Transcript
Classical Optics Theory of propagation, interference and diffraction of light Dr. Axel Kuhn, Oxford 2008/09
lecture notes and problem sets http://www.physics.ox.ac.uk/Users/Ewart/index.htm
http://www.physics.ox.ac.uk/atomphoton/presentations.html lecture 1
Classical Optics – Literature Hecht, Optics Klein and Furtak, Optics Smith, King & Wilkins, Optics and Photonics Brooker, Modern Classical Optics Born and Wolf, Principles of Optics
Paul Ewart‘s lecture notes: http://www.physics.ox.ac.uk/Users/Ewart/index.htm lecture 1
Classical Optics – Relevance Astronomy and Cosmology Microscopy Spectroscopy and Atomic Theory Quantum Theory and Applications Relativity Theory Lasers and Applications Modern Applications (opto-electronics, display technology, optical coatings, telecommunication, consumer electronics) lecture 1
Classical Optics – Relevance
lecture 1
Astronomical observatory, Hawaii, 4200m above sea level.
Classical Optics – Relevance Hubble space telescope, 2.4 m mirror
lecture 1
Classical Optics – Relevance
Classical Optics – Relevance
lecture 1
fruit fly
Classical Optics – Relevance
lecture 1
Optical Microscope
Classical Optics – Relevance
CD/DVD player optical pickup system lecture 1
Classical Optics – Relevance Coherent Light !Laser Physics Holography Telecommunications Quantum optics Quantum computing Ultra-cold atoms Laser nuclear ignition Medical applications Engineering Chemistry Environmental sensing Metrology ... and many more lecture 1
Classical Optics – Outline Revision of geometrical optics ! reflection, refraction, imaging systems
Physical optics – Wave nature of light ! interference and diffraction
Fourier methods in optics ! Fresnel-Kirchhoff integral, Abbé theory of imaging
Diffraction-based optical instruments ! 2-slit, grating, Michelson and Fabry-Perot Interferometer
Dielectric surfaces and boundaries ! multilayer (anti)reflection coatings
Polarized Light lecture 1
Geometrical Optics – Outline Geometrical optics Fermat‘s principle Snell‘s law (reflection and refraction) Thin-lens approximation Principal planes Optical instruments Aperture and field stops Pinhole camera ! wave optics lecture 1
Geometrical Optics Ignoring the wave nature of light Basic theory for optical instruments Fermat‘s Principle Light propagating between two points follows a path, or paths, for which the time taken is an extremum (minimum)
lecture 1
Geometrical Optics Fermat‘s Principle Light propagating between two points follows a path, or paths, for which the time taken is an extremum (minimum)
Reflection:
Θ1 = ΦR
incidence angle = reflection angle
Refraction: Snell‘s law n1 sin Θ1 = n2 sin Θ2 lecture 1
ΦR
Ray tracing – Revision focussing with spherical surfaces
parallel bundles ! image sphere
object sphere ! image sphere lecture 1
Ray tracing – Revision paraxial approximation (thin lens)
parallel bundles ! focal plane @ f from Hecht, Optics
object plane ! image plane lecture 1
1 1 1 + = = (n − 1) u v f
!
1 1 + R1 R2
"
Lensmaker‘s formula
2nd year Optics Axel Kuhn, 2008/09
Ray tracing – Revision
http://www.physics.ox.ac.uk/ atomphoton/presentations.html
Geometrical optics Fermat‘s principle Snell‘s law (reflection and refraction) Curved surface ! focussing lens Small-angle approximation Paraxial approximation Thin-lens approximation 1 1 1 + = = (n − 1) u v f
!
1 1 + R1 R2
Lensmaker‘s formula
lecture 2
Ray tracing – Revision u
v Focal point axis
Focal point
1 1 1 + = u v f lecture 2
"
thin lens formula
Form follows Function Feynman‘s analysis of a thin lens all optical paths from S to P of same OPL all paths in phase (constructive interference) from Hecht, Optics
lecture 2
Principal Planes
location of equivalent thin lens lecture 2
Principal Planes
location of equivalent thin lens lecture 2
Principal Planes lens system
u
1 1 1 + = u v f lecture 2
v
thin lens equation applies with u and v measured from the two principal planes
Simple Magnifying Glas
angular magnification
" Object at near point
M= !/" Eyepiece of Telescopes, Microscopes etc.
! Virtual image at near point Short focal length lens lecture 2
Telephoto Lens
equivalent thin lens lecture 2
Wide Angle Lens
lecture 2
Astronomical Telescope
angular magnification = !/" = fo/fE lecture 2
Galilean Telescope
Telescope (Galilean)
!
!"
!#
!
e 1.6 '(!)'$#*+*,'-*.#/!!
$ " !!" " ! % !! # !!
angular magnification = !/" = fo/fE
Telescope (Newtonian) lecture 2
!%
Newtonian Telescope
!#
!
angular e 1.7 magnification = !/" '(!)'$#*+*,'-*.#/!!
!
$ " !!" " ! % !! # !!
-12!+.,'&!&2#$-1!.+!-12!.342,-*52!)*((.(!'#6!7+.(!'!0812(*,'&!)*((.(!0%(+',29!2: = fo/fE 2!('6*%0!.+!,%(5'-%(2;!
Compound Microscope lecture 2 !"
!#
The Compound Microscope
Objective magnification = v/u Eyepiece magnifies real image of object lecture 2
Apertures, Pupils and Field Stops
Amount of light? ! Aperture and focal length Field-of-view? ! Field stop in (virtual) image plane
lecture 2
Apertures, Pupils and Field Stops entrance pupil = image of aperture stop (seen from object)
exit pupil = image of aperture stop (seen from image)
from Hecht, Optics
Apertures, Pupils and Field Stops Vignetting: Intensity reduction far off-axis
from Hecht, Optics
lecture 2
Apertures, Pupils and Field Stops What size to make the lenses & apertures?
lecture 2
Eye piece ~ pupil size Objective: Image in eye-piece ~ pupil size
Apertures, Pupils and Field Stops What size to make the lenses & apertures? Aperture stop
lecture 2
Eye piece ~ pupil size Objective: Image in eye-piece ~ pupil size
Apertures, Pupils and Field Stops
Aperture stop
Field stop
limiting the Intensity
limiting the field-of-view
lecture 2
Apertures, Pupils and Field Stops ILLUMINATION OF OPTICAL INSTRUMENTS f-number focal length f /no. = entrance pupil diameter
intensity in the image plane lecture 2
∝
!
1 f /no.
"2
The Pinhole Camera
optimum pinhole size contradicts expectations from geometrical optics from Hecht, Optics
lecture 2
Summary of Week 1
2nd year Optics Axel Kuhn, 2008/09
http://www.physics.ox.ac.uk/ atomphoton/presentations.html
Geometrical optics Fermat‘s principle Snell‘s law (reflection and refraction) Thin-lens approximation Principal planes Optical instruments Aperture and field stops Pinhole camera ! wave optics lecture 3