The 2p-3d Electron Transition Multiplet of Ar +13 : A Stellar Density Diagnostic Laura Heeter Kristina Naranjo-Rivera 2003-04.

Slides:



Advertisements
Similar presentations
Collisional-Radiative Modeling of EBIT Spectra of High-Z Ions Yuri Ralchenko National Institute of Standards and Technology Gaithersburg, MD ADAS.
Advertisements

Cristina Chifor SESI Student Intern 2005 Solar Physics, Code 612 NASA/Goddard Space Flight Center Mentors: Dr. Ken Phillips & Dr. Brian Dennis FE AND FE/NI.
Fitting X-ray Spectra with Imperfect Models Nancy S. Brickhouse Harvard-Smithsonian Center for Astrophysics Acknowledgments to Randall Smith and Adam Foster.
Bayesian modelling of a diagnostic helium beam ADAS workshop, Armagh Observatory, October 4th, 2010 Maciej Krychowiak M. Brix, D. Dodt, R. König, O. Schmitz,
Super-Hot Thermal Plasmas in Solar Flares
Min Huang Fudan University, Shanghai Modern Physics Institute, Shanghai EBIT Lab,
Astrophysical Priorities for Accurate X-ray Spectroscopic Diagnostics Nancy S. Brickhouse Harvard-Smithsonian Center for Astrophysics In Collaboration.
Ionization and Recombination with Electrons: Laboratory Measurements and Observational Consequences Daniel Wolf Savin Columbia Astrophysics Laboratory.
COOL STARS and ATOMIC PHYSICS Andrea Dupree Harvard-Smithsonian CfA 7 Aug High Accuracy Atomic Physics In Astronomy.
Measuring the Temperature of Hot Solar Flare Plasma with RHESSI Amir Caspi 1,2, Sam Krucker 2, Robert P. Lin 1,2 1 Department of Physics, University of.
Ionization, Resonance excitation, fluorescence, and lasers The ground state of an atom is the state where all electrons are in the lowest available energy.
Possibility for Coronal Magnetic Field Measurements by EUV and X-ray Spectroscopy Sophie Canton (Charge exchange) Matt Carpenter (Algorithms,CX) Jaan Lepson.
Introduction Radioactive nuclei decay in numerous ways: emitting electrons, protons, neutrons, alpha particles, gamma rays, x-rays, or some combination.
X-Ray Spectroscopy. 1 eV 100 eV 10 eV Energy (keV) The need for high resolution X-ray spectroscopy Astrophysical Plasmas: Simulation of the emission from.
Charge-Exchange Mechanism of X-ray Emission V. Kharchenko ITAMP, Harvard-Smithsonian Center for Astrophysics, Cambridge 1. Introduction - interaction between.
Superhot DEM (or DF?) RHESSI continuum with TRACE or EIT FeXXIV, SUMER FeXXI, GOES, or whatever.
Astrophysics Research Projects: massive star winds, x-ray emission, theoretical models, spectroscopy, laboratory plasma astrophysics David Cohen on leave.
Photoionization Modeling: the K Lines and Edges of Iron P. Palmeri (UMH-Belgium) T. Kallman (GSFC/NASA-USA) C. Mendoza & M. Bautista (IVIC-Venezuela) J.
A New View of Accretion Shock Structure Nancy S. Brickhouse Harvard-Smithsonian Center for Astrophysics Collaborators: Steve Cranmer, Andrea Dupree, Juan.
July 11 X-Ray Gratings Workshop Capella Grating Data and the Emission Line Project - An Update Priya Desai (CfA) Nancy Brickhouse Jeremy Drake Dave Huenenmoerder.
Stars Introduction To “Atomic Astrophysics and Spectroscopy” (AAS) Anil Pradhan and Sultana Nahar Cambridge University Press 2011 Details at:
4-1 Chap. 7 (Optical Instruments), Chap. 8 (Optical Atomic Spectroscopy) General design of optical instruments Sources of radiation Selection of wavelength.
990901EIS_RR_Science.1 Science Investigation Goals and Instrument Requirements Dr. George A. Doschek EIS US Principal Investigator Naval Research Laboratory.
Fast imaging of global eigenmodes in the H-1 heliac ABSTRACT We report a study of coherent plasma instabilities in the H-1 plasma using a synchronous gated.
Pressure diagnostic for the trap center of Electron beam ion trap by EUV spectroscopy Guiyun Liang 梁贵云 National Astronomical Observatories, CAS Beijing,
Multiwavelength observations of a partially occulted solar flare Laura Bone, John C.Brown, Lyndsay Fletcher.
Spectral Analysis, Uncertainties in Atomic Data, And AtomDB Randall Smith, Adam Foster (SAO) Stuart Loch & Connor Ballance, Auburn University Michael Witthoeft,
Lab 12 Atomic spectra and atomic structure
Atomic Spectroscopy for Space Applications: Galactic Evolution l M. P. Ruffoni, J. C. Pickering, G. Nave, C. Allende-Prieto.
