# Presentation: 161402

## PhotoionizationTim Kallman NASA/GSFC

*What is photoionization?*
- Removal of a bound electron by a photon
- Loosely refers to any situation where external photons are the dominant source of ionization (and heating)
*Outline:*
- Review of coronal plasma
- Effect of photoionization
- Background, definitions
- Examples

## Coronal ionization

- Assume all processes are in a steady state, so that for each ion species the rate of creation= rate of destruction
- Also assume that electron velocity distribution is Maxwellian, kTion ~kT  electron, so that electron collisions are much  more frequent  than ion collisions.
- Ion destruction is due to electron impact  ionization by thermal electrons
- Ion creation is due to recombination (radiative and dielectronic)
- The fraction of an ion peaks when the electron temperature is kTe~(0.7)I

## Slide 3

## Slide 4

## Photoionization

- What happens when an external photon source illuminates the gas?
- The photons ionize the atoms in the gas.
- The photoelectrons created in this way collide with ambient electrons (mostly) and heat the gas
- The gas cools by radiation
-  The gas temperature adjusts so that the heating and cooling balance

- In a photoionized gas  the temperature is not  a  free parameter
- and
- The ionization balance is determined by the shape and strength of the radiation field

## Slide 6

## Processes

- Photoionization (+heating)
- Recombination (+cooling)
- Dielectronic recombination (+cooling)
- Collisional ionization (cooling)
- Collisional excitation(cooling)
- Compton scattering
- Others (more later)

## Slide 8

## Slide 9

## Ionization and Thermal Balance

- For each ion:
-  Ionization         =      recombination
-   ~photon flux          ~electron density
- For the gas as a whole
-   Heating            =       cooling
-  ~photon flux             ~electron density
- => All results depend on the ratio photon flux/gas density or "ionization parameter"

## Slide 11

## Slide 13

## Consequences of Photoionization

- Temperature lower for same ionization than coronal, T~0.1 Eth/k
- Temperature is not a free parameter
- Temperature depends on global shape of spectrum
- At high ionization parameter, the gas is fully ionized, and the temperature is determined by Compton scattering and inverse T=<E>/4k
- Ionization balance is more 'democratic'
- Microphysical processes, such as dielectronic recombination, differ
- Observed spectrum differs

## Observed Spectrum: Emission

- In coronal gas, need kTe~E to collisionally excite lines.
- In a photoionized gas there are fewer lines which satisfy this condition.
- Excitation is often by recombination cascade
- Also get recombination continua (RRCs) due to recombination by cold electrons directly to the ground state.  The width of these features is directly proportional to temperature
- Due to the democratic ionization balance, it is more likely that diverse ions such as N VII, O VIII, Si XIV can coexist and emit efficiently than it would be in a coronal gas
- Inner shell ionization and fluorescence is also important in gases where the ionization state is low enough to allow ions with filled  shells to exist.

## Slide 16

## Helium-like ion level diagram

## Density dependence of He-like lines

- Coronal                   photoionized

- (Porquet and Dubau 1998)

## Chandra HETGS spectrum of Vela X-1

- (Shulz et al. 2002)

## Chandra HETGS spectrum of Capella

- (Canizares et al. 2000)

## Emission spectrum of NGC 1068

- NGC 1068 is the prototype of Seyfert 2 galaxies, i.e. AGN in which our direct line of sight to the nucleus is blocked by a thick ring of cold material.
- If so, we should see emission from photoionized material in the 'hole' of the doughnut, even though we don't see the nucleus directly
- Chandra HETGS X-ray spectra appear to confirm this prediction

## Slide 22

## Slide 23

## Iron K Lines

- Widely Emitted by all stages of iron, due to the efficiency of the K shell fluorescence process, and expected to be bright due to the relative abundance of iron.observed from all classes of (photoionized) X-ray sources.
- Are likely to probe the hottest and most highly ionized regions of photoionized gases, due to the high atomic number of iron.
- As discovered by ASCA, this line shows evidence for relativistic broadening in Seyfert galaxies and some black hole candidates.
- The combined effects of special and general relativity broaden and redden the line profile, and the shape depends on the inclination of the accretion disk and on the range of radii where emission occurs.

## Line Broadening by Black Hole Disk Emission

- Fabian et al. 2000

## Iron K Line from Seyfert Galaxy MCG-6-30-15

- Tanaka et al., 1995

## Absorption

- Absorption by interstellar material is in every spectrum, but absorption is uniquely associated with photoionized sources.
- A crude approximation for the photoabsorption cross section of a hydrogenic ion is that the cross section is ~Z-2  at the threshold energy, and that the threshold energy scales ~Z2.
- In addition, the cosmic abundances of the elements decrease approximately ~Z-4  above carbon
- So the net cross section scales as E-3, and large jumps in absorption are not expected at the thresholds.
- Detection of such edges are indicative of abundance anomalies or partial ionization of the gas

## Cross section for photoionization for abundant

-  elements vs. wavelength (Zombeck)

## Interstellar absorption (Morrison and McCammon; Zombeck)

## Example 4:  Photoabsorption spectrum of the Seyfert 1 galaxy MCG-6-30-15

- MCG-6-30-15 is a relatively bright Seyfert 1 galaxy
- ASCA discovered the first relativistically broadened iron K lines from this source, and it remains one of the most extreme examples of this phenomenon.
- ASCA also discovered features which were interpreted as absorption by O VII and O VIII photoionization 'edges', i.e. Photons absorbed in photoionizing these ions from the ground state.
- The first  Chandra spectra failed to find the same features.

## Chandra HETG Spectrum of MCG-6-30-15

## Relativistically broadened O VII Emission

## Simple Absorption (O VII, O VIII)l

## Including O VII 1s-np absorption

## Iron n=2-3 UTAs (Fe II-V)

## Fe I L shell photoionization

## Best fit: OVII + Fe UTA

## Summary: Absorption spectra of MCG-6-30-15

- The spectrum in the 15-20 A (0.6-0.8 keV) band observed with Chandra and XMM gratings contains complex features which do not fit with simple photoelectric absorption
- The O VII absorption edge is not at the energy expected, 16.8 A  (739 eV)
- One possible explanation is relativistically broadened emission in the O VIII Lalpha line (and N VII).
- Combined effects of the 1s-np absorption + n=2-3 transitions of iron + n=2 photoabsorption  appear to provide a good fit without requiring an exotic explanation.

## Summary

- 'Photoionization' is likely important in a wide range of astrophysical situations, including AGN, galactic binaries (BHT, XRB, CV), and the physics of photoabsorption is in every spectrum.
- Photoionization equilibrium differs from coronal equilibrium in significant ways, i.e. Lower temperature, more democratic ion distribution.
- The spectra emitted by photoionized plasmas contain characteristic features which have use as diagnostics.
- Absorption spectroscopy is (essentially) unique to photoionized sources, and is more important than was thought 5 yrs ago

## What’s Missing

- Time dependence:
- time average spectrum may not be the same as the response to the time average ionizing spectrum
- Gas we see may be transiently ionized due to, eg., gas flow
- Radiative transfer
- Non-thermal gases
- Multi-component

## Where to go from here

- Tools
-  Cloudy
- Xstar
- Photoion
- APEC
- Books
- Osterbrock ‘Astrophysics of Gaseous Nebulae’ (Ferland)
- Mihalas ‘Stellar Atmospheres’