TY - JOUR
T1 - On the infrared coincidence
T2 - What is the jet contribution to the X-ray power law in GX 339–4?
AU - Russell, David M.
N1 - Publisher Copyright:
© 2023 Wiley-VCH GmbH.
PY - 2023/5
Y1 - 2023/5
N2 - The hard X-ray power law, prominent in the hard state in black hole X-ray binaries, is generally due to thermal Comptonization in the corona. Optically thin synchrotron emission from compact jets is commonly seen at infrared wavelengths in the hard state. The extent of this spectrum to higher energies remains uncertain. Here, a multi-wavelength study of GX 339–4 is presented. The infrared (IR) to X-ray spectral index is measured and compared to the X-ray spectral index fitted separately. On some dates in which the jet dominates the IR emission, the X-ray power law and the IR to X-ray power-law spectral indices are both in the range (Formula presented.) (where (Formula presented.)), that is, photon index, (Formula presented.). This suggests they could be the same power law with the same origin, or that this is a coincidence. On other dates in the hard state, (Formula presented.), ruling out a common origin. It is likely that Comptonization dominates on most dates, as expected. However, the X-ray power law never appears to be fainter than the jet power law extrapolated from IR to X-ray, implying that the jet contribution imposes a lower limit to the X-ray flux. If confirmed, this would imply the cooling break in the synchrotron spectrum probably resides at X-ray or higher energies. It is suggested that X-ray spectral fitting should include an extra power law with a break (ideally fit to IR too).
AB - The hard X-ray power law, prominent in the hard state in black hole X-ray binaries, is generally due to thermal Comptonization in the corona. Optically thin synchrotron emission from compact jets is commonly seen at infrared wavelengths in the hard state. The extent of this spectrum to higher energies remains uncertain. Here, a multi-wavelength study of GX 339–4 is presented. The infrared (IR) to X-ray spectral index is measured and compared to the X-ray spectral index fitted separately. On some dates in which the jet dominates the IR emission, the X-ray power law and the IR to X-ray power-law spectral indices are both in the range (Formula presented.) (where (Formula presented.)), that is, photon index, (Formula presented.). This suggests they could be the same power law with the same origin, or that this is a coincidence. On other dates in the hard state, (Formula presented.), ruling out a common origin. It is likely that Comptonization dominates on most dates, as expected. However, the X-ray power law never appears to be fainter than the jet power law extrapolated from IR to X-ray, implying that the jet contribution imposes a lower limit to the X-ray flux. If confirmed, this would imply the cooling break in the synchrotron spectrum probably resides at X-ray or higher energies. It is suggested that X-ray spectral fitting should include an extra power law with a break (ideally fit to IR too).
KW - X-rays: Binaries
KW - accretion
KW - accretion disks
KW - black hole physics
KW - stars: Neutron
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U2 - 10.1002/asna.20230017
DO - 10.1002/asna.20230017
M3 - Article
AN - SCOPUS:85147988976
SN - 0004-6337
VL - 344
JO - Astronomische Nachrichten
JF - Astronomische Nachrichten
IS - 4
M1 - e230017
ER -