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FIAS Scientific Report 2011 - Frankfurt Institute for Advanced Studies ...

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Applications of a chiral SU(3) model <strong>for</strong> the binding energies of nuclei, driplines of nuclei and<br />

hyper-nuclei, and the mass-radius relation of neutron stars<br />

Collaborators: T. Schürhoff 1,2 , S. Schramm 1 , C. Samanta 3,4<br />

1 <strong>Frankfurt</strong> <strong>Institute</strong> <strong>for</strong> <strong>Advanced</strong> <strong>Studies</strong>, 2 <strong>Institute</strong> <strong>for</strong> Theoretical Physics (ITP), Goethe University, <strong>Frankfurt</strong>, 3 Saha<br />

<strong>Institute</strong> of Nuclear Physics, Kolkata, India, 4 Department of Physics, Virginia Commonwealth University, Richmond,<br />

VA, USA<br />

One of the major goals in contemporary nuclear physics is the determination of the equation of state of hadronic<br />

matter. This will allow <strong>for</strong> a great many applications, both on the experimental and theoretical side, <strong>for</strong> example<br />

in supernova simulations. In order to theoretically study hadrons, we look at the binding energies of nuclei and<br />

compare the results of our model with experimental results. We can reproduce the binding energies of nuclei<br />

over the whole nuclide chart up to 0.7 % and work to improve our fitting parameters.<br />

We also study the driplines of normal and hyper-nuclei and extrapolate to regions not experimentally accessible<br />

at the moment. This is of interest <strong>for</strong> upcoming experiments at GSI. We find that the extrapolation of drip-lines<br />

is very much model dependent.<br />

In addition, we study the effect of the change of the fitting parameters of our model <strong>for</strong> the mass-radius relation<br />

of neutron stars. There, parameter changes only have a very marginal effect.<br />

Figure 1: The dripline determination of the hyper-nucleus Magnesium 40 containing one Λ hyperon. Plotted<br />

is the the de<strong>for</strong>mation β versus the total binding energy in MeV. The nucleus will move to the de<strong>for</strong>mation<br />

with the lowest binding energy, i.e. the minimum. The dripline is that nucleus <strong>for</strong> which the addition of further<br />

particles, here neutrons, will no longer yield an increase in binding energy.<br />

Related publications in <strong>2011</strong>:<br />

1) S. Schramm, V. Dexheimer, R. Negreiros, T. Schürhoff, Nuclear matter, nuclei and neutron stars in hadron<br />

and and quark-hadron models, in Symposium on Advances in Nuclear Physics in our time, Goa, India, 28.<br />

Nov. - 2. Dec. 2010, <strong>2011</strong>. arXiv:1102.2325 [nucl-th].<br />

2) S. Schramm, R. Negreiros, J. Steinheimer, T. Schürhoff, V. Dexheimer, Properties and stability of hybrid<br />

stars, in Strangeness in Quark matter (SQM<strong>2011</strong>), Krakow, Poland, 18.-24. Sept. <strong>2011</strong>. arXiv:1112.1853<br />

[astro-ph.SR].<br />

61

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