Magnetically driven relativistic jet in the high-redshift blazar OH 471

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Volume 685 (May 2024)

A&A, 685 (2024) L11

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Table A.1.

RATAN-600 continuum radiometer parameters.

f₀	Δf₀	ΔF	FWHM_{RA × Dec}
(GHz)	(GHz)	(mJy beam⁻¹)
22.3	2.5	50	$0 \overset{'}{.} 17 \times 1 \overset{'}{.} 6$ $0{{\overset{\prime}{.}}}17 \times 1{{\overset{\prime}{.}}}6$
11.2	1.4	15	$0 \overset{'}{.} 34 \times 3 \overset{'}{.} 2$ $0{{\overset{\prime}{.}}}34 \times 3{{\overset{\prime}{.}}}2$
8.2	1.0	10	$0 \overset{'}{.} 47 \times 4 \overset{'}{.} 4$ $0{{\overset{\prime}{.}}}47 \times 4{{\overset{\prime}{.}}}4$
4.7	0.6	8	$0 \overset{'}{.} 81 \times 7 \overset{'}{.} 6$ $0{{\overset{\prime}{.}}}81 \times 7{{\overset{\prime}{.}}}6$
2.25	0.08	40	$1 \overset{'}{.} 71 \times 15 \overset{'}{.} 8$ $1{{\overset{\prime}{.}}}71 \times 15{{\overset{\prime}{.}}}8$
1.25	0.08	200	$3 \overset{'}{.} 07 \times 27 \overset{'}{.} 2$ $3{{\overset{\prime}{.}}}07 \times 27{{\overset{\prime}{.}}}2$

Notes. The central frequency f₀, the bandwidth Δf₀, the detection limit for point sources per transit ΔF. FWHM_{RA × Dec} is the angular resolution along RA and Dec calculated for the average angles.

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