Modeling Non-Equilbirum Plasma. Adam Foster

Similar documents
What we learned we don t know from Hitomi

Unraveling the Origin of Overionized Plasma in the Galactic Supernova Remnant W49B

Hitomi constraints on the atomic codes

A. N. Jadhav 1. Yeshwant Mahavidyalaya, Nanded. Maharashtra, India.

AGN Physics of the Ionized Gas Physical conditions in the NLR Physical conditions in the BLR LINERs Emission-Line Diagnostics High-Energy Effects

X-ray spectroscopy of nearby galactic nuclear regions

X-ray Radiation, Absorption, and Scattering

Processes and Diagnostics in Collisional Plasmas

X-ray Radiation, Absorption, and Scattering

Calculating Radiative Recombination Continuum From a Hot Plasma

R. Clark, D. Humbert, K. Sheikh Nuclear Data Section

EDS User School. Principles of Electron Beam Microanalysis

CONTRIBUTION FUNCTION OF MOLYBDENUM ATOM AND IONS IN ASTROPHYSICAL AND LABORATORY PLASMA AS A FUNCTION OF ELECTRON TEMPERATURE

Randall Smith (CfA) Collaborators: N. Brickhouse, A. Foster, H. Yamaguchi (CfA), J. Wilms (Erlangen), Li Ji (PMO)

The CHIANTI Atomic Database

arxiv: v1 [astro-ph.he] 29 Aug 2011

Effect of iron ionization balance on X-ray spectral analysis

AtomDB: X-ray Diagnostics of Astrophysical Plasmas

Collisional-Radiative Models and the Emission of Light

The Non Equilibrium Ionization Model in ISIS

Plasma Spectroscopy Inferences from Line Emission

arxiv: v1 [astro-ph.he] 3 Jul 2012

The Diffuse ISM Friday, February 11, 2011

Advanced SPEX models. Jelle Kaastra

Auger & X-ray Fluorescence

Theory of optically thin emission line spectroscopy

Uncertainties on atomic data

Photoionized Gas Ionization Equilibrium

Monte Carlo Simulator to Study High Mass X-ray Binary System

Journal of Advances in Applied Sciences and Technology (2015) Vol. 2 Issue 2-3 Page 27-33

Formation and Evolution. of the SS 433 Jets. Herman L. Marshall (MIT Kavli Institute) Sebastian Heinz (University Wisconsin)

LECTURE NOTES. Ay/Ge 132 ATOMIC AND MOLECULAR PROCESSES IN ASTRONOMY AND PLANETARY SCIENCE. Geoffrey A. Blake. Fall term 2016 Caltech

Atomic and Molecular Data Activities for Fusion Research in JAEA. T. Nakano Japan Atomic Energy Agency

Numerical Modeling of Radiative Kinetic Plasmas

Discovery of Emission Lines in the X-ray Spectrum of the Perseus Cluster

Deciphering the accretion structure in Vela X-1

ICF Capsule Implosions with Mid-Z Dopants

arxiv: v2 [astro-ph.he] 20 Nov 2017

Thermal Equilibrium in Nebulae 1. For an ionized nebula under steady conditions, heating and cooling processes that in

CMFGEN. Associate every atomic species with a given identification number

Production of HCI with an electron beam ion trap

H- and He-like X-ray emission due to charge exchange

This work was performed under the auspices of the U.S. Department of Energy by Lawrence Livermore National Laboratory under contract

The Interstellar Medium

Supernova Remnant Science with AXIS. Brian Williams & Hiroya Yamaguchi

NIST Research on Spectroscopy and Collisional-Radiative Modeling of Highly-Charged Ions of Tungsten

Joint ICTP-IAEA Workshop on Fusion Plasma Modelling using Atomic and Molecular Data January 2012

Plasmas occur over a vast range of conditions Temperature. Spectroscopy of Dense Plasmas. Population Kinetics Models

13 Synthesis of heavier elements. introduc)on to Astrophysics, C. Bertulani, Texas A&M-Commerce 1

arxiv: v1 [astro-ph.he] 16 Jan 2017

NASA Public Access Author manuscript Astrophys J. Author manuscript; available in PMC 2016 September 15.

Example: model a star using a two layer model: Radiation starts from the inner layer as blackbody radiation at temperature T in. T out.

Clusters and Groups of Galaxies

What can we learn from the AGN radio quiet continuum with SIMBOL-X?

