Low-frequency, bottom-interacting pulse propagation in range-dependent oceans

1988 ◽  
Vol 13 (4) ◽  
pp. 222-228 ◽  
Author(s):  
M.D. Collins
2016 ◽  
Vol 140 (1) ◽  
pp. 216-228 ◽  
Author(s):  
Rex K. Andrew ◽  
Andrew Ganse ◽  
Andrew W. White ◽  
James A. Mercer ◽  
Matthew A. Dzieciuch ◽  
...  

Open Physics ◽  
2019 ◽  
Vol 17 (1) ◽  
pp. 200-205
Author(s):  
Rena J. Kasumova ◽  
Gulnara A. Safarova ◽  
Asmar R. Ahmadova

Abstract The parametric interaction of optical wave pulses in metamaterials is considered in the first approximation of the theory of dispersion. The interaction between the quasi-monochromatic pump wave and the wave pulse at the total frequency with quadratic phase modulation is assumed. The results of calculation of the shape of the spectrum of an excited signal wave at a difference frequency are presented for low frequency pumping. It is shown that the effects of group mismatch in metamaterials lead to a narrowing of the spectrum of the excited wave. With an increase in the modulation degree of a weak exciting wave, the spectrum of the excited wave broadens.


2015 ◽  
Vol 138 (2) ◽  
pp. 735-747 ◽  
Author(s):  
Donald G. Albert ◽  
Michelle E. Swearingen ◽  
Frank E. Perron ◽  
David L. Carbee

Author(s):  
K. Hama

The lateral line organs of the sea eel consist of canal and pit organs which are different in function. The former is a low frequency vibration detector whereas the latter functions as an ion receptor as well as a mechano receptor.The fine structure of the sensory epithelia of both organs were studied by means of ordinary transmission electron microscope, high voltage electron microscope and of surface scanning electron microscope.The sensory cells of the canal organ are polarized in front-caudal direction and those of the pit organ are polarized in dorso-ventral direction. The sensory epithelia of both organs have thinner surface coats compared to the surrounding ordinary epithelial cells, which have very thick fuzzy coatings on the apical surface.


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