Nonperturbative zero modes in the Kraichnan model for turbulent advection

Physical Review E - Statistical Physics, Plasmas, Fluids, and Related Interdisciplinary Topics

Volumn 55, Issue 4, 1997, Pages R3836-R3839

  Gat, Omri ^a   L'vov, Victor S ^a   Podivilov, Evgenii ^a   Procaccia, Itamar ^a  

^a WEIZMANN INSTITUTE OF SCIENCE   (Israel)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 0001002879     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.55.R3836     Document Type: Article

References (12)

1. R.H. Kraichnan, Phys. Fluids PFLDAS11, 945(1968).
2. R.H. Kraichnan, Phys. Rev. Lett. PRLTAO72, 1016(1994).
3. K. Gawedzki and A. Kupiainen, Phys. Rev. Lett. PRLTAO75, 3834(1995).
4. M. Chertkov, G. Falkovich, I. Kolokolov, and V. Lebedev, Phys. Rev. E PLEEE852, 4924(1995).
5. R.H. Kraichnan, V. Yakhot, and S. Chen, Phys. Rev. Lett. PRLTAO75, 240(1995).
6. A. Fairhall, O. Gat, V.S. L'vov, and I. Procaccia, Phys. Rev. E PLEEE853, 3518(1996).
7. E.S.C. Ching, V.S. L'vov, and I. Procaccia, Phys. Rev. E PLEEE854, 4520R (1996).
8. E.S.C. Ching, V.S. L'vov, E. Podivilov, and I. Procaccia, Phys. Rev. E PLEEE854, 6364(1996).
9. There are other possibilities that make (Formula presented) relevant. One is putting on a fixed gradient (see 10) and another is to consider the fusion of three points in higher-order correlations; see 6 .
10. B. Shraiman and E. Siggia, C. R. Acad. Sci. II, Mech. Phys. Chim. Sci. Univers. Sci. Terre CRAMED321, 279(1995).
11. V.S. L'vov and I. Procaccia, Phys. Rev. Lett. PRLTAO76, 2898(1996).
12. R.H. Kraichnan (private communication).