2 The solar atmosphere

X-ray spectroscopy of low-mass X-ray binaries

Lec. 4 Thermal Properties & Line Diagnostics for HII Regions

Spectral signatures of the impulsive energy release in SMM BCS spectra

Physics and Chemistry of the Interstellar Medium

The AtomDB Charge Exchange Model

Radiative Properties of Krypton Plasma & Emission of Krypton DPP Source in Water-Window Spectral Range

Solar wind diagnostic using both insitu and spectroscopic measurements

Unveiling the spatial structure of the overionized plasma in the supernova remnant W49B

Aspects and prospects of

Notes on Photoionized Regions Wednesday, January 12, 2011

Photoionization Modelling of H II Region for Oxygen Ions

Detailed Study of a Turbulent multiphase multicomponent ISM

Physics of heavy multiply-charged ions: Studies on the borderile of atomic and nuclear physics

AG Draconis. A high density plasma laboratory. Dr Peter Young Collaborators A.K. Dupree S.J. Kenyon B. Espey T.B.

Astrophysics of Gaseous Nebulae and Active Galactic Nuclei

Heavy Element Nucleosynthesis. A summary of the nucleosynthesis of light elements is as follows

Basic principles of x-ray production

CHIANTI An atomic database for astrophysical plasmas

Where are oxygen synthesized in stars?

X-raying galactic feedback in nearby disk galaxies. Q. Daniel Wang University of Massachusetts

Radiation Detection for the Beta- Delayed Alpha and Gamma Decay of 20 Na. Ellen Simmons

Radiative-collisional processes in electron-tungsten ions collisions: quasiclassical calculations and data

Spectral analysis of K-shell X-ray emission of magnesium plasma produced by ultrashort high-intensity laser pulse irradiation

1 of 5 14/10/ :21

Combinatorial RF Magnetron Sputtering for Rapid Materials Discovery: Methodology and Applications

Integral field spectroscopy of Orion proplyds: metallicity and other proper7es

Basics, types Evolution. Novae. Spectra (days after eruption) Nova shells (months to years after eruption) Abundances

Thermal pressure vs. magnetic pressure

7. Non-LTE basic concepts

Astr 5465 March 6, 2018 Abundances in Late-type Galaxies Spectra of HII Regions Offer a High-Precision Means for Measuring Abundance (of Gas)

X-ray Spectroscopy of Massive Star Winds: Shocks, Mass-Loss Rates, and Clumping

LINE INTENSITY RATIOS IN THE EIS RANGE SENSITIVE TO ELECTRON DENSITIES IN 10 7 K PLASMAS

International Atomic Energy Agency, Vienna, Austria. Charge Transfer in Collisions of Ions with atoms and molecules.

Extreme ultraviolet spectroscopy of highly charged argon ions at the Berlin EBIT

Today: general condition for threshold operation physics of atomic, vibrational, rotational gain media intro to the Lorentz model

GA A25842 STUDY OF NON-LTE SPECTRA DEPENDENCE ON TARGET MASS IN SHORT PULSE LASER EXPERIMENTS

EXTREME ULTRAVIOLET AND SOFT X-RAY LASERS

The chemistry and thermodynamics of Pop III star formation

Collisional-Radiative Model of Molecular Hydrogen

New Atomic Data For Iron-Peak Elements For Use In Astrophysical Modeling. Nathalia Alzate

arxiv: v1 [astro-ph.he] 11 Mar 2011

EXCITATION RATE COEFFICIENTS OF MOLYBDENUM ATOM AND IONS IN ASTROPHYSICAL PLASMA AS A FUNCTION OF ELECTRON TEMPERATURE

Detailed Study of the X-ray Absorption in the ISM

PoS(INTEGRAL 2010)167

Atomic Absorption & Atomic Fluorescence Spectrometry

Transcription:

Modeling Non-Equilbirum Plasma Adam Foster

Definition CIE plasma: a plasma which is in collisional ionization equilibrium NEI plasma: a collisional plasma which is not in CIE

Ionization Balance dn ( z) =N e S(z 1 z) N (z 1) dt ( N e S(z z+ 1) + N e α( z z 1) + N H C (z z 1)) N ( z) + N e α( z+ 1 z) N ( z+ 1)+ N H C( z+ 1 z) N ( z+ 1)

Ionization Balance dn ( z) =N e S( z 1 z) N ( z 1) dt populating ( N e S ( z z+ 1) + Neα ( z z 1) + NHC ( z z 1) )N ( z) + N e α( z+ 1 z) N ( z+ 1) + N H C ( z+ 1 z) N (z+ 1 ) set dn ( z) =0 dt CIE ionbal: S( z 1 z) N ( z 1)+ α( z+ 1 z) N ( z+ 1)=( N e S(z z+ 1)+ N e α( z z 1)) N (z ) depopulating

