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Title: Hydrodynamics and critical slowing down

Abstract

We will introduce an effective theory which extends hydrodynamics into a regime where the critical slowing down would otherwise make hydrodynamics inapplicable.

Authors:
 [1];  [2]
  1. Univ. of Illinois, Chicago, IL (United States)
  2. Massachusetts Inst. of Technology (MIT), Cambridge, MA (United States)
Publication Date:
Research Org.:
Univ. of Illinois, Chicago, IL (United States); Massachusetts Inst. of Technology (MIT), Cambridge, MA (United States)
Sponsoring Org.:
USDOE Office of Science (SC), Nuclear Physics (NP) (SC-26)
OSTI Identifier:
1501426
Grant/Contract Number:  
FG02-01ER41195
Resource Type:
Accepted Manuscript
Journal Name:
Nuclear Physics. A
Additional Journal Information:
Journal Volume: 967; Journal Issue: C; Journal ID: ISSN 0375-9474
Publisher:
Elsevier
Country of Publication:
United States
Language:
English
Subject:
71 CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS; Fluid Flow; Hydrodynamics; Slowing-Down

Citation Formats

Stephanov, M., and Yin, Y. Hydrodynamics and critical slowing down. United States: N. p., 2017. Web. doi:10.1016/j.nuclphysa.2017.06.051.
Stephanov, M., & Yin, Y. Hydrodynamics and critical slowing down. United States. doi:10.1016/j.nuclphysa.2017.06.051.
Stephanov, M., and Yin, Y. Mon . "Hydrodynamics and critical slowing down". United States. doi:10.1016/j.nuclphysa.2017.06.051. https://www.osti.gov/servlets/purl/1501426.
@article{osti_1501426,
title = {Hydrodynamics and critical slowing down},
author = {Stephanov, M. and Yin, Y.},
abstractNote = {We will introduce an effective theory which extends hydrodynamics into a regime where the critical slowing down would otherwise make hydrodynamics inapplicable.},
doi = {10.1016/j.nuclphysa.2017.06.051},
journal = {Nuclear Physics. A},
number = C,
volume = 967,
place = {United States},
year = {2017},
month = {9}
}

Journal Article:
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Figures / Tables:

Fig. 1. Fig. 1. : The spectrum of linearized Hydro+. The conventional hydrodynamics is valid in Regime I, for as long as the relaxation ratemore » $Γ$ is faster than the sound oscillation rate. The sound attenuation coefficient $γ$L ∼ ζ/w ∼ $c$$^2_s$/$Γ$ diverges as $Γ$→ 0. In Regime II the sound is the fastest mode and its attenuation rate is slower.« less

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