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Complex heavy-quark potential at finite temperature from lattice QCD
Alexander Rothkopf1, Tetsuo Hatsuda, Shoichi Sasaki
1Department of Physics, The University of Tokyo, Tokyo 113-0031, Japan.
Physical Review Letters
|June 12, 2012
Summary
We calculated the complex potential between heavy quarks at high temperatures for the first time. An imaginary part emerges above the critical temperature, indicating heavy quarkonium melting in the quark-gluon plasma.
Area of Science:
- High Energy Physics
- Quantum Chromodynamics
- Statistical Mechanics
Background:
- Heavy quark systems are crucial for understanding the quark-gluon plasma.
- The behavior of heavy quarkonia across the deconfinement transition is not fully understood.
Purpose of the Study:
- To calculate the complex potential between a heavy quark and antiquark at finite temperature.
- To investigate the properties of heavy quarkonia in the quark-gluon plasma.
Main Methods:
- Lattice Quantum Chromodynamics (LQCD) calculations.
- Utilizing the spectral function of the thermal Wilson loop.
- Analyzing the real and imaginary parts of the potential at various separations.
Main Results:
- First-ever calculation of the complex potential between heavy quarks at finite temperature.
- Confirmation of a non-zero imaginary potential above the critical temperature (Tc).
- The imaginary potential increases with separation distance (r).
Conclusions:
- The imaginary potential signifies interactions with the gluonic environment.
- These interactions are key to the melting of heavy quarkonia in the quark-gluon plasma.
- Provides new insights into the properties of deconfined matter.
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