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SS 433 MAXI 4–10 keV data give a smaller 6.29-day term in 2020–2026 than in 2014–2019 with fixed clocks

We measured a known orbital and precession frequency combination in public SS 433 X-ray data. We fit fixed clocks, calendar-year offsets, and orbital and precession Fourier profiles. In MAXI 4–10 keV data, the fitted semi-amplitude is 1.188 × 10^-3 photon cm^-2 s^-1 in 2014–2019 and 0.200 × 10^-3 in 2020–2026. The early-minus-late amplitude is 0.988 × 10^-3. A full-residual wild calculation with 324-day blocks gives a 95% interval of 0.523–1.305 × 10^-3. A direct test of equal sine and cosine coefficients gives p = 0.0007. Both models allow separate orbital and precession profiles in each interval. The contrast stays positive after a camera calibration date cut, equal weights, eight harmonics, and an updated orbital clock. BAT does not clearly establish the same amplitude change. These exploratory tests assume an adequate mean model and sufficiently independent, symmetric noise blocks. They do not identify a unique physical cause or establish a new period. A joint upper and lower combination fit does not clearly reject equal amplitudes. A noiseless control shows how a precession phase cut can create a large false peak if an orbital harmonic is omitted. We preserve the raw light curves, provenance, selections, coefficients, source code, figures, and repeat instructions.

SS 433 · MAXI · Swift BAT · X-ray binaries · nutation · combination frequencies · time series · sampling window · reproducible research

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References

7
  1. usesSS 433 BAT data from 2014 to 2026 do not identify a separate 6.290-day term under an orbit and precession product model sci:sha256:a768840986aa1e8d5c2fe03814c277c6319daefd96d375f2a4f5782bc71b98f1

    We use its limit on the physical interpretation of an exact orbital and precession combination. We extend the test to MAXI and a direct interval contrast.

  2. usesdoi:10.1093/mnras/stt1715

    This work reports the known hard X-ray signal and gives the fixed orbital and precession clocks used here.

  3. doi:10.1134/S106377371607001X

    This earlier MAXI study describes periodic power and sampling effects in SS 433. Our interval comparison uses later data and a different test.

  4. usesdoi:10.1088/0067-0049/209/1/14

    This paper describes the public Swift/BAT transient monitor data used here.

  5. usesdoi:10.1093/pasj/61.5.999

    This paper describes MAXI, which supplied the public light curves used here.

  6. usesdoi:10.1093/pasj/63.sp3.S635

    This paper describes the MAXI Gas Slit Camera used for the source measurements.

  7. usesdoi:10.1016/j.newast.2023.102060

    We use its quadratic orbital ephemeris for a stated clock check.

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