2019MNRAS.484..146E


Query : 2019MNRAS.484..146E

2019MNRAS.484..146E - Mon. Not. R. Astron. Soc., 484, 146-160 (2019/March-3)

Episodic excursions of low-mass protostars on the Hertzsprung-Russell diagram.

ELBAKYAN V.G., VOROBYOV E.I., RAB C., MEYER D.M.-A., GUDEL M., HOSOKAWA T. and YORKE H.

Abstract (from CDS):

Following our recent work devoted to the effect of accretion on the pre-main-sequence evolution of low-mass stars, we perform a detailed analysis of episodic excursions of low-mass protostars in the Hertzsprung-Russell (H-R) diagram triggered by strong mass accretion bursts typical of FU Orionis-type objects (FUors). These excursions reveal themselves as sharp increases in the stellar total luminosity and/or effective temperature of the protostar and can last from hundreds to a few thousands of years, depending on the burst strength and characteristics of the protostar. During the excursions, low-mass protostars occupy the same part of the H-R diagram as young intermediate-mass protostars in the quiescent phase of accretion. Moreover, the time spent by low-mass protostars in these regions is on average a factor of several longer than that spent by the intermediate-mass stars in quiescence. During the excursions, low-mass protostars pass close to the position of most known FUors in the H-R diagram, but owing to intrinsic ambiguity the model stellar evolutionary tracks are unreliable in determining the FUor properties. We find that the photospheric luminosity in the outburst state may dominate the accretion luminosity already after a few years after the onset of the outburst, meaning that the mass accretion rates of known FUors inferred from the bolometric luminosity may be systematically overestimated, especially in the fading phase.

Abstract Copyright: © 2018 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): methods: numerical - circumstellar matter - stars: evolution - stars: flares

Simbad objects: 24

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Number of rows : 24
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* V710 Cas Or* 00 36 45.9936324072 +63 28 52.969968696           ~ 95 0
2 V* V710 Cas B Or* 00 36 46.6000505712 +63 28 57.612490644     15.50     ~ 57 0
3 [SA98] PP 13S* * 04 10 40.8 +38 07 55           ~ 10 0
4 RAFGL 5123 Y*O 04 31 34.07736 +18 08 04.9020           K3V/M3III 900 0
5 V* V883 Ori Or* 05 38 18.1018261392 -07 02 26.017707120           F:I: 274 0
6 JCMTSF J054027.4-072732 IR 05 40 27.4 -07 27 33           ~ 12 0
7 V* V2775 Ori Or* 05 42 48.48792 -08 16 34.7448           ~ 79 0
8 V* FU Ori Or* 05 45 22.3647842544 +09 04 12.291320064   10.72 9.60     F0Iab 888 1
9 V* V1647 Ori Or* 05 46 13.1370578472 -00 06 04.885093296     18.1     M3.9 317 1
10 NGC 2264 OpC 06 40 53.7 +09 52 32           ~ 1876 0
11 V* V912 Mon Or* 06 40 59.3018740704 +09 35 52.389900096         16.50 GIII 37 0
12 V* V900 Mon Or* 06 57 22.2231738936 -08 23 17.690708868   15.94 14.71     ~ 40 0
13 V* Z CMa Ae* 07 03 43.1599411656 -11 33 06.209065836 10.51 9.99 8.80     B5/8eq+F5/7 601 3
14 V* V646 Pup Or* 07 50 35.5923145848 -33 06 23.905800180   13.96 12.65 12.04   ~ 77 0
15 V* GM Cha Or* 11 09 28.55424 -76 33 28.1376           M3.5-M6.5 56 0
16 IRAS 16289-4449 Or* 16 32 32.19264 -44 55 30.6552       15.95   ~ 149 1
17 IRAS 18272+0114 Or* 18 29 49.13016 +01 16 20.6472           ~ 82 1
18 Parsamian 21 Or* 19 29 00.8740757136 +09 38 42.862226208   15.18 14.07 13.93   F5Iabe 95 0
19 V* V1515 Cyg Or* 20 23 48.0158573016 +42 12 25.781279076   15.26 13.39 12.03   G0/G2Ib 260 0
20 V* V2492 Cyg Or* 20 51 26.2367188536 +44 05 23.869354488   20.2   18.3   F-GII/MI 107 0
21 V* V2493 Cyg Or* 20 58 17.0280367392 +43 53 43.341681156   19.678 18.023 17.67 15.233 M4.6 139 0
22 EM* LkHA 190 Or* 20 58 53.7335347296 +44 15 28.388727720   14.26 12.33 12.13   F7/G3I/IIe 530 0
23 EM* LkHA 120 Or* 21 01 09.2070147480 +50 21 44.806779000 13.37 13.09 11.99 11.75   F0/F4-G5 203 1
24 V* V1735 Cyg Or* 21 47 20.6628414360 +47 32 03.857457372           ~ 170 0

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