MICHAEL ROTONDO* R. RUFFINI*°^ S-S. XUE*° *DEPARTMENT OF PHYSICS AND ICRA, UNIVERSITY OF ROME “SAPIENZA” °ICRANET, PESCARA ^ICRANET,UNIVERSITY OF NICE.

Slides:



Advertisements
Similar presentations
Radioactivity.
Advertisements

Stellar Structure Section 6: Introduction to Stellar Evolution Lecture 18 – Mass-radius relation for black dwarfs Chandrasekhar limiting mass Comparison.
X X X X X10 14.
Susan CartwrightOur Evolving Universe1 The Deaths of Stars n What happens to stars when the helium runs out? l l do they simply fade into oblivion? l l.
Stellar Evolution Describe how a protostar becomes a star.
End States Read Your Textbook: Foundations of Astronomy
"Now I am become Death, the destroyer of worlds." Robert Oppenheimer after the first test of the atomic bomb.
Neutron Stars and Black Holes
The neutron radius of 208 Pb and neutron star structure. guitar nebula, neutron star bow wave.
Unstable Nuclei and Radioactive Decay
Chapter 30 Nuclear Physics
BASIC CONCEPTS.  Summary-1  The net nuclear charge in a nuclear species is equal to + Ze, where Z is the atomic number and e is the magnitude.
Electron-positron pair productions in gravitational collapses In collaboration with Wen-Biao Han, & Remo Ruffini ICRANet & Physics Department, University.
Coulomb Interaction in quantum structures - Effects of
Neutron Stars and Black Holes PHYS390: Astrophysics Professor Lee Carkner Lecture 18.
P460 - Quan. Stats. III1 Nuclei Protons and neutrons in nuclei separately fill their energy levels: 1s, 1p, 1d, 2s, 2p, 2d, 3s…………… (we’ll see in 461 their.
Modern Physics LECTURE II.
Nuclear Force and Particles
Nuclear Energy. Nuclear energy is all around us and can be used for medical purposes. Nuclear energy is when an atom is split and releases energy or particles.
Wednesday, Mar. 23, 2005PHYS 3446, Spring 2005 Jae Yu 1 PHYS 3446 – Lecture #14 Wednesday, Mar. 23, 2005 Dr. Jae Yu Elementary Particle Properties Forces.
Particle Physics Professor Kay Kinoshita University of Cincinnati.
 14.1 The Uncertainty Principle  14.2 The Effect of Observation  14.4 Quantum Reality  14.5 Toward a Post-Newtonian Worldview  14.6 Observing Atomic.
Atoms and Their Structure Chapter 4. Atoms Elements are made of particles called atoms Atoms are the smallest pieces of matter that contain all the properties.
Modern Physics Modern Physics Global Mechanics Global Mechanics Astrophysics Astrophysics Cosmology and The Little Bang Cosmology and The Little Bang.
Subatomic Physics Chapter Properties of the Nucleus The nucleus is the small, dense core of an atom. Atoms that have the same atomic number but.
1 Astro-Particle Physics 3 Acceleration mechanisms Manfred Jeitler.
She-Sheng XUE ICRANet, Pescara, Italy how the gravitational energy transfers to the electromagnetic energy for Gamma-Ray-Bursts. 1) Electron-positron production,
Changes in the Nucleus Objectives: 1. Describe the changes that accompany nuclear reactions. 2. Define radioactivity. Key Terms: nuclear reaction, strong.
Chapter 12.1 Learning Goals  Apply an understanding of electric charge to describe the structure of atoms.  Identify and describe particles which comprise.
Alpha Decay A Helium- 4 nucleus (two protons and two neutrons). Is produced by nuclear fission Massive nucleus breaks apart into two less-massive nuclei.
Types of Nuclear Decay. Alpha Decay (α) Emission of an alpha (α) particle which is a Helium nuclide. During an alpha decay, a nucleus is able to reach.
Nuclear Chemistry Chapter 25. What do you think of when you hear Nuclear Chemistry?
Radioactive Decay Radioactivity results from having an unstable nucleus. When these nuclei lose energy and break apart, decay occurs. Radioactive decay.
3-4 Changes in the Nucleus
Black Holes in General Relativity and Astrophysics Theoretical Physics Colloquium on Cosmology 2008/2009 Michiel Bouwhuis.
