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  1. Minutes of the 9th Session of ICO, section 10(c), J. Opt. Soc. Am. 63, 906 (1973).
  2. J. Terrien, Bureau International des Poids et Mesures, Pavillon de Breteuil, F92, Sèvres, France.
  3. P. Jacquinot, Japan. J. Appl. Phys. 4, suppl. 1, 447 (1965).
  4. J. W. Schofield, J. Ring, Optical Instruments and Techniques (Oriel, Newcastle upon Tyne, 1970), p. 21.
  5. International Lighting Vocabulary, 3rd Ed. (International Commission on Illumination, Bureau Central de la CIE, 4 avenue du Recteur Poincaré, 75, Paris 16, France), Publ. CIE No. 17 (E-1.1) (1970).
  6. P. Jacquinot, Rep. Progr. Phys. 23, 276 (1960).
    [Crossref]
  7. W. J. Hurley, J. Chem. Educ. 43, 236 (1966).
    [Crossref]
  8. H. A. Gebbie, R. Q. Twiss, Rep. Progr. Phys. 29, 752.
  9. L. Mertz, Transformations in Optics (Wiley, New York, 1965), p. 15.
  10. W. H. Steel, J. Opt. Soc. Am. 54, 152 (1964).
    [Crossref]
  11. W. H. Steel, Interferometry (Cambridge U. P., Cambridge, 1967), p. 28.
  12. This form should be regarded as a paraxial approximation. For larger angles, n y tanα is the invariant for perfect optical systems and n y sinα for systems free from coma.

1973 (1)

Minutes of the 9th Session of ICO, section 10(c), J. Opt. Soc. Am. 63, 906 (1973).

1966 (1)

W. J. Hurley, J. Chem. Educ. 43, 236 (1966).
[Crossref]

1965 (1)

P. Jacquinot, Japan. J. Appl. Phys. 4, suppl. 1, 447 (1965).

1964 (1)

W. H. Steel, J. Opt. Soc. Am. 54, 152 (1964).
[Crossref]

1960 (1)

P. Jacquinot, Rep. Progr. Phys. 23, 276 (1960).
[Crossref]

Gebbie, H. A.

H. A. Gebbie, R. Q. Twiss, Rep. Progr. Phys. 29, 752.

Hurley, W. J.

W. J. Hurley, J. Chem. Educ. 43, 236 (1966).
[Crossref]

Jacquinot, P.

P. Jacquinot, Japan. J. Appl. Phys. 4, suppl. 1, 447 (1965).

P. Jacquinot, Rep. Progr. Phys. 23, 276 (1960).
[Crossref]

Mertz, L.

L. Mertz, Transformations in Optics (Wiley, New York, 1965), p. 15.

Ring, J.

J. W. Schofield, J. Ring, Optical Instruments and Techniques (Oriel, Newcastle upon Tyne, 1970), p. 21.

Schofield, J. W.

J. W. Schofield, J. Ring, Optical Instruments and Techniques (Oriel, Newcastle upon Tyne, 1970), p. 21.

Steel, W. H.

W. H. Steel, J. Opt. Soc. Am. 54, 152 (1964).
[Crossref]

W. H. Steel, Interferometry (Cambridge U. P., Cambridge, 1967), p. 28.

Terrien, J.

J. Terrien, Bureau International des Poids et Mesures, Pavillon de Breteuil, F92, Sèvres, France.

Twiss, R. Q.

H. A. Gebbie, R. Q. Twiss, Rep. Progr. Phys. 29, 752.

J. Chem. Educ. (1)

W. J. Hurley, J. Chem. Educ. 43, 236 (1966).
[Crossref]

J. Opt. Soc. Am. (2)

W. H. Steel, J. Opt. Soc. Am. 54, 152 (1964).
[Crossref]

Minutes of the 9th Session of ICO, section 10(c), J. Opt. Soc. Am. 63, 906 (1973).

Japan. J. Appl. Phys. (1)

P. Jacquinot, Japan. J. Appl. Phys. 4, suppl. 1, 447 (1965).

Rep. Progr. Phys. (2)

H. A. Gebbie, R. Q. Twiss, Rep. Progr. Phys. 29, 752.

P. Jacquinot, Rep. Progr. Phys. 23, 276 (1960).
[Crossref]

Other (6)

L. Mertz, Transformations in Optics (Wiley, New York, 1965), p. 15.

W. H. Steel, Interferometry (Cambridge U. P., Cambridge, 1967), p. 28.

This form should be regarded as a paraxial approximation. For larger angles, n y tanα is the invariant for perfect optical systems and n y sinα for systems free from coma.

J. W. Schofield, J. Ring, Optical Instruments and Techniques (Oriel, Newcastle upon Tyne, 1970), p. 21.

International Lighting Vocabulary, 3rd Ed. (International Commission on Illumination, Bureau Central de la CIE, 4 avenue du Recteur Poincaré, 75, Paris 16, France), Publ. CIE No. 17 (E-1.1) (1970).

J. Terrien, Bureau International des Poids et Mesures, Pavillon de Breteuil, F92, Sèvres, France.

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Equations (3)

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G = n 2 A Ω ,
Φ = τ G L ,
g = n y α ,

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