ft
: Fourier transform
go
: geometric optics
wo
: wave optics
Main reference
- Lectures from Prof. Brad Osgood (Stanford)
ft_01
- Analysis and synthesis of period function
- Fourier series of function with period 1
- Inner product between functions
- Complex exponential as orthonormal basis for functions
ft_02
- Fourier series of function with period T
- Setup for Fourier transform as Fourier series with T goes to infinity
- Variables of Fourier and inverse Fourier transform
ft_03
- Shifting property
- Scaling property
- Derivative property
- Duality with reversed function
ft_04
- Convolution
- Convolution in one domain is multiplication in the other domain
- Convolution is commutative
ft_05
- Problem with classic Fourier transform definition
- Rapidly decreasing functions that work for classic definition
- Test function and distribution
- Delta function as distribution
- Ordinary function as distribution
- Fourier transform in context of distribution
- Some examples
ft_06
- Sampling property of delta function via multiplication
- Shifting property of delta function via convolution
- Scaling of delta function
ft_07
- Setup for Shah function
- Definition
- Poisson summation formula and Fourier transform of Shah function
ft_08
- Sampling theorem for bandlimited function
- Aliasing with undersampling
- Example of aliasing
ft_09
- Setup for discrete Fourier transform (DFT)
- Sampled form of function in time domain
- Continuous Fourier transform of sampled form of function
- Sampling in frequency domain to get sampled form of Fourier transform (of sampled form of function)
- Replace sampled forms with discrete functions
- Define DFT
ft_10
- Discrete complex exponentials
- Orthogonality between discrete complex exponentials
- Define inverse DFT
- Some examples of DFT
- Periodicity induced by discrete complex exponentials
- Duality for reversed function
- Shifting property in DFT
ft_11
- Discrete version of convolution
- Commutative and shifting property in convolution
ft_12
- Discrete version of delta function
- Multiplication and convolution with discrete delta function
ft_13
- Definition of linear system
- Sampling is a linear system
- Integration with kernel as infinite dimensional matrix multiplication
- Integration with kernel is the only form of continuous linear system
- Delta function and impulse response
- Impulse response of Fourier transform
ft_14
- Linear system in the case of convolution
- Delay operator
- Convolution with a delayed function is delay of (convolution with the function)
- Linear time-invariant system (LTI)
- Convolution is the only form of LTI system
ft_15
- Fourier transform of LTI system
- Complex exponentials are eigenfunctions of LTI system
ft_16
- Discrete LTI system with matrix-vector multiplication
- Complex exponentials are eigenvectors of discrete LTI system
ft_17
- 2D Fourier transform
- Spatial frequency
ft_18
- High dimensional Fourier transform of separable functions
ft_19
- Shifting property of high dimensional Fourier transform
- General scaling property of high dimensional Fourier transform
- Properties of high dimensional delta function
ft_20
- 2D Shah function and its Fourier transform
ft_ex_01
- Example: Fraunhofer diffraction
- Setup
- Far field approximation
- When nature is doing Fourier transform
- Far field diffraction pattern for common aperture functions
Main reference
- Lectures from Sander Konijnenberg (ASML)
go_01
- Convex and concave lens
- Real and virtual image
go_02
- Reflection
- Refraction and Snell's law
go_03
- Free space propagation
- Single thin lens propagation
- Paraxial approximation
- Transfer matrix
- Imaging condition
go_04
- Magnification factor
- Magnifier
- Microscope
- Telescope
go_05
- Chief ray and marginal ray
- Aperture
- Depth of focus
wo_01
- The concept of phase
- Wave equation
- Complex notation
- Plane wave
wo_02
- Refraction and Snell's law from plane wave equation
- Total internal reflection and Evanescent field
wo_03
- Spherical wave equation
wo_04
- Huygens–Fresnel principle
wo_05
- Double slit (point source) far field pattern
- As addition of complex-valued fields approximated as plane waves
- As path difference over integer multiple of wavelength
wo_06
- Diffraction grating with slits of negligible width (point source)
- Diffraction grating with slits of non-negligible width
- Grating spectroscopy
- Chromatic resolving power (resolvance)
- Free spectral range
- Numerical aperture (NA)
wo_07
- Michelson interferometry
- Tilted beam interference
- Haidinger pattern
wo_08
- Decompose initial field into plane waves with angular spectrum
- Propagate plane waves with plane wave equation
- Reconstruct field after propagation using angular spectrum
wo_09
- Huygens' principle
- Propagation of field using Rayleigh-Sommerfeld (R-S) integral
- R-S integral under Fresnel approximation
- R-S integral under Fraunhofer approximation
- Short notation for quadratic phase factor
- When is Fresnel approximation valid
- When is Fraunhofer approximation valid
- Fresnel number