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2.4. The radio counterpart: NVSS J182614−145054 51<br />

Table 2.2: EVN array used in the LS 5039 observations.<br />

Antenna Co<strong>de</strong> Location Diameter DPFU (a) Tsys (b)<br />

[m] [K Jy −1 ] [K]<br />

Effelsberg EB Germany 100 1.47 27<br />

Jodrell Bank JB U.K. 25 0.11 40<br />

Cambridge CM U.K. 32 0.21 38<br />

Westerbork WB Netherlands 14×25 1.0 67<br />

Medicina MC Italy 32 0.15 53<br />

Noto NT Italy 32 0.16 47<br />

Toruń TR Poland 32 0.15 31<br />

(a) Degrees per flux unit. (b) Best value during the experiment.<br />

32 MHz bandwidth. We analyzed the left hand circular polarization data excluding<br />

1 MHz channel at both edges of the band, yielding a final bandwidth of 14 MHz.<br />

The correlator integration time was of 4 s. Standard reduction and imaging analysis<br />

were carried out using aips and difmap.<br />

To complement the amplitu<strong>de</strong> calibration, we interleaved cross-scans (in azimuth<br />

and elevation) with the 100 m Effelsberg antenna to measure the radio source flux<br />

<strong>de</strong>nsities (A. Kraus, private communication). We fitted a Gaussian function to the<br />

flux-<strong>de</strong>nsity response for every cross-scan, and we averaged the different Gaussians.<br />

We linked the flux <strong>de</strong>nsity scale by observing primary calibrators such as 3C 286,<br />

3C 48, or NGC 7027 (see e.g. Kraus 1997 or Peng et al. 2000).<br />

Unfortunately, the flux <strong>de</strong>nsity monitoring with the Effelsberg antenna was not<br />

reliable due to contamination effects by the galactic plane diffuse emission and/or by<br />

the close SNR G016.8−01.1. However, inspection of the shortest MERLIN baselines<br />

reveals a constant flux <strong>de</strong>nsity during the full run. That allowed us to image the<br />

source directly without splitting the data in time blocks. We present the obtained<br />

EVN and MERLIN images in Figs. 2.8 and 2.9, respectively. The MERLIN image is<br />

presented convolved with a circular beam, equivalent in solid angle to the interfero-<br />

metric synthesized beam of 142×46 mas at position angle (P.A.) 1.15 ◦ . Our images<br />

clearly show that LS 5039 has a two-si<strong>de</strong>d jet emanating from a central core. In<br />

both images the southeast (SE) jet is brighter and larger than the northwest (NW)<br />

one, as can be seen in Table 2.3, where we have quoted the flux <strong>de</strong>nsities of the core<br />

and the jets and the lengths and P.A. of the jets. Their total lengths are ∼ 60 mas<br />

in the EVN image and ∼ 300 mas in the MERLIN one.

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