A Lunar Occultation of the Crab Nebula at 1420 Mc/sec.

1966 ◽  
Vol 71 ◽  
pp. 167 ◽  
Author(s):  
T. Krishnan ◽  
S. H. Zisk ◽  
D. D. Cudaback
Nature ◽  
1964 ◽  
Vol 203 (4941) ◽  
pp. 171-173 ◽  
Author(s):  
B. H. ANDREW ◽  
N. J. B. A. BRANSON ◽  
D. WILLS

Nature ◽  
1975 ◽  
Vol 255 (5508) ◽  
pp. 465-466 ◽  
Author(s):  
Y. FUKADA ◽  
S. HAYAKAWA ◽  
I. KASAHARA ◽  
F. MAKINO ◽  
Y. TANAKA ◽  
...  

1975 ◽  
Vol 201 ◽  
pp. L15 ◽  
Author(s):  
R. Staubert ◽  
E. Kendziorra ◽  
J. Truemper ◽  
C. Reppin ◽  
J. A. Hoffman ◽  
...  

1975 ◽  
Vol 197 ◽  
pp. L83 ◽  
Author(s):  
G. R. Ricker ◽  
S. G. Ryckman ◽  
J. E. Ballintine ◽  
J. P. Doty ◽  
P. M. Downey ◽  
...  

Science ◽  
1964 ◽  
Vol 146 (3646) ◽  
pp. 912-917 ◽  
Author(s):  
S. Bowyer ◽  
E. T. Byram ◽  
T. A. Chubb ◽  
H. Friedman

1959 ◽  
Vol 9 ◽  
pp. 47-49
Author(s):  
B. Elsmore

Observations of a lunar occultation of a radio source may provide information concerning both the distribution of radio “brightness” across the source and its accurate position. For sources of which these results are already fairly well known, observations at long wavelengths may be used to derive the density of the lunar atmosphere [1]. During recent years two such occultations have been observed at Cambridge: one, the occultation of IC 443, the large-diameter radio source in the constellation of Gemini, from which the density of the lunar atmosphere was estimated to be less than 10–12 of that of the density of the terrestrial atmosphere [2] and [3]; and two, the occultation of the Crab nebula on 1956 January 24 [4].


1965 ◽  
Vol 23 ◽  
pp. 227-239 ◽  
Author(s):  
Par S. Bowyer ◽  
E. T. Byram ◽  
T. A. Chubb ◽  
H. Friedman

Ten discrete sources of X-rays have been identified from observations made with Geiger counters aboard unstabilized Aerobee rockets. The distribution of sources is flattened toward the galactic plane. Tau XR-1 is an X-ray source within one arc minute of the center of the Crab Nebula and of angular diameter one arc minute as determined from observation of a lunar occultation. The position of the strongest source, Sco XR-1, is known to about 0.5 degree and the remaining eight sources to about 1.5 degree. Three X-ray sources, Sco XR-1, Cyg XR-1, and Cyg XR-2, are not accompanied by any known optical or radio objects at their positions. Oph XR-1 matches the position of the Kepler SN 1604 and Sgr XR-1 is within 2.3 degrees of Sgr A. The remaining five sources are not sufficiently well resolved or positioned to permit identifications with optical or radio sources. The X-ray flux from the Crab Nebula is compatible with synchrotron spectrum with index — 1.1 and the flux of 1.8 × 10-8 erg cm-2 s-1 (1.5-8 Å) fits the extrapolated optical synchrotron spectrum with the same index.


1987 ◽  
Vol 99 ◽  
pp. 387 ◽  
Author(s):  
A. G. Weisenberger ◽  
J. A. Phillips ◽  
S. T. Gottesman ◽  
T. D. Carr

1966 ◽  
Vol 19 (3) ◽  
pp. 409 ◽  

Measurements of the intensity and percentage linear polarization of the Crab nebula radiation at 404 and 1420 Mc/s were made during the partial occultation of .June 21, 1963. The radio occultation curves are similar in shape to that calculated from the isophotes of the optical continuum and show the same principal features. However, the ratio of radio to optical brightness varies in a systematic way across the source, the ratio being greater at the edges than in the central regions. This steepening of the spectral index towards the outer edges continues in the radio frequency range from 1420 to 404 Mc/s. The 1420 Mc/s linear polarization is stronger in the inner areas (2,5%) than in the outer areas (< 1%) of the source.


1979 ◽  
Vol 234 ◽  
pp. 485 ◽  
Author(s):  
F. P. Maloney ◽  
S. T. Gottesman

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