2002ApJ...577..322M


Query : 2002ApJ...577..322M

2002ApJ...577..322M - Astrophys. J., 577, 322-336 (2002/September-3)

Toward an empirical theory of pulsar emission. VII. On the spectral behavior of conal beam radii and emission heights.

MITRA D. and RANKIN J.M.

Abstract (from CDS):

In this paper we return to the old problem of conal component pair widths and profile dimensions. Observationally, we consider a set of 10 pulsars with prominent conal component pairs for which well-measured profiles exist over the largest frequency range now possible. Apart from some tendency to narrow at high frequency, the conal components exhibit almost constant widths. We use all three profile measures, the component separation as well as the outside half-power and 10% widths, to determine conal beam radii, which are the focus of our subsequent analysis. These radii at different frequencies are well fitted by a relationship introduced by Thorsett, but the resulting parameters are highly correlated. Three different types of behavior are found: one group of stars exhibits a continuous variation of beam radius that can be extrapolated down to the stellar surface along the ``last open field lines'', a second group exhibits beam radii that asymptotically approach a minimum high-frequency value that is 3-5 times larger, and a third set shows almost no spectral change in beam radius at all. The first two behaviors are associated with outer-cone component pairs, whereas the constant separation appears to reflect inner-cone emission. The first group, remarkably, can be fitted by a Thorsett relation in which the constant term is constrained to be the field tangent direction at the edge of the polar cap ρpc, but the others cannot. The first group can also be fitted well using an index of -(1)/(3), but the second group cannot. We first compute heights from the conal beam radii, assuming dipolar fields and emission along the last open field lines, which we find are again well fitted by a suitable Thorsett relation. Here we find that the first group can be fitted using a constant term hpcof 10 km and also that the first two groups are remarkably well fitted by an index of -(2)/(3). We then argue that physical emission heights can be estimated using the component separation along an interior annulus of field lines having their ``feet'' about halfway out on the polar cap–such values agree well with most existing height values based on physical criteria. Therefore, we find that ``radius-to-frequency'' mapping is associated with outer-cone component pairs. The near constant behavior of inner cones is thus arresting. We explore possible interrelationships between the spectral behavior of the component and profile widths produced by both the field line flaring and the changing sight line geometry. We also attempt to understand the physical implications of the parameter values resulting from the Thorsett relation fits.

Abstract Copyright: ∼

Journal keyword(s): Magnetohydrodynamics: MHD - Plasmas - Stars: Pulsars: General - Radiation Mechanisms: Nonthermal

CDS comments: p. 334 (note 5) : PSR 0402-61 is a misprint for 0402+61 ?

Simbad objects: 33

goto Full paper

goto View the references in ADS

Number of rows : 33
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 B0148-06 Psr 01 51 22.71800 -06 35 02.9800           ~ 112 0
2 PSR B0149-16 Psr 01 52 10.85400 -16 37 53.6300           ~ 130 0
3 PSR B0301+19 Psr 03 04 33.115 +19 32 51.40           ~ 247 0
4 PSR B0329+54 Psr 03 32 59.3370698592 +54 34 45.028206408           ~ 690 1
5 PSR B0402+61 Psr 04 06 30.0806 +61 38 41.408           ~ 90 1
6 PSR B0450-18 Psr 04 52 34.11900 -17 59 23.1500           ~ 203 1
7 PSR B0450+55 Psr 04 54 07.709 +55 43 41.51           ~ 174 0
8 PSR B0523+11 Psr 05 25 56.49800 +11 15 18.8000           ~ 125 1
9 PSR B0525+21 Psr 05 28 52.308 +22 00 01.00     14.30     ~ 370 0
10 PSR B0751+32 Psr 07 54 40.688 +32 31 56.20           ~ 88 0
11 PSR B0834+06 Psr 08 37 05.64620 +06 10 15.8700           ~ 472 0
12 PSR B0919+06 Psr 09 22 13.85000 +06 38 19.0000           ~ 329 1
13 PSR B1133+16 Psr 11 36 03.09460 +15 51 15.9000           ~ 715 0
14 PSR B1221-63 Psr 12 24 22.2740 -64 07 53.834           ~ 122 0
15 PSR B1237+25 Psr 12 39 40.386 +24 53 49.87           ~ 497 1
16 PSR B1451-68 Psr 14 56 00.0175876848 -68 43 40.034742348           ~ 203 0
17 PSR B1508+55 Psr 15 09 25.674 +55 31 32.90           ~ 322 1
18 PSR B1541+09 Psr 15 43 38.82000 +09 29 16.4000           ~ 215 1
19 PSR B1604-00 Psr 16 07 12.078 -00 32 40.98           ~ 228 1
20 PSR B1702-19 Psr 17 05 36.09300 -19 06 39.2000           ~ 191 1
21 PSR B1706-16 Psr 17 09 26.45200 -16 40 59.2000           ~ 247 0
22 PSR B1727-47 Psr 17 31 42.21000 -47 44 38.7000           ~ 166 0
23 PSR B1737+13 Psr 17 40 07.3455 +13 11 56.690           ~ 191 0
24 PSR B1747-46 Psr 17 51 42.18500 -46 57 26.7200           ~ 124 0
25 PSR B1818-04 Psr 18 20 52.5920 -04 27 37.120           ~ 230 0
26 PSR B1821+05 Psr 18 23 30.9731 +05 50 24.310           ~ 136 0
27 PSR B1839+09 Psr 18 41 55.92100 +09 12 07.2900           ~ 134 0
28 PSR B1857-26 Psr 19 00 47.54200 -26 00 44.8000           ~ 195 1
29 PSR B1919+21 Psr 19 21 44.815 +21 53 02.25           ~ 411 0
30 PSR B2020+28 Psr 20 22 37.0671 +28 54 23.104           ~ 330 1
31 PSR B2044+15 Psr 20 46 39.33600 +15 40 33.6000           ~ 109 0
32 PSR B2045-16 Psr 20 48 35.74000 -16 16 45.0000           ~ 344 0
33 PSR B2319+60 Psr 23 21 55.213 +60 24 30.71     13.80     ~ 200 0

To bookmark this query, right click on this link: simbad:objects in 2002ApJ...577..322M and select 'bookmark this link' or equivalent in the popup menu