Topological Charge Distribution and $CP^1$ Model with $θ$ Term

Physics – High Energy Physics – High Energy Physics - Lattice

Scientific paper

Rate now

  [ 0.00 ] – not rated yet Voters 0   Comments 0

Details

22 pages, plaintex, one table, seven figures

Scientific paper

10.1143/PTP.95.175

The two dimensional $CP^1$ model with $\theta$ term is simulated. We compute the topological charge distribution $P(Q)$ by employing the ``set method" and ``trial function method", which are effective in the calculations for very wide range of $Q$ and large volume. The distribution $P(Q)$ shows the Gaussian behavior in the small $\beta$ (inverse coupling constant) region and deviates from it in the large $\beta$ region. The free energy and its moment are calculated as a function of $\theta$. For small $\beta$, the partition function is given by the elliptic theta function, and the distribution of its zeros on the complex $\theta$ plane leads to the first order phase transition at $\theta=\pi$. In the large $\beta$ region, on the other hand, this first order phase transition disappears, but definite conclusion concerning the transition is not reached due to large errors.

No associations

LandOfFree

Say what you really think

Search LandOfFree.com for scientists and scientific papers. Rate them and share your experience with other people.

Rating

Topological Charge Distribution and $CP^1$ Model with $θ$ Term does not yet have a rating. At this time, there are no reviews or comments for this scientific paper.

If you have personal experience with Topological Charge Distribution and $CP^1$ Model with $θ$ Term, we encourage you to share that experience with our LandOfFree.com community. Your opinion is very important and Topological Charge Distribution and $CP^1$ Model with $θ$ Term will most certainly appreciate the feedback.

Rate now

     

Profile ID: LFWR-SCP-O-677700

  Search
All data on this website is collected from public sources. Our data reflects the most accurate information available at the time of publication.