Abstract

We consider the possibility of a laser that employs Bremsstrahlung radiation.

© 1976 Optical Society of America

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References

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  1. G. Chapline and L. Wood, Phys. Today 28, 40 (1975).
    [Crossref]
  2. D. Marcuse, Bell Syst. Teen. J., September1962, p. 1557–1571. See also D. Marcuse, Engineering Quantum Electrodynamics (Harcourt, Brace, and World, New York, 1970), Chap. 4, Sec. 5.
    [Crossref]
  3. O. S. Lieu and E. E. H. Shin, Appl. Phys. Lett. 20, 511 (1972).
    [Crossref]

1975 (1)

G. Chapline and L. Wood, Phys. Today 28, 40 (1975).
[Crossref]

1972 (1)

O. S. Lieu and E. E. H. Shin, Appl. Phys. Lett. 20, 511 (1972).
[Crossref]

1962 (1)

D. Marcuse, Bell Syst. Teen. J., September1962, p. 1557–1571. See also D. Marcuse, Engineering Quantum Electrodynamics (Harcourt, Brace, and World, New York, 1970), Chap. 4, Sec. 5.
[Crossref]

Chapline, G.

G. Chapline and L. Wood, Phys. Today 28, 40 (1975).
[Crossref]

Lieu, O. S.

O. S. Lieu and E. E. H. Shin, Appl. Phys. Lett. 20, 511 (1972).
[Crossref]

Marcuse, D.

D. Marcuse, Bell Syst. Teen. J., September1962, p. 1557–1571. See also D. Marcuse, Engineering Quantum Electrodynamics (Harcourt, Brace, and World, New York, 1970), Chap. 4, Sec. 5.
[Crossref]

Shin, E. E. H.

O. S. Lieu and E. E. H. Shin, Appl. Phys. Lett. 20, 511 (1972).
[Crossref]

Wood, L.

G. Chapline and L. Wood, Phys. Today 28, 40 (1975).
[Crossref]

Appl. Phys. Lett. (1)

O. S. Lieu and E. E. H. Shin, Appl. Phys. Lett. 20, 511 (1972).
[Crossref]

Bell Syst. Teen. J. (1)

D. Marcuse, Bell Syst. Teen. J., September1962, p. 1557–1571. See also D. Marcuse, Engineering Quantum Electrodynamics (Harcourt, Brace, and World, New York, 1970), Chap. 4, Sec. 5.
[Crossref]

Phys. Today (1)

G. Chapline and L. Wood, Phys. Today 28, 40 (1975).
[Crossref]

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Equations (13)

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n ˙ n = 8 e 6 Z 2 n i n e m 3 v 3 ν 2 ( ln 2 m v 2 h ν - 1 ) .
g = 8 e 6 Z 2 n i n e c m 3 v 3 ν 2 ( ln 2 m v 2 h ν - 1 ) .
g = 3.7 × 10 17 Z 2 n i n e / v 7 .
v D = e 2 E 2 ¯ / m 2 c ω 2 .
v D = S / n e m c 2 ,
p = S / n e c 2 .
S = n c ω ,
S / c 2 = n μ c = n e p ,
l = n = S / c ω ,
l e = 2 3 n e m R v ϕ .
v ϕ = 3 2 ( S / m c n e ω R ) .
tan α = v D v ϕ = 2 3 ω R c = 4 π 3 R λ ,
v ϕ = 3.5 × 10 - 23 P / R 3 .