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Thermal width of the upsilon at large 't Hooft coupling
Jorge Noronha1, Adrian Dumitru
1Department of Physics, Columbia University, 538 West 120 Street, New York, New York 10027, USA.
The heavy quark potential in a strongly coupled plasma gains an imaginary part at finite temperatures, causing heavy quarkonia states to acquire a thermal width. This finding predicts Upsilon suppression in heavy-ion collisions, offering a way to estimate initial plasma temperatures.
Area of Science:
- High-energy physics
- Quantum chromodynamics
- String theory
Background:
- The behavior of strongly coupled plasma is crucial for understanding heavy-ion collisions.
- Heavy quarkonia states are sensitive probes of the plasma environment.
Purpose of the Study:
- To investigate the thermal width of heavy quarkonia in a strongly coupled plasma using the anti-de Sitter/conformal field theory correspondence.
- To explore the implications of the heavy quark potential's imaginary part for experimental observations.
Main Methods:
- Utilizing the anti-de Sitter/conformal field theory (AdS/CFT) correspondence.
- Analyzing the dual gravity description of a strongly coupled plasma with heavy quarks.
- Examining thermal fluctuations of classical strings in the bulk.
Main Results:
- The heavy quark potential develops an imaginary part at finite temperatures.
- Deeply bound heavy quarkonia states acquire a small, non-zero thermal width under specific conditions (large 't Hooft coupling and large number of colors).
- Thermal fluctuations of the classical string's bottom in the bulk contribute to the imaginary part.
Conclusions:
- The study predicts a significant suppression of Upsilon mesons in heavy-ion collisions.
- The observed suppression can potentially be used to estimate the initial temperature of the strongly coupled plasma.
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