Search for photospheric footpoints of quiet Sun transition region loops

Similar documents
Results from Chromospheric Magnetic Field Measurements

Observable consequences

Non-spot magnetic fields

A STUDY OF TRANSITION REGION AND CORONAL DOPPLER SHIFTS IN A SOLAR CORONAL HOLE. M. D. Popescu 1,2 and J. G. Doyle 1

arxiv: v2 [astro-ph.sr] 2 Oct 2012

Results from Chromospheric Magnetic Field Measurements

The Emission Heights of Transition Region Lines in an Equatorial Coronal Hole and the Surrounding Quiet Sun

Stellar coronae and the Sun

Plumes as seen in the Ultraviolet

Measuring the Magnetic Vector with the Hei Å Line: A Rich New World

The low solar corona and the stars

pre Proposal in response to the 2010 call for a medium-size mission opportunity in ESA s science programme for a launch in 2022.

Modern observational techniques for coronal studies

Solar-B. Report from Kyoto 8-11 Nov Meeting organized by K. Shibata Kwasan and Hida Observatories of Kyoto University

2 The solar atmosphere

Recent Highlights on Solar Coronal Abundances from Hinode

New insights from. observation. Hinode-VTT He Andreas Lagg (MPS) Saku Tsuneta (NAOJ) Ryohko Ishikawa (NAOJ/Univ. Tokyo)

The Sun s Dynamic Atmosphere

The Solar Chromosphere

arxiv:astro-ph/ v1 26 Sep 2003

The Solar Chromosphere

PLASMA FLOWS GUIDED BY STRONG MAGNETIC FIELDS IN THE SOLAR CORONA

Gelu M. Nita. New Jersey Institute of Technology

What do we see on the face of the Sun? Lecture 3: The solar atmosphere

An EUV Bright Point as seen by SUMER, CDS, MDI and EIT on-board SoHO

SMALL SCALE SOLAR MAGNETIC FIELDS. M. J. Martínez González Instituto de Astrofísica de Canarias

Virtual Solar Observatory

1. Solar Atmosphere Surface Features and Magnetic Fields

Comparison of F 10.7 and Coronal EUV Emission using DEMs

High resolution analysis of a magnetic bubble emerging through the solar atmosphere

1. INTRODUCTION 2. OBSERVATIONS AND DATA REDUCTION. The Astrophysical Journal, 502:L85 L90, 1998 July 20

Astronomy. Astrophysics. G-band spectral synthesis and diagnostics of simulated solar magneto-convection

Chromospheric magnetic fields of an active region filament measured using the He I triplet

Observations of Solar Jets

arxiv: v2 [astro-ph.sr] 24 Jul 2009

Chapter 1. Introduction. 1.1 Why study the sun?

Supporting Calculations for NASA s IRIS Mission. I. Overview

Temporal evolution of different temperature plasma during explosive events

The Evershed flow and the brightness of the penumbra. Luis R. Bellot Rubio Instituto de Astrofísica de Andalucía (CSIC) Granada, Spain

This article appeared in a journal published by Elsevier. The attached copy is furnished to the author for internal non-commercial research and

Variation of coronal line widths on and off the disk

Name: Date: 2. The temperature of the Sun's photosphere is A) close to 1 million K. B) about 10,000 K. C) 5800 K. D) 4300 K.

AIA DATA ANALYSIS OVERVIEW OF THE AIA INSTRUMENT

HOW TO USE MAGNETIC FIELD INFORMATION FOR CORONAL LOOP IDENTIFICATION. 1. Introduction

λ D and T i can be obtained (cf., e.g. Mariska 1992) 1 In the text we use rounded values sufficient to identify the lines.

What drives the solar wind and where does the coronal magnetic field originate from?

Advances in measuring the chromospheric magnetic field using the He triplet

Microwave and hard X-ray imaging observations of energetic electrons in solar flares: event of 2003 June 17

Near-IR internetwork spectro-polarimetry at different heliocentric angles ABSTRACT

ON THE STOKES V AMPLITUDE RATIO AS AN INDICATOR OF THE FIELD STRENGTH IN THE SOLAR INTERNETWORK

EUV line intensity distribution in the solar atmosphere: differences between a polar coronal hole and its equatorial extension

Magnetic strength analysis in the quiet Sun regions using the Mn I line at 553 nm

Solar Magnetic Fields Jun 07 UA/NSO Summer School 1

Introduction to Daytime Astronomical Polarimetry

arxiv:astro-ph/ v1 12 Jul 2002

THE MYSTERIOUS SOLAR CHROMOSPHERE

Vector Magnetic Field Diagnostics using Hanle Effect

IRIS views on how the low solar atmosphere is energized

Multi-wavelength VLA and Spacecraft Observations of Evolving Coronal Structures Outside Flares

Large scale properties of coronal heating along the solar cycle

DETERMINATION OF THE FORMATION TEMPERATURE OF Si IV IN THE SOLAR TRANSITION REGION

Solar EUV Spectral Irradiance: Measurements. Frank Eparvier

Phys 100 Astronomy (Dr. Ilias Fernini) Review Questions for Chapter 8

arxiv:astro-ph/ v1 18 Apr 2006

O 5+ at a heliocentric distance of about 2.5 R.

