2011ApJ...727...92M


Query : 2011ApJ...727...92M

2011ApJ...727...92M - Astrophys. J., 727, 92 (2011/February-1)

Toward an empirical theory of pulsar emission. IX. On the peculiar properties and geometric regularity of lyne and manchester's "partial cone" pulsars.

MITRA D. and RANKIN J.M.

Abstract (from CDS):

Lyne & Manchester identified a group of some 50 pulsars they called "partial cones" which they found difficult to classify and interpret. They were notable for their asymmetric average profiles and asymmetric polarization position angle (PPA) traverses, wherein the steepest gradient (SG) point fell toward one edge of the total intensity profile. Over the last two decades, this population of pulsars has raised cautions regarding the core/cone model of the radio pulsar emission beam which implies a high degree of order, symmetry, and geometric regularity. In this paper, we reinvestigate this population "partial cone" pulsars on the basis of new single pulse polarimetric observations of 39 of them, observed with the Giant Meterwave Radio Telescope in India and the Arecibo Observatory in Puerto Rico. These highly sensitive observations help us to establish that most of these "partial cones" exhibit a core/cone structure just as did the "normal" pulsars studied in the earlier papers of this series. In short, we find that many of these "partial cones" are partial in the sense that the emission above different areas of their polar caps can be (highly) asymmetric. However, when studied closely we find that their emission geometries are overall identical to a core/double cone structure encountered earlier–that is, with specific conal dimensions scaling as the polar cap size. Further, the "partial cone" population includes a number of stars with conal single profiles that are asymmetric at meter wavelengths for unknown reasons (e.g., like those of B0809+74 or B0943+10). We find that aberration-retardation appears to play a role in distorting the core/cone emission-beam structure in rapidly rotating pulsars. We also find several additional examples of highly polarized pre- and postcursor features that do not appear to be generated at low altitude but rather at high altitude, far from the usual polar flux tube emission sites of the core and conal radiation.

Abstract Copyright: ∼

Journal keyword(s): magnetohydrodynamics, MHD - methods: data analysis - polarization - pulsars: general - radiation mechanisms: non-thermal

