Contains report on one research project.National Aeronautics and Space Administration (Grant NGL 22-009-016)National Science Foundation (Grant GP-14854)National Science Foundation (Grant GP-13056

Batchelor, R. A.

Ewing, M. S.

Price, R. M.

Staelin, David H.

Sutton, J. M.

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II. RADIO ASTRONOMYAcademic and Research StaffProf. A. H. Barrett Prof. D. H. Staelin R. A. BatchelorProf. B. F. Burke J. W. Barrett D. C. PapaProf. R. M. Price C. A. ZapataGraduate StudentsM. S. Ewing P. C. Myers J. W. WatersH. F. Hinteregger G. D. Papadopoulos A. R. WhitneyP. L. Kebabian P. W. Rosenkranz T. T. Wilheit, Jr.C. A. Knight P. R. Schwartz W. J. WilsonA. PULSAR OBSERVATIONSHigh time resolution observations at 115 MHz and 150 MHz have confirmed themarching subpulse behavior of CP1919 and AP2015+28 reported by Drake and Craft,Iand have revealed similar behavior in MP0031 and CP0808 (Fig. II-1). The marchingpatterns for all four pulsars slope in the same sense; i. e., subpulses occur slightlyearlier within the average pulse window with each succeeding pulse. Similar, but moreambiguous, results have been obtained for CP0834.Drake and Craft described the phenomenon by a single parameter, the Class 2Period P2', which is the mean separation of the marching or Class 2 pulses and is muchshorter than the basic pulsar period P 1 and incommensurate with it. We define a thirdperiod, the pattern period P 3, as the time between successive appearances of Class 2pulses in a given time window of the average pulse. Values of P', P2, and P 3 aregiven in Table I-i.Each of the marching patterns in Fig. II-1 can be represented by a series ofsloping lines connecting the Class 2 pulses in consecutive pulses. The average separa-tions of these lines, P 2 and P3' are approximately unchanged from day to day and monthto month, but the slopes and separations of individual lines show variations of ~+20%.In the case of MP0031, the width of the Class 2 pulses is approximately 0. 2 P 2, whichshows that the modulation process is not sinusoidal.The pulsars MP0031 and CP1919 also exhibit periodicities in pulse intensity of theorder of 2 min and 6 min, respectively. The slow periodic variations were first notedin MP0031, as illustrated in Fig. 11-2. On this strip chart record the pulse intensitiesvary, with a period of ~2 min. Examination of several hours of MP0031 data suggeststhat the effect is often, but not always, evident, and that the period sometimes varies20% or more over several minutes. The day-to-day variation does not appear to beThis work was supported by the National Aeronautics and Space Administration(Grant NGL 22-009-016) and the National Science Foundation (Grants GP-14854 andGP- 13056).QPR No. 97600 50TIME (MILLISECONDS)10050S40-S30 -z)2010'X9I999I9XX9XIX.•XIXXXXX * *XXXX *" .xxlxx. . 9.• *XIX* * xxxf:!NI IsIx• eX..(X"° • °XX** *° .o•**xx..*IXXXX Kexx* - *°9 ..XX*X#I4!XX • •*XXIXX*X#I(III 9XX('I X•*X II II*XX! !X CXIIx x-- X# .xx.'.X..XX*....XN#O X°x *x99..xx... ....• 9# X XXI (a-- i , ,, a.. xs .. ..xxxxx x.. :!!Xx- X,(:-xxrXI I" ~**XXXX * * *II0 20. X...••X ,-- , --" ---p (b)40 60TIME (MILLISECONDS)Systematic variations of pulse shape observed for (a) MP0031 and(b) CP0808 on August 13, 1969. Each horizontal line representsa time window centered approximately on the average pulse, andsuccessive windows are separated precisely by the pulsar period.Relative intensities: 1 (.), 2 (X), 3 (#). Filter-bank resolution100 kHz. Sweep ranges: (a) 155-151 MHz, (b) 151-143 MHz.QPR No. 976050403020*XX***** ...XX X*XXX*X°.•Fig. II- 1.~°Table II-1. Periodicities in pulsars.Pulsar P 1  P 2  P 3(s) (ms) (s)0031 0.943 58 6.80808 1. 292 53 14.40834 1.274 110 2.741919 1. 337 15. 5 5. 92015 0.558 10.7* 2. 62F. D. Drake231 (1968).and H. D. Craft, Jr., Nature 220,Fig. II-2. Strip chart record of pulses from MP0031 recordedat 158. 5 MHz (upper) and 112. 5 MHz (lower).QPR No. 97(II. RADIO ASTRONOMY)much greater. A suggestion of the short-term variation is evident in Fig. 11-2.The 2-min periodicity is also evident in pulse-intensity spectra. Four pulse-intensity spectra of MP0031, observed at different times and at different frequencies,are shown in Fig. 1I-3. The spectra were computed by first extracting the strengthsMP 003100092 Hz140 MHz 8/1200051 HzCP 1919230 MHz 11/10Fig. 11- 3.Pulse intensity spectra for MP0031(upper four spectra), and CP1919(lower four spectra). Spectra illus-trate the periodic behavior of pulsebursts. Spectra were computed using512 and 1024 pulses for MP0031 andCP1919, respectively. The dates indi-cate when the data were recorded in1969.110 MHz 8/14140 MHz 8/14140 MHz 8/130 00029 Hz 2 3 4 x 10-2 HzFREQUENCYof 512 consecutive pulses from 30-ms sampled data observed with a 50-channel radiom-eter. The strengths of each of the 512 pulses were integrated over bandwidths ofeither 1.5 MHz or 5.0 MHz, after the effects of dispersion were removed by a computer.These 512 numbers were then Fourier-transformed to yield the illustrated spectra.The spectra at 140, 142. 