17 IDENTIFYING SOLAR FEATURES Photosphere
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Modelling Quasi-Periodic Pulsations in Solar and Stellar Flares
Space Sci Rev (2018) 214:45 https://doi.org/10.1007/s11214-018-0478-5 Modelling Quasi-Periodic Pulsations in Solar and Stellar Flares J.A. McLaughlin1 · V. M . N a k a r i a ko v 2,3,4 · M. Dominique5 · P. Jelínek6 · S. Takasao7 Received: 19 May 2017 / Accepted: 24 January 2018 / Published online: 6 February 2018 © The Author(s) 2018. This article is published with open access at Springerlink.com Abstract Solar flare emission is detected in all EM bands and variations in flux density of solar energetic particles. Often the EM radiation generated in solar and stellar flares shows a pronounced oscillatory pattern, with characteristic periods ranging from a fraction of a second to several minutes. These oscillations are referred to as quasi-periodic pulsa- tions (QPPs), to emphasise that they often contain apparent amplitude and period modu- lation. We review the current understanding of quasi-periodic pulsations in solar and stel- lar flares. In particular, we focus on the possible physical mechanisms, with an emphasis on the underlying physics that generates the resultant range of periodicities. These physi- cal mechanisms include MHD oscillations, self-oscillatory mechanisms, oscillatory recon- nection/reconnection reversal, wave-driven reconnection, two loop coalescence, MHD flow B J.A. McLaughlin [email protected] V.M. Nakariakov [email protected] M. Dominique [email protected] P. Jelínek [email protected] S. Takasao [email protected] 1 Northumbria University, Newcastle upon Tyne, NE1 8ST, UK 2 Centre for Fusion, Space and Astrophysics, University of Warwick, Coventry CV4 7AL, UK 3 School of Space Research, Kyung Hee University, Yongin, 446-701, Gyeonggi, Korea 4 St. -
On the Solar Chromosphere Observed at the Limb with Hinode
The Astrophysical Journal, 719:469–473, 2010 August 10 doi:10.1088/0004-637X/719/1/469 C 2010. The American Astronomical Society. All rights reserved. Printed in the U.S.A. ON THE SOLAR CHROMOSPHERE OBSERVED AT THE LIMB WITH HINODE Philip G. Judge1 and Mats Carlsson2 1 High Altitude Observatory, National Center for Atmospheric Research, P.O. Box 3000, Boulder, CO 80307-3000, USA 2 Institute of Theoretical Astrophysics, P.O. Box 1029, Blindern, N-0315 Oslo, Norway Received 2010 March 8; accepted 2010 April 8; published 2010 July 21 ABSTRACT Broadband images in the Ca ii H line, from the Broadband Filter Imager (BFI) instrument on the Hinode spacecraft, show emission from spicules emerging from and visible right down to the observed limb. Surprisingly, little absorption of spicule light is seen along their lengths. We present formal solutions to the transfer equation for given (ad hoc) source functions, including a stratified chromosphere from which spicules emanate. The model parameters are broadly compatible with earlier studies of spicules. The visibility of Ca ii spicules down to the limb in Hinode data seems to require that spicule emission be Doppler shifted relative to the stratified atmosphere, either by supersonic turbulent or organized spicular motion. The non-spicule component of the chromosphere is almost invisible in the broadband BFI data, but we predict that it will be clearly visible in high spectral resolution data. Broadband Ca ii H limb images give the false impression that the chromosphere is dominated by spicules. Our analysis serves as a reminder that the absence of a signature can be as significant as its presence. -
Arxiv:0906.0144V1 [Physics.Hist-Ph] 31 May 2009 Event
