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Complex Plasmas as a Model for the Quark-Gluon-Plasma Liquid

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Presentation on theme: "Complex Plasmas as a Model for the Quark-Gluon-Plasma Liquid"— Presentation transcript:

1 Complex Plasmas as a Model for the Quark-Gluon-Plasma Liquid
Markus H. Thoma* Max-Planck-Institute for Extraterrestrial Physics Strongly Coupled Plasmas Complex Plasmas Applications to the Quark-Gluon Plasma * Supported by DLR (BMBF)

2 Strongly Coupled Plasmas
Plasma = ionized gas, 99% of visible matter in Universe Plasmas generated by high temperatures, electric fields, or radiation Classifications: Non-relativistic – relativistic plasmas (pair plasmas, QGP) Classical – quantum plasmas (white dwarfs, QGP) Ideal – strongly coupled plasmas (complex plasmas, QGP)

3

4 Coulomb coupling parameter
Q: charge of plasma particles d: inter particle distance T: plasma temperature Ideal plasmas: G << 1 (most plasmas: G < 10-3) Strongly coupled plasmas: G > O (1) Examples: ion component in white dwarfs, high-density plasmas at GSI Non-perturbative description, e.g., molecular dynamics One-component plasma, pure Coulomb interaction (repulsive): G > 172 g Coulomb crystal

5 Debye screening g Yukawa systems
Additional parameter: k = d/lD Liquid phase: G > O (1) Purely repulsive interaction g no gas-liquid transition, only supercritical fluid

6 2. Complex Plasmas Dusty or complex plasmas = multi component plasmas containing ions, electrons, neutral gas, and microparticles, e.g., dust Example: low temperature neon plasma in a dc- or rf discharge

7 Injection of microparticles with diameter
1 – 10 mm High electron mobility g microparticles collect electrons on surface g large negative charge: Q = 103 – 105 e Inter particle distance about 200 mm g G >> 1 g plasma crystal (predicted 1986, discovered 1994 at MPE) Observation: illumination by laser sheet and recorded by CCD camera

8 Melting of plasma crystal by
pressure reduction less neutral gas friction gtemperature increase gdecrease of Coulomb coupling parameter G = Q2/(dT)

9 Quantitive analysis of equation of state and determination of G:
pair correlation function Crystal: long range order sharp peaks at the nearest neighbors, next to nearest neighbors and so on Liquid: short range order (incompressibility) gonly one clear peak corresponding to inter particle distance plus one or two broad and small peaks Gas: no order gno clear peaks

10 Gravity has strong influence on microparticles gmicrogravity experiments

11 Applications of complex plasmas:
1. Model system for phase transitions, crystallization, dynamical behavior of liquids and plasmas on the microscopic level 2. Astrophysics: comets, interstellar plasmas, star and planet formation, planetary rings, … 3. Technology: plasma coating and etching, e.g. microchip production, problem: dust contamination

12 3. Applications to the Quark-Gluon Plasma
Estimate of interaction parameter C = 4/3 (quarks), C = 3 (gluons) T = 200 MeV g aS = d = 0.5 fm Ultrarelativistic plasma: magnetic interaction as important as electric G = 1.5 – 6 g QGP Liquid? RHIC data (hydrodynamical description with small viscosity, fast thermalization) indicate QGP Liquid Attractive and repulsive interaction g gas-liquid transition at a temperature of a few hundred MeV

13 Static structure function (Fourier transform of pair correlation function)
g experimental and theoretical analysis of liquids Hard Thermal Loop approximation (T >> Tc): interacting gas QCD lattice simulations g QGP liquid?

14 Strongly coupled plasmas g cross section enhancement
Reason: Coulomb radius, rC = Q2/E, larger than Debye screening length lD = 1/mD g modification of Coulomb scattering theory g enhancement of ion-microparticle interaction (ion drag force) QGP: rC /lD = 1 – 5 g parton cross section enhancement by factor 2 – 9 small mean free path l (corresponding to small viscostity h ~ l) and fast thermalization. Additional cross section enhancement by non-linear and non-perturbative effects Implication: enhancement of collisional energy loss, suppression of radiative energy loss by LPM effect (formation time) g jet quenching

15 Conclusions Strongly coupled plasmas are of increasing importance in
fundamental research as well as technology QGP and complex plasmas are important examples of strongly coupled plasmas QGP is the most challenging strongly coupled plasma Complex plasmas can easily be studied and used as a model for the QGP (phase transitions, correlation functions, cross sections, …) RHIC and ISS provide very important information on strongly coupled plasmas


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