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This gallery explores the intricate relationship between light and its polarization properties, particularly focusing on sinusoidal waves, birefringence, and their implications in nature and technology. It illustrates how different crystal structures affect light's refractive indices and introduces key concepts such as linear dichroism, circular polarization, and optical activity. By examining species like the cuttlefish and scarab beetle, we gain insights into how these organisms utilize polarization for navigation and communication. This resource is aimed at enhancing comprehension of light behavior in various contexts.
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Waves, Light & Quanta Tim Freegarde Web Gallery of Art; National Gallery, London
where Sinusoidal waves z • simple harmonic motion • circular motion
wavenumber • spectroscopists’ at , wavenumber • wavelength Sinusoidal waves
angular frequency • frequency • period Sinusoidal waves at ,
Birefringence • asymmetry in crystal structure causes two different refractive indices • opposite polarizations follow different paths through crystal • birefringence, double refraction 5
light is a transverse wave: perpendicular to Optical polarization • for any wavevector, there are two field components • any wave may be written as a superposition of the two polarizations
conductivity of wire grid depends upon field polarization • electric fields perpendicular to the wires are transmitted Linear dichroism • fields parallel to the wires are absorbed WIRE GRID POLARIZER
Malus’ law • amplitude transmission • intensity transmission WIRE GRID POLARIZER
crystals may similarly show absorption which depends upon linear polarization • absorption also depends upon wavelength • polarization therefore determines crystal colour Linear dichroism • pleochroism, dichroism, trichroism TOURMALINE
CUTTLEFISH (sepia officinalis) MAN’S VIEW CUTTLEFISH VIEW • the European cuttlefish also has polarization-sensitive vision • … and can change its colour and polarization! Polarization in nature (red = horizontal polarization)
SCARAB BEETLE LEFT CIRCULAR POLARIZED LIGHT RIGHT CIRCULAR POLARIZED LIGHT • absorption may also depend upon circular polarization • the scarab beetle has polarization-sensitive vision, which it uses for navigation Circular dichroism • the beetle’s own colour depends upon the circular polarization
CH3 CH3 CH3 CH3 CH2 CH2 H H • optical activity is birefringence for circular polarizations • an asymmetry between right and left allows opposing circular polarizations to have differing refractive indices Optical activity (circular birefringence) l-limonene (orange) r-limonene (lemon) • optical activity rotates the polarization plane of linearly polarized light CHIRAL MOLECULES • may be observed in vapours, liquids and solids
Categories of optical polarization • linear (plane) polarization • non-equal components in phase • circular polarization • equal components 90° out of phase • elliptical polarization • all other cases 13
Polarizing components LINEAR CIRCULAR POLARIZER (filter/separator) WAVEPLATE (retarder) 14
Waveplates (retarders) • at normal incidence, a birefringent material retards one polarization relative to the other • linearly polarized light becomes elliptically polarized WAVEPLATE 15
circular polarization RCP plane of incidence • right- or left-handed rotation when looking towards source perpendicular • traces out opposite (right- or left-) handed thread Polarization notation parallel • linear (plane) polarization • parallel or perpendicular to plane of incidence • plane of incidence contains wavevector and normal to surface
Polarization by scattering cdoswell.com/tips3.htm
Brewster’s angle • reflected light fully (s-) polarized
www.paddling.net/sameboat/archives/sameboat496.html Brewster’s angle • reflected light fully (s-) polarized
Malus’ law • amplitude transmission • intensity transmission WIRE GRID POLARIZER
e.g. linear polarization at angle • wavevector insufficient to define electromagnetic wave • we must additionally define the polarization vector Characterizing the optical polarization
if the polarization state may be represented by a Jones vector Jones vector calculus JONES MATRIX • then the action of an optical element may be described by a matrix
transmission by horizontal polarizer retardation by waveplate projection onto rotated axes • if the polarization state may be represented by a Jones vector • then the action of an optical element may be described by a matrix Jones vector calculus JONES MATRIX
asymmetry in crystal structure causes two different refractive indices • opposite polarizations follow different paths through crystal Birefringence • birefringence, double refraction
Linear polarizers (analyzers) 38.5º o-ray • birefringence results in different angles of refraction and total internal reflection e-ray • many different designs, offering different geometries and acceptance angles e-ray o-ray s-ray • a similar function results from multiple reflection p-ray 25
at normal incidence, a birefringent material retards one polarization relative to the other • linearly polarized light becomes elliptically polarized Waveplates (retarders) WAVEPLATE
adjust variable fixed • a variable waveplate uses two wedges to provide a variable thickness of birefringent crystal • a further crystal, oriented with the fast and slow axes interchanged, allows the retardation to be adjusted around zero Compensators SOLEIL COMPENSATOR • with a single, fixed first section, this is a ‘single order’ (or ‘zero order’) waveplate for small constant retardation
light is a transverse wave: perpendicular to Electromagnetic waves • Faraday • Ampère
atomic electrons move in response to electric field • resulting atomic dipole radiates field which adds to original z Dielectrics • Faraday • Ampère