2026A&A...706A.241L


Query : 2026A&A...706A.241L

2026A&A...706A.241L - Astronomy and Astrophysics, volume 706A241 (2026/2-1)

A scaling relationship for nonthermal radio emission from ordered magnetospheres II. Investigating the efficiency of relativistic electron production in the magnetospheres of BA-type stars.

LETO P., OWOCKI S., TRIGILIO C., CAVALLARO F., DAS B., SHULTZ M.E., BUEMI C.S., UMANA G., FOSSATI L., IGNACE R., KRTICKA J., OSKINOVA L.M., PILLITTERI I., BORDIU C., BUFANO F., CERRIGONE L., INGALLINERA A., LORU S., RIGGI S., RUGGERI A.C., UD-DOULA A. and LEONE F.

Abstract (from CDS):

Context. Magnetic BA-type stars typically host dipole-like magnetospheres. When detected as nonthermal radio sources, their luminosities are correlated with the stellar magnetic field and rotation speed. Rotation is crucial because the mechanism undergirding the relativistic electron production is powered by centrifugal breakouts (CBOs). Small-scale breakouts occur wherever magnetic tension does not balance out the centrifugal force, resulting in magnetic reconnection and particle acceleration.
Aims. To investigate how physical conditions at the site of the CBOs affect the efficiency of the nonthermal electron acceleration mechanism, we broadly explore the parameter space governing radio emission by increasing the available sample of radio-loud magnetic stars.
Methods. High-sensitivity VLA observations of 32 early-type magnetic stars were performed in the hope of identifying new centrifugally supported magnetospheres (CMs) and associated CBOs. We calculated the radio spectra produced by the gyrosynchrotron emission mechanism using a 3D modeling of a dipole-shaped corotating magnetosphere. We evaluated combinations of stellar parameters and equatorial thermal plasma densities. The number of relativistic electrons was constrained by the need to produce the emission level predicted by the well-known empirical scaling relationship for the radio emission from magnetic BA stars.
Results. About half of the observed early-type magnetic stars were detected, with radio luminosities that show an excellent agreement with the expected values, reinforcing the robust nature of the scaling relationship for CBO-powered radio emission. Comparing the competing centrifugal and magnetic effects on plasma locked in a rigidly rotating magnetosphere, we located the site of CBOs and inferred the local plasma density. We then estimated the efficiency of the CBO-powered acceleration mechanism needed to produce enough nonthermal electrons to support the expected radio emission level.
Conclusions. Given a constant acceleration efficiency, relativistic electrons represent a fixed fraction of the local thermal plasma. Thus, we find that dense magnetospheres host many more energetic particles than less dense ones; consequently, with the other parameters remaining similar, they are shown to be intrinsically brighter radio sources.

Abstract Copyright: © The Authors 2026

Journal keyword(s): acceleration of particles - magnetic reconnection - radiation mechanisms: non-thermal - stars: early-type - stars: magnetic field - radio continuum: stars

