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Dive into the research topics where H. N. Smitha is active.

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Featured researches published by H. N. Smitha.


The Astrophysical Journal | 2011

Polarized Line Formation with J-state Interference in the Presence of Magnetic Fields. I. Partial Frequency Redistribution in the Collisionless Regime

H. N. Smitha; M. Sampoorna; K. N. Nagendra; J. O. Stenflo

Quantum interference phenomena play a fundamental role in astrophysical spectra that are formed by coherent scattering processes. Here we derive a partial frequency redistribution (PRD) matrix that includes J-state interference in the presence of magnetic fields of arbitrary strength. The paper focuses on PRD in the collisionless regime, which in the traditional PRD terminology is referred to as Hummers type-II scattering. By limiting the treatment to the linear Zeeman regime, for which the Zeeman splitting is much smaller than the fine-structure splitting, it is possible to formulate analytical expressions for the PRD matrices. In the special case of non-magnetic scattering we recover the redistribution matrix derived from an independent quantum electrodynamic formulation based on the metalevel theory.


Astronomy and Astrophysics | 2011

Observations of the forward scattering Hanle effect in the Ca I 4227 Å line

M. Bianda; R. Ramelli; L. S. Anusha; J. O. Stenflo; K. N. Nagendra; R. Holzreuter; H. Sampoorna M. Frisch; H. N. Smitha

Chromospheric magnetic fields are notoriously difficult to measure. The chromospheric lines are broad, while the fields are producing a minuscule Zeeman-effect polarization. A promising diagnostic alternative is provided by the forward-scattering Hanle effect, which can be recorded in chromospheric lines such as the He i 10830 A and the Ca i 4227 A lines. We present a set of spectropolarimetric observations of the full Stokes vector obtained near the center of the solar disk in the Ca i 4227 A line with the ZIMPOL polarimeter at the IRSOL observatory. We detect a number of interesting forward-scattering Hanle effect signatures, which we model successfully using polarized radiative transfer. Here we focus on the observational aspects, while a separate companion paper deals with the theoretical modeling.


Astronomy and Astrophysics | 2012

J-state interference signatures in the second solar spectrum - Modeling the Cr i triplet at 5204–5208 Å

H. N. Smitha; K. N. Nagendra; J. O. Stenflo; M. Bianda; M. Sampoorna; Renzo Ramelli; L. S. Anusha

The scattering polarization in the solar spectrum is traditionally modeled with each spectral line treated separately, but this is generally inadequate for multiplets where J-state interference plays a significant role. Through simultaneous observations of all the 3 lines of a Cr i triplet, combined with realistic radiative transfer modeling of the data, we show that it is necessary to include J-state interference consistently when modeling lines with partially interacting fine structure components. Polarized line formation theory that includes J-state interference effects together with partial frequency redistribution for a two-term atom is used to model the observations. Collisional frequency redistribution is also accounted for. We show that the resonance polarization in the Cr i triplet is strongly affected by the partial frequency redistribution effects in the line core and near wing peaks. The Cr i triplet is quite sensitive to the temperature structure of the photospheric layers. Our complete frequency redistribution calculations in semi-empirical models of the solar atmosphere cannot reproduce the observed near wing polarization or the cross-over of the Stokes Q/I line polarization about the continuum polarization level that is due to the J-state interference. When however partial frequency redistribution is included, a good fit to these features can be achieved. Further, to obtain a good fit to the far wings, a small temperature enhancement of the FALF model in the photospheric layers is necessary.


The Astrophysical Journal | 2014

CENTER-TO-LIMB OBSERVATIONS AND MODELING OF THE Ca I 4227 Å LINE

H. D. Supriya; H. N. Smitha; K. N. Nagendra; J. O. Stenflo; M. Bianda; Renzo Ramelli; B. Ravindra; L. S. Anusha

The observed center-to-limb variation (CLV) of the scattering polarization in different lines of the Second Solar Spectrum can be used to constrain the height variation of various atmospheric parameters, in particular the magnetic fields via the Hanle effect. Here we attempt to model non-magnetic CLV observations of the


The Astrophysical Journal | 2012

POLARIZED LINE TRANSFER WITH F-STATE INTERFERENCE IN A NON-MAGNETIC MEDIUM: PARTIAL FREQUENCY REDISTRIBUTION EFFECTS IN THE COLLISIONLESS REGIME

H. N. Smitha; K. Sowmya; K. N. Nagendra; M. Sampoorna; J. O. Stenflo

Q/I


Astronomy and Astrophysics | 2011

Radiative transfer with J-state interference in a two-term atom - Partial frequency redistribution in the non-magnetic case

H. N. Smitha; K. N. Nagendra; M. Sampoorna; J. O. Stenflo

profiles of the Ca I 4227 A line recorded with the ZIMPOL-3 at IRSOL. For modeling, we use the polarized radiative transfer with partial frequency redistribution with a number of realistic 1-D model atmospheres. We find that all the standard FAL model atmospheres, used by us, fail to simultaneously fit the observed (


The Astrophysical Journal | 2013

MODELING THE QUANTUM INTERFERENCE SIGNATURES OF THE Ba II D2 4554 Å LINE IN THE SECOND SOLAR SPECTRUM

H. N. Smitha; K. N. Nagendra; J. O. Stenflo; M. Sampoorna

I


The Astrophysical Journal | 2014

The quantum interference effects in the SC II 4247 Å line of the second solar spectrum

H. N. Smitha; K. N. Nagendra; J. O. Stenflo; M. Bianda; Renzo Ramelli

,


Journal of Quantitative Spectroscopy & Radiative Transfer | 2013

Polarized line formation with J-state interference in the presence of magnetic fields: A Heuristic treatment of collisional frequency redistribution

H. N. Smitha; K. N. Nagendra; M. Sampoorna; J. O. Stenflo

Q/I


Monthly Notices of the Royal Astronomical Society | 2013

Quantum interference with angle-dependent partial frequency redistribution: solution of the polarized line transfer in the non-magnetic case

H. D. Supriya; H. N. Smitha; K. N. Nagendra; B. Ravindra; M. Sampoorna

) at all the limb distances (

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K. N. Nagendra

Indian Institute of Astrophysics

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M. Sampoorna

Indian Institute of Astrophysics

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L. S. Anusha

Indian Institute of Astrophysics

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B. Ravindra

Indian Institute of Astrophysics

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H. D. Supriya

Indian Institute of Astrophysics

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H. Sampoorna M. Frisch

Indian Institute of Astrophysics

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K. Sowmya

Indian Institute of Astrophysics

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L. S. Anusha

Indian Institute of Astrophysics

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