Solar physics at the Kodaikanal Observatory: A Historical Perspective S. S. Hasan, D.C.V. Mallik, S. P. Bagare & S. P. Rajaguru Indian Institute of Astrophysics, Bangalore, India 1 Background The Kodaikanal Observatory traces its origins to the East India Company which started an observatory in Madras \for promoting the knowledge of as- tronomy, geography and navigation in India". Observations began in 1787 at the initiative of William Petrie, an officer of the Company, with the use of two 3-in achromatic telescopes, two astronomical clocks with compound penduumns and a transit instrument. By the early 19th century the Madras Observatory had already established a reputation as a leading astronomical centre devoted to work on the fundamental positions of stars, and a principal source of stellar positions for most of the southern hemisphere stars. John Goldingham (1796 - 1805, 1812 - 1830), T. G. Taylor (1830 - 1848), W. S. Jacob (1849 - 1858) and Norman R. Pogson (1861 - 1891) were successive Government Astronomers who led the activities in Madras. Scientific high- lights of the work included a catalogue of 11,000 southern stars produced by the Madras Observatory in 1844 under Taylor's direction using the new 5-ft transit instrument. The observatory had recently acquired a transit circle by Troughton and Simms which was mounted and ready for use in 1862. Norman Pogson, a well known astronomer whose name is associated with the modern definition of the magnitude scale and who had considerable experience with transit instruments in England, put this instrument to good use. With the help of his Indian assistants, Pogson measured accurate positions of about 50,000 stars from 1861 until his death in 1891. -
Estimate of Plasma Temperatures Across a CME-Driven Shock from a Comparison Between EUV and Radio Data
Solar Phys (2020) 295:124 https://doi.org/10.1007/s11207-020-01686-0 Estimate of Plasma Temperatures Across a CME-Driven Shock from a Comparison Between EUV and Radio Data Federica Frassati1 · Salvatore Mancuso1 · Alessandro Bemporad1 Received: 9 March 2020 / Accepted: 6 August 2020 / Published online: 8 September 2020 © The Author(s) 2020 Abstract In this work, we analyze the evolution of an EUV wave front associated with a solar eruption that occurred on 30 October 2014, with the aim of investigating, through differential emission measure (DEM) analysis, the physical properties of the plasma com- pressed and heated by the accompanying shock wave. The EUV wave was observed by the Atmospheric Imaging Assembly (AIA) onboard the Solar Dynamics Observatory (SDO) and was accompanied by the detection of a metric Type II burst observed by ground-based radio spectrographs. The EUV signature of the shock wave was also detected in two of the AIA channels centered at 193 Å and 211 Å as an EUV intensity enhancement propagating ahead of the associated CME. The density compression ratio X of the shock as inferred from the analysis of the EUV data is X ≈ 1.23, in agreement with independent estimates obtained from the analysis of the Type II band-splitting of the radio data and inferred by adopting the upstream–downstream interpretation. By applying the Rankine–Hugoniot jump conditions under the hypothesis of a perpendicular shock, we also estimate the temperature ratio as TD/TU ≈ 1.55 and the post-shock temperature as TD ≈ 2.75 MK. The modest compression ratio and temperature jump derived from the EUV analysis at the shock passage are typical of weak coronal shocks. -
Magnetism, Dynamo Action and the Solar-Stellar Connection
Living Rev. Sol. Phys. (2017) 14:4 DOI 10.1007/s41116-017-0007-8 REVIEW ARTICLE Magnetism, dynamo action and the solar-stellar connection Allan Sacha Brun1 · Matthew K. Browning2 Received: 23 August 2016 / Accepted: 28 July 2017 © The Author(s) 2017. This article is an open access publication Abstract The Sun and other stars are magnetic: magnetism pervades their interiors and affects their evolution in a variety of ways. In the Sun, both the fields themselves and their influence on other phenomena can be uncovered in exquisite detail, but these observations sample only a moment in a single star’s life. By turning to observa- tions of other stars, and to theory and simulation, we may infer other aspects of the magnetism—e.g., its dependence on stellar age, mass, or rotation rate—that would be invisible from close study of the Sun alone. Here, we review observations and theory of magnetism in the Sun and other stars, with a partial focus on the “Solar-stellar connec- tion”: i.e., ways in which studies of other stars have influenced our understanding of the Sun and vice versa. We briefly review techniques by which magnetic fields can be measured (or their presence otherwise inferred) in stars, and then highlight some key observational findings uncovered by such measurements, focusing (in many cases) on those that offer particularly direct constraints on theories of how the fields are built and maintained. We turn then to a discussion of how the fields arise in different objects: first, we summarize some essential elements of convection and dynamo theory, includ- ing a very brief discussion of mean-field theory and related concepts. -
