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Fundamental Behavior of Light

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Title: Fundamental Behavior of Light


1
Fundamental Behavior of Light
  • Light AS A Wave
  • gtLight can be treated as an Electromagnetic Wave
    with time varying electric (E(x)) and magnetic
    fields (B(y)).
  • E and B have an orthogonal relationship
    propagating through space (homogeneous medium).
  • Assuming a sinusoidal traveling wave along the z
    axis the general mathematical form of this event
    can be stated as

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Electromagnetic Fields and Light
  • The surface with which a wave has constant face
    is referred to as a Wavefront.
  • Faradays Law states that time varying magnetic
    fields result in time varying electric fields.
  • The two fields always accompany one another with
    the same frequency and propagation constant but
    transverse to one another in direction
  • Typically it is the electric field component that
    is referred to, when dealing with non conductive
    matter as the electric field is responsible for
    displacing electrons in molecules or ions in a
    crystal and therefore determines the Polarization
    of matter.
  • The Optical Field refers to the electric field.

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Phase Velocity (Constant Phase)
  • There is a relationship in time and space for a
    given phase.
  • A surface where the phase of a wave is constant
    is called a wavefront.
  • When the all electric fields within a wavefront
    are in phase in the x,y plane a phase velocity
    can be determined by

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Phase Velocity (Constant Phase)
  • It is of importance to know the phase difference
    at a given point in time between two points on a
    wave.
  • If 2 points are separated by then phase
    difference is because is the same
    for each point.
  • If the phase difference is 0 or multiples of 2 pi
    then the two points are in phase. Therefore

8
Maxwells Wave Equation
  • A perfect plane wave propagates without
    divergence. The amplitude of plane wave is not
    dependant on distance from a reference point and
    is the same at all points on a given (x,y) plane
    perpendicular to k. As planes travel to infinity
    they have infinite energy. Ideal with infinitely
    large source.
  • A perfect spherical wave a traveling field
    emerging from a point EM source where the
    amplitude decays with distance r. k vectors
    diverge out as wave propagates and constant phase
    surfaces become larger.Optical divergence for the
    spherical wave is 360 degrees.Point source. Real
    EM source has finite size and power.

9
Maxwells Wave Equation
  • The field amplitude at any point r from the
    source is given by
  • May require transformation from cartesian to
    spherical coordinates.
  • Divergent Beam Wavefronts slowly bend away
    spreading the wave. Plane waves are typically
    used for explaining behavior of light rays as the
    nature of discussion is for a point far away from
    a source that approximates a small spatial
    region and the wavefront appears as a plane in
    that immediate area.

10
Beam Divergence
  • Consider a Gaussian beam travelling along the
    z-axis.
  • The light intensity distribution across the beam
    cross-section is Gaussian.
  • Beam diameter 2 increases as the beam travels
    along z with the cross sectional area at
    that point contains 85 of the beam power.
  • The waist and spot size is where the wavefronts
    are parallel at 2 and the waist radius is
    .
  • Beam divergence is given by

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Index of Refraction
  • The oscillating electric field of an EM wave
    travelling in a dielectric medium polarizes
    molecules of the medium at the frequency of
    operation.
  • The field and induced molecular dipoles become
    coupled.
  • Result? The polarization mechanism delays the
    propagation of the EM wave with respect to a
    vacuum.
  • The relative permittivity ( ) is a measure of
    the ease with which a medium becomes polarized.

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Index of Refraction
  • An EM wave traveling in a nonmagnetic medium of
    relative permittivity will have a phase velocity
    given by

15
Index of Refraction
  • Polarization and optical frequency range ( )
  • gtInfrared frequencies and below is
    due to
  • both electronic and ionic
    polarization.
  • gt Balance of optical range is due to
  • electronic polarization as ionic
    polarization
  • too slow to respond to the field.
  • Refractive Index is the ratio of C in free space
    to C in a medium.

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Index of Refraction
  • Isotropic non crystalline solids such as glass,
    water and cubic crystals ( one refractive index
    in all directions
  • Anisotropic- all crystal except for cubic
    crystal.
  • Note The relative permittivity for many
    materials can vary considerably over a frequency
    range.

17
Relative Permittivity
  • Relative permittivity (dielectric constant)
    of materials is frequency dependant of the EM
    wave.
  • Relative permittivity can vary over a great range
    for many materials due to polarization
    mechanisms.
  • For optical only electronic polarization responds
    to the oscillating field.

18
Group Velocity
  • In practice monochromatic waves do not exist.
  • Groups of waves can differ in wavelength as they
    travel along a z direction.
  • Consider two waves interfering and generating a
    wave packet.
  • An oscillating field develops at a mean frequency
    that is amplitude modulated by a more slowly
    varying field at a frequency of .
  • Emax moves with a wavevector (group
    velocity)

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Group Velocity
  • Group velocity defines the speed with which the
    enevelope propagates.
  • The amplitude variations of the envelope (Emax)
    travel with velocity while the phase
    variations of the electric field travel at the
    phase velocity V.

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