APOGEE: The Apache Point Observatory Galactic Evolution Experiment l M. P. Ruffoni 1, J. C. Pickering 1, E. Den Hartog 2, G. Nave 3, J. Lawler 2, C. Allende-Prieto.
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.
Negative Ions in IEC Devices David R. Boris 2009 US-Japan IEC Workshop 12 th October, 2009 This work performed at The University of Wisconsin Fusion Technology.
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.
Diagnostics of non-thermal n-distribution Kulinová, A. AÚ AVČR, Ondřejov, ČR FMFI UK, Bratislava, SR.
Plasma diagnostics using spectroscopic techniques
Topic 2 Atomic Theory SL+HL. Topic 2.1 The atom Position ChargeRelative Mass Proton; p + Nucleus 1+ 1 Neutron; n Nucleus 0 1 Electron; e - Cloud/orbitals.
Anisotropic dielectronic resonances from magnetic-dipole lines Yuri Ralchenko National Institute of Standards and Technology Gaithersburg, MD, USA ADAS.
Diagnosing the Shock from Accretion onto a Young Star Nancy S. Brickhouse Harvard-Smithsonian Center for Astrophysics Collaborators: Steve Cranmer, Moritz.
Oct. 11, Review: BB radiation enables measure of both stellar temperature T, and surface flux, F s The shift of the peak λ, to have a maximum flux.
VUV-diagnostics of inelastic collision processes in low temperature hydrogen plasmas J. Komppula & JYFL ion source group University of Jyväskylä Department.
Electronic Transitions of Palladium Monoboride and Platinum Monoboride Y.W. Ng, H.F. Pang, Y. S. Wong, Yue Qian, and A. S-C. Cheung Department of Chemistry.
POST CME EVENTS: COOL JETS AND CURRENT SHEET EVOLUTION A. Bemporad, G. Poletto, S. T. Suess IAU Symposium 226 Coronal and Stellar Mass Ejections September.
On the Stark broadening of Cr II spectral lines in atmospheres of DB white dwarfs Z. Simić 1, M. S. Dimitrijević 1,2, A. Kovačević 3, S. Sahal-Bréchot.
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,
UCL DEPT. OF SPACE & CLIMATE PHYSICS SOLAR & STELLAR PHYSICS GROUP Atomic Data for Astrophysics VOTADA VO Tools and Atomic Data for Astrophysics Giulio.
NIST Spectroscopic Research on Heavy Elements Wolfgang L Wiese National Institute of Standards and Technology (NIST), USA.
The CHIANTI Atomic Database An Overview of Data, Software and Applications Dr Peter Young George Mason University, USA NASA Goddard Space Flight Center,
Laboratory Astrophysics using an Engineering Model XRS Microcalorimeter Array NASA/GSFCLLNL. F. Scott PorterPeter Beiersdorfer Keith GendreauGreg Brown.
XUV monochromatic imaging spectroscopy in the SPIRIT experiment on the CORONAS-F mission I. Diagnostics of solar corona plasma by means of EUV Spectroheliograph.
Fourier Transform Emission Spectroscopy of Some New Bands of ReN R. S. Ram Department of Chemistry, University of Arizona, Tucson, AZ and P. F. Bernath.
Simulation of CHANDRA X-Ray Spectral Observations of  Pup (O4 If) J. J. MacFarlane, P. Wang Prism Computational Sciences Madison, WI J. P. Cassinelli,
Unit 12: Part 2 Quantum Physics. Overview Quantization: Planck’s Hypothesis Quanta of Light: Photons and the Photoelectric Effect Quantum “Particles”:
Spectrogram 2-40 A for varying temperature. Spectra this is how we find out what everything is made of Vinay Kashyap Smithsonian Astrophysical Observatory.
UCL DEPT. OF SPACE & CLIMATE PHYSICS SOLAR & STELLAR PHYSICS GROUP Atomic Data for Astrophysics VOTada VO Tools and Atomic Data for Astrophysics Giulio.
High Energy Observational Astrophysics. 1 Processes that emit X-rays and Gamma rays.
X-ray Spectroscopy of Coronal Plasmas Ken Phillips Scientific Associate, Natural History Museum, and Honorary Prof., QUB 1.
Milan S. Dimitrijević and Nenad Milovanović
Nonthermal distributions in the solar and stellar coronae
Mass Spectronomer.
Atomic Absorption Spectroscopy
Study of the resonance states in 27P by using
Studying Transition Region Phenomena with Solar-B/EIS
Overview of the Low Energy Telescope and its Performance in-orbit
Chromospheric and Transition Region Dynamics
VOTADA VO Tools and Atomic Data for Astrophysics
Dione’s O2 Exosphere C. J. Hansen January 2013.
5.4 Learning from Light Our goals for learning
-Short Talk- The soft X-ray characteristics of solar flares, both with and without associated CMEs Kay H.R.M., Harra L.K., Matthews S.A., Culhane J.L.,
UVIS Titan T0, TA Analysis
Presentation transcript:

