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onEyes!
Nose!
http://www.mbari.org/news/news_releases/2009/barreleye/barreleye.html!
7.1 !
Lecture 14: Polarization of Light!
Waves and Optics !
[Extra notes available on wattle]!
7.2 !
Contents!
• This lecture contains the following slides:! – Title! – Contents! – Polarization! – Example of polarization mathematics 1! – Example of polarization mathematics 2! – Example of polarization mathematics 3! – Jones vectors! – Jones vector examples 1 & 2! – Jones vector example 3! – A few polarization terms! – Poincaré basis! – Poincaré sphere! – Summary! – Octopus Vision! – Exercise 1: standard form Jones vector!
7.3 !
Polarization!
ˆ ˆ E ( z,t ) = H E 0 H exp(i( kz " #t + $ H )) + V E 0V exp(i( kz " #t + $V ))
• Assume k is in the z direction (i.e. choose z axis well!).! – V is the unit vector in the y direction (Vertical)! – H is the unit vector in the x direction (Horizontal)! – Taking out the phase of H as a common factor:!
!
ˆ ˆ E ( z,t ) = ( H E 0 H + V E 0V e i("V #" H ) ) e i(kz#$t +" H )
!The phase on the outside won’t change the polarisation state, it all depends on !" = ("V - "H). !
!
7.4 !
Example of polarization mathematics 1!
• Example 1: When !" = 0.!
ˆ ˆ E ( z,t ) = ( H E 0 H + V E 0V ) e i(kz"#t +$ H )
– In this case, we get linearly polarized light, with the angle = arctan(E0V/E0H)!
!
– – – – –
E0V = 0, then Horizontally polarized! E0H = 0, then Vertically polarized! E0V= E0H, then Diagonally polarized! E0V= -E0H, then anti-Diagonally polarized! NB: !" = #, is same as having a negative sign in one of the coefficients.!
7.5 !
Example of polarization mathematics 2!
ˆ ˆ ˆ ˆ E ( z,t ) = ( H E 0 H + V E 0V e"i# / 2 ) e i(kz"$t +% H ) = ( H E 0 H " iV E 0V ) e i(kz"$t +% H ) ˆ ˆ & Re[E ( z,t )] = H E cos(kz " $t + % ) + V E sin(kz " $t + % )
0H H 0V H
• Example 2: When !" = #/2.!
!
– E0V is 90º out-of-phase (in quadrature) with the phasor of E0H.! – The direction...