Living By Chemistry SECOND EDITION Unit 1: ALCHEMY Matter, Atomic Structure, and Bonding.
IB Assessment Statements Topic 13.2, Nuclear Physics Explain how the radii of nuclei may be estimated from charged particle scattering experiments.
Neutron Star. Gravitational Crush The balance point to maintain degenerate matter is 1.4 M . When the mass of the core is greater than 1.4 M , electrons.
Phys 102 – Lecture 27 The strong & weak nuclear forces.
Structure of an Atom. The Three subatomic particles of an atom: Proton Neutron Electron.
Types of Radioactive Decay Kinetics of Decay Nuclear Transmutations
Nuclear Chemistry. ATOMIC REVIEW: Atomic number = # of protons # of neutrons = mass # - atomic # protons & neutrons are in the nucleus.
ELECTROWEAK UNIFICATION Ryan Clark, Cong Nguyen, Robert Kruse and Blake Watson PHYS-3313, Fall 2013 University of Texas Arlington December 2, 2013.
Nuclear Reactions Nuclear Reactions.
What is radioactivity? lecture 9.1 Gamma ray bursts from a star collapsing into a Black Hole.
Some theoretical aspects of Magnetars Monika Sinha Indian Institute of Technology Jodhpur.
Nucleosynthesis in decompressed Neutron stars crust matter Sarmistha Banik Collaborators: Smruti Smita Lenka & B. Hareesh Gautham BITS-PILANI, Hyderabad.
The cosmic connection There is a very close connection between particle physics and astrophysics. I’m going to show two examples: Type II supernovas Dark.
STAAR Ladder to Success Rung 7. – Alpha particles are helium nuclei with low penetrating power; they can be shielded by paper or cloth. – Beta particles.
Chapter 14 Section 14.1.
ELECTROMAGNETIC PARTICLE: MASS, SPIN, CHARGE, AND MAGNETIC MOMENT Alexander A. Chernitskii.
Neutron Stars & Black Holes. Neutron Stars and Black Holes I. Neutron Stars A. Remnant from the collapse of a _________. B. During the core collapse of.
Monday, Feb. 7, 2005PHYS 3446, Spring 2005 Jae Yu 1 PHYS 3446 – Lecture #6 Monday, Feb. 7, 2005 Dr. Jae Yu 1.Nature of the Nuclear Force Short Range Nature.
Monday, Oct. 2, 2006PHYS 3446, Fall 2006 Jae Yu 1 PHYS 3446 – Lecture #8 Monday, Oct. 2, 2006 Dr. Jae Yu 1.Nuclear Models Shell Model Collective Model.
Aim: Why do fission and fusion reactions release so much energy? Essential Questions : Compare and contrast nuclear fission with fusion. Distinguish between.
NUCLEAR ENERGY. The daughter nuclei in the reaction above are highly unstable. They decay by beta emission until they reach stable nuclei.
The Effects of Gravity. Identify the source of gravitational forces and fields Identify the source of gravitational forces and fields. Identify the strongest.
Nuclear Stability and Decay 1500 different nuclei are known. Only 264 are stable and do not decay. The stability of a nucleus depends on its neutron-to-
Alpha Radiation. Label the helium atom and fill in the table: P_____ N_____ E_____ { N_____ ParticleMassCharge Proton Neutron Electron eutron lectron.
Unstable Nuclei and Radioactive Decay. Radioactivity (Radioactive decay) The process by which some substances spontaneously emit radiation. Radioactive.
NUCLEAR CHEMISTRY Chapter 20. Nuclear Chemistry Radioactivity is the emission of subatomic particles or high- energy electromagnetic radiation by the.
Stars, Galaxies, and the Universe Section 2 Section 2: Stellar Evolution Preview Objectives Classifying Stars Star Formation The Main-Sequence Stage Leaving.
She-Sheng XUE ICRANet, Pescara, Italy How the gravitational energy transfers to the electromagnetic energy for Gamma-Ray-Bursts. 1)Electron-positron production,
Fulfilling Einstein’s Dream Institute for Advanced Study
Middleweight Stars 4-12 solar masses.
8.3. The Electron Gas in Metals
From Atoms, to Nucleons, to Quarks
ATOMS CHEM-IS-TRY.
Chapter 14 Section 14.1.
Three kinds of particle emission
Presentation transcript:

