Title: The neutron radius of 208Pb and neutron star structure.
1The neutron radius of 208Pb and neutron star
structure.
- http//www.astro.cornell.edu/shami/guitar/
guitar nebula, neutron star bow wave
2Outline
- The big picture
- Neutrons in nuclei
- Neutron stars and nuclear matter
- Conclusion
3Phase diagram of waterThe state of matter
depends on pressure, temperature, and density.
4New phases of matter
- We see in the case of water that new phases of
matter appear at pressures far from our normal
experience, for example, Ice XI at 1 million
atmospheres. - What would happen to matter if we could continue
to crush it under high pressure? - What is the phase diagram of matter under extreme
conditions?
5World map in 1532 Typus Cosmographicus
Universalis, S. Grynaeus/H. Hoblein/S. Münster,
6Danger in new territories!What we dont know for
a fact we can compensate for by imagination.
7Physical properties of systems containing nuclear
matter
8Phase diagram of nuclear matter
9Nuclei and Neutron Stars
- Nuclei are the central cores of atoms. Almost all
the visible mass in the universe is in protons
and nuclei. - Neutron stars are the collapsed iron cores of
massive stars ( stars with masses greater than 8
solar masses). These stars no longer generate
energy internally by nuclear fusion, although
they can be the sites of huge bursts of energy.
10Equation of state (eos) connects nuclear physics
and neutron stars
11Interactions affect the EOS
12Measuring matter in small boxes
- We measure the angle of scatter, a, of high
energy electrons ( E 1 GeV) from nuclei. - R 5.5 x 10-13 cm, dR 0.2 F/ Pg. ,1F 10-13 cm
- Pg. photon momentum in GeV
13Electron Scattering gives very precise
information on charge distributions in the nucleus
14The neutron distribution is not so well known as
the proton .
- Photons couple poorly to neutral neutrons
compared to the charged protons. - However, electrons interact with nucleons via the
weak interaction too. - The Z0 boson of the weak interaction interacts
several times more strongly with neutrons than
with protons. - Weak interaction scattering is a tough
experimental challenge.
15Rn Rp for two different theories of the nuclear
mean field
16Look for helicity asymmetry in electron scattering
17Helicity dependent Scattering Asymmetry for
Polarized Electrons
18Aerial View of JLab Accelerator
19Hall A Spectrometers
20High Power Cryogenic Lead Target Built and tested
at CSLA
21High rate integrating detector
22What keeps a star stable?
23Formation of Neutron stars
24Quantum Ideal Gas
25Final state of a massive neutron star
26A 12 km radius neutron star in Los Angeles
27Complementary Laboratories
28Nuclear parameter dependence of N-star radius
calculations
29Neutron Star Structure
30Some statistics of n-stars
- More than 1100 n-stars have been detected,
primarily as pulsars - The masses tend to center about 1.4 solar masses
and the limits expected are 0.2but the creation mechanism may fix the mass at
1.4 Msun - Radius determinations are difficult and
controversial in the 7 to 15 km range - Reliable measurements of M and R would place
severe restraints on the EOS - Pulsars have high velocities, avg 450 km/s
indicating an asymmetrical core collapse
31Are there areas of the phase diagram that have
never been populated in the history of the
Universe?