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References

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  1. J. N. Howard, Appl. Opt. 4, 676 (1965).
  2. S. S. Ballard, Appl. Opt. 4, 219 (1965).
    [Crossref]
  3. G. Wald, Science 150, 1239 (1965).
    [Crossref] [PubMed]
  4. M. Born, E. Wolf, Principles of Optics (The Macmillan Company, New York, 1964), p. 180.
  5. W. N. Hartley, J. Chem. Soc. 43, 390 (1883).
    [Crossref]
  6. H. Kayser, Tabelle der Schwingunzszahlen (S. Hirzel, Leipzig, 1925).
  7. Rayleigh (J. W. Strutt), Nature 27, 559 (1883).
    [Crossref]
  8. Natl. Bur. Std. Tech. News Bull. 48, 61 (1964).
  9. IEEE Std. No. 260 (Jan.1965).

1965 (4)

1964 (1)

Natl. Bur. Std. Tech. News Bull. 48, 61 (1964).

1883 (2)

W. N. Hartley, J. Chem. Soc. 43, 390 (1883).
[Crossref]

Rayleigh (J. W. Strutt), Nature 27, 559 (1883).
[Crossref]

Ballard, S. S.

Born, M.

M. Born, E. Wolf, Principles of Optics (The Macmillan Company, New York, 1964), p. 180.

Hartley, W. N.

W. N. Hartley, J. Chem. Soc. 43, 390 (1883).
[Crossref]

Howard, J. N.

Kayser, H.

H. Kayser, Tabelle der Schwingunzszahlen (S. Hirzel, Leipzig, 1925).

Rayleigh,

Rayleigh (J. W. Strutt), Nature 27, 559 (1883).
[Crossref]

Wald, G.

G. Wald, Science 150, 1239 (1965).
[Crossref] [PubMed]

Wolf, E.

M. Born, E. Wolf, Principles of Optics (The Macmillan Company, New York, 1964), p. 180.

Appl. Opt. (2)

IEEE Std. No. 260 (1)

IEEE Std. No. 260 (Jan.1965).

J. Chem. Soc. (1)

W. N. Hartley, J. Chem. Soc. 43, 390 (1883).
[Crossref]

Natl. Bur. Std. Tech. News Bull. (1)

Natl. Bur. Std. Tech. News Bull. 48, 61 (1964).

Nature (1)

Rayleigh (J. W. Strutt), Nature 27, 559 (1883).
[Crossref]

Science (1)

G. Wald, Science 150, 1239 (1965).
[Crossref] [PubMed]

Other (2)

M. Born, E. Wolf, Principles of Optics (The Macmillan Company, New York, 1964), p. 180.

H. Kayser, Tabelle der Schwingunzszahlen (S. Hirzel, Leipzig, 1925).

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Figures (2)

Fig. 1
Fig. 1

Optical excitation of dry air at 35 mtorr 80 keV protons.

Fig. 2
Fig. 2

The radiant energy spectrum.

Equations (11)

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d x / d λ = f d θ / d λ ,
d ( sin θ - sin i ) = m λ ,
d x / d λ = m f / ( d cos θ ) .
d x / d λ = f ( b / a ) ( d η / d λ ) ,
ν ¯ = 1 / λ .
λ vac = η λ air
ν ¯ vac = 1 / η λ air ,
ν = v / λ = c / η λ ,
E = h ν = h c / η λ .
1 THz 10 12 c / s .
1 μ ~ 10 , 000 Å ~ 10 , 000 cm - 1 ~ 300 THz ~ 1.24 eV .

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