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Measuring the orbital inclination of Z Andromedae from Rayleigh scattering

A. Skopal, N. Shagatova

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Abstract

\n Context. The orbital inclination of the symbiotic prototype Z And has not been established yet. At present, two very different values are considered, i ~ 44° and i ≳ 73°. The correct value of i is a key parameter in, for example, modeling the highly-collimated jets of Z And. \n Aims. To measure the orbital inclination of Z And. \n Methods. First, we derive the hydrogen column density (nH), which causes the Rayleigh scattering of the far-UV spectrum at the orbital phase φ = 0.961 ± 0.018. Second, we calculate nH as a function of i and φ for the ionization structure during the quiescent phase. Third, we compare the nH(i,φ) models with the observed value. \n Results. The most probable shaping of the H i/H ii boundaries and the uncertainties in the orbital phase limit i of Z And to 59°−2°/+3°. Systematic errors given by using different wind velocity laws can increase i up to ~74°. A high value of i is supported independently by the orbitally related variation in the far-UV continuum and the obscuration of the O i] λ1641 Å emission line around the inferior conjunction of the giant.\n Conclusions. The derived value of the inclination of the Z And orbital plane allows treating satellite components of Hα and Hβ emission lines as highly-collimated jets. \n

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\n Context. The orbital inclination of the symbiotic prototype Z And has not been established yet. At present, two very different values are considered, i ~ 44° and i ≳ 73°. The correct value of i is a key parameter in, for example, modeling the highly-collimated jets of Z And. \n Aims. To measure the orbital inclination of Z And. \n Methods. First, we derive the hydrogen column density (nH), which causes the Rayleigh scattering of the far-UV spectrum at the orbital phase φ = 0.961 ± 0.018. Second, we calculate nH as a function of i and φ for the ionization structure during the quiescent phase. Third, we compare the nH(i,φ) models with the observed value. \n Results. The most probable shaping of the H i/H ii boundaries and the uncertainties in the orbital phase limit i of Z And to 59°−2°/+3°. Systematic errors given by using different wind velocity laws can increase i up to ~74°. A high value of i is supported independently by the orbitally related variation in the far-UV continuum and the obscuration of the O i] λ1641 Å emission line around the inferior conjunction of the giant.\n Conclusions. The derived value of the inclination of the Z And orbital plane allows treating satellite components of Hα and Hβ emission lines as highly-collimated jets. \n

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Available abstract

\n Context. The orbital inclination of the symbiotic prototype Z And has not been established yet. At present, two very different values are considered, i ~ 44° and i ≳ 73°. The correct value of i is a key parameter in, for example, modeling the highly-collimated jets of Z And. \n Aims. To measure the orbital inclination of Z And. \n Methods. First, we derive the hydrogen column density (nH), which causes the Rayleigh scattering of the far-UV spectrum at the orbital phase φ = 0.961 ± 0.018. Second, we calculate nH as a function of i and φ for the ionization structure during the quiescent phase. Third, we compare the nH(i,φ) models with the observed value. \n Results. The most probable shaping of the H i/H ii boundaries and the uncertainties in the orbital phase limit i of Z And to 59°−2°/+3°. Systematic errors given by using different wind velocity laws can increase i up to ~74°. A high value of i is supported independently by the orbitally related variation in the far-UV continuum and the obscuration of the O i] λ1641 Å emission line around the inferior conjunction of the giant.\n Conclusions. The derived value of the inclination of the Z And orbital plane allows treating satellite components of Hα and Hβ emission lines as highly-collimated jets. \n

Key concepts: Context (archaeology), Orbital inclination, Collimated light, Rayleigh scattering, Physics, Scattering, Astrophysics, Orbital elements

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