2007A&A...461..669R


Query : 2007A&A...461..669R

2007A&A...461..669R - Astronomy and Astrophysics, volume 461669-678 (2007/1-2)

A deep XMM-Newton X-ray observation of the Chamaeleon I dark cloud.

ROBRADE J. and SCHMITT J.H.M.M.

Abstract (from CDS):

Low-mass stars are known to exhibit strong X-ray emission during the early stages of evolution. Nearby star forming regions are ideal targets to study the X-ray properties of pre-main sequence stars. A deep XMM-Newton exposure is used to investigate X-ray properties of the pre-main sequence population of the Chamaeleon I star forming region. The northern-eastern fringe of the Chameleon I dark cloud was observed with XMM-Newton, revisiting a region observed with ROSAT 15years ago. Centered on the extended X-ray source CHXR 49 we are able to resolve it into three major contributing components and to analyse their spectral properties. Furthermore, the deep exposure allows not only the detection of numerous, previously unknown X-ray sources, but also the investigation of variability and the study of the X-ray properties for the brighter targets in the field. We use EPIC spectra, to determine X-ray brightness, coronal temperatures and emission measures for these sources, compare the properties of classical and weak-line T Tauri stars and make a comparison with results from the ROSAT observation. X-ray properties of T Tauri stars in Cha I are presented. The XMM-Newton images resolve some previously blended X-ray sources, confirm several possible ones and detect many new X-ray targets, resulting in the most comprehensive list with 71 X-ray sources in the northern Cha I dark cloud. The analysis of medium resolution spectra shows an overlapping distribution of spectral properties for classical and weak-line T Tauri stars, with the X-ray brighter stars having hotter coronae and a higher LX/Lbol ratio. X-ray luminosity correlates with bolometric luminosity, whereas the LX/Lbol ratio is slightly lower for the classical T Tauri stars. Large flares as well as a low iron and a high neon abundance are found in both types of T Tauri stars. Abundance pattern, plasma temperatures and emission measure distributions during quiescent phases are attributed to a high level of magnetic activity as the dominant source of their X-ray emission.

Abstract Copyright: ∼

Journal keyword(s): stars: activity - stars: coronae - stars: late-type - stars: pre-main sequence - X-rays: stars

VizieR on-line data: <Available at CDS (J/A+A/461/669): table4.dat>

Nomenclature: Table 4: CHXX NN (Nos 1-71).

CDS comments: Table 4: The first number 71 is a misprint for 70!

