretion disk formation, and to jittering jets.

A simulation of 3-pairs of opposite jets launched within 0.15 seconds inside a core of a massive star just after the formation of the new neutron star. A full 3D simulation. We argue that such jets explode massive stars. PhD of Oded Papish

(1) What we see (2) What we see and simulate (3) What we simulate but don t see Pleasantness Review: The role of jets: from common envelope to nebulae (4) What we don t see and did not simulate yet: Jets during the common envelope phase, and the grazing envelope evolution (GEE).

RGB, AGB, Massive giant Secondary E bind α CE GM a core 2 final at 2 a only 0.5 E has been released, at 4 a only 0.25 E M final bind final bind. Not enough envelope mass to take angular momentum and energy!! (See Soker, N. 2013, NewA, 18, 18 for mor edetails on the problem with α ). CE

From Jan Staff&

Jets: Can be launched outside and inside the envelope RGB, AGB, Massive giant Secondary Jets are launched and remove the envelope (neutron stars and main sequence, but not white dwarfs). (Soker, N. 2014, accepted by astro-ph; arxiv:1404.5234 ) Final common envelope process by migration and accretion from circumbinary gas, as in young stars. ** Outcomes: (1) More mergers at the end of the CE (might lead to a Type Ia supernova in case of a WD companion). (2) In some cases when jets are efficient in removing gas, a Grazing Envelope Evolution (GEE).

Summary: From well observed jet-shaping of nebulae around stars, and in clusters of galaxies, where energy is deposited by jets, we argue that jets play major roles in other cases. Issue / Process Common envelope parameter Grazing envelope evolution (GEE) Supernova Ia Remnants Core-collapse supernovae α CE Very high accretion rates to a companion main sequence star Most others Parameter commonly used Never heard of. So, see Soker, N., 2015, ApJ, 800, 114 Four different other scenarios By neutrinos Not possible My view which is strongly supported by Problematic. Instead use Jets and migration (but no jets for WDs!!) Takes place in many cases The core degenerate scenario: SNIP (Danny Tsebrenko) Neutrino mechanisms have a generic problem. Explosion by jets 0.01-1 Mo/yr Shiber, Schreier, Soker (2015), astro-ph, accepted my wife and three kids Orsola de Marco (but she doesn t know it yet) my psychiatrist The clerk in charge of early retirement in the Technion. All of the above