Data

LBA observations for project V607 semester 2021OCTS

Commonwealth Scientific and Industrial Research Organisation
van Den Eijnden, Jakob ; Miller-Jones, James ; Maccarone, Tom ; Russell, Thomas ; Atri, Pikky
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ctx_ver=Z39.88-2004&rft_val_fmt=info%3Aofi%2Ffmt%3Akev%3Amtx%3Adc&rfr_id=info%3Asid%2FANDS&rft_id=https://data.csiro.au/collection/csiro:CASDA-ATOA-V607-2021OCTS?tab=data DataDownload&rft.title=LBA observations for project V607 semester 2021OCTS&rft.identifier=http://hdl.handle.net/102.100.100/634787?index=1&rft.publisher=Commonwealth Scientific and Industrial Research Organisation&rft.description=High-mass X-ray binaries hosting a neutron star accretor have only recently been detected as radio sources. While for transient systems, their radio emission is likely caused by jets launched from their accretion flow, the origin of this emission remains unconfirmed for the persistently accreting sources. Lacking large variations in accretion properties that can be tied to changes in radio, three options remain for these persistent sources: (i) thermal/free-free stellar wind emission, or non-thermal/synchrotron emission from (ii) jets or (iii) accretion wake shocks. The stellar wind emission is expected to have a low brightness temperature (1e4-1e5 K) and large extent (100-200 binary orbits), especially compared to higher brightness temperatures (up to 1e12 K) possible for the synchrotron processes. Therefore, we propose a 12-hour single-run LBA observation of the radio-brightest neutron star high-mass X-ray binary, 4U 1700-37. If the source is unresolved at a 2 mas resolution, we can rule out the thermal emission scenario from both brightness temperature and size arguments. If the emission is instead resolved, its morphology will distinguish between a wind or jet scenario. Then, we will independently measure the wind mass loss rates and velocity, or the jet emission height, depending on the emission origin, while we place limits on the other mechanism.&rft.creator=van Den Eijnden, Jakob &rft.creator=Miller-Jones, James &rft.creator=Maccarone, Tom &rft.creator=Russell, Thomas &rft.creator=Atri, Pikky &rft.date=2024&rft.edition=v1&rft_rights=Creative Commons Attribution 4.0 International Licence https://creativecommons.org/licenses/by/4.0/&rft_rights=Data is accessible online and may be reused in accordance with licence conditions&rft_rights=All Rights (including copyright) CSIRO 2024.&rft_subject=pulsars&rft_subject=neutron stars&rft_subject=compact binaries and/or black holes&rft_subject=Astronomical sciences not elsewhere classified&rft_subject=Astronomical sciences&rft_subject=PHYSICAL SCIENCES&rft.type=dataset&rft.language=English Access the data

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High-mass X-ray binaries hosting a neutron star accretor have only recently been detected as radio sources. While for transient systems, their radio emission is likely caused by jets launched from their accretion flow, the origin of this emission remains unconfirmed for the persistently accreting sources. Lacking large variations in accretion properties that can be tied to changes in radio, three options remain for these persistent sources: (i) thermal/free-free stellar wind emission, or non-thermal/synchrotron emission from (ii) jets or (iii) accretion wake shocks. The stellar wind emission is expected to have a low brightness temperature (1e4-1e5 K) and large extent (100-200 binary orbits), especially compared to higher brightness temperatures (up to 1e12 K) possible for the synchrotron processes. Therefore, we propose a 12-hour single-run LBA observation of the radio-brightest neutron star high-mass X-ray binary, 4U 1700-37. If the source is unresolved at a 2 mas resolution, we can rule out the thermal emission scenario from both brightness temperature and size arguments. If the emission is instead resolved, its morphology will distinguish between a wind or jet scenario. Then, we will independently measure the wind mass loss rates and velocity, or the jet emission height, depending on the emission origin, while we place limits on the other mechanism.

Available: 2024-04-19

Data time period: 2021-10-01 to 2022-03-31

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ACN 633 798 857