2011
DOI: 10.1088/2041-8205/732/2/l27
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Extremely Broad Radio Recombination Maser Lines Toward the High-Velocity Ionized Jet in Cepheus a Hw2

Abstract: We present the first detection of the H40α, H34α and H31α radio recombination lines (RRLs) at millimeter wavelengths toward the high-velocity, ionized jet in the Cepheus A HW2 star forming region. From our single-dish and interferometric observations, we find that the measured RRLs show extremely broad asymmetric line profiles with zero-intensity linewidths of ∼1100 km s −1 . From the linewidths, we estimate a terminal velocity for the ionized gas in the jet of ≥500 km s −1 , consistent with that obtained from… Show more

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Cited by 34 publications
(28 citation statements)
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“…∼ 270 km/s in low-mass stars to ∼ 1000 km/s in high-mass stars . The average velocity of optical jets is ∼ 750 km/s (Mundt & Ray 1994), a value comparable to Jiménez-Serra et al (2011) and Martí et al (1998) estimates of ∼ 500 km/s in Cepheus A HW2 and HH 80-81 respectively. Whereas the average velocity in optical jets is ∼ 750 km/s, a value of v t = 500 km/s, estimated via proper motion of a radio jet (Martí et al 1998) was adopted as a reasonable approximation of the sample's jets' terminal velocity, in calculating the mass loss rate.…”
Section: Mass Loss Ratesupporting
confidence: 68%
“…∼ 270 km/s in low-mass stars to ∼ 1000 km/s in high-mass stars . The average velocity of optical jets is ∼ 750 km/s (Mundt & Ray 1994), a value comparable to Jiménez-Serra et al (2011) and Martí et al (1998) estimates of ∼ 500 km/s in Cepheus A HW2 and HH 80-81 respectively. Whereas the average velocity in optical jets is ∼ 750 km/s, a value of v t = 500 km/s, estimated via proper motion of a radio jet (Martí et al 1998) was adopted as a reasonable approximation of the sample's jets' terminal velocity, in calculating the mass loss rate.…”
Section: Mass Loss Ratesupporting
confidence: 68%
“…Extremely broad millimeter recombination lines of a possible maser nature have been reported from the high-velocity ionized jet Cep A HW2 (Jiménez-Serra et al 2011). In this case, the difference between the LTE and non-LTE models is less than a factor of two and in some of the transitions it is necessary to multiply the non-LTE model intensities by a factor of several to agree with the observations.…”
Section: Non-lte Radio Recombination Linesmentioning
confidence: 89%
“…A possible drawback of (sub)mm RLs is that the free-free continuum may be contaminated by dust emission. Another problem is that they are out of LTE more easily than cm lines, so their interpretation may require careful modeling (e.g., Jiménez-Serra et al 2011;Peters et al 2012). As shown below, our simple LTE interpretation seems to be reasonable, but it is possible that a significant fraction of the 1.3-mm continuum comes from dust in the line of sight.…”
Section: Appendix A: Linewidth Of Recombination Linesmentioning
confidence: 89%