Studies of Liquid Turbulence Using Double-Pulsed Particle Correlation

Author(s):  
R. J. Adrian ◽  
P. W. Offutt ◽  
Z.-C. Liu ◽  
T. J. Hanratty ◽  
C. C. Landreth
Keyword(s):  
2007 ◽  
Vol 16 (07n08) ◽  
pp. 1982-1987
Author(s):  
◽  
N. N. AJITANAND

Recent experimental investigations have focussed on the abnormal spatial distribution of away side jet fragments as signals of significant medium induced effects. A variety of theoretical models including recent string-theory based efforts have supported the notion of Mach Cone like effects in the low viscosity QGP fluid. However, the presence of significant flow fields may deflect the fragmentation direction producing a significantly differing type of jet topology from that of the Mach cone. Three particle correlation functions constitute a powerful method whereby the predominance of one or the other type of mechanism can be differentiated. In this work the use of such an approach will be demonstrated via simulations and the results of its application to RHIC data will be presented.


2003 ◽  
Vol 29 (1) ◽  
pp. 13-21 ◽  
Author(s):  
Csaba Peltz ◽  
András Baranyai ◽  
Ariel A. Chialvo ◽  
Peter T. Cummings

1995 ◽  
Vol 583 ◽  
pp. 395-400 ◽  
Author(s):  
B. Erazmus ◽  
R. Lednicky ◽  
V.L. Lyuboshitz ◽  
L. Martin ◽  
D. Nouais ◽  
...  

1979 ◽  
Vol 24 (15) ◽  
pp. 535-539 ◽  
Author(s):  
N. Suzuki ◽  
S. Suzuki

2013 ◽  
Vol 8 (4) ◽  
pp. 25-34
Author(s):  
Oleg Shevchenko ◽  
Nikolay Vinokurov

The startup from noise problem in SASE FELs is usually treated in linear approximation. In this case amplification of initial density fluctuations may be calculated, and averaging over initial conditions may be fulfilled explicitly. In general nonlinear case the direct averaging is not applicable. During last years we developed the approach based on the BBGKY hierarchy for the n-particle distribution functions. The interaction of particles in FEL is retarded. Nevertheless, using special time-coordinate transformation, it is possible to eliminate the interaction lag and then to write down the BBGKY equations. Similar to plasma physics, the equations may be truncated after the second one (for the two-particle correlation function). Using this approach we consider several particular cases which illustrate some peculiar features of the SASE FEL operation


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