CIE ionization balance

Non-Equilibrium Ionization Needs a source of hot or cold electrons. sudden adiabatic expansion & cooling shock heating Solar Flare Cas A Solar Flare

Ionization Balance dn ( z) =N e S( z 1 z) N ( z 1) dt ( N e S ( z z+ 1) + Ne α ( z z 1) + NHC ( z z 1) )N ( z) + N e α( z+ 1 z) N ( z+ 1) + N H C ( z+ 1 z) N (z+ 1 ) d N ( z) ( z) = N e A N dt Solve ionization fraction equations explicitly, see, e.g. matrix eigenvector method (Smith & Hughes 2010).

Timescales No difference noted at Net < 107 cm-3s (4 months @ 1cm-3) Equilibrium at Net>2x1012cm-3s (60,000 years @ 1cm-3)

Part 1 summary NEI plasma can exist over a wide range of timescales. It dramatically changes the set of ions visible in a typical temperature plasma

Emitting processes from NEI Plasma

Emitting processes from NEI Plasma

Excitation Ionization Recombination

Summary of relevant processes X +(z-1) X+z X+(z+1) Direct Ionization Excitation-autoionization Collisional excitation Dielectronic recombination Radiative Recombination

Ionizing Plasma Signifiers

Ionizing Plasma Signifiers

Ionizing Plasma Signifiers

Ionizing Plasma Signifiers ionizes

Fluorescence Yield Li-like 1s 2s2 Ar~z5 Aa~z2 ~ no fluorescence for light elements Gorczyca+ 2006 Ar ωk = Aa+ Ar

Yamaguchi+2014 Line Centroid shifts with Ion

Yamaguchi+2014 Line Centroid shifts with Ion

Recombining Plasma Line ratio shifts enhanced forbidden line Presence & enhancement of DR satellite lines. Low line intensities, n=3 1 transition reduced

Continuum Processes Driven By Brems Ne, Te RRC N 2-photon Nz+, ~Te (z+1)+, Te Ionizing Recombining Notes ~ Enhanced Shape truly representative of current Te Reduced (none) Enhanced Edges appear in recombining plasma ~ no effect ~ no effect Not useful as NEI diagnostic ~ Reduced

W49B T_init=3.2keV T_final=1.5keV Net=2x1010cm-3s

W49B 20ks SXS simulation RRC

NEI Modeling with AtomDB Calculate Ionbal Iion=N+z-1Neεion(Te) Iexc=N+zNeεexc(Te) Sum Spectrum! Irec=N+z+1Neεrec(Te)

Back to those processes Excitation Ionization Recombination

Show me the data! Level resolved recombination data: Badnell+ Level resolved fluorescence yield data: only for lowest 2-3 levels of some ions Inner shell excitation data: Rare! (Liang for Lilike) Inner shell ionization: Coulomb-Born-Exchange (Beigman 1996). Otherwise... nothing

Large scale data generation Fill in the blanks! Large scale FAC runs Inner shell excitation up to n=4 Inner shell ionization creating holes in n=1,2,3 shells Autoionization from all doubly excited levels Database size: 300Mb 18Gb.

~Fe XII Kα Kβ 6keV plasma ~Fe XVII Ni Kα Cr Fe XXV Kδ+ Ionizing Plasma Spectrum

Line ratio diagnostics 1s2 2s 1s 2s forbidden line regular ratios Recombine statistically greater 1s 2s 3P1 pop

Modeling a Recombining Plasma Ozawa+2009 Ozawa+2009 Quantity Ozawa AtomDB 3.0 kte 1.5keV 1.5keV Fe 4.44 2.43 Ni 10.9 3.63 norm 0.16 0.16

Summary on Features on NEI Real Te can still be obtained from brems. Recombining plasma show RRC egdes Ionizing plasmas will show inner shell heavy ion lines if they are hot enough (kt>2kev) Both ionization and recombination lead to an enhanced forbidden line Much room for improvement on the inner shell atomic data Models are available in XSPEC, SPEX etc.

NEI Models in XSPEC Nei: single time, single temperature snapshot emissivity. Rnei: same as vnei, but can specify initial temperature Pshock: Parallel shock. Multiple times in a single temperature Npshock: As pshock, but with separate ion and electron temperatures

Plug plug plug The beta4 version of NEI is available on the website. Works in all XSPEC models. Need to download updated beta data. www.atomdb.org