scholarly journals Bio-Electric Potential under the Light Stimuli of Pholiota nameko. (Part 1). Relationship between the Bio-Electric Potential and the Light Wave Length.

1999 ◽  
Vol 11 (3) ◽  
pp. 209-213 ◽  
Author(s):  
Naoki TAKAHASHI ◽  
Junji HIRAMA ◽  
Toshio MIYAMOTO ◽  
Masakiyo HORIOKA ◽  
Norifumi HIROTA
1997 ◽  
Vol 9 (4) ◽  
pp. 278-281 ◽  
Author(s):  
Junji HIRAMA ◽  
Naoki TAKAHASHI ◽  
Toshio MIYAMATO ◽  
Hiroyasu MIURA ◽  
Shinji TAZAWA

2005 ◽  
Vol 17 (1) ◽  
pp. 11-18 ◽  
Author(s):  
Hideyuki YANAGIBASHI ◽  
Junji HIRAMA ◽  
Kaori SAKAMOTO ◽  
Toshio MIYAMOTO

1914 ◽  
Vol 33 ◽  
pp. 156-165
Author(s):  
R. A. Houstoun

In this paper a short account will be given of the present state of the theory of the absorption of light, with special reference to the results gained in this series of investigations.Theories of the dispersion of light may be divided into two classes: (1) those in which the body is regarded as consisting of particles which vibrate under the influence of the light wave; and (2) those in which the body is regarded as consisting of obstacles which diffract the light wave. According to (2), light is scattered, not absorbed; a wave going through the body diminishes in intensity, but the energy lost is radiated out laterally without change of wave-length.


2020 ◽  
Vol 30 (3) ◽  
pp. 19-28
Author(s):  
V. B. Khabarov ◽  
◽  
А. К. Buryak ◽  
Keyword(s):  

1921 ◽  
Vol 40 ◽  
pp. 34-42
Author(s):  
R. A. Houstoun

§ 1. Let us suppose that a light wave is being propagated and absorbed in a homogeneous medium. Take OY as the direction of propagation, and consider a slice of the medium bounded by two planes at right angles to the direction of propagation and distant dy apart; dy is small in comparison with the wave-length. Let x=f(t) denote the mean displacement of the electrons, and let X = A cos gt denote the electric intensity of the light wave in the slice, measured in electrostatic units. Then the average rate at which work is being done on an electron is


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