scholarly journals Experimental observation of three-dimensional non-paraxial accelerating beams

2020 ◽  
Vol 28 (12) ◽  
pp. 17653 ◽  
Author(s):  
L. Li ◽  
Y. Jiang ◽  
P. Jiang ◽  
X. Li ◽  
Y. Qiu ◽  
...  
1986 ◽  
Vol 34 (10) ◽  
pp. 6719-6724 ◽  
Author(s):  
Sung-Ik Lee ◽  
Yi Song ◽  
Tae Won Noh ◽  
Xiao-Dong Chen ◽  
James R. Gaines

2002 ◽  
Vol 577 (1) ◽  
pp. L63-L66 ◽  
Author(s):  
M. R. Brown ◽  
C. D. Cothran ◽  
M. Landreman ◽  
D. Schlossberg ◽  
W. H. Matthaeus

1997 ◽  
Author(s):  
E. Timofeev ◽  
K. Takayama ◽  
P. Voinovich ◽  
E. Timofeev ◽  
K. Takayama ◽  
...  

2016 ◽  
Vol 808 ◽  
pp. 168-188 ◽  
Author(s):  
Beomchan Park ◽  
Yeunwoo Cho

Gravity–capillary solitary waves are generated by a moving ‘air-suction’ forcing instead of a moving ‘air-blowing’ forcing. The air-suction forcing moves horizontally over the surface of deep water with speeds close to the minimum linear phase speed $c_{min}=23~\text{cm}~\text{s}^{-1}$. Three different states are observed according to forcing speeds below $c_{min}$. At relatively low speeds below $c_{min}$, small-amplitude linear circular depressions are observed, and they move steadily ahead of and along with the moving forcing. As the forcing speed increases close to $c_{min}$, however, nonlinear three-dimensional (3-D) gravity–capillary solitary waves are observed, and they move steadily ahead of and along with the moving forcing. Finally, when the forcing speed is very close to $c_{min}$, oblique shedding phenomena of 3-D gravity–capillary solitary waves are observed ahead of the moving forcing. We found that all the linear and nonlinear wave patterns generated by the air-suction forcing correspond to those generated by the air-blowing forcing. The main difference is that 3-D gravity–capillary solitary waves are observed ‘ahead of’ the air-suction forcing whereas the same waves are observed ‘behind’ the air-blowing forcing.


1968 ◽  
Vol 32 (3) ◽  
pp. 619-624 ◽  
Author(s):  
Stephen H. Davis

Using Stuart's shape assumption and a condition of maximum heat transport it is found that the preferred number of finite roll cells present in Bénard convection in athree-dimensional rectangular boxtends todecreasewith increasing supercritical Rayleigh number in contradiction to the behaviour in an infinite layer but in accordance with experimental observation.This ‘end effect’ might explain the similar observation of wave-number decrease in the Taylor instability between rotating cylinders.


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