Comprehensive Characterization of Solar Eruptions with Remote and In-Situ Observations, and Modeling: the Major Solar Events on 4 November 2015
Solar Physics DOI: 10.1007/•••••-•••-•••-••••-• Comprehensive Characterization of Solar Eruptions With Remote and In-Situ Observations, and Modeling: The Major Solar Events on 4 November 2015 Iver H. Cairns?1 · Kamen A. Kozarev2 · Nariaki V. Nitta3 · Neus Agueda4 · Markus Battarbee5,6 · Eoin P. Carley7 · Nina Dresing8 · Ra´ulG´omez-Herrero9 · Karl-Ludwig Klein10 · David Lario11,12 · Jens Pomoell13 · Carolina Salas-Matamoros10,14 · Astrid M. Veronig15 · Bo Li1 · Patrick McCauley1 B Iver H. Cairns? [email protected],+61 2 9351 3961 Kamen A. Kozarev [email protected] Nariaki V. Nitta [email protected] Neus Agueda [email protected] Markus Battarbee [email protected] Eoin P. Carley [email protected] Nina Dresing [email protected] Ra´ulG´omez-Herrero [email protected] Karl-Ludwig Klein [email protected] David Lario [email protected] Jens Pomoell jens.pomoell@helsinki.fi Carolina Salas-Matamoros [email protected] Astrid M. Veronig arXiv:1910.03319v1 [astro-ph.SR] 8 Oct 2019 [email protected] Bo Li [email protected] SOLA: overview_51_8Oct19.tex; 9 October 2019; 0:35; p. 1 ISSI team: I.H. Cairns et al. c Springer •••• Abstract Solar energetic particles (SEPs) are an important product of solar activity. They are connected to solar active regions and flares, coronal mass ejections (CMEs), EUV waves, shocks, Type II and III radio emissions, and X- ray bursts. These phenomena are major probes of the partition of energy in solar eruptions, as well as for the organization, dynamics, and relaxation of coronal and interplanetary magnetic fields. -
What Causes the High Apparent Speeds in Chromospheric and Transition Region Spicules on the Sun?
The Astrophysical Journal Letters, 849:L7 (7pp), 2017 November 1 https://doi.org/10.3847/2041-8213/aa9272 © 2017. The American Astronomical Society. All rights reserved. What Causes the High Apparent Speeds in Chromospheric and Transition Region Spicules on the Sun? Bart De Pontieu1,2 , Juan Martínez-Sykora1,3 , and Georgios Chintzoglou1,4 1 Lockheed Martin Solar and Astrophysics Laboratory, Palo Alto, CA 94304, USA; [email protected] 2 Institute of Theoretical Astrophysics, University of Oslo, P.O. Box 1029 Blindern, NO-0315 Oslo, Norway 3 Bay Area Environmental Research Institute, Petaluma, CA 94952, USA 4 University Corporation for Atmospheric Research, Boulder, CO 80307-3000, USA Received 2017 June 22; revised 2017 October 5; accepted 2017 October 9; published 2017 October 23 Abstract Spicules are the most ubuiquitous type of jets in the solar atmosphere. The advent of high-resolution imaging and spectroscopy from the Interface Region Imaging Spectrograph (IRIS) and ground-based observatories has revealed the presence of very high apparent motions of order 100–300 km s−1 in spicules, as measured in the plane of the sky. However, line of sight measurements of such high speeds have been difficult to obtain, with values deduced from Doppler shifts in spectral lines typically of order 30–70 km s−1. In this work, we resolve this long-standing discrepancy using recent 2.5D radiative MHD simulations. This simulation has revealed a novel driving mechanism for spicules in which ambipolar diffusion resulting from ion-neutral interactions plays a key role. In our simulation, we often see that the upward propagation of magnetic waves and electrical currents from the low chromosphere into already existing spicules can lead to rapid heating when the currents are rapidly dissipated by ambipolar diffusion. -
The Sun's Dynamic Atmosphere
