ADAS workshop, Auburn University

Slides:



Advertisements
Similar presentations
Effetti di non stazionarietà nella dinamica di ionizzazione di un plasma prodotto da impulsi laser ai ns L. Labate, C.A. Cecchetti, M. Galimberti, A. Giulietti,
Advertisements

L. Teriaca, IMPRS Seminar, Lindau 08/12/04 Spectroscopy of the solar Transition Region and Corona L. Teriaca.
Raman Spectroscopy A) Introduction IR Raman
 -Ray Emission Probabilities Edgardo Browne Decay Data Evaluation Project Workshop May 12 – 14, 2008 Bucharest, Romania.
The synthetic emission spectra for the electron non-thermal distributions by using CHIANTI Elena Dzifčáková Department of Astronomy, Physics of the Earth.
Atomic Absorption Spectroscopy (AAS) The Visible Spectra.
Estimating the Chromospheric Absorption of Transition Region Moss Emission Bart De Pontieu, Viggo H. Hansteen, Scott W. McIntosh, Spiros Patsourakos.
Global Warming and Climate Sensitivity Professor Dennis L. Hartmann Department of Atmospheric Sciences University of Washington Seattle, Washington.
17.1 Mass Spectrometry Learning Objectives:
ALFVEN WAVES IN A POLAR CORONAL HOLE FROM HINODE/EIS OFF LIMB OBSERVATIONS Bemporad A. & Abbo L. –
Ionization, Resonance excitation, fluorescence, and lasers The ground state of an atom is the state where all electrons are in the lowest available energy.
1 B.Ricci* What have we learnt about the Sun from the measurement of 8B neutrino flux? Experimental results SSM predictions SSM uncertainties on  (8B)
Solar Prominence Properties derived from the UV-EUV SUMER spectral atlas S. Parenti, J.-C. Vial, P. Lemaire IAS, Univeristé Paris Sud.
Superhot DEM (or DF?) RHESSI continuum with TRACE or EIT FeXXIV, SUMER FeXXI, GOES, or whatever.
Suprit Singh Talk for the IUCAA Grad-school course in Inter-stellar medium given by Dr. A N Ramaprakash 15 th April 2KX.
Lecture 3 Spectra. Stellar spectra Stellar spectra show interesting trends as a function of temperature: Increasing temperature.
The Classification of Stellar Spectra
Age dependence of EM in AR Cores... and... Some thoughts on the Accuracy of Atomic Data Helen Mason, Durgesh Tripathi, Brendan O’Dwyer and Giulio Del Zanna.
 How does the wavelength of a light beam and the size of a slit it is going through control the amount of diffraction? DO WORK STOP.
Atomic Spectroscopy for Space Applications: Galactic Evolution l M. P. Ruffoni, J. C. Pickering, G. Nave, C. Allende-Prieto.
Average Lifetime Atoms stay in an excited level only for a short time (about 10-8 [sec]), and then they return to a lower energy level by spontaneous emission.
The Influence of the Return Current and the Electron Beam on the X-Ray Flare Spectra Elena Dzifčáková, Marian Karlický Astronomical Institute of the Academy.
Peter Young* George Mason University, VA Uri Feldman Artep Inc, MD *Work funded by NSF and NASA.
The Influence of the Return Current and Electron Beam on the EUV and X-Ray Flare Emission E. Dzifčáková, M. Karlický Astronomical Institute of the Academy.
Ch 8: Stars & the H-R Diagram  Nick Devereux 2006 Revised 9/12/2012.
Data Needs for Simulations of Electron-driven Processes in Planetary and Cometary Atmospheres by Laurence Campbell & Michael J. Brunger School of Chemical.
Modelling the radiative signature of turbulent heating in coronal loops. S. Parenti 1, E. Buchlin 2, S. Galtier 1 and J-C. Vial 1, P. J. Cargill 3 1. IAS,
Introduction to Plasma- Surface Interactions Lecture 3 Atomic and Molecular Processes.
ADAS workshop, Auburn University1 Generalised collisional-radiative modelling for Silicon and beyond Alessandra Giunta.