Simbad objects: 36

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Number of rows : 36
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* CG And a2* 00 00 43.6344938328 +45 15 12.007059804   6.299 6.347     A0IIspSiSrHg 161 0
2 * gam02 Ari PM* 01 53 31.8129284424 +19 17 37.879979172   4.49 4.52     A2IVpSiSrCr 162 0
3 * gam01 Ari PM* 01 53 31.8192032943 +19 17 45.430793660   4.558 4.589 6.71   A0Vnp_lB 85 0
4 * nu. For a2* 02 04 29.4455576134 -29 17 48.496908718 4.01 4.52 4.69 4.73 4.87 B9.5IIIspSi 153 0
5 * iot Cas a2* 02 29 03.94780 +67 24 08.9170           A3IIIpSr+F5V 268 0
6 HD 21699 Pu* 03 32 08.6084197968 +48 01 24.528548676 4.81 5.355 5.461     B9III 220 0
7 V* HZ Aur a2* 05 06 08.3584818960 +33 55 07.279039380   7.03 7.07     B9p 194 0
8 V* V1099 Ori Pu* 05 32 13.0812769464 -01 36 01.745707500 7.6 8.18 8.29     B8II 107 0
9 * 12 CMa a2* 06 47 01.4835271104 -21 00 55.451696472 5.27 5.89 6.08     B7II/III 152 0
10 V* V592 Mon a2* 06 50 42.3030217728 -08 02 27.587802588 6.31 6.29 6.29     B9V 120 0
11 * 26 CMa Pu* 07 12 12.2147085456 -25 56 33.316082736 5.03 5.736 5.897     B2IV/V 93 0
12 * 49 Cam a2* 07 46 27.4146675768 +62 49 49.882910592   6.750 6.458     A7VpSrCrEuSiKsn 146 0
13 * 53 Cam a2* 08 01 42.4403874648 +60 19 27.806833200   6.177 6.008     A3VpSrSiCrEu 410 0
14 HD 74067 a2* 08 40 19.1757463872 -40 15 49.936471416   5.18 5.22     kB8hA0III(CrEu) 76 0
15 * bet Hya a2* 11 52 54.52149 -33 54 29.2672 3.85 4.18 4.28 4.27 4.35 kB8hB8HeA0VSi 110 0
16 * 84 UMa a2* 13 46 35.6567876472 +54 25 57.643558644   5.632 5.675     A0VpSrCrEu 168 0
17 V* V828 Cen a2* 14 03 27.4674533712 -41 25 24.032196948   5.986 6.088     ApSi 102 0
18 V* CS Vir a2* 14 18 38.2505609712 -18 42 57.465294264 5.86 5.90 5.90     ApSi(Cr) 322 0
19 * mu. Lib ** 14 49 19.05130 -14 08 56.4766 5.33 5.38 5.31     ApSrEuCr 122 0
20 HD 133029 a2* 15 00 38.7178984848 +47 16 38.791986348   6.250 6.351     A0VspSiSrCr 222 0
21 * bet CrB a2* 15 27 49.7540595700 +29 06 20.494640434 4.08 3.97 3.68 3.50 3.45 F2VpSrCrEuSi 703 0
22 * chi Ser a2* 15 41 47.4147355608 +12 50 51.093705840 5.42 5.37 5.33 5.28 5.32 A2VpMnEu(Sr) 194 0
23 V* BP Boo a2* 15 42 50.7602109000 +52 21 39.243860316   5.430 5.482     A0VpSiCr 140 0
24 HD 142184 Be* 15 53 55.8637866220 -23 58 41.143370530 4.77 5.352 5.402     B2V 261 1
25 V* V928 Sco a2* 15 57 48.8021454576 -23 31 38.294134176   6.755 6.771     B8/9III 123 0
26 V* V952 Sco a2* 16 10 15.9221226696 -26 54 32.879906064   6.634 6.587     ApSi 93 0
27 * rho Oph A SB* 16 25 35.1185711280 -23 26 49.831640736 4.3 5.22 5.05     B1V 444 0
28 V* V773 Her a2* 16 36 42.9385265832 +15 29 50.827223688   6.296 6.355     A2VpSiSrCr 114 0
29 HD 151346 Ro* 16 47 46.5285400080 -23 58 27.525918576 8.12 8.31 7.90     B8II 92 0
30 * 52 Her a2* 16 49 14.21821 +45 58 59.9620   4.914 4.823     A1VpSiSrCr 267 0
31 HD 164224 * 18 00 57.6150005880 -20 59 17.208523788   8.67 8.49     ApSiCr 27 0
32 HD 168856 * 18 22 10.8205486968 -07 29 55.602976200   7.13 7.05     ApSi 48 0
33 HD 175132 * 18 52 07.2499320864 +41 22 59.680929396   6.187 6.269     B9IIIpSi 62 0
34 HD 182180 * 19 24 30.1801035096 -27 51 57.389455476 5.22 5.889 6.011     B2Vnn 128 0
35 HD 183339 Pu* 19 25 46.7645404704 +58 01 38.356203360 5.88 6.450 6.594     B7IV 95 0
36 HD 345439 Be* 19 58 48.4896519480 +23 05 21.559730172   11.61 11.11 11.37   B1V-B2V 41 0

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