2005
DOI: 10.1111/j.1365-2966.2005.09368.x
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SS 433: results of a recent multiwavelength campaign

Abstract: We conducted a multiwavelength campaign in 2002 September–October, to observe SS 433. We used the Giant Meter Radio Telescope for radio observations, the Physical Research Laboratory Infrared Telescope at Mt Abu for infrared (IR), the ARIES telescope at Nainital for optical photometry, the telescope at the Vainu Bappu observatory for spectral measurements and the Rossi X‐ray Timing Explorer for X‐ray observations. We find sharp variations in intensity on time‐scales of a few minutes in the X‐ray, IR and radio … Show more

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Cited by 12 publications
(8 citation statements)
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“…However, assuming flare stages are reported with accurate time-stamping and a dependence of these on orbital phase is discerned, we remark that this would be circumstantial evidence that there is ellipticity in the binary orbit of SS433, supporting our discussion in Section 3.1. Chakrabarti et al (2005) present a study of the variability of SS433's emission at radio, IR and optical wavelengths and report that there is typically a delay of 2 d between IR and radio variability. It seems plausible that this delay arises as type-2 flare peaks move from high radio frequency to low radio frequency as bolides expand and thus transition from being optically thick at a given frequency to optically thin.…”
Section: Clustering Timing and Phasing Of Flaresmentioning
confidence: 99%
“…However, assuming flare stages are reported with accurate time-stamping and a dependence of these on orbital phase is discerned, we remark that this would be circumstantial evidence that there is ellipticity in the binary orbit of SS433, supporting our discussion in Section 3.1. Chakrabarti et al (2005) present a study of the variability of SS433's emission at radio, IR and optical wavelengths and report that there is typically a delay of 2 d between IR and radio variability. It seems plausible that this delay arises as type-2 flare peaks move from high radio frequency to low radio frequency as bolides expand and thus transition from being optically thick at a given frequency to optically thin.…”
Section: Clustering Timing and Phasing Of Flaresmentioning
confidence: 99%
“…However, assuming flare stages are reported with accurate time-stamping and a dependence of these on orbital phase is discerned, we remark that this would be circumstantial evidence that there is ellipticity in the binary orbit of SS433, supporting our discussion in Sec 3.1. Chakrabarti et al (2005) present a study of the variability of SS433's emission at radio, infra-red and optical wavelengths and report that there is typically a delay of two days between infrared and radio variability. It seems plausible that this delay arises as type-2 flare peaks move from high radio frequency to low radio frequency as bolides expand and thus transition from being optically thick at a given frequency to optically thin.…”
Section: Clustering Timing and Phasing Of Flaresmentioning
confidence: 99%
“…: [293,90]; evolutionary status: [381]; absorption features from accretion disc wind? : [25]; sharp variations in the X-ray, IR and radio, double X-ray Fe line profiles from the jet: [85]; massive ejection event with a QPO-like feature near 0.1 Hz: [398]; extended radio emission: [48]; X-ray dominated by precessing jets: [551,476]; bullet-like jets: [84]; highly ionized Doppler-shifted iron emission lines: [511]; identifiable deviations from the traditional kinematic model: [49]; rapid chaotic optical variability: [647] Pos. (x 0.6"): [344]; also known as EXO 1912+097: [443]; a HMXB with a NS: [670]; variable absorption column density: [670]; bright iron line: [670] Pos.…”
Section: Conclusion and Remarksmentioning
confidence: 99%