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“Gaussian beam”

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(1)

27. Gaussian Beam 27. Gaussian Beam

: Gaussian function

“Gaussian beam”

(2)

How to determine - Beam size W at z - beam waist

- beam radius

- divergence angle

(3)

Wave Equation

: Helmholtz equation

( wavenumber )

“The wave equation for monochromatic waves”

Now, let’s start with the wave equation in free-space

(4)

Paraxial Helmholtz equation Paraxial Helmholtz equation

ÎSlowly varying envelope approximation of the Helmholtz equation Î Paraxial Helmholtz equation.

: Helmholtz equation

: Consider a plane wave propagating in z-direction

: Slowly varying approximation

2 2

2

2 2

T

x y

⎛ ∇ ≡ ∂ + ∂ ⎞

⎜ ∂ ∂ ⎟

⎝ ⎠

(5)

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 modulated

by a complex envelope A(r) that is a slowly varying function of position:

The complex envelope A(r) must satisfy the paraxial Helmholtz equation

(6)

Gaussian beam Gaussian beam

W0 : beam waist where,

Gaussian beam

2

0 0

z π W λ

⎛ = ⎞

⎜ ⎟

⎝ ⎠

z0 : Rayleigh range

(7)

Gaussian beam

Gaussian beam

(8)

Intensity of Gaussian beam Intensity of Gaussian beam

The intensity is a Gaussian function of the radial distance ρ. Æ This is why the wave is called a Gaussian beam.

On the beam axis (ρ = 0)

At z = z0 , I = Io/2

(9)

Gaussian beam : Power Gaussian 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 ρ in the transverse plane at position z to the total power is

(10)

( ρ

0

= a )

Power ratio clipped by aperture

(11)

Beam radius Beam radius

At the Beam waist : Waist radius = W0

Spot size = 2W0

(divergence angle) (far-field)

(12)

Depth of Focus Depth of Focus

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

beam area at waist

= λ

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

(13)

Depth of focus, Rayleigh range, and Beam waist

(14)

Gaussian parameters

: Relationships between parameters Gaussian parameters

: Relationships between parameters

(15)

Phase of the Gaussian beam Phase of the Gaussian beam

kz : the phase of a plane wave.

: a phase retardation ranging from - π/2 to - π/2 . : This phase retardation corresponds to an excess delay of the wavefront in comparison with a plane wave or a spherical wave

The total accumulated excess retardation as the wave travels from

Guoy effect

(16)

Wavefront - bending Wavefront - bending

Wavefronts (= surfaces of constant phase) :

(17)

Wavefronts near the focus Wavefronts near the focus

Wave fronts:

π/2 phase shift

relative to

spherical wave

(18)

TRANSMISSION THROUGH OPTICAL COMPONENTS TRANSMISSION THROUGH OPTICAL COMPONENTS

A. Transmission Through a Thin Lens

(19)

Gaussian beam relaying

(20)

Gaussian beam Focusing

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

If (2 z0 ) >> f ,

(21)

Other Beams

higher order beams

Other Beams

higher order beams

Hermite-Gaussian

Bessel Beams

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