Matrix Methods for Optics Flashcards

1
Q

What does the matrix method allow us to achieve and how?

A

Using the paraxial approximation and matrices, we can analyse changes in ray height and direction

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2
Q

What is the paraxial approximation?

A

tan 𝛼0 β‰… 𝛼0

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3
Q

What is the matrix form of the translation matrix?

A

y1 = |1 L | |yo|
𝛼1 = |0 1 | |𝛼0|
y is the height and alpha is the angle

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4
Q

What is the refraction matrix?

A

y’ = | 1 0| |y|
𝛼’ = |(1/R)((n/n’)-1) n/n’ | |𝛼|

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5
Q

what is the reflection matrix?

A

y’ = |1 0 | |y|
𝛼’ = |2/R 1 | |𝛼|

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6
Q

What order do matrices operate on light?

A

the order in which the optical interfaces do

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7
Q

What is the whole system ray transfer matrix?

A

M = MNMN-1…M2M1

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8
Q

what is the thin lens matrix?

A

M = | 1 0|
|-1/f 1|

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9
Q

What is the form of the transfer matrix?

A

M = |A B|
|C D|

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10
Q

What is the determinant of the transfer matrix in terms of the starting and ending refractive indices?

A

Det = AD-BC = no/nt

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11
Q

What are the linear equations from the ABCD matrix?

A

yf = Ayo + B𝛼0
𝛼𝑓 = Cy0 + D𝛼0

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12
Q

What happens if D = 0 in the ABCD matrix?

A

𝛼𝑓 = 𝐢𝑦0 so is independent of the input angle
input plane coincides with the front focal plane

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13
Q

What happens if A = 0 in the ABCD matrix?

A

yf = B𝛼0 and the output rays are independent of the input height and all converge at the same output height
they form at the back focal plane

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14
Q

What happens if B = 0 in the ABCD matrix?

A

yf = Ay0 implying conjugate points
A will be the linear magnification

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15
Q

What happens if C=0 in the ABCD matrix?

A

𝛼𝑓 = 𝐷𝛼0 indicating parallel rays coming in produce parallel rays coming out
D is the angular magnification

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16
Q

What is the matric for refraction at a plane surface

A

yf = |1 0||y0|
𝛼𝑓 = |0 n1/n2||𝛼0|