Huygens' principle


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Huy·gens' principle

 (hī′gənz)
n.
The principle that any point on a wave front of light may be regarded as the source of secondary waves and that the surface that is tangent to the secondary waves can be used to determine the future position of the wave front.

[After Christiaan Huygens.]
American Heritage® Dictionary of the English Language, Fifth Edition. Copyright © 2016 by Houghton Mifflin Harcourt Publishing Company. Published by Houghton Mifflin Harcourt Publishing Company. All rights reserved.
References in periodicals archive ?
They allow Huygens' Principle to be realized in fact, with unprecedented control and shaping of the overall wave, at wide bandwidths, with multiple layers if desired.
In this paper, we show that many electromagnetic theorems still exist in this discrete electromagnetic theory with DEC, such as Huygens' principle, reciprocity theorem, Poynting's theorem and uniqueness theorem.
Therefore, Huygens' principle for both scalar and electromagnetic waves can be derived in this discrete world.
In modern physics, and following Feynman's developments and using appropriate field operators such as Green's functions, Huygens' principle also finds exact mathematical expression through the Chapman-Kolmogorov equation, (49) which is the equation of motion of Markov processes.
Given that Huygens' principle in its modern form, presents as a highly potent and successful representation of electromagnetic propagation, yet equally presents as both nonlocal and non-separable, such a depiction may then be thought to recommend itself as the model of choice for a possible reformulation of the special relativity theory in a post-EPR context.
This is similar to Huygens' Principle (20), proposed for optics more than three centuries ago.
This is a significant departure from the classical formulation of Huygens' principle, where a reverse flow of energy on the positive side of the aperture is precluded by the explicit assumption that light does not travel backwards.
The Kirchhoff and Rayleigh-Sommerfeld integral equations (1) and (2) are alternative forms of the theorem of Helmholtz (5), which expresses Huygens' principle in terms of a scalar wave function U and its normal derivatives without assuming specific attributes of this function, except that it is continuous and twice differentiable with continuous derivatives and obeys the homogeneous wave equation,