An upper limit to hydrogen ionization rates from radio recombination-line observations toward 3C123

1984 ◽  
Vol 89 ◽  
pp. 668 ◽  
Author(s):  
H. E. Payne ◽  
E. E. Salpeter ◽  
Y. Terzian
2019 ◽  
Vol 489 (4) ◽  
pp. 4862-4874
Author(s):  
L G Hou ◽  
X Y Gao

ABSTRACT Many of the Spitzer infrared bubbles identified by the Milky Way Project (MWP) are suggested to be $\rm{H \small {II}} $ regions in nature. More than 70 per cent of the ∼5000 known bubbles do not have radio recombination line (RRL) observations, hence have not been confirmed as $\rm{H \small {II}} $ regions. A systematic RRL survey should be helpful to identify the nature of the bubbles. With the Shanghai TianMa 65-m radio telescope, we searched for RRLs towards 216 selected Spitzer bubbles by simultaneously observing 19 RRLs in the C band (4–8 GHz). RRLs are detected in the directions of 75 of the 216 targets. 31 of the 75 RRL sources are classified as new detections, which are possibly from new $\rm{H \small {II}} $ regions or diffuse warm ionized medium; 36 of them are probably from the outskirts of nearby bright $\rm{H \small {II}} $ regions, rather than bubble-encircled ionized gas; and the detected RRLs towards 8 bubbles are identified from known $\rm{H \small {II}} $ regions. For 58 of the 75 RRL sources, we obtained their distances after resolving the kinematic distance ambiguity by combining the results of the H2CO absorption method, the $\rm{H \small {I}} $ emission/absorption method, and the $\rm{H \small {I}} $ self-absorption method. The low detection rate of new $\rm{H \small {II}} $ regions implies that a number of MWP bubbles in the DR1 catalogue are too faint if they are $\rm{H \small {II}} $ regions.


2004 ◽  
Vol 616 (2) ◽  
pp. 783-803 ◽  
Author(s):  
C. A. Rodriguez‐Rico ◽  
F. Viallefond ◽  
J.‐H. Zhao ◽  
W. M. Goss ◽  
K. R. Anantharamaiah

2007 ◽  
Vol 668 (1) ◽  
pp. 625-625 ◽  
Author(s):  
C. A. Rodriguez‐Rico ◽  
W. M. Goss ◽  
F. Viallefond ◽  
J.‐H. Zhao ◽  
Y. Gomez ◽  
...  

1998 ◽  
Vol 15 (1-4) ◽  
pp. 281-289 ◽  
Author(s):  
D. Ershov ◽  
S. A. Gulyaev ◽  
A. Ivanchik ◽  
D. A. Varshalovich ◽  
A. Tsivilev

2021 ◽  
Vol 21 (8) ◽  
pp. 209
Author(s):  
Chuan-Peng Zhang ◽  
Jin-Long Xu ◽  
Guang-Xing Li ◽  
Li-Gang Hou ◽  
Nai-Ping Yu ◽  
...  

1989 ◽  
Vol 136 ◽  
pp. 607-616 ◽  
Author(s):  
K. R. Anantharamaiah ◽  
V. Radhakrishnan ◽  
D. Morris ◽  
M. Vivekanand ◽  
D. Downes ◽  
...  

Several attempts were made to detect the possible radio recombination lines of positronium near the galactic center. An absorption feature seen at λ6cm, in the D-configuration of the VLA was not confirmed by subsequent observations at λ6cm and λ20cm using the B and C configurations of the VLA. An observation at λ3mm using the IRAM 30m telescope also did not detect any line. On the basis of one recombination line photon for every positron (McClintock 1984), our non-detections imply an upper limit to the positron production rate of < 3.1 × 1043 s−1, within about 2″ of the galactic center.


2019 ◽  
Vol 627 ◽  
pp. L6 ◽  
Author(s):  
L. T. Maud ◽  
R. Cesaroni ◽  
M. S. N. Kumar ◽  
V. M. Rivilla ◽  
A. Ginsburg ◽  
...  

We present the highest angular resolution (∼20 × 15 mas–44 × 33 au) Atacama Large Millimeter/sub-millimeter Array (ALMA) observations that are currently possible of the proto-O-star G17.64+0.16 in Band 6. The Cycle 5 observations with baselines out to 16 km probe scales < 50 au and reveal the rotating disc around G17.64+0.16, a massive forming O-type star. The disc has a ring-like enhancement in the dust emission that is especially visible as arc structures to the north and south. The Keplerian kinematics are most prominently seen in the vibrationally excited water line, H2O 55, 0−64, 3 ν2 = 1 (Eu = 3461.9 K). The mass of the central source found by modelling the Keplerian rotation is consistent with 45 ± 10 M⊙. The H30α (231.9 GHz) radio-recombination line and the SiO (5-4) molecular line were detected at up to the ∼10σ level. The estimated disc mass is 0.6 − 2.6 M⊙ under the optically thin assumption. Analysis of the Toomre Q parameter in the optically thin regime indicates that the disc stability is highly dependent on temperature. The disc currently appears stable for temperatures > 150 K; this does not preclude that the substructures formed earlier through disc fragmentation.


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