ACTIVE REGION FILAMENTS MIGHT HARBOR WEAK MAGNETIC FIELDS
ABSTRACT Recent spectropolarimetric observations of active region filaments have revealed polarization profiles with signatures typical of the strong field Zeeman regime. The conspicuous absence in those observations of scattering polarization and Hanle effect signatures was then pointed out by some...
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Published in: | The Astrophysical journal Vol. 822; no. 1; p. 50 |
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Abstract | ABSTRACT Recent spectropolarimetric observations of active region filaments have revealed polarization profiles with signatures typical of the strong field Zeeman regime. The conspicuous absence in those observations of scattering polarization and Hanle effect signatures was then pointed out by some authors. This was interpreted as either a signature of mixed "turbulent" field components or as a result of optical thickness. In this article, we present a natural scenario to explain these Zeeman-only spectropolarimetric observations of active region (AR) filaments. We propose a two-component model, one on top of the other. Both components have horizontal fields, with the azimuth difference between them being close to 90°. The component that lies lower in the atmosphere is permeated by a strong field of the order of 600 G, while the upper component has much weaker fields, of the order of 10 G. The ensuing scattering polarization signatures of the individual components have opposite signs, so its combination along the line of sight reduces-and even can cancel out-the Hanle signatures, giving rise to an apparent Zeeman-only profile. This model is also applicable to other chromospheric structures seen in absorption above ARs. |
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AbstractList | ABSTRACT Recent spectropolarimetric observations of active region filaments have revealed polarization profiles with signatures typical of the strong field Zeeman regime. The conspicuous absence in those observations of scattering polarization and Hanle effect signatures was then pointed out by some authors. This was interpreted as either a signature of mixed "turbulent" field components or as a result of optical thickness. In this article, we present a natural scenario to explain these Zeeman-only spectropolarimetric observations of active region (AR) filaments. We propose a two-component model, one on top of the other. Both components have horizontal fields, with the azimuth difference between them being close to 90°. The component that lies lower in the atmosphere is permeated by a strong field of the order of 600 G, while the upper component has much weaker fields, of the order of 10 G. The ensuing scattering polarization signatures of the individual components have opposite signs, so its combination along the line of sight reduces-and even can cancel out-the Hanle signatures, giving rise to an apparent Zeeman-only profile. This model is also applicable to other chromospheric structures seen in absorption above ARs. Recent spectropolarimetric observations of active region filaments have revealed polarization profiles with signatures typical of the strong field Zeeman regime. The conspicuous absence in those observations of scattering polarization and Hanle effect signatures was then pointed out by some authors. This was interpreted as either a signature of mixed “turbulent” field components or as a result of optical thickness. In this article, we present a natural scenario to explain these Zeeman-only spectropolarimetric observations of active region (AR) filaments. We propose a two-component model, one on top of the other. Both components have horizontal fields, with the azimuth difference between them being close to 90°. The component that lies lower in the atmosphere is permeated by a strong field of the order of 600 G, while the upper component has much weaker fields, of the order of 10 G. The ensuing scattering polarization signatures of the individual components have opposite signs, so its combination along the line of sight reduces—and even can cancel out—the Hanle signatures, giving rise to an apparent Zeeman-only profile. This model is also applicable to other chromospheric structures seen in absorption above ARs. Recent spectropolarimetric observations of active region filaments have revealed polarization profiles with signatures typical of the strong field Zeeman regime. The conspicuous absence in those observations of scattering polarization and Hanle effect signatures was then pointed out by some authors. This was interpreted as either a signature of mixed "turbulent" field components or as a result of optical thickness. In this article, we present a natural scenario to explain these Zeeman-only spectropolarimetric observations of active region (AR) filaments. We propose a two-component model, one on top of the other. Both components have horizontal fields, with the azimuth difference between them being close to 90[degrees]. The component that lies lower in the atmosphere is permeated by a strong field of the order of 600 G, while the upper component has much weaker fields, of the order of 10 G. The ensuing scattering polarization signatures of the individual components have opposite signs, so its combination along the line of sight reduces-and even can cancel out-the Hanle signatures, giving rise to an apparent Zeeman-only profile. This model is also applicable to other chromospheric structures seen in absorption above ARs. |
Author | Díaz Baso, C. J. Asensio Ramos, A. Martínez González, M. J. |
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References | Asensio Ramos (apj523207bib2) 2008; 683 Kuckein (apj523207bib11) 2010; 81 Trujillo Bueno (apj523207bib27) 2010; 19 Orozco Suárez (apj523207bib22) 2015; 803 Kuckein (apj523207bib10) 2009; 501 Wiehr (apj523207bib30) 1991; 247 Judge (apj523207bib8) 2009; 493 Casini (apj523207bib6) 2009; 701 Landi Degl’Innocenti (apj523207bib13) 2004 López Ariste (apj523207bib16) 2005; 436 Aulanier (apj523207bib3) 2003; 402 Mackay (apj523207bib17) 2010; 151 Kuckein (apj523207bib12) 2012; 539 Orozco Suárez (apj523207bib21) 2014; 566 Asensio Ramos (apj523207bib1) 2010; 81 Sahal-Brechot (apj523207bib23) 1977; 59 Xu (apj523207bib32) 2010; 520 Trujillo Bueno (apj523207bib28) 2007; 655 Leroy (apj523207bib14) 1977; 54 Martínez González (apj523207bib19) 2015; 802 López Ariste (apj523207bib15) 2006; 456 Centeno (apj523207bib7) 2010; 708 Martínez González (apj523207bib18) 2012; 759 Sasso (apj523207bib24) 2011; 526 Solanki (apj523207bib25) 2003; 425 Xu (apj523207bib31) 2012; 749 Trujillo Bueno (apj523207bib26) 2003 Casini (apj523207bib5) 2003; 598 Kippenhahn (apj523207bib9) 1957; 43 Merenda (apj523207bib20) 2006; 642 Trujillo Bueno (apj523207bib29) 2002; 415 Yelles Chaouche (apj523207bib33) 2012; 748 Bommier (apj523207bib4) 1981; 100 |
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Snippet | ABSTRACT Recent spectropolarimetric observations of active region filaments have revealed polarization profiles with signatures typical of the strong field... Recent spectropolarimetric observations of active region filaments have revealed polarization profiles with signatures typical of the strong field Zeeman... |
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SubjectTerms | ABSORPTION ASTROPHYSICS, COSMOLOGY AND ASTRONOMY CHROMOSPHERE FILAMENTS Line of sight MAGNETIC FIELDS ORIENTATION POLARIMETRY POLARIZATION RADIANT HEAT TRANSFER radiative transfer SCATTERING Signatures SPACE DEPENDENCE SPECTROSCOPY SUN Sun: chromosphere Sun: filaments, prominences Sun: magnetic fields THICKNESS Turbulence ZEEMAN EFFECT |
Title | ACTIVE REGION FILAMENTS MIGHT HARBOR WEAK MAGNETIC FIELDS |
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