Lecture 16 The Sun’s Dynamic Atmosphere Jiong Qiu, MSU Physics Department Guiding Questions 1. What is the temperature and density structure of the Sun’s atmosphere? Does the atmosphere cool off farther away from the Sun’s center? 2. What intrinsic properties of the Sun are reflected in the photospheric observations of limb darkening and granulation? 3. What are major observational signatures in the dynamic chromosphere? 4. What might cause the heating of the upper atmosphere? Can Sound waves heat the upper atmosphere of the Sun? 5. Where does the solar wind come from? 15.1 Introduction The Sun’s atmosphere is composed of three major layers, the photosphere, chromosphere, and corona. The different layers have different temperatures, densities, and distinctive features, and are observed at different wavelengths. Structure of the Sun 15.2 Photosphere The photosphere is the thin (~500 km) bottom layer in the Sun’s atmosphere, where the atmosphere is optically thin, so that photons make their way out and travel unimpeded. Ex.1: the mean free path of photons in the photosphere and the radiative zone. The photosphere is seen in visible light continuum (so- called white light). Observable features on the photosphere include: • Limb darkening: from the disk center to the limb, the brightness fades. • Sun spots: dark areas of magnetic field concentration in low-mid latitudes. • Granulation: convection cells appearing as light patches divided by dark boundaries. Q: does the full moon exhibit limb darkening? Limb Darkening: limb darkening phenomenon indicates that temperature decreases with altitude in the photosphere. Modeling the limb darkening profile tells us the structure of the stellar atmosphere. -
A Small-Scale Filament Eruption Inducing Moreton Wave, Euv Wave and Coronal Mass Ejection
Draft version April 17, 2020 Preprint typeset using LATEX style AASTeX6 v. 1.0 A SMALL-SCALE FILAMENT ERUPTION INDUCING MORETON WAVE, EUV WAVE AND CORONAL MASS EJECTION Jincheng Wang1,2,3, Xiaoli Yan1,2, Defang Kong1,2, Zhike Xue1,2, Liheng Yang1,2, Qiaoling Li1,4 1Yunnan Observatories, Chinese Academy of Sciences, Kunming 650011, People.s Republic of China. 2Center for Astronomical Mega-Science, Chinese Academy of Sciences, 20A Datun Road, Chaoyang District, Beijing, 100012, People.s Republic of China 3CAS Key Laboratory of Solar Activity, National Astronomical Observatories, Beijing 100012, China 4University of Chinese Academy of Sciences, Yuquan Road, Shijingshan Block Beijing 100049, People.s Republic of China ABSTRACT With the launch of SDO, many EUV waves were observed during solar eruptions. However, the joint observations of Moreton and EUV waves are still relatively rare. We present an event that a small-scale filament eruption simultaneously results in a Moreton wave, an EUV wave and a Coronal Mass Ejection in active region NOAA 12740. Firstly, we find that some dark elongate lanes or fila- mentary structures in the photosphere existed under the small-scale filament and drifted downward, which manifests that the small-scale filament was emerging and lifting from subsurface. Secondly, combining the simultaneous observations in different Extreme UltraViolet (EUV) and Hα passbands, we study the kinematic characteristics of the Moreton and EUV waves. The comparable propagat- ing velocities and the similar morphology of Moreton and different passbands EUV wavefronts were obtained. We deduce that Moreton and different passbands EUV waves were the perturbations in dif- ferent temperature-associated layers induced by the coronal magneto-hydrodynamic shock wave. -
Solar Activity and Its Evolution Across the Corona: Recent Advances
J. Space Weather Space Clim. 3 (2013) A18 DOI: 10.1051/swsc/2013039 Ó F. Zuccarello et al., Published by EDP Sciences 2013 RESEARCH ARTICLE OPEN ACCESS Solar activity and its evolution across the corona: recent advances Francesca Zuccarello1,*, Laura Balmaceda2, Gael Cessateur3, Hebe Cremades4, Salvatore L. Guglielmino5, Jean Lilensten6, Thierry Dudok de Wit7, Matthieu Kretzschmar7, Fernando M. Lopez2, Marilena Mierla8,9,10, Susanna Parenti8, Jens Pomoell11, Paolo Romano5, Luciano Rodriguez8, Nandita Srivastava12, Rami Vainio11, Matt West8, and Francesco P. Zuccarello13 1 Dipartimento di Fisica e Astronomia, Sez. Astrofisica, Universita` di Catania, Via S. Sofia 78, 95123 Catania, Italy *Corresponding author: [email protected] 2 Instituto de Ciencias Astrono´micas, de la Tierra y el Espacio, ICATE-CONICET, Av. Espan˜a