Simbad objects: 60

goto Full paper

goto View the references in ADS

Number of rows : 60
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 PSR B0138+59 Psr 01 41 39.938 +60 09 32.30     12.85     ~ 120 0
2 PSR B0254-53 Psr 02 55 56.2925 -53 04 21.275           ~ 71 0
3 PSR B0329+54 Psr 03 32 59.3370698592 +54 34 45.028206408           ~ 690 1
4 PSR B0355+54 Psr 03 58 53.7165 +54 13 13.727           ~ 465 1
5 PSR B0450+55 Psr 04 54 07.709 +55 43 41.51           ~ 174 0
6 PSR B0525+21 Psr 05 28 52.308 +22 00 01.00     14.30     ~ 370 0
7 V* CM Tau Psr 05 34 31.9474694616 +22 00 52.153698024           ~ 5476 0
8 PSR B0540+23 Psr 05 43 09.65 +23 29 06.1     14.40     ~ 278 0
9 PSR B0643+80 Psr 06 53 15.090 +80 52 00.22           ~ 65 0
10 PSR B0656+14 Psr 06 59 48.18800 +14 14 19.2000   24.85 24.90     ~ 943 1
11 PSR B0740-28 Psr 07 42 49.0730 -28 22 43.510           ~ 445 0
12 PSR B0809+74 Psr 08 14 59.500 +74 29 05.70           ~ 425 0
13 PSR B0834+06 Psr 08 37 05.64620 +06 10 15.8700           ~ 472 0
14 PSR B0906-17 Psr 09 08 38.22700 -17 39 39.9000           ~ 100 0
15 PSR B0919+06 Psr 09 22 13.85000 +06 38 19.0000           ~ 329 1
16 PSR B0943+10 Psr 09 46 07.31 +09 51 57.3           ~ 364 1
17 PSR B1054-62 Psr 10 56 25.5840 -62 58 47.690           ~ 94 0
18 PSR B1055-52 Psr 10 57 59.0450 -52 26 56.330           ~ 757 0
19 PSR B1112+50 Psr 11 15 38.400 +50 30 12.29           ~ 154 0
20 PSR B1221-63 Psr 12 24 22.2740 -64 07 53.834           ~ 122 0
21 PSR B1237+25 Psr 12 39 40.386 +24 53 49.87           ~ 497 1
22 PSR B1240-64 Psr 12 43 17.2912183824 -64 23 23.082548820           ~ 119 0
23 PSR B1322+83 Psr 13 21 45.6315 +83 23 39.432           ~ 70 0
24 PSR B1356-60 Psr 13 59 58.2480 -60 38 07.550           ~ 131 0
25 PSR B1426-66 Psr 14 30 40.73200 -66 23 05.5460           ~ 102 0
26 PSR B1449-64 Psr 14 53 32.6546 -64 13 16.047           ~ 158 0
27 PSR B1530+27 Psr 15 32 10.3646 +27 45 49.623           ~ 122 0
28 PSR B1530-53 Psr 15 34 08.3012586672 -53 34 20.547404184           ~ 80 0
29 PSR B1540-06 Psr 15 43 30.1373 -06 20 45.332           ~ 131 1
30 PSR B1556-44 Psr 15 59 41.5290 -44 38 45.740           ~ 140 0
31 PSR B1604-00 Psr 16 07 12.078 -00 32 40.98           ~ 228 1
32 PSR B1612+07 Psr 16 14 40.906 +07 37 31.00           ~ 101 0
33 PSR B1641-45 Psr 16 44 49.28482 -45 59 09.6360     12.60     ~ 217 0
34 PSR B1648-42 Psr 16 51 48.79700 -42 46 09.9700           ~ 72 0
35 PSR B1700-18 Psr 17 03 51.10200 -18 46 13.0000           ~ 64 0
36 PSR B1732-07 Psr 17 35 04.9730 -07 24 52.130           ~ 74 0
37 PSR B1742-30 Psr 17 45 56.30810 -30 40 23.3000           ~ 182 0
38 PSR B1745-12 Psr 17 48 17.4310 -13 00 53.400           ~ 68 0
39 PSR B1756-22 Psr 17 59 24.16400 -22 05 33.0000           ~ 60 0
40 PSR B1822-09 Psr 18 25 30.62000 -09 35 22.0000           ~ 382 0
41 PSR B1842+14 Psr 18 44 54.8946 +14 54 14.120           ~ 127 0
42 PSR B1851-14 Psr 18 54 44.3000 -14 21 19.000           ~ 41 0
43 PSR B1859+07 Psr 19 01 39.02000 +07 16 33.6000     14.03     ~ 88 0
44 PSR B1900+05 Psr 19 02 42.60000 +05 56 25.8000           ~ 86 0
45 PSR B1907-03 Psr 19 10 29.7137636760 -03 09 54.925338636           ~ 62 0
46 PSR B1910+20 Psr 19 12 43.3391 +21 04 33.926           ~ 81 0
47 PSR B1913+10 Psr 19 15 29.99300 +10 09 43.5800           ~ 102 0
48 PSR B1915+13 Psr 19 17 39.79400 +13 53 57.1600           ~ 190 0
49 PSR B1919+21 Psr 19 21 44.815 +21 53 02.25           ~ 411 0
50 PSR B1924+16 Psr 19 26 45.322 +16 48 32.78           ~ 90 0
51 PSR B1930+22 Psr 19 32 22.8565447656 +22 20 52.063074024     14.52     ~ 149 0
52 PSR B1937-26 Psr 19 41 00.41690 -26 02 05.8840           ~ 84 0
53 PSR B1944+22 Psr 19 46 24.89 +22 44 59.4     14.20     ~ 37 0
54 PSR B1944+17 Psr 19 46 53.044 +18 05 41.24           ~ 252 0
55 PSR B2021+51 Psr 20 22 49.8730 +51 54 50.233           ~ 288 1
56 PSR B2043-04 Psr 20 46 00.17600 -04 21 26.3000           ~ 87 0
57 PSR B2053+36 Psr 20 55 31.3552 +36 30 21.489           ~ 103 0
58 PSR B2217+47 Psr 22 19 48.139 +47 54 53.93           ~ 230 0
59 PSR B2223+65 Psr 22 25 52.8627 +65 35 36.371           ~ 342 0
60 PSR B2327-20 Psr 23 30 26.98600 -20 05 29.7500           ~ 133 0

To bookmark this query, right click on this link: simbad:objects in 2011ApJ...727...92M and select 'bookmark this link' or equivalent in the popup menu