2005A&A...439..635A


Query : 2005A&A...439..635A

2005A&A...439..635A - Astronomy and Astrophysics, volume 439, 635-643 (2005/8-4)

TeV gamma-ray observations of SS-433 and a survey of the surrounding field with the HEGRA IACT-System.

AHARONIAN F., AKHPERJANIAN A., BEILICKE M., BERNLOEHR K., BOERST H.-G., BOJAHR H., BOLZ O., COARASA T., CONTRERAS J., CORTINA J., DENNINGHOFF S., FONSECA V., GIRMA M., GOETTING N., HEINZELMANN G., HERMANN G., HEUSLER A., HOFMANN W., HORNS D., JUNG I., KANKANYAN R., KESTEL M., KOHNLE A., KONOPELKO A., KRANICH D., LAMPEITL H., LOPEZ M., LORENZ E., LUCARELLI F., MANG O., MAZIN D., MEYER H., MIRZOYAN R., MORALEJO A., ONA-WILHELMI E., PANTER M., PLYASHESHNIKOV A., PUEHLHOFER G., DE LOS REYES R., RHODE W., RIPKEN J., ROWELL G.P., SAHAKIAN V., SAMORSKI M., SCHILLING M., SIEMS M., SOBZYNSKA D., STAMM W., TLUCZYKONT M., VITALE V., VOELK H.J., WIEDNER C.A. and WITTEK W.

Abstract (from CDS):

We present results of a search for TeV γ-ray emission from the microquasar SS-433 and the surrounding region covering a ∼8°x8° field of view. Analysis of data taken with the HEGRA stereoscopic system of imaging atmospheric Cerenkov imaging telescopes reveals no evidence of steady or variable emission from any position. Observation times of over 100 h have been achieved in central parts of the field of view. We set 99% confidence level upper limits to a number of a-priori-chosen objects of interest, including SS-443 and its interaction regions, 32 pulsars, 3 supernova remnants and the GeV source GeV J1907+0537. Our upper limit of 3.2% Crab flux (for energies E>0.8TeV) for the eastern-lobe region e3 of SS-433 permits, after comparison with X-ray fluxes, a lower limit of B≥19 µG on the post-shocked magnetic field in this region. An ensemble upper limit at 0.3% Crab flux (E>0.7TeV) from a subset (11) of the 32 pulsars implies a maximum of 4.5% of the spin-down pulsar power is available for TeV γ-ray production. For one of the SNR in our FoV, 3C 396, recent Chandra observations suggest that a central pulsar-driven wind nebula may be the source of X-ray emission. Our upper limit implies that a maximum of 0.1% of the spin-down power from the central source of 3C 396 would be available for TeV γ-rays.

Abstract Copyright:

Journal keyword(s): gamma rays: observations - stars: individual: SS-433

Nomenclature: Table 3, Fig.3: [AAB2005] SS 433 Knot N (Nod 2, 3).

CDS comments: In Abstract GEV J1907+0537 is a probable misprint for GEV J1907+0557.

Simbad objects: 44

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Number of rows : 44
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 PSR B1858+04.1 Psr 19 01 10.3 +04 13 51           ~ 16 0
2 PSR B1859+03 Psr 19 01 31.7700 +03 31 04.960           ~ 140 0
3 PSR B1859+07 Psr 19 01 38.936 +07 16 34.80     14.03     ~ 75 0
4 PSR J1902+0723 Psr 19 02 13.54 +07 23 51.0           ~ 11 0
5 PSR B1900+05 Psr 19 02 42.620 +05 56 25.92           ~ 78 0
6 PSR B1900+06 Psr 19 02 50.277 +06 16 33.45           ~ 55 0
7 2EG J1903+0529 Q? 19 03 54.0 +05 31 17           ~ 32 1
8 PSR J1904+0800 Psr 19 04 03.50 +08 00 52.6           ~ 14 0
9 SNR G039.2-00.3 SNR 19 04 03.9 +05 26 56           ~ 192 1
10 PSR B1902+04.1 Psr 19 04 31.382 +04 12 05.90           ~ 23 0
11 PSR B1902+06.1 Psr 19 05 06.849 +06 16 16.70           ~ 21 0
12 PSR B1903+07 Psr 19 05 53.62 +07 09 19.4           ~ 37 0
13 PSR B1904+06 Psr 19 06 35.244 +06 41 02.90           ~ 49 0
14 SNR G040.5-00.5 SNR 19 07.2 +06 31           ~ 90 0
15 PSR J1907+0345 Psr 19 07 14.54 +03 45 10.6           ~ 10 0
16 AX J1907.4+0549 X 19 07 21.3 +05 49 14           ~ 5 0
17 SNR G041.1-00.3 SNR 19 07 22.6 +07 10 44           ~ 228 2
18 PSR B1904+05.5 Psr 19 07 23.34 +05 34 53.0           ~ 6 0
19 PSR B1905+07.5 Psr 19 07 44.118 +07 40 22.60           ~ 9 0
20 PSR J1907+06 Psr 19 07 54.751 +06 02 15.79           ~ 128 0
21 PSR J1908+0500 Psr 19 08 05.162 +05 00 54.45           ~ 14 0
22 PSR B1905+04 Psr 19 08 16.15 +04 57 41.0           ~ 12 0
23 PSR J1908+0734 Psr 19 08 17.010 +07 34 14.36           ~ 35 0
24 PSR B1905+08.5 Psr 19 08 18.51 +08 39 59.2           ~ 10 0
25 PSR B1907+02 Psr 19 09 38.3210 +02 54 49.900           ~ 84 0
26 PSR B1907+06.1 Psr 19 09 51.21 +06 16 51.8           ~ 8 0
27 [SO97] w2 reg 19 10 +05.0           ~ 4 0
28 PSR B1907+03 Psr 19 10 09.06 +03 58 28.0     14.10     ~ 88 0
29 PSR J1910+0714 Psr 19 10 18.597 +07 14 11.80           ~ 21 0
30 PSR B1907+05.4 Psr 19 10 26.51 +05 34 09.0           ~ 6 0
31 SS 433 HXB 19 11 49.5647697480 +04 58 57.827127648   16.854 14.643     A3/7I 2123 4
32 SNR G039.7-02.0 SNR 19 12 20 +04 55.0           ~ 353 1
33 PSR B1910+08.4 Psr 19 13 00.50 +08 32 05.1           ~ 21 0
34 PSR J1913+0446 Psr 19 13 50.82 +04 46 06.0           ~ 13 0
35 PSR J1915+07 Psr 19 15 01.94 +07 52 09.2           ~ 12 0
36 PSR J1915+0738 Psr 19 15 24.80 +07 38 31.4           ~ 11 0
37 PSR J1916+07 Psr 19 16 51.5 +07 48 00           ~ 11 0
38 PSR J1918+08 Psr 19 17 48.853 +08 34 54.63           ~ 12 0
39 PSR J1918+0734 Psr 19 18 +07.6           ~ 2 0
40 PSR B1923+04 Psr 19 26 24.4600 +04 31 31.900           ~ 66 0
41 [SO97] w1 reg ~ ~           ~ 2 0
42 [SO97] e1 reg ~ ~           ~ 4 0
43 [SO97] e3 reg ~ ~           ~ 4 0
44 [SO97] e2 reg ~ ~           ~ 4 0

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