MICHAEL ROTONDO* R. RUFFINI*°^ S-S. XUE*° *DEPARTMENT OF PHYSICS AND ICRA, UNIVERSITY OF ROME “SAPIENZA” °ICRANET, PESCARA ^ICRANET,UNIVERSITY OF NICE “SOPHIA ANTIPOLIS” THIRD STUECKELBERG MEETING JULY , PESCARA, ITALY

The energy source as crucial factor in the understanding of astrophysical phenomena

Some astrophysical open problems The problem of the almost known equations of state for neutron stars which are not able to reproduce the observations in millisecond binary pulsars The problem of explaining the energetics of the emission of the remnant during the collapse to a neutron star The problem of formation of the supercritical fields during the collapse to a black hole It is our opinion that the solution of these problems could find their natural explanation from a yet unexplored field : the electro-dynamical structure of a neutron star. In this work we outline a few crucial ideas of how a Thomas-Fermi approach to neutron stars can indeed represent an important step in identify this crucial feature.

Thomas-Fermi model

White Dwarfs and Neutron Stars as Thomas-Fermi systems

The relativistic Thomas-Fermi equation

The essential role of the non-point-like nucleus

Electrodynamics of nuclear matter in bulk n, p, e

Electromagnetic components Proton component Poisson equation Electron component

The dimensionless Thomas-Fermi equation

The neutron component and the A-Np relation

Generalized A-Np relation and the penetration of electrons inside the core

The ultra-relativistic approximation

Coulomb potential energy and electric field

The electric field and the muon/pion production

Gravitational and electrodynamical stability

The inapplicability of the free test particle approximation

Neutral nuclear matter cores vs supercharged ones

Consequences for Neutron Stars

Different proton profiles

Conclusions 1- The requirement of beta decay equilibrium appears to be necessary for obtaining from first principles the phenomenological relations between A and Np adopted in superheavy nuclei. 2-The Thomas-Fermi equation is a good example of the possibility that collective effects of relativistic quantum statistics leads to electric fields in astrophysical situations with values much larger than the ones suggested by the test particle approximation. 3-The possibility of having stable massive cores describable based solely on gravitational, electromagnetic and weak interactions and relativistic quantum statistics opens a whole new scenario for the study of neutron star configurations close to their critical mass and the subsequent approach to process of gravitational collapse to a Kerr-Newman black hole.

References [1] J. Ferreirinho, R. Ruffini, L. Stella, Phys. Lett. B 91, (1980) 442. [2] R.Ruffini, M. Rotondo, S.S. Xue, Int. Journal of Modern Phys. D Vol. 16, No. 1 (2007) 1-9. [3] A.B. Migdal, D.N. Voskresenskii, V.S. Popov, Sov. Phys. JETP 45 (3), (1977) 436. [4] R.Rotondo, R. Ruffini, S.S.Xue, in the “Proceedings of the fourth Italian-Sino Workshop on Relativistic Astrophysics”, C.L. Bianco, S.S. Xue (eds.), AIP Conf. Proc. 966, 147 (2008). [5] B. Patricelli, R.Rotondo, R. Ruffini, in the “Proceedings of the fourth Italian-Sino Workshop on Relativistic Astrophysics”, C.L. Bianco, S.S. Xue (eds.), AIP Conf. Proc. 966, 143 (2008). [6] J. Madsen, Phys. Rev. Lett., Vol. 100, (2008). [7] R.Ruffini, M. Rotondo, S.S. Xue, submitted to Phys. Rev. Lett. (2008).