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  1. For a comment on the accuracy of wavenumber determinations in the infrared region of the spectrum with a scanning spectrometer, see D. H. Rank, G. D. Saksena, G. Skorinko, D. P. Eastman, T. A. Wiggins, T. K. McCubbin, J. Opt. Soc. Amer. 49, 1217 (1959).
    [CrossRef]
  2. A. A. Hoag, W. C. Miller, Appl. Opt. 8, 2417 (1969).
    [CrossRef] [PubMed]
  3. Kodak Plates and Films for Science and Industry, Kodak Publication P-9, First Edition (Eastman Kodak Co., 1967), pp. 10d–12d.
  4. See, for example, A. D. May, G. Varghese, J. C. Stryland, H. L. Welsh, Can. J. Phys. 42, 1058 (1964); K. S. Jammu, G. E. St. John, H. L. Welsh, Can. J. Phys. 44, 797 (1966); D. W. Lepard, D. E. Shaw, H. L. Welsh, Can. J. Phys. 44, 2353 (1966); D. E. Shaw, H. L. Welsh, Can. J. Phys. 45, 3823 (1967).
    [CrossRef]
  5. W. C. Miller, “Reduction of Low Intensity Reciprocity Failure in Photographic Plates by Controlled Baking,” AAS Photo-Bulletin No. 2 (1970), p. 15.
  6. J. C. Marchant, A. G. Millikan, J. Opt. Soc. Amer. 55, 907 (1965).
  7. A. Weber, S. P. S. Porto, L. E. Cheesman, J. J. Barrett, J. Opt. Soc. Amer. 57, 19 (1967).
    [CrossRef]
  8. A. G. Smith, H. W. Schrader, W. W. Richardson, Appl. Opt. 10, 1597(1971).
    [CrossRef] [PubMed]

1971 (1)

1969 (1)

1967 (1)

A. Weber, S. P. S. Porto, L. E. Cheesman, J. J. Barrett, J. Opt. Soc. Amer. 57, 19 (1967).
[CrossRef]

1965 (1)

J. C. Marchant, A. G. Millikan, J. Opt. Soc. Amer. 55, 907 (1965).

1964 (1)

See, for example, A. D. May, G. Varghese, J. C. Stryland, H. L. Welsh, Can. J. Phys. 42, 1058 (1964); K. S. Jammu, G. E. St. John, H. L. Welsh, Can. J. Phys. 44, 797 (1966); D. W. Lepard, D. E. Shaw, H. L. Welsh, Can. J. Phys. 44, 2353 (1966); D. E. Shaw, H. L. Welsh, Can. J. Phys. 45, 3823 (1967).
[CrossRef]

1959 (1)

For a comment on the accuracy of wavenumber determinations in the infrared region of the spectrum with a scanning spectrometer, see D. H. Rank, G. D. Saksena, G. Skorinko, D. P. Eastman, T. A. Wiggins, T. K. McCubbin, J. Opt. Soc. Amer. 49, 1217 (1959).
[CrossRef]

Barrett, J. J.

A. Weber, S. P. S. Porto, L. E. Cheesman, J. J. Barrett, J. Opt. Soc. Amer. 57, 19 (1967).
[CrossRef]

Cheesman, L. E.

A. Weber, S. P. S. Porto, L. E. Cheesman, J. J. Barrett, J. Opt. Soc. Amer. 57, 19 (1967).
[CrossRef]

Eastman, D. P.

For a comment on the accuracy of wavenumber determinations in the infrared region of the spectrum with a scanning spectrometer, see D. H. Rank, G. D. Saksena, G. Skorinko, D. P. Eastman, T. A. Wiggins, T. K. McCubbin, J. Opt. Soc. Amer. 49, 1217 (1959).
[CrossRef]

Hoag, A. A.

Marchant, J. C.

J. C. Marchant, A. G. Millikan, J. Opt. Soc. Amer. 55, 907 (1965).

May, A. D.

See, for example, A. D. May, G. Varghese, J. C. Stryland, H. L. Welsh, Can. J. Phys. 42, 1058 (1964); K. S. Jammu, G. E. St. John, H. L. Welsh, Can. J. Phys. 44, 797 (1966); D. W. Lepard, D. E. Shaw, H. L. Welsh, Can. J. Phys. 44, 2353 (1966); D. E. Shaw, H. L. Welsh, Can. J. Phys. 45, 3823 (1967).
[CrossRef]

McCubbin, T. K.

For a comment on the accuracy of wavenumber determinations in the infrared region of the spectrum with a scanning spectrometer, see D. H. Rank, G. D. Saksena, G. Skorinko, D. P. Eastman, T. A. Wiggins, T. K. McCubbin, J. Opt. Soc. Amer. 49, 1217 (1959).
[CrossRef]

Miller, W. C.

A. A. Hoag, W. C. Miller, Appl. Opt. 8, 2417 (1969).
[CrossRef] [PubMed]

W. C. Miller, “Reduction of Low Intensity Reciprocity Failure in Photographic Plates by Controlled Baking,” AAS Photo-Bulletin No. 2 (1970), p. 15.

Millikan, A. G.

J. C. Marchant, A. G. Millikan, J. Opt. Soc. Amer. 55, 907 (1965).

Porto, S. P. S.

A. Weber, S. P. S. Porto, L. E. Cheesman, J. J. Barrett, J. Opt. Soc. Amer. 57, 19 (1967).
[CrossRef]

Rank, D. H.

For a comment on the accuracy of wavenumber determinations in the infrared region of the spectrum with a scanning spectrometer, see D. H. Rank, G. D. Saksena, G. Skorinko, D. P. Eastman, T. A. Wiggins, T. K. McCubbin, J. Opt. Soc. Amer. 49, 1217 (1959).
[CrossRef]

Richardson, W. W.