5, and 166 MHz peak at frequencies corresponding to periodsof 196, 108, and 137 s, respectively. These variations in period appear to be a func-tion of time rather than of observing frequency, and are compatible with those inferredfrom the strip chart records. At 230 MHz the effect is generally less evident.Another important feature of this new periodicity is also evident in Fig. II-1,particularly in the upper trace, recorded at 158. 8 MHz. That is, the pulse-intensitypattern which repeats at -2-min intervals is neither sinusoidal nor impulsive; rather,QPR No. 97 n(II. RADIO ASTRONOMY)it appears to be composed of more than one burst event, each event repeating at -2-minintervals and each appearing or fading independently. The upper trace appears to bedominated by two events, each of which survives -15 min. Detection of the periodicityis sometimes more difficult because the entire 2-min period is active, or at other timesbecause the period may vary more than 20%/ over many minutes.A second pulsar exhibiting these properties is CP1919 for which 1024-pulse powerdensity spectra are shown in Fig. 11-3. The spectra peak at -0. 0029 Hz, which cor-responds to a period of -345 s. In each case, two or three harmonics are also evident.The harmonics apparently arise from the short duration of the individual burst events.CP1919 is more stable than MP0031, but is similar, in that the effect is less evidentat 230 MHz. Pulse strengths vary in a fashion similar to that for MP0031, so that oneor two excited regions are typically present, each region surviving approximately20-30 min. These excited regions may develop or fade either abruptly or slowly, andoccasionally only an isolated burst is seen which does not repeat in the following cycle.The repetitive appearance of pulse-intensity patterns with more than one excitedregion supports the suggestion that some sort of waves are circulating about the pulsarand modulating the pulse intensity. Although such waves could conceivably reside onthe surface of the star, it is more likely that they are waves in the circumpulsar plasma,and although they could circulate along a complex spatial trajectory, it seems morelikely that they would travel in an approximately circular orbit. Each burst of pulsesthen corresponds to a region of this circulating plasma ring which favors pulse emis-sion. These enhancement regions survive approximately 10-20 min and may come orgo abruptly. By monitoring the waxing and waning of such regions it may be possibleto learn something about the meteorology of the plasma envelope surrounding the star,under the assumption that this plasma circulation model is correct.One very interesting aspect of the long-period phenomenon is that it may be relatedto the second periodicity discovered by Drake and Craft.IOne possible interpretation of the second-periodicity phenomenon is that those wavescirculating about the pulsar producing the long-period variations also have short-periodwaves associated with them producing the short-term variations. If the long-period andshort-period waves circulate about the star at the same angular velocities, then the longperiod, designated P 4 , must be related to the other periods asPP3P P4 P22This "period equation" predicts values of the circulation period of P4 of 111 s and 509 sfor MP0031 and CP1919, respectively, based on nonsimultaneous measurements of P 2and P 3 (Sutton et al. 2). The predicted P 4 of 111 s for MP0031 is 32% less than the meanof the representative periods evident in Fig. II-2,that is, 196, 108, and 137 s, and theQPR No. 97(II. RADIO ASTRONOMY)predicted P4 of 509 s for CP1919 is 47% greater than the observed 345 s. A smallamount of data is available which permits P 2, P 3, and P4 to be measured simulta-neously. On one occasion the predicted P 4 for MP0031 was 154 s, 36% more than theobserved value.D. H. Staelin, R. M. Price, M. S. Ewing,R. A. Batchelor, J. M. Sutton(Dr. John M. Sutton is with the National Radio Astronomy Observatory, Greenbank,West Virginia.)References1. F. D. Drake and H. D. Craft, Jr., Nature 220, 231 (1968).2. J. M. Sutton, D. H. Staelin, R. M. Price, and R. Weimer, Astrophys. J. 159, L89(1970).QPR No. 97

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