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  1. F. Abelès, J. Phys. Radium 11, 310 (1950).
    [CrossRef]
  2. G. Jungk, Phys. Status. Solidi. A 34, 69 (1976).
    [CrossRef]
  3. A. R. Reisinger, H. B. Morris, K. L. Lawley, Opt. Eng. 20, 111 (1981).
    [CrossRef]
  4. R. M. A. Azzam, A.-R. M. Zaghloul, J. Opt. (Paris) 8, 201 (1977).
    [CrossRef]
  5. G. Jungk, Phys. Status Solidi A 42, 267 (1977).
    [CrossRef]
  6. A.-R. M. Zaghloul, R. M. A. Azzam, J. Opt. Soc. Am. 67, 1286 (1977).
    [CrossRef]
  7. A.-R. M. Zaghloul, R. M. A. Azzam, N. M. Bashara, J. Opt. Soc. Am. 65, 1043 (1975).
    [CrossRef]
  8. See, for example, R. M. A. Azzam, N. M. Bashara, Ellipsometry and Polarized Light (North-Holland, Amsterdam, 1977), Sec. 4.4.
  9. R. M. A. Azzam, A.-R. M. Zaghloul, N. M. Bashara, J. Opt. Soc. Am. 65, 252 (1975).
    [CrossRef]
  10. Exact mirror-image symmetry with respect to the real axis occurs only if the substrate is transparent. Substrate absorption causes asymmetry.
  11. For example, by use of circular polarization filters (e.g., of the sheet type) of known handedness.

1981 (1)

A. R. Reisinger, H. B. Morris, K. L. Lawley, Opt. Eng. 20, 111 (1981).
[CrossRef]

1977 (3)

R. M. A. Azzam, A.-R. M. Zaghloul, J. Opt. (Paris) 8, 201 (1977).
[CrossRef]

G. Jungk, Phys. Status Solidi A 42, 267 (1977).
[CrossRef]

A.-R. M. Zaghloul, R. M. A. Azzam, J. Opt. Soc. Am. 67, 1286 (1977).
[CrossRef]

1976 (1)

G. Jungk, Phys. Status. Solidi. A 34, 69 (1976).
[CrossRef]

1975 (2)

1950 (1)

F. Abelès, J. Phys. Radium 11, 310 (1950).
[CrossRef]

Abelès, F.

F. Abelès, J. Phys. Radium 11, 310 (1950).
[CrossRef]

Azzam, R. M. A.

R. M. A. Azzam, A.-R. M. Zaghloul, J. Opt. (Paris) 8, 201 (1977).
[CrossRef]

A.-R. M. Zaghloul, R. M. A. Azzam, J. Opt. Soc. Am. 67, 1286 (1977).
[CrossRef]

A.-R. M. Zaghloul, R. M. A. Azzam, N. M. Bashara, J. Opt. Soc. Am. 65, 1043 (1975).
[CrossRef]

R. M. A. Azzam, A.-R. M. Zaghloul, N. M. Bashara, J. Opt. Soc. Am. 65, 252 (1975).
[CrossRef]

See, for example, R. M. A. Azzam, N. M. Bashara, Ellipsometry and Polarized Light (North-Holland, Amsterdam, 1977), Sec. 4.4.

Bashara, N. M.

A.-R. M. Zaghloul, R. M. A. Azzam, N. M. Bashara, J. Opt. Soc. Am. 65, 1043 (1975).
[CrossRef]

R. M. A. Azzam, A.-R. M. Zaghloul, N. M. Bashara, J. Opt. Soc. Am. 65, 252 (1975).
[CrossRef]

See, for example, R. M. A. Azzam, N. M. Bashara, Ellipsometry and Polarized Light (North-Holland, Amsterdam, 1977), Sec. 4.4.

Jungk, G.

G. Jungk, Phys. Status Solidi A 42, 267 (1977).
[CrossRef]

G. Jungk, Phys. Status. Solidi. A 34, 69 (1976).
[CrossRef]

Lawley, K. L.

A. R. Reisinger, H. B. Morris, K. L. Lawley, Opt. Eng. 20, 111 (1981).
[CrossRef]

Morris, H. B.

A. R. Reisinger, H. B. Morris, K. L. Lawley, Opt. Eng. 20, 111 (1981).
[CrossRef]

Reisinger, A. R.

A. R. Reisinger, H. B. Morris, K. L. Lawley, Opt. Eng. 20, 111 (1981).
[CrossRef]

Zaghloul, A.-R. M.

J. Opt. (Paris) (1)

R. M. A. Azzam, A.-R. M. Zaghloul, J. Opt. (Paris) 8, 201 (1977).
[CrossRef]

J. Opt. Soc. Am. (3)

J. Phys. Radium (1)

F. Abelès, J. Phys. Radium 11, 310 (1950).
[CrossRef]

Opt. Eng. (1)

A. R. Reisinger, H. B. Morris, K. L. Lawley, Opt. Eng. 20, 111 (1981).
[CrossRef]

Phys. Status Solidi A (1)

G. Jungk, Phys. Status Solidi A 42, 267 (1977).
[CrossRef]

Phys. Status. Solidi. A (1)

G. Jungk, Phys. Status. Solidi. A 34, 69 (1976).
[CrossRef]

Other (3)

Exact mirror-image symmetry with respect to the real axis occurs only if the substrate is transparent. Substrate absorption causes asymmetry.

For example, by use of circular polarization filters (e.g., of the sheet type) of known handedness.

See, for example, R. M. A. Azzam, N. M. Bashara, Ellipsometry and Polarized Light (North-Holland, Amsterdam, 1977), Sec. 4.4.

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Equations (10)

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ρ = A + B X + C X 2 D + E X + F X 2 ,
A = r 01 p , B = r 12 p + r 01 p r 01 s r 12 s , C = r 01 s r 12 p r 12 s , D = r 01 s , E = r 12 s + r 01 p r 02 s r 12 p , F = r 01 p r 12 p r 12 s ;
X = exp [ - j 2 π ( d / D ϕ ) ] ,
D ϕ = λ 2 ( N 1 2 - N 0 2 sin - 2 ϕ ) - 1 / 2 .
ρ = 1.
ρ = ( A + B cos θ + C cos 2 θ ) - j ( B sin θ + C sin 2 θ ) ( D + E cos θ + F cos 2 θ ) - j ( E sin θ + F sin 2 θ ) .
α 2 cos 2 θ + α 1 cos θ + α 0 = 0 ,
α 0 = ( A 2 + B 2 + C 2 ) - ( D 2 + E 2 + F 2 ) - 2 ( A C - D F ) , α 1 = 2 B ( A + C ) - 2 E ( D + F ) , α 2 = 4 ( A C - D F ) .
cos θ = [ - α 1 ± ( α 1 2 - 4 α 0 α 2 ) 1 / 2 ] / 2 α 2 .
d = ( θ / 2 π ) D ϕ ,

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