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1 Matrix methods in paraxial optics Wednesday September 25, 2002
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2 Matrices in paraxial Optics Translation (in homogeneous medium) 0000 L yoyoyoyo y
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3 Matrix methods in paraxial optics Refraction at a spherical interface y ’’’’φ ’’’’ nn’
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4 Matrix methods in paraxial optics Refraction at a spherical interface y ’’’’φ ’’’’ nn’
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5 Matrix methods in paraxial optics Lens matrix n nLnLnLnLn’ For the complete system Note order – matrices do not, in general, commute.
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6 Matrix methods in paraxial optics
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7 Matrix properties
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8 Matrices: General Properties For system in air, n=n’=1
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9 System matrix
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10 System matrix: Special Cases (a) D = 0 f = Cy o (independent of o ) yoyoyoyo ffff Input plane is the first focal plane
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11 System matrix: Special Cases (b) A = 0 y f = B o (independent of y o ) oooo yfyfyfyf Output plane is the second focal plane
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12 System matrix: Special Cases (c) B = 0 y f = Ay o yfyfyfyf Input and output plane are conjugate – A = magnification yoyoyoyo
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13 System matrix: Special Cases (d) C = 0 f = D o (independent of y o ) Telescopic system – parallel rays in : parallel rays out oooo ffff
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14 Examples: Thin lens Recall that for a thick lens For a thin lens, d=0
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15 Examples: Thin lens Recall that for a thick lens For a thin lens, d=0 In air, n=n’=1
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16 Imaging with thin lens in air oooo ’’’’ ss’ yoyoyoyoy’ Inputplane Output plane
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17 Imaging with thin lens in air For thin lens: A=1 B=0 D=1 C=-1/f y’ = A’y o + B’ o
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18 Imaging with thin lens in air y’ = A’y o + B’ o For imaging, y’ must be independent of o B’ = 0 B’ = As + B + Css’ + Ds’ = 0 s + 0 + (-1/f)ss’ + s’ = 0 For thin lens: A=1 B=0 D=1 C=-1/f
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19 Examples: Thick Lens n nfnfnfnfn’ yoyoyoyo y’ H’ h’ x’ f’ ’’’’ h’ = - ( f’ - x’ )
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20 Cardinal points of a thick lens
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21 Cardinal points of a thick lens
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22 Cardinal points of a thick lens Recall that for a thick lens As we have found before h can be recovered in a similar manner, along with other cardinal points
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