The 2p-3d Electron Transition Multiplet of Ar +13 : A Stellar Density Diagnostic Laura Heeter Kristina Naranjo-Rivera

Introduction Applications Density and temperature diagnostic for astrophysics -Stellar corona, solar flairs -Naturally occurring thermal plasma -Chandra Observatory x-ray data

L-shell spectral peaks Simple Structure Density sensitivity (Å)

Lepson et al. Survey 2p-3d Ar +13 Spectral Peaks

Trabert et al. Study 3d 1 5/2 3d 1 3/2 2p 2 3/ 2 Metastable State 2p 1 3/2 Ground State 2p 1 1/2 Forbidden Transition Metastable level- 9.7 ms atomic lifetime

Theory 3d 1 5/2 3d 1 3/2 2p 2 3/ 2 Metastable State 2p 1 3/2 Ground State 2p 1 1/2 Forbidden Transition Wavelength (Å) Dr. Ming Feng-Gu –Peak intensities will invert with increased beam current density –Increased excitation to metastable state 2p 1 3/2

Hypothesis Sensitivity to beam current density Increased electron excitation to metastable level

Objective Stellar Object EBIT Ar +13 Emission Spectra Density? DensityAr +13 Emission Spectra Electon Beam Ion Trap

EBIT Liquid Helium Reservoir Liquid Nitrogen Reservoir Trapping Region Collector Electron Gun Superconducting Helmholtz Magnet

Methods Prepare EBIT Excite Ar to Ar +13 Determine Constant Beam Energy Collect & Analyze Spectral Images Calculate Intensity Ratios Compare Experimental and Theoretical Data

Results Inverse relationship: beam current and intensity ratio

Results vs. Theory Wavelength (Å)

Comparison to Theoretical Models Density (cm –3 ) Ar +13 experimental data Monoenergetic beam Maxwellian plasma model

Discussion Increased population of metastable state occurred as beam current density increased Accuracy promises Ar +13 as a useful density diagnostic

Further Studies Broader density range Use other more abundant elements –Mg, Fe, Ni, and more –Currently Fe +21 is being tested

Acknowledgements The EBIT Team –Dr. Peter Beiersdorfer –Edward Magee –Dr. Hui Chen –Dr. Elmar Träbert –Ming Feng-Gu Ms. Fruen and the Research Class

The 2p-3d Electron Transition Multiplet of Ar +13 : A Stellar Density Diagnostic Laura Heeter Kristina Naranjo-Rivera

Elaboration of Methods: Analyze Ar +13 Spectra Igor Pro N +5 calibration Sum like data

Calculate Intensity Ratios R = (I (3d5/2→2p3/2) + I (3d3/2→2p3/2) ) / I (3d3/2→2p1/2)