On the 3D structure of the magnetic eld in regions of emerging ux

arxiv: v1 [astro-ph] 5 Dec 2007

Next quiz: Monday, October 24 Chp. 6 (nothing on telescopes) Chp. 7 a few problems from previous material cough, cough, gravity, cough, cough...

The Sun. Basic Properties. Radius: Mass: Luminosity: Effective Temperature:

Photospheric and chromospheric polarimetry of solar flares

Chapter 8 The Sun Our Star

Solar radiation and plasma diagnostics. Nicolas Labrosse School of Physics and Astronomy, University of Glasgow

The solar atmosphere

The Sun. 1a. The Photosphere. A. The Solar Atmosphere. 1b. Limb Darkening. A. Solar Atmosphere. B. Phenomena (Sunspots) C.

On the nature of Ellermanbombs and microflaresas observed with the 1.5m GREGOR telescope

Double Coronal Hard and Soft X-Ray Source as Evidence of Magnetic Reconnection: The M1.4 Flare 1

The Role of Magnetic Topology in the Heating of Active Region Coronal Loops

UV spectro-polarimetry with CLASP & CLASP2 sounding rocket experiments

PROPERTIES OF SOLAR POLAR CORONAL PLUMES CONSTRAINED BY ULTRAVIOLET CORONAGRAPH SPECTROMETER DATA

Date of delivery: 29 June 2011 Journal and vol/article ref: IAU Number of pages (not including this page): 7

Flare Energy Release in the Low Atmosphere

Evidence for a siphon flow ending near the edge of a pore

arxiv: v1 [astro-ph.sr] 26 Jan 2010

Comparison between the polar coronal holes during the Cycle22/23 and Cycle 23/24 minima using magnetic, microwave, and EUV butterfly diagrams

POLAR PLUME ANATOMY: RESULTS OF A COORDINATED OBSERVATION

The Sun's atmosphere and magnetic field

Pros and Cons (Advantages and Disadvantages) of Various Magnetic Field Extrapolation Techniques

1-4-1A. Sun Structure

arxiv: v1 [astro-ph.sr] 25 Nov 2016

Physics of the Sun s Hot Atmosphere

Chromospheric signatures of small-scale flux emergence as observed with NST and Hinode instruments

Internetwork Horizontal Magnetic Fields in the Quiet Sun Chromosphere: Results from a Joint Hinode/VTT Study

Lecture 6: Our star, the Sun

arxiv: v1 [astro-ph.sr] 25 Oct 2013

Solar Physics with Radio Observations, Proceedings of Nobeyama Symposium 1998, NRO Report 479. Flare Loop Geometry. Nariaki Nitta

The Sun. 1a. The Photosphere. A. The Solar Atmosphere. 1b. Limb Darkening. A. Solar Atmosphere. B. Phenomena (Sunspots) C.

Magnetic Fields in the Atmospheres of the Sun and Stars

CORONAL HEATING ORIGINS OF SOLAR SPECTRAL IRRADIANCE

Publ. Astron. Obs. Belgrade No. 90 (2010), A CASE OF FILAMENT ACTIVE REGION INTERACTION

Influence of Mass Flows on the Energy Balance and Structure of the Solar Transition Region

Transcription:

Search for photospheric footpoints of quiet Sun transition region loops L. Teriaca Max Planck Institut für Sonnensystemforschung Submitted to A&A as Sánchez Almeida, Teriaca, Sütterlin, Spadaro, Schühle, and Rutten

The Transition Region The Transition Region (TR) is defined as the temperature region between 20 kk and 1 MK and, as such, strongly emits in the VUV spectral range. Classical, static, models depict it as a thin (10 to 100 km) thermal interface between the hot corona and the cooler photosphere.

The Transition Region The failure of such models in reproducing observed quantities such as the emission measure and the limb brightening curves of TR lines together with high resolution observations has changed this view. Most of the emission comes from cold (T<0.5 MK) loops Dowdy et al. 1986. Filamentary TR structures Dere et al 1997.

The Transition Region - Corona The lower TR (T<0.7 MK) is formed by many loop-like structures 10 to 20 long located along and across network boundaries, with widths at or below the SUMER resolution of 1.5. From these data it seems that the majority of the TR emission, particularly in the quiet Sun, does not simply connect the chromosphere with the corona Feldman et al 1999.

