Angular size of the high energy X-ray source in the Crab nebula
Angular size of high energy X ray source in Crab Nebula from balloon-borne X ray modulation collimator
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Angular size of high energy X ray source in Crab Nebula from balloon-borne X ray modulation collimator
Runaway stars and pulsars near Crab Nebula, discussing binary system explosion and remnant motion
Crab Nebula filametary system, examining excitation conditions in terms of ionization and heating by HF radiation
Crab Nebula pulsar NP 0532 optical timing, measuring frequency, arrival times and pulse interval
Crab Nebula pulsar PSR 0531 plus 21 at 410-1664 MHz, noting mean pulse profiles and spectral indices
Crab Nebula and pulsar NP 0532 X ray spectra discussing pulse profile, emission and interstellar absorption
Crab Nebula emissions on 4 and 6 November 1970, observing optical circular polarization
Crab Nebula pulsar magnetic field structure, discussing linear polarization modifications and wisps
Crab Nebula pulsar NP0532 radio observations, noting long term slowing down and irregular perturbations in periodicity
Crab Nebula model, discussing electromagnetic field time variation and electron acceleration and synchrotron emission
Time variable dispersion of Crab Nebula pulsar, showing coincidence with occultation by solar corona
Crab Nebula pulsar timing observations, correcting arrival times to solar system barycenter and dispersion effect
Tables of Crab Nebula pulsar radio pulse arrival times at Arecibo observatory
Observations of the Crab nebula are described, which were made under the OAO 2/NASA guest-investigator program with WEP stellar photometers. The 10 foot-diameter focal plane diaphragm was ample enough to accept the 4 ft X 6 ft image. The logarithm of the integrated relative intensity per wavelength interval, corrected for sky background, and the rms error, from 11 passbands in the range 4250 to 1380 A, are given. No correction was given for polarization of light. The data were converted to logarithm of the flux density per frequency interval and plotted on scales of log nu (Hz) and of reciprocal microns with two adjustments.
A search in many small regions of the Crab Nebula has resulted in the detection of a small component of circular polarization. The variation of the sign and magnitude with position in the Nebula indicates that the polarization is of interstellar origin. On the basis of the polarity, strength, and colour dependence, it is concluded that the composition of the aligned grains causing this polarization is dielectric. Metallic particles are clearly ruled out. Some stars have also been observed with negative results.
Observations of the Crab Nebula pulsar at meter wavelengths using very long baseline interferometry techniques have been made. At 196.5 MHz, no resolution of the pulsar is observed, all the pulse shapes observed with the interferometers are similar to single-dish profiles, and all the power pulsates. At 111.5 MHz, in addition to the pulsing power, there is always a steady component, presumably due to multipath propagation effects. The pulsar is slightly resolved at 111.5 MHz with an apparent angular diameter of 0.07 plus or minus 0.01 sec. Fifty per cent linear polarization of the time-averaged power is observed at 196.5 MHz; at 111.5 MHz, 20% of the total time-averaged power is polarized, and 35% of the pulsing power is polarized. The steady component is unpolarized. The total flux of the steady plus pulsating component appears to remain constant, while the distribution of power between these components varies.
Results of an occultation experiment carried out on June 14-15, 1969, when the Crab Nebula pulsar passed within 80 min of arc from the center of the sun. For a time interval of two months around this event comparisons are made of the reception times of pulses at frequencies of 111.5, 196.5, and 430 MHz for the purpose of determining the contribution of the solar corona to the integrated electron density along the total path length to the pulsar. For impact parameters between 5 and 12 solar radii the measured integrated densities are not incompatible with those that can be derived from a spherically symmetric Baumbach-Allen model. The systematic differences in density obtained at each observation frequency can be explained in terms of refraction effects.