Line list of HD 18 O rotation-vibration transitions for atmospheric applications Semen MIKHAILENKO, Olga NAUMENKO, and Sergei TASHKUN Laboratory of Theoretical.
Evidence of Energy Levels. e-e- e-e- Ground state Excited state Electrons can only be at specific energy levels, NOT between levels.
1 Introduction to Atomic Spectroscopy Lecture 10.
NON-THERMAL   DISTRIBUTIONS AND THE CORONAL EMISSION J. Dudík 1, A. Kulinová 1,2, E. Dzifčáková 1,2, M. Karlický 2 1 – OAA KAFZM FMFI, Univerzita Komenského,
Chemistry XXI Unit 2 How do we determine structure? The central goal of this unit is to help you develop ways of thinking that can be used to predict the.
X-shooter spectroscopy of the GRB090926A afterglow Valerio D’Elia (ASDC/INAF-OAR) & The X-shooter GRB collaboration April, 22nd Kyoto - Japan.
atomic excitation and ionisation
Elemental Analysis using Atomic Absorption and Emission Spectroscopy Bodhisatwa Das.
The CHIANTI Atomic Database An Overview of Data, Software and Applications Dr Peter Young George Mason University, USA NASA Goddard Space Flight Center,
The 2p-3d Electron Transition Multiplet of Ar +13 : A Stellar Density Diagnostic Laura Heeter Kristina Naranjo-Rivera
Özkan ŞAHİN & Tadeusz KOWALSKI Uludağ University, Physics Department, Bursa – TURKEY Faculty of Physics and Applied Computer Science, AGH University of.
IAS 20 June 2013 Celebrating the achievements of Alan Gabriel Laboratory spectroscopy Exploring the process of dielectronic recombination S. Volonte.
UCL DEPT. OF SPACE & CLIMATE PHYSICS SOLAR & STELLAR PHYSICS GROUP Atomic Data for Astrophysics VOTada VO Tools and Atomic Data for Astrophysics Giulio.
Atomic Physics Quantum Physics 2002 Recommended Reading: Harris Chapter 7.
An Experimental Approach to the Prediction of Complete Millimeter and Submillimeter Spectra at Astrophysical Temperatures Ivan Medvedev and Frank C. De.
What Are the Implications of Optical Closure Using Measurements from the Two Column Aerosol Project? J.D. Fast 1, L.K. Berg 1, E. Kassianov 1, D. Chand.
Saturation Roi Levy. Motivation To show the deference between linear and non linear spectroscopy To understand how saturation spectroscopy is been applied.
Raman Spectroscopy BY Dr. Bhawna.
Spectral classification of galaxies of LAMOST DR3
Electron-impact excitation of Be-like Mg
K-x-ray Emission in Fast O5+ on Ar Collisions
It should be no surprise that the Schrödinger result exactly matches the Bohr result. Recall that Bohr was able to explain the spectrum of the H atom,
Where do these spectral lines come from?
Laser and its applications
UVIS Saturn Atmosphere Occultation Prospectus
Lecture 3 Radiative Transfer
Bohr Model of the Atom Objective: Discuss the Bohr model of the atom and calculate the energy of the photon emitted or absorbed by an electron as it.
MODELS OF EMISSION LINE PROFILES AND SPECTRAL ENERGY DISTRIBUTIONS
Quantum Physics Atomic spectra and atomic energy states.
How precisely do we know the antineutrino source spectrum from a nuclear reactor? Klaus Schreckenbach (TU München) Klaus Schreckenbach.
7.1 Explained.
Atomic Absorption Spectroscopy
Laser and its applications
Raman Spectroscopy A) Introduction IR Raman
Monitoring Saturn's Upper Atmosphere Density Variations Using
Studying Transition Region Phenomena with Solar-B/EIS
VOTADA VO Tools and Atomic Data for Astrophysics
Spectroscopy of solar prominences simultaneously from space and ground
UVIS Titan T0, TA Analysis
Constraining the Nuclear Equation of State via Nuclear Structure observables 曹李刚 中科院近物所 第十四届全国核结构大会,湖州,
Bohr’s Model of Atomic Quantization
Presentation transcript:

ADAS workshop, Auburn University Anomalous O IV line ratios in the solar spectrum Alessandra Giunta 07-10-11 ADAS workshop, Auburn University

O IV lines in the solar spectrum SoHO/SUMER Intensity Wavelength/Å SoHO/CDS Intensity Wavelength/Å Hinode/EIS Intensity Wavelength/Å 07-10-11 ADAS workshop, Auburn University

ADAS workshop, Auburn University Problem Muglach et al. (2010) found that the measured O IV I(787.7 Å)/I(279.9 Å) ratio is lower than the predicted ratio by a factor 2-5 and the derived electron temperature is in the range of logT=5.58-6.07, much higher than the formation temperature in ionisation equilibrium. ▪ They used: - observations taken during SUMER/EIS campaign in April 2007 - atomic data from CHIANTI v. 5.2.1. ▪ They investigated various possible causes: - instrumental and observational effects - presence of additional processes (photo-excitation, self-absorption, non-Maxwellian distribution). ▪ They did not solve the discrepancy, with the implication that non equilibrium ionisation state may be present. 07-10-11 ADAS workshop, Auburn University

ADAS workshop, Auburn University Approach ▪ A new observational data set taken during the joint SUMER/CDS/EIS campaign of April 2009 is explored. ▪ The ratio I(787.7 Å)/I(279.9 Å) is re-examined and other three O IV ratios are investigated: - I(554.5Å)/I(279.9 Å) temperature dependent - I(787.7 Å)/I(554.5 Å) temperature dependent - I(787.7 Å)/I(b790 Å) temperature independent ▪ The atomic data for these ratios are revised comparing three datasets: - CHIANTI v. 5.2.1 - Revised (CHIANTI + Sampson, 1995) - Aggarwal & Keenan (2008) 07-10-11 ADAS workshop, Auburn University

ADAS workshop, Auburn University Observational domain ▪ Observational data taken from SUMER, CDS and EIS have been calibrated using the standard procedures. ▪ The co-alignment has been done using common emission lines or lines emitted from the same ion. ▪ The cross-calibration has been performed through direct line comparison and spectroscopic methods. ▪ The observed R=I(787.7 Å)/I(279.9 Å) ratio obtained is: logR=1.8 (the intensity units are photons cm-2 s-1) 07-10-11 ADAS workshop, Auburn University

ADAS workshop, Auburn University Atomic domain Three atomic datasets are examined: ▪ CHIANTI ▪ Revised ▪ Aggarwal & Keenan (2008) CHIANTI The main source for the effective collision strengths (Y-values) is Zhang et al. (1994) for the first 15 levels and Sampson (1995) for the other 110 levels. However only transitions which involve the first 5 levels are included in the model. A-value for transitions amongst levels from 6 to 15 are also included, but not the corresponding Y-values. Revised This dataset has been built up merging the CHIANTI data with the DW calculations of Sampson to add the whole set of missing Y-values. Aggarwal & Keenan (2008) These are the most recent R-matrix calculations for O3+ available in literature and include transitions which involve the n=4 levels. 07-10-11 ADAS workshop, Auburn University

Atomic data comparison The main difference lies in the population of the upper level (2s23s 2S1/2), called N279, from which the line at 279.9 Å originates. rv = Revised ch = CHIANTI ak = Aggarwal & Keenan 07-10-11 ADAS workshop, Auburn University

ADAS workshop, Auburn University Results Comparison between the observed and theoretical values for the ratio I(787.7 Å)/I(279.9 Å). The electron temperature derived in this work is logT=5.17-5.39, close to the temperature expected under the assumption of ionisation equilibrium. rv = Revised ch = CHIANTI ak = Aggarwal & Keenan logT=5.58-6.07 logT=5.17-5.39 formation temperature 07-10-11 ADAS workshop, Auburn University

Other line ratio comparison Temperature dependent line ratios As further check, the three other O IV ratios are illustrated, comparing the measurements with theoretical data. Since the discrepancy is caused by the intensity of the line at 279.9 Å, the I(554.5Å)/I(279.9 Å) ratio shows the same behaviour as I(787.7Å)/I(279.9 Å), unlike the other two ratios. I(554.5Å)/I(279.9 Å) Temperature independent line ratio logT=5.17 I(787.7 Å)/I(b790 Å) I(787.7 Å)/I(554.5 Å) rv = Revised ch = CHIANTI ak = Aggarwal & Keenan 07-10-11 ADAS workshop, Auburn University

ADAS workshop, Auburn University Discussion The Muglach et al. (2010) O IV discrepancy has been solved, however some issues arise from this work: ▪ the uncertainties of atomic data and model can affect substantially the interpretation of the observed emission ▪ the completeness (complete system of A-values and Y-values) and top-up does matter in the population model ▪ new R-matrix calculation for O3+ are desirable to add more confidence in the currently available atomic data. 07-10-11 ADAS workshop, Auburn University