Sur 1512, J5402DSP, San Juan, Argentina 3 Physical-Meteorological Observatory/World Radiation Center, Davos, Switzerland 4 Universidad Tecnolo´gica Nacional – Facultad Regional Mendoza/CONICET, Rodrı´guez 273, M5502AJE, Mendoza, Argentina 5 INAF – Osservatorio Astrofisico di Catania, Via S. Sofia 78, 95123, Catania, Italy 6 UJF-Grenoble 1/CNRS-INSU, Institut de Plane´tologie et d’Astrophysique de Grenoble (IPAG) UMR 5274, 38041 Grenoble, France 7 LPC2E/CNRS (UMR 7328) and University of Orle´ans, 3A avenue de la Recherche Scientifique, 45071 Orle´ans Cedex 2, France 8 Solar – Terrestrial Center of Excellence – SIDC, Royal Observatory of Belgium, Av. Circulaire 3, 1180 Brussels, Belgium 9 Institute of Geodynamics -
What Controls Spicule Velocities and Heights? Color of R
ado. What Controls Spicule Velocities and Heights? Color of R. Hammer, A. Nesis Kiepenheuer-Institut furÄ Sonnenphysik University Abstract. Numerous mechanisms have been suggested to drive spicules. Many of them need a careful ¯ne-tuning of free parameters in order to achieve the basic characteristics, like velocity and height, of observed 2003 spicules. There might, however, be general physical mechanisms that control these properties. We show that whenever upper chromospheric Sun, plasma is exposed to a signi¯cantly non-hydrostatic pressure gradient, The it starts moving upward at the observed speeds. The plasma can reach & signi¯cant heights, at least if it receives some net chromospheric heat- ing during the rising phase. Therefore, such a hydrodynamic mechanism might help other (magnetic) drivers to control the basic properties of spicules. We suggest therefore to consider a new class of spicule driv- Systems, ing mechanisms, in which the plasma is not only accelerated by wave or magnetic forces from below, but also by the generation of a low pressure lar region above the chromosphere. Such a situation could arise e.g. due to Stel an instability in magnetic loops or as a result of the recon¯guration of open ¯eld lines. Stars, ol Co 1. Introduction on Classical spicules are needle-shaped chromospheric extensions, which can be seen in strong chromospheric lines to protrude out of the solar limb. They are highly dynamic and consist of plasma with properties characteristic of the upper 4 11 ¡3 Workshop chromosphere (temperature ¼ 10 K, electron density of order 10 cm ) that moves at supersonic speeds of 20 ¡ 30 km s¡1 up to heights of 5000 ¡ 10000 km, with a typical lifetime of 5 ¡ 10 min (e.g., Beckers 1972). -
Absorption Phenomena and a Probable Blast Wave in the 13 July 2004 Eruptive Event
Solar Physics DOI: 10.1007/•••••-•••-•••-••••-• Absorption Phenomena and a Probable Blast Wave in the 13 July 2004 Eruptive Event V.V. Grechnev1 · A.M. Uralov1 · V.A. Slemzin2 · I.M. Chertok3 · I.V. Kuzmenko4 · K. Shibasaki5 Received ; accepted c Springer •••• Abstract We present a case study of the 13 July 2004 solar event, in which disturbances caused by eruption of a filament from an active region embraced a quarter of the visible solar surface. Remarkable are absorption phenomena observed in the SOHO/EIT 304 A˚ channel; they were also visible in the EIT 195 A˚ channel, in the Hα line, and even in total radio flux records. Coronal and Moreton waves were also observed. Multi-spectral data allowed reconstructing an overall picture of the event. An explosive filament eruption and related impulsive flare produced a CME and blast shock, both of which decelerated and propagated independently. Coronal and Moreton waves were kinematically close and both decelerated in accordance with an expected motion of the coronal blast shock. The CME did not resemble a classical three-component structure, probably, because some part of the ejected mass fell back onto the Sun. Quantitative evaluations from different observations provide close estimates of the falling mass, ∼ 3 · 1015 g, which is close to the estimated mass of the CME. The falling material was responsible for the observed large-scale absorption phenomena, in particular, shallow widespread moving dimmings observed at 195 A.˚ By contrast, deep quasi-stationary dimmings observed in this band near the eruption center were due to plasma density decrease in coronal structures.