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Noting, the equation indicates that the group speed is equal to the phase velocity only when the refractive index is a constant (in dependent to the frequency) or the frequency is a constant (independent to the wavenumber). In this case both phase and group velocity are independent of frequency and equal to c/n.
When referring to polarization states, the p-polarization refers to the polarization plane parallel to the polarization axis of the polarizer being used ("p" is for "parallel"). The s-polarization refers to the polarization plane perpendicular to the polarization axis of the polarizer. A linear polarizer, by design, polarizes light in the p-polarization.
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In the linear algebra of real matrices, Hermitian operators are simply symmetric matrices. A basic example is the inertia matrix of a solid body in Newtonian dynamics. The orthonormal eigenvectors of the inertia matrix give the directions of the principal axes of inertia of the body.
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Otherwise, if they vary with freuqency, the medium is called dispersive, the relation w=w(k) is known as the dispersion relation of the medium.
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An orthonormal complete set of eigenvectors or eigenfunctions is an example of a so-called “basis.” In general, a basis is a minimal set of vectors or functions that you can write all other vectors or functions in terms of. For example, the unit vectors , , and are a basis for normal three-dimensional space. Every three-dimensional vector can be written as a linear combination of the three.
S&P polarization refers to the plane in which the electric field of a light wave is oscillating. S-Polarization is the plane of polarization perpendicular to the page (coming out of the monitor screen). P-polarization is the plane of polarization parallel to the page (in the plane of the monitor screen). See figure below:
Most operators in quantum mechanics are of a special kind called Hermitian. This section lists their most important properties.
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In a given medium, both the phase velocity and group velocity depend on the frequency and on the medium's material properties (refractive index)
The first says that you can swap and if you take the complex conjugate. (It is simply a reflection of the fact that if you change the sides in an inner product, you turn it into its complex conjugate. Normally, that puts the operator at the other side, but for a Hermitian operator, it does not make a difference.) The second is important because ordinary real numbers typically occupy a special place in the grand scheme of things. (The fact that the inner product is real merely reflects the fact that if a number is equal to its complex conjugate, it must be real; if there was an in it, the number would change by a complex conjugate.)