Saksena, G. D.

For a comment on the accuracy of wavenumber determinations in the infrared region of the spectrum with a scanning spectrometer, see D. H. Rank, G. D. Saksena, G. Skorinko, D. P. Eastman, T. A. Wiggins, T. K. McCubbin, J. Opt. Soc. Amer. 49, 1217 (1959).
[CrossRef]

Schrader, H. W.

Skorinko, G.

For a comment on the accuracy of wavenumber determinations in the infrared region of the spectrum with a scanning spectrometer, see D. H. Rank, G. D. Saksena, G. Skorinko, D. P. Eastman, T. A. Wiggins, T. K. McCubbin, J. Opt. Soc. Amer. 49, 1217 (1959).
[CrossRef]

Smith, A. G.

Stryland, J. C.

See, for example, A. D. May, G. Varghese, J. C. Stryland, H. L. Welsh, Can. J. Phys. 42, 1058 (1964); K. S. Jammu, G. E. St. John, H. L. Welsh, Can. J. Phys. 44, 797 (1966); D. W. Lepard, D. E. Shaw, H. L. Welsh, Can. J. Phys. 44, 2353 (1966); D. E. Shaw, H. L. Welsh, Can. J. Phys. 45, 3823 (1967).
[CrossRef]

Varghese, G.

See, for example, A. D. May, G. Varghese, J. C. Stryland, H. L. Welsh, Can. J. Phys. 42, 1058 (1964); K. S. Jammu, G. E. St. John, H. L. Welsh, Can. J. Phys. 44, 797 (1966); D. W. Lepard, D. E. Shaw, H. L. Welsh, Can. J. Phys. 44, 2353 (1966); D. E. Shaw, H. L. Welsh, Can. J. Phys. 45, 3823 (1967).
[CrossRef]

Weber, A.

A. Weber, S. P. S. Porto, L. E. Cheesman, J. J. Barrett, J. Opt. Soc. Amer. 57, 19 (1967).
[CrossRef]

Welsh, H. L.

See, for example, A. D. May, G. Varghese, J. C. Stryland, H. L. Welsh, Can. J. Phys. 42, 1058 (1964); K. S. Jammu, G. E. St. John, H. L. Welsh, Can. J. Phys. 44, 797 (1966); D. W. Lepard, D. E. Shaw, H. L. Welsh, Can. J. Phys. 44, 2353 (1966); D. E. Shaw, H. L. Welsh, Can. J. Phys. 45, 3823 (1967).
[CrossRef]

Wiggins, T. A.

For a comment on the accuracy of wavenumber determinations in the infrared region of the spectrum with a scanning spectrometer, see D. H. Rank, G. D. Saksena, G. Skorinko, D. P. Eastman, T. A. Wiggins, T. K. McCubbin, J. Opt. Soc. Amer. 49, 1217 (1959).
[CrossRef]

Appl. Opt. (2)

Can. J. Phys. (1)

See, for example, A. D. May, G. Varghese, J. C. Stryland, H. L. Welsh, Can. J. Phys. 42, 1058 (1964); K. S. Jammu, G. E. St. John, H. L. Welsh, Can. J. Phys. 44, 797 (1966); D. W. Lepard, D. E. Shaw, H. L. Welsh, Can. J. Phys. 44, 2353 (1966); D. E. Shaw, H. L. Welsh, Can. J. Phys. 45, 3823 (1967).
[CrossRef]

J. Opt. Soc. Amer. (3)

For a comment on the accuracy of wavenumber determinations in the infrared region of the spectrum with a scanning spectrometer, see D. H. Rank, G. D. Saksena, G. Skorinko, D. P. Eastman, T. A. Wiggins, T. K. McCubbin, J. Opt. Soc. Amer. 49, 1217 (1959).
[CrossRef]

J. C. Marchant, A. G. Millikan, J. Opt. Soc. Amer. 55, 907 (1965).

A. Weber, S. P. S. Porto, L. E. Cheesman, J. J. Barrett, J. Opt. Soc. Amer. 57, 19 (1967).
[CrossRef]

Other (2)

W. C. Miller, “Reduction of Low Intensity Reciprocity Failure in Photographic Plates by Controlled Baking,” AAS Photo-Bulletin No. 2 (1970), p. 15.

Kodak Plates and Films for Science and Industry, Kodak Publication P-9, First Edition (Eastman Kodak Co., 1967), pp. 10d–12d.

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Figures (1)

Fig. 1
Fig. 1

The Stokes side of the pure rotational Raman spectrum of borazole (B3N3H6) photographed on Kodak 103a-J (middle spectrum) and baked (53-58)°C for 32.5 h) Kodak IIIa-J (bottom spectrum) plates. The calibration spectrum (top), recorded from the tenth to seventeenth overlapping orders, is that of thorium emitted by a hollow cathode lamp with neon gas filling. Three of the thorium lines are identified in the figure. The Raman spectrum was excited by the λ = 4880 Å line of a mode-locked argon laser, with the multiple-pass Raman cell located inside the laser cavity.7 For each spectrum the exposure time was 3 h. The assignments shown identify the S-branch lines of the 11B3N3H6 symmetric top molecule. The three additional lines that lie in the interval between two neighboring S-branch lines (say between J = 22 and J = 23) are identified as an R-branch line of 11B3N3H6 and an S- and R-branch pair of the quasi-symmetric top molecule 11B210BN3H6. Beyond J = 35 only an S-branch line of 11B210BN3H6 remains visible in the interval.

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