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Hadronic density of states from string theory.
Leopoldo A Pando Zayas1, Diana Vaman
1Michigan Center for Theoretical Physics, University of Michigan, Ann Arbor, Michigan 48109-1120A, USA. lpandoz@umich.edu
Physical Review Letters
|October 4, 2003
Summary
This study calculates the partition function for hadronic states in N=1 super Yang-Mills (SYM) theory, revealing a Hagedorn density of states. A semiclassical string approximation confirms this Hagedorn behavior for confining gauge theories with supergravity duals.
Area of Science:
- String Theory
- Quantum Field Theory
- High-Energy Physics
Background:
- The Maldacena-Nùñez embedding provides a framework to study N=1 super Yang-Mills (SYM) theory using string theory and supergravity duals.
- Understanding the behavior of gauge theories at finite temperatures is crucial for comprehending phenomena like the Hagedorn transition.
Purpose of the Study:
- To perform an exact calculation of the finite temperature partition function for hadronic states in a specific limit of N=1 SYM.
- To propose and analyze a semiclassical string approximation for the finite temperature partition function of confining gauge theories with supergravity duals.
Main Methods:
- Exact calculation of the partition function for hadronic states in the Penrose-Güven limit of the Maldacena-Nùñez embedding.
- Developing a semiclassical string approximation by expanding around classical solutions with temporal windings.
Main Results:
- The study establishes that the N=1 SYM theory exhibits a Hagedorn density of states.
- The semiclassical approximation reveals a hadronic energy density of states of a Hagedorn type.
- The coefficient in the Hagedorn density is determined by the gauge theory string tension, consistent with confining theories.
Conclusions:
- The proposed semiclassical approximation effectively captures the Hagedorn behavior of hadronic states in confining gauge theories with supergravity duals.
- This approach provides insights into the states of pure N=1 SYM theory without projecting onto states of large U(1) charge.