39
So far •Geometrical Optics Reflection and refraction from planar and spherical int erfaces Imaging condition in the paraxial approximation Apertures & stops Aberrations (violations of the imaging condition due to terms of order higher than paraxial or due to dispersio n) Limits of validity of geometrical optics: feature s of interest are much bigger than the wavelength λ Problem: point objects/images are smaller than λ!!! So light focusing at a single point is an artifact of ou r approximations To understand light behavior at scales ~ λ we need to ta ke into account the wave nature of light.

So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Embed Size (px)

Citation preview

Page 1: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

So far

•Geometrical Optics– Reflection and refraction from planar and spherical interfaces– Imaging condition in the paraxial approximation– Apertures & stops– Aberrations (violations of the imaging condition due to terms of o

rder higher than paraxial or due to dispersion)

• Limits of validity of geometrical optics: features of interest are much bigger than the wavelength λ– Problem: point objects/images are smaller than λ!!!– So light focusing at a single point is an artifact of our approximati

ons– To understand light behavior at scales ~ λ we need to take into a

ccount the wave nature of light.

Page 2: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Step #1 towards wave optics: electro-dynamics

• Electromagnetic fields (definitions and properties) in vacuo

• Electromagnetic fields in matter• Maxwell’s equations

– Integral form– Differential form– Energy flux and the Poyntingvector

• The electromagnetic wave equation

Page 3: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Electric and magnetic forces

Page 4: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Note the units…

Page 5: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Electric and magnetic fields

Page 6: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Gauss Law: electric fields

Page 7: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Gauss Law: magnetic fields

Page 8: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Faraday’s Law: electromotive force

Page 9: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Ampere’s Law: magnetic induction

Page 10: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Maxwell’s equations(in vacuo)

Page 11: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Electric fields in dielectric media

atom under electric field:•charge neutrality is preserved•spatial distribution of chargesbecomes assymetric

Spatially variant polarizationinduces localcharge imbalances

(bound charges)

Page 12: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Electric displacement

Gauss Law:

Electric displacement field:

Linear, isotropic polarizability:

Page 13: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

General cases of polarization

Linear, isotropic polarizability:

Linear, anisotropic polarizability:

Nonlinear, isotropic polarizability:

Page 14: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Constitutive relationships

polarization

magnetization

E: electric fieldD: electric displacement

B: magnetic inductionH: magnetic field

Page 15: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Maxwell’s equations(in matter)

Page 16: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Maxwell’s equations wave equation(in linear, anisotropic, non-magnetic matter, no free

charges/currents)

matter spatially and temporally invariant

electromagneticwave equation

Page 17: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Maxwell’s equations wave equation(in linear, anisotropic, non-magnetic matter, no free

charges/currents)

Page 18: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Light velocity and refractive index

cvacuum: speed of lightin vacuum

0

n: index of refraction

c≡cvacuum/n:speed of lightin medium of refr. index n

Page 19: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Simplified (1D, scalar) wave equation

• E is a scalar quantity (e.g. the component Ey of an electric field E)•the geometry is symmetric in x, y the ⇒ x, yderivatives are zero

Page 20: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Special case: harmonic solution

Page 21: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Complex representation of waves

angular frequency

wave-number

complex representation

complex amplitude or " phasor"

Page 22: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Time reversal

Page 23: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Superposition

Page 24: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

What is the solution to the wave equation?

• In general: the solution is an (arbitrary) superposition of propagating waves

• Usually, we have to impose– initial conditions (as in any differential equation)– boundary condition (as in most partial differential

equations)

Example: initial value problem

Page 25: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

What is the solution to the wave equation?

• In general: the solution is an (arbitrary) superposition of propagating waves

• Usually, we have to impose– initial conditions (as in any differential equation)– boundary condition (as in most partial differential

equations)

• Boundary conditions: we will not deal much with them in this class, but it is worth noting that physically they explain interesting phenomena such as waveguiding from the wave point of view (we saw already one explanation as TIR).

Page 26: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Elementary waves:plane, spherical

Page 27: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

The EM vector wave equation

Page 28: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Harmonic solution in 3D: plane wave

Page 29: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Plane wave propagating

Page 30: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Complex representation of 3D waves

complex representation

complex amplitude or " phasor"

" Wavefront"

Page 31: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Plane wave

Page 32: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Plane wave

(Cartesian coordinate vector)

solves wave equation iff

Page 33: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Plane wave

(Cartesian coordinate vector)

constant phase condition :

wave - front is a plane

" wavefront":

Page 34: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Plane wave propagating

Page 35: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Plane wave propagating

Page 36: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Spherical waveequation of wavefront

“point”source

exponential notation

paraxial approximation

Outgoingrays

Page 37: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

Spherical wave

parabolic wavefronts paraxial approximation/paraxial approximation//Gaussian beams/Gaussian beams

spherical wavefronts

exactexact

Page 38: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

The role of lenses

Page 39: So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures

The role of lenses