Simbad objects: 82

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Number of rows : 82
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* BP Tau Or* 04 19 15.8339827632 +29 06 26.926959492   13.13 12.12 11.89   K5/7Ve 721 0
2 V* T Tau TT* 04 21 59.4319873992 +19 32 06.432393336   11.22 10.12 9.80   K0IV/Ve 1456 1
3 M 42 HII 05 35 16.8 -05 23 15           ~ 4411 0
4 V* TW Hya TT* 11 01 51.9053285064 -34 42 17.033218380   11.94 10.50 10.626 9.18 K6Ve 2144 1
5 NAME Cha 1 MoC 11 06 48 -77 18.0           ~ 1266 1
6 CHXX 1 X 11 07 58.1 -76 24 43           ~ 1 0
7 CHXX 2 * 11 08 17.4601960704 -76 16 34.631175216           ~ 1 0
8 CHXX 3 * 11 09 02.7880822272 -76 15 03.455147160           ~ 1 0
9 HJM C 1-15 Or* 11 09 13.8188326128 -76 28 39.682556400         13.91 M4Ve 37 0
10 [CCE98] 1-74 TT* 11 09 17.6942588064 -76 27 57.926988648   15.48 13.92   11.72 K4Ve 51 0
11 V* HU Cha Or* 11 09 18.12888 -76 30 29.2500         14.99 M1/2e 57 0
12 V* VZ Cha Or* 11 09 23.7739008528 -76 23 20.857480836   13.82 12.94   12.14 K7e 162 0
13 CHXX 8 X 11 09 31.7 -76 18 18           ~ 1 0
14 CHX 15b Or* 11 09 40.0612946232 -76 28 39.236612160   15.68 14.04   11.66 K8Ve 43 0
15 CHXX 10 X 11 09 49.3 -76 19 32           ~ 1 0
16 CHXX 11 X 11 09 51.3 -76 27 16           ~ 2 0
17 V* HX Cha Or* 11 09 54.062760 -76 29 25.54332       16.08 14.03 M3.5+M7 73 0
18 V* WY Cha Or* 11 10 07.0339153464 -76 29 37.674167388   15.29 13.87   11.62 K8Ve 95 1
19 CHXX 14 X 11 10 08.5 -76 15 55           ~ 1 0
20 CHXX 15 X 11 10 08.8 -76 19 43           ~ 1 0
21 CHXX 16 LM* 11 10 22.2523149192 -76 25 13.841167332         16.58 M8.0 42 0
22 CHXX 17 X 11 10 22.7 -76 27 16           ~ 2 0
23 CHXX 18 X 11 10 25.4 -76 20 07           ~ 1 0
24 CHXX 19 X 11 10 27.4 -76 27 17           ~ 2 0
25 CHXX 20 X 11 10 29.8 -76 23 09           ~ 1 0
26 CHXX 21 X 11 10 33.1 -76 20 55           ~ 1 0
27 2XMM J111042.3-761911 AG? 11 10 42.2 -76 19 13           ~ 2 0
28 2MASS J11105039-7618145 * 11 10 50.3965129680 -76 18 14.615139636           ~ 2 0
29 CHXR 81 AG? 11 10 52.2803289048 -76 26 22.490530872           ~ 3 0
30 CHXX 24 X 11 10 52.4 -76 15 32           ~ 1 0
31 CHXR 80 AG? 11 10 52.7 -76 28 10           ~ 5 0
32 [GK2001] 38 Y*O 11 10 53.2 -76 16 53           ~ 2 0
33 CHXX 27 * 11 10 53.3323478208 -76 16 55.940314476           ~ 1 0
34 CHXX 28 * 11 10 53.9929143144 -76 14 29.037143400           ~ 1 0
35 CHXX 29 X 11 10 55.6 -76 16 29           ~ 1 0
36 [GK2001] 40 Y*O 11 10 58.2 -76 17 56           ~ 3 0
37 2MASS J11105830-7617580 * 11 10 58.2919102968 -76 17 57.872465376           ~ 1 0
38 CHXX 31 X 11 11 04.2 -76 24 28           ~ 1 0
39 CHXX 32 X 11 11 13.8 -76 20 02           ~ 1 0
40 CHXX 33 * 11 11 30.5039285160 -76 20 03.048340200           ~ 1 0
41 CHXX 34 X 11 11 39.6 -76 23 07           ~ 1 0
42 V* XX Cha Or* 11 11 39.6728641032 -76 20 15.032221548   16.67 15.28   12.56 M3Ve 137 1
43 CHXX 36 X 11 11 44.2 -76 12 49           ~ 1 0
44 CHX 18N TT* 11 11 46.3370290776 -76 20 08.948823324   13.27 11.96   10.37 K5IVe 93 1
45 CHXX 38 X 11 11 49.1 -76 30 31           ~ 2 0
46 CHX 18 X 11 11 49.8 -76 19 48           ~ 64 1
47 Hn 15 Y*O 11 11 54.024360 -76 19 30.93132   16.02 14.37 13.98 11.88 M2.5+M3.5 27 1
48 CHXX 40 X 11 12 03.9 -76 26 10           ~ 1 0
49 CHXX 41 X 11 12 05.3 -76 19 00           ~ 1 0
50 CHXX 42 X 11 12 05.6 -76 31 38           ~ 2 0
51 CHXX 43 * 11 12 06.4919534976 -76 19 31.173269016           ~ 1 0
52 Sz 40 Or* 11 12 09.8312703024 -76 34 36.490702728   15.2     13.41 M4.5Ve 79 0
53 CHXX 45 X 11 12 17.5 -76 19 16           ~ 1 0
54 CHXX 46 * 11 12 18.8416209936 -76 17 39.929587836           ~ 1 0
55 CHXX 47 X 11 12 20.1 -76 31 44           ~ 2 0
56 2XMM J111222.2-761838 AG? 11 12 22.2 -76 18 38           ~ 2 0
57 CHXX 49 X 11 12 22.9 -76 23 08           ~ 1 0
58 CHXR 53 Y*O 11 12 27.7473960768 -76 25 29.181423144   16.22 14.72     M3V 16 0
59 CHXX 51 X 11 12 34.8 -76 26 54           ~ 1 0
60 CHXX 52 * 11 12 40.4575749528 -76 08 19.732437276           ~ 1 0
61 CHXX 53 X 11 12 41.2 -76 10 56           ~ 1 0
62 CHXX 54 X 11 12 53.0 -76 13 55           ~ 1 0
63 Hn 18 Or* 11 13 24.4522663344 -76 29 22.868165508         13.51 M4Ve 53 0
64 CHXR 58 AG? 11 13 27.021 -76 31 46.97         15.97 ~ 3 0
65 HJM E 1-4 Or* 11 13 27.3678427440 -76 34 16.632434316   15.96 14.35   12.10 K8Ve 32 0
66 2MASS J11132747-7620175 SB* 11 13 27.4719317160 -76 20 17.558565432           ~ 7 0
67 CHXR 60 X 11 13 28.0 -76 29 10           M4.25 21 0
68 CHXX 59 X 11 13 28.1 -76 13 10           ~ 1 0
69 Hn 19 Or* 11 13 29.6961323352 -76 29 01.376928888         13.42 M4Ve 38 0
70 CHXX 61 X 11 13 34.2 -76 15 38           ~ 1 0
71 CHXX 62 X 11 13 46.2 -76 26 46           ~ 1 0
72 CHXX 63 X 11 14 05.6 -76 18 51           ~ 1 0
73 CHXX 64 X 11 14 15.2 -76 21 41           ~ 1 0
74 Hn 20 Or* 11 14 15.5356101936 -76 27 36.568161144         13.24 M4Ve 32 0
75 2MASS J11142906-7625399 Or* 11 14 29.0610261864 -76 25 40.118842992     17.73   14.46 M5.5e 16 0
76 CHXX 66 * 11 14 29.0773903488 -76 11 49.098644160           ~ 1 0
77 CHXX 68 X 11 14 42.5 -76 10 19           ~ 1 0
78 CHXX 69 X 11 14 46.5 -76 24 14           ~ 1 0
79 CHXX 70 X 11 14 49.3 -76 22 49           ~ 1 0
80 CHXX 71 X 11 15 11.0 -76 20 24           ~ 1 0
81 NAME Chamaeleon Region SFR 11 55 -78.0           ~ 887 0
82 HD 319139 SB* 18 14 10.4818675368 -32 47 34.516836060   11.47 10.68   9.11 K5+K7 423 0

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