The Transition Region and the Chromosphere However, there are also difficulties at connecting the TR with the chromosphere. Most strikingly, the width of the chromospheric brightening along the cell boundaries is much narrower than the widths of the bright TR structures. Feldman et al. 2001.

What are the footpoint of the TR Structures? When comparing the TR structures with a MDI magnetogram, only some of the larger loops appear obviously connected to magnetic polarities. What about the rest? Teriaca et al. 2004.

Where is the photospheric field? Classical (e.g., MDI) magnetograms do not have enough spatial resolution to detect the field in the interior of the supergranular cells. However, this field has been observed as weak Hanle depolarization (e.g., Trujillo Bueno et al. 2001) and Zeeman polarization (e.g., Dominguez Cerdeña et al. 2003) and small bright points (e.g., de Wijn et al. 2005). Finally, numerical simulations (e.g., Vögler & Schüssler 2007) and observations (e.g., Dominguez Cerdeña et al. 2006) indicate that a complex magnetic field pervades the non-magnetic quiet photosphere. Theoretical arguments suggest that large part of these photospheric fields reaches the TR and the corona (e.g., Jendersie & Peter 2006).

Observations: Photospheric field Inter-granular G-band (CH band around 430 nm) Bright Points (GBPs) have size below 250 km (0.35" possibly < 0.2"). They can be used as a proxy of (1-2) kg magnetic fields (e.g., Berger et al. 1995, 1998). Although kg fields represent only a very small fraction of the quiet Sun magnetic structures (e.g., Socas-Navarro & Sánchez Almeida 2002), these fields still trace a significant fraction of the total magnetic energy and are expected to reach and tip-over at greater altitudes (Domínguez Cerdeña et al. 2006).

Observations: Photospheric field Speckle reconstructed DOT images in the G-band can reach the diffraction limit of 0.2. Ca II H line core images are also taken.

Observations: Transition Region Structures SUMER rasters were taken in a wavelength range including the C III 97.7 nm line. This line is formed in the mid TR (T 8 10 4 K) and is one of the brightest lines in the VUV spectrum. As such, it is an ideal tracer of the TR loops. It allows high S:N spectra to be acquired with exposure times of few seconds.

Observations: Transition Region Structures

Data Co-alignment: SUMER vs MDI Full Disk MDI magnetograms are aligned with SUMER scans by comparing the absolute magnetic flux and the scans in both the pseudo/continuum and H I Ly γ. The error in the alignment is considered to be between 1 and 2 Iso-contours of 7 G and 15 G absolute magnetic flux traced over the SUMER scan in the pseudocontinuum.

Data Co-alignment: DOT vs MDI DOT images are both rotated (by the angle between the geocentric North and the solar rotational North) and shifted with respect to SOHO images. After rotating (angle taken from the ephemeris), the DOT images in the Ca II H are aligned with MDI maps of the absolute magnetic flux. The error in the alignment is considered to be around 1. DOT G-band images are finally aligned to DOT Ca II H images by cross-correlation. The error in the alignment is well below 1.

GBPs vs TR radiances GBP are clearly related to the bright TR structures. GBPs seem to avoid the brightest cores.

GBPs vs TR radiances GBPs are clearly related to the bright TR structures. GBPs seem to avoid the brightest cores.

GBPs vs TR line shifts GBP avoids the regions of larger velocities.

GBPs vs TR line shifts GBP avoids the regions of larger velocities. GBPs are associated to areas that show an excess redshift of about 1.9 km/s.

GBPs vs TR line widths GBP avoids the regions of larger widths.

GBPs vs TR explosive events Although based on a very limited statistics (7 events), there never were GBPs within the SUMER pixel showing explosive events.

Summary & Conclusions We cannot find a clear evidence that GBPs are the foot-points of TR loops, i.e. there is not a clear relationship between the GBPs pattern and the TR structures. However, we find evidences that indicate that a link between the two phenomena may exist. In particular, the radiance (velocity) distribution of SUMER pixels associated to GBPs appear shifted towards larger radiances (downward directed velocities) than the overall distribution. The excess of red-shift in areas containing GBPs is particularly interesting as it may indicate a larger amount of vertical field, as would be expected closer to the foot-points.

Summary & Conclusions This may suggest loop foot-points to be connected to multiple magnetic elements in the photosphere via a complex system of field lines. A similar scenario has been suggested for moss areas, bright EUV regions at the base of hot (3 to 5 MK) AR loops. Berger et al. 1999

Summary & Conclusions GBPs seem to avoid explosive events. Although based on a very small statistics this may provide clues on the mechanisms responsible for such events. Further observations here are needed.

Future Work New SUMER rasters have been acquired during the recent SUMER campaign together with DOT. They provide a much more extended dataset to investigate the relationship between GBPs and TR structures.

Thank you