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  1. Harold Lamport and Hans Zinsser (to be published).
  2. Erich W. Marchand (personal communication, January10, 1958).I am grateful for Dr. Marchand’s response to our inquiry. He has informed me that the substance of his reply will be sent as a letter to the Editor of this Journal.

Lamport, Harold

Harold Lamport and Hans Zinsser (to be published).

Marchand, Erich W.

Erich W. Marchand (personal communication, January10, 1958).I am grateful for Dr. Marchand’s response to our inquiry. He has informed me that the substance of his reply will be sent as a letter to the Editor of this Journal.

Zinsser, Hans

Harold Lamport and Hans Zinsser (to be published).

Other (2)

Harold Lamport and Hans Zinsser (to be published).

Erich W. Marchand (personal communication, January10, 1958).I am grateful for Dr. Marchand’s response to our inquiry. He has informed me that the substance of his reply will be sent as a letter to the Editor of this Journal.

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Figures (1)

Fig. 1
Fig. 1

The average distribution of light flux by a narrow slit vibrating harmonically, 20% amplitude modulated at a much lower frequency. The values near the carrier amplitude (A)±20% are not calculated because the width of the slit is not negligible in these regions. Instead, the values are estimated to provide a continuous curve, the estimated part being represented as a broken line.

Equations (4)

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I x 0 = c / ( D 2 - x 0 2 ) 1 2 x 0 2 < D 2 .
i x 0 = 2 T - T / 4 T / 4 I x 0 d t             and             D = A ( 1 + m sin ω t ) , i x 0 = 2 c A T - T / 4 T / 4 d t [ ( 1 + m sin ω t ) 2 - b 2 ] 1 2 ,
i x 0 = c π A ( 1 m B ) 1 2 K [ ( b / B ) 1 2 ] ,
i x 0 = c π A ( 1 2 m B ) 1 2 K [ ( B / b ) 1 2 ] .