2008A&A...477....1M


Query : 2008A&A...477....1M

2008A&A...477....1M - Astronomy and Astrophysics, volume 4771-7 (2008/1-1)

Magnetic field upper limits for jet formation.

MASSI M. and KAUFMAN BERNADO M.

Abstract (from CDS):

Very high magnetic fields at the surface of neutron stars or in the accretion disk of black holes inhibit the production of jets. We quantify here the magnetic field strength for jet formation. By using the Alfven Radius, RA, we study what we call the basic condition, RA/R*=1 or RA/RLSO=1 (LSO, last stable orbit), in its dependency on the magnetic field strength and the mass accretion rate, and we analyse these results in 3-D and 2-D plots in the case of neutron star and black hole accretor systems, respectively. For this purpose, we did a systematic search of all available observational data for magnetic field strength and the mass accretion rate. The association of a classical X-ray pulsar (i.e. B∼1012G) with jets is excluded even if accreting at the Eddington critical rate. Z-sources may develop jets for B≲108.2G, whereas Atoll-sources are potential sources of jets if B≲107.7G. It is not ruled out that a millisecond X-ray pulsar could develop jets, at least for those sources where B≲107.5G. In this case the millisecond X-ray pulsar could switch to a microquasar phase during its maximum accretion rate. For stellar-mass black hole X-ray binaries, the condition is that B≲1.35x108G and B≲5x108G at the last stable orbit for a Schwarzschild and a Kerr black hole, respectively. For active galactic nuclei (AGNs), it reaches B≲105.9G for each kind of black hole. These theoretical results are in complete agreement with available observational data.

Abstract Copyright: ∼

Journal keyword(s): stars: magnetic fields - X-rays: binaries - accretion, accretion disks - galaxies: active

Simbad objects: 22

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Number of rows : 22
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 V* V1037 Cas LXB 00 29 03.06 +59 34 19.0           ~ 283 1
2 LS I +61 303 HXB 02 40 31.6644419688 +61 13 45.593918580 11.27 11.61 10.75 10.19 9.55 B0Ve 903 2
3 V* V518 Per HXB 04 21 42.7227473352 +32 54 26.939156184           M4.5V 670 0
4 V* KV UMa HXB 11 18 10.7930420496 +48 02 12.314730120           K5V-M1V 865 0
5 NAME Circinus Galaxy Sy2 14 13 09.906 -65 20 20.47   10.89 9.84 10.6 10.0 ~ 1331 1
6 V* BR Cir HXB 15 20 40.8532547060 -57 10 00.206639033   21.4 21.4     B5-A0I 849 1
7 V* V381 Nor HXB 15 50 58.6637920704 -56 28 35.258385000           K3III 1254 0
8 V* V818 Sco LXB 16 19 55.0692669024 -15 38 25.017666540 11.60 12.40 11.1     Oev 1730 0
9 V* V1033 Sco HXB 16 54 00.1423963019 -39 50 44.761701340       16.14   F3-6IV 1980 0
10 V* V821 Ara LXB 17 02 49.3876391280 -48 47 23.087954544         15.322 ~ 2237 0
11 2E 3938 HXB 17 43 54.7 -29 44 44           ~ 693 1
12 AX J1748.0-2829 LXB 17 48 05.060 -28 28 25.80     13.60     ~ 189 0
13 2CXO J180112.3-254436 HXB 18 01 12.4783119670 -25 44 35.694663099           AV 417 1
14 SAX J1808.4-3658 LXB 18 08 27.58 -36 58 43.9           ~ 1051 0
15 V* V4641 Sgr HXB 18 19 21.6343259256 -25 24 25.849595952     13.654 13.479 13.139 B9III 530 0
16 V* V479 Sct HXB 18 26 15.0561548880 -14 50 54.247274304 12.02 12.23 11.27 11.04   ON6V((f))z 613 2
17 V* V406 Vul HXB 18 58 41.49127200 +22 39 29.7746640           G5V-K0V 409 0
18 SS 433 HXB 19 11 49.5647697480 +04 58 57.827127648   16.854 14.643     A7Ib 2253 4
19 Granat 1915+105 HXB 19 15 11.55576 +10 56 44.9052           ~ 2810 0
20 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4590 0
21 V* V404 Cyg HXB 20 24 03.8247037434 +33 52 01.961154861           G9/K0III/V 1370 0
22 V* V1521 Cyg HXB 20 32 25.78 +40 57 27.9           WN4/5-6/7 2035 2

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