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27 Gaussian Beams

Date post: 02-Apr-2018
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    27. Gaussian Beam

    27. Gaussian Beam

    : Gaussian function

    Gaussian beam

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    How to determine

    - Beam size W at z- beam waist- beam radius- divergence angle

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    Wave Equation

    : Helmholtz equation

    ( wavenumber )

    The wave equation for monochromatic waves

    Now, lets start with the wave equation in free-space

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    Paraxial Helmholtz equationParaxial Helmholtz equation

    Slowly varying envelope approximation of the Helmholtz equation

    Paraxial Helmholtz equation.

    : Helmholtz equation

    : Consider a plane wave propagating in z-direction

    : Slowly varying approximation

    2 2

    2

    2 2Tx y

    +

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    One simple solution to the paraxial Helmholtz equation : paraboloidal waves

    Another solution of the paraxial Helmholtz equation : Gaussian beams

    A paraxial wave is a plane wave e-jkz modulatedby a complex envelopeA(r) that is a slowly varying function of position:

    The complex envelopeA(r) must satisfy the paraxial Helmholtz equation

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    Gaussian beamGaussian beam

    W0 : beam waist

    where,

    Gaussian beam

    2

    0 0z W

    =

    z0 : Rayleigh range

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    Gaussian beamGaussian beam

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    Intensity of Gaussian beamIntensity of Gaussian beam

    The intensity is a Gaussian functionof the radial distance .

    This is why the wave is called a Gaussian beam.

    On the beam axis ( = 0)

    At z = z0 , I = Io/2

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    Gaussian beam : PowerGaussian beam : Power

    The result is independent of z, as expected.The beam power is one-half the peak intensity times the beam area.

    The ratio of the power carried within a circle of radius in the transverseplane at position z to the total power is

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    ( )0 a =

    Power ratio clipped by aperture

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    Beam radiusBeam radius

    At the Beam waist :

    Waist radius =W0Spot size =2W0

    (divergence angle)(far-field)

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    Depth of FocusDepth of Focus

    The axial distance within which the beam radius lies within a factor root(2) ofits minimum value (i.e., its area lies within a factor of 2 of its minimum) isknown as the depth of focus or confocal parameter

    beam area at waist

    =

    A small spot size and a long depth of focus cannot be obtained simultaneously !

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    Depth of focus, Rayleigh range, and Beam waist

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    Gaussian parameters

    : Relationships between parameters

    Gaussian parameters

    : Relationships between parameters

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    Phase of the Gaussian beamPhase of the Gaussian beam

    kz : the phase of a plane wave.

    : aphase retardation

    ranging from - /2 to - /2 .

    : This phase retardation corresponds to an excessdelay of the wavefront in comparison with a planewave or a spherical wave

    The total accumulated excess retardation as the wave travels from

    Guoy effect

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    Wavefront - bendingWavefront - bending

    Wavefronts (= surfaces of constant phase) :

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    Wavefronts near the focusWavefronts near the focus

    Wave fronts:

    /2 phase shiftrelative to

    spherical wave

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    TRANSMISSION THROUGH OPTICAL COMPONENTSTRANSMISSION THROUGH OPTICAL COMPONENTS

    A. Transmission Through a Thin Lens

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    Gaussian beam relaying

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    Gaussian beam Focusing

    If a lens is placed at the waist of a Gaussian beam,

    If (2 z0 ) >> f ,

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    Other Beamshigher order beams

    Other Beamshigher order beams

    Hermite-GaussianBessel Beams


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