Gaussian_Beams Flashcards

1
Q

What is the Helmholtz equation?

A

The Helmholtz equation is ∇²U + k²U = 0, where U is the wave function and k is the wave number.

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2
Q

What assumption is made in the paraxial approximation?

A

The paraxial approximation assumes that the amplitude A does not change significantly as z varies over a scale of one wavelength, implying small angles between rays and the propagation axis.

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3
Q

Explain the paraxial Helmholtz equation.

A

The paraxial Helmholtz equation is ∇²_T A - 2ik ∂A/∂z = 0, where ∇²_T is the transverse Laplacian, and it describes the slowly varying envelope approximation (SVEA) of the wave function.

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4
Q

What is the complex envelope of a Gaussian beam?

A

The complex envelope of a Gaussian beam is A_G(x, y, z) = A1/q(z) * e^(-ik(x² + y²)/2q(z)), with q(z) = z + iz₀.

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5
Q

How is the beam width W(z) of a Gaussian beam defined?

A

The beam width W(z) is given by W(z) = W₀ * sqrt(1 + (z/z₀)²), where W₀ is the beam waist and z₀ is the Rayleigh range.

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6
Q

Describe the radius of wavefront curvature R(z) for a Gaussian beam.

A

The radius of wavefront curvature R(z) is defined as R(z) = z * [1 + (z₀/z)²], where z₀ is the Rayleigh range.

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7
Q

What is the Hermite-Gaussian function Gl(u)?

A

The Hermite-Gaussian function Gl(u) is defined as Gl(u) = Hl(u)e^(-u²/2), where Hl(u) are Hermite polynomials.

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8
Q

What are Laguerre-Gaussian beams and when are they used?

A

Laguerre-Gaussian beams are solutions to the paraxial Helmholtz equation in cylindrical coordinates, often used in situations with cylindrical symmetry, such as in optical resonators.

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9
Q

What is a Bessel beam and how does it differ from Gaussian beams?

A

A Bessel beam is a solution to the Helmholtz equation with a non-diffracting intensity profile, characterized by Bessel functions. Unlike Gaussian beams, Bessel beams do not diffract and carry infinite power.

Diffraction: Bending around obstacle or spreading beam width

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10
Q

How are Bessel beams used in optical tweezers?

A

Bessel beams are used in optical tweezers due to their constant gradient as a function of z, allowing them to guide particles over long distances with precision.

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