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  1. E. T. Jaynes and F. W. Cummings, Proc. IEEE 51, 89 (1963).
    [Crossref]
  2. M. D. Crisp and E. T. Jaynes, Phys. Rev. 179, 1253 (1969).
    [Crossref]
  3. R. K. Nesbet, Phys. Rev. Letters 27, 553 (1971).
    [Crossref]
  4. See for example, M. Born and E. Wolf, Principles of Optics, 4th ed. (Pergamon, Oxford, 1970), Sec. 2.2.3.
  5. See for example, L. I. Schiff, Quantum Mechanics, 3rd ed. (McGraw–Hill, New York, 1968), Sec. 57.
  6. See for example, P. C. Clemmow, The Plane Wave Spectrum Representation of Electromagnetic Fields (Pergamon, Oxford, 1966).

1971 (1)

R. K. Nesbet, Phys. Rev. Letters 27, 553 (1971).
[Crossref]

1969 (1)

M. D. Crisp and E. T. Jaynes, Phys. Rev. 179, 1253 (1969).
[Crossref]

1963 (1)

E. T. Jaynes and F. W. Cummings, Proc. IEEE 51, 89 (1963).
[Crossref]

Born, M.

See for example, M. Born and E. Wolf, Principles of Optics, 4th ed. (Pergamon, Oxford, 1970), Sec. 2.2.3.

Clemmow, P. C.

See for example, P. C. Clemmow, The Plane Wave Spectrum Representation of Electromagnetic Fields (Pergamon, Oxford, 1966).

Crisp, M. D.

M. D. Crisp and E. T. Jaynes, Phys. Rev. 179, 1253 (1969).
[Crossref]

Cummings, F. W.

E. T. Jaynes and F. W. Cummings, Proc. IEEE 51, 89 (1963).
[Crossref]

Jaynes, E. T.

M. D. Crisp and E. T. Jaynes, Phys. Rev. 179, 1253 (1969).
[Crossref]

E. T. Jaynes and F. W. Cummings, Proc. IEEE 51, 89 (1963).
[Crossref]

Nesbet, R. K.

R. K. Nesbet, Phys. Rev. Letters 27, 553 (1971).
[Crossref]

Schiff, L. I.

See for example, L. I. Schiff, Quantum Mechanics, 3rd ed. (McGraw–Hill, New York, 1968), Sec. 57.

Wolf, E.

See for example, M. Born and E. Wolf, Principles of Optics, 4th ed. (Pergamon, Oxford, 1970), Sec. 2.2.3.

Phys. Rev. (1)

M. D. Crisp and E. T. Jaynes, Phys. Rev. 179, 1253 (1969).
[Crossref]

Phys. Rev. Letters (1)

R. K. Nesbet, Phys. Rev. Letters 27, 553 (1971).
[Crossref]

Proc. IEEE (1)

E. T. Jaynes and F. W. Cummings, Proc. IEEE 51, 89 (1963).
[Crossref]

Other (3)

See for example, M. Born and E. Wolf, Principles of Optics, 4th ed. (Pergamon, Oxford, 1970), Sec. 2.2.3.

See for example, L. I. Schiff, Quantum Mechanics, 3rd ed. (McGraw–Hill, New York, 1968), Sec. 57.

See for example, P. C. Clemmow, The Plane Wave Spectrum Representation of Electromagnetic Fields (Pergamon, Oxford, 1966).

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Equations (15)

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E ( r , t ) = [ ( 3 / r 3 ) p ( t - r / c ) + ( 3 / c r 2 ) p ˙ ( t - r / c ) + ( 1 / c 2 r ) p ¨ ( t - r / c ) ] ( n · ϱ ) ϱ - [ ( 1 / r 3 ) p ( t - r / c ) + ( 1 / c r 2 ) p ˙ ( t - r / c ) + ( 1 / c 2 r ) p ¨ ( t - r / c ) ] n
H ( r , t ) = [ ( 1 / c r 2 ) p ˙ ( t - r / c ) + ( 1 / c 2 r ) p ¨ ( t - r / c ) ] ( n × ϱ ) .
F ( t ) = 2 3 { ( 1 / r 3 ) p ( t - r / c ) p ˙ ( t - r / c ) + ( 1 / c r 2 ) [ p ( t - r / c ) p ¨ ( t - r / c ) + p ˙ 2 ( t - r / c ) ] + ( 2 / c 2 r ) p ˙ ( t - r / c ) p ¨ ( t - r / c ) + ( 1 / c 3 ) p ¨ 2 ( t - r / c ) } = 2 3 { d d t [ p 2 ( t - r / c ) 2 r 3 + p ( t - r / c ) p ˙ ( t - r / c ) c r 2 + p ˙ 2 ( t - r / c ) c 2 r ] + p ¨ 2 ( t - r / c ) c 3 } .
p ( t ) = p 0 f ( t ) cos [ ω t + ϕ ( t ) ] ,
f ˙ ( t ) ω f ( t ) ;             ϕ ˙ ( t ) ω .
F ( t ) = p 0 2 3 [ f ( t ) f ˙ ( t ) r 3 ( 1 + 8 π 2 r 2 λ 2 ) + 1 c r 2 d d t [ f ( t ) f ˙ ( t ) ] + ω 4 c 3 f 2 ( t ) ] ,
( d / d t ) f ( t ) f ˙ ( t ) ω f ( t ) f ˙ ( t ) ,
F ( t ) = 1 3 p 0 2 [ 1 2 r 3 d d t f 2 ( t ) + ω 4 c 3 f 2 ( t ) ] .
p 0 2 f 0 2 / 6 r 3 E = ( p 0 2 ω 4 / 3 c 3 ) 0 f 2 ( t ) d t = ( p 0 2 ω 4 / 6 c 3 ) f 0 2 T ,
T c 3 / r 0 3 ω 4 ,
T = c 3 / r 0 3 ω 4 ,
T q = 3 h c 3 / 4 e 2 ω 3 2 r 1 2 ,
T q ~ T ,
( 1 / 2 r 0 3 ) ( d / d t ) f 2 ( t ) + ω 4 / c 3 f 2 ( t ) = 0.
f ( t ) = f 0 exp ( - t / T ) ,