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L U N D UN I V E R S I T Y
Fluorescence and resonant ionization in Eta Carinae
           - an astrophysical laboratory




                    Henrik Hartman, Lund University, Sweden

      Current Development in Atomic, Molecular and Optical Physics, Delhi 2011
                                                                                 1
L U N D UN I V E R S I T Y




Laboratory Astrophysics @ Lund University




                             -   Stellar high resolution spectroscopy (VLT; HST)
                             -   High-resolution FTS measurements of dishcarges (Edlén lab)
                             -   Lifetime measurements: LIF on laser produced plasmas (LLC)




                                                                                        2
L U N D UN I V E R S I T Y




Collaborators

  Lund/Malmö: H.Nilsson, H.Lundberg, L.Engström, S.Huldt, T.Lennartsson,
  T.Brage, P.Jönsson, N.Ryde, (S.Johansson & V.Letokhov)

  Eta Carinae: T.Gull (NASA), M.Bautista, V.Fivet (U Mich), J.Groh(MPIfI)

  Lifetimes: E.Biemont group (th, Liege), S.Mannervik group (exp, Stockholm)




  Thanks to:
  CDAMOP2011 organizers
  Swedish Science Council (VR),
  Swedish National Space Board (SNSB)                     Johansson & Letokhov (deceased 2009)




                                                                                         3
L U N D UN I V E R S I T Y




Outline

  -    Introduction, Eta Carinae

  -    Fluorescence

  -    Selective ionization (RETPI – Resonance Enhanced Two-Photon
       Ionization) for SiIII and FeIII

  -    Outlook




                                                                     4
L U N D UN I V E R S I T Y




   Eta Carinae


                 Homunculus



                 Central stars

                                      Strontium filament
Weigelt blobs




                                                           10”
                                 1”         HST / WFPC2 image
                                                            5
L U N D UN I V E R S I T Y




 5.54 year periodicity observed in X-ray




RXTE-obsverations, courtesy of M.Corcoran.




                                             K. Nielsen

                                                          6
L U N D UN I V E R S I T Y




Eta Carinae

Maximum state
– the radiation from the central
star is driving the
photoprocesses in the Weigelt
condensation.




Minimum state
– the radiation from the central
star is blocked for several
months. The transition into the
minimum is referred to as the
spectroscopic event.



                                   7
L U N D UN I V E R S I T Y




The Bowen mechanism (fluorescence)




                                     8
L U N D UN I V E R S I T Y




Fluorescence lines in HST spectra of WB




                                          9
L U N D UN I V E R S I T Y




Temporal variations of HI and FeII lines

                             The temporal variations during the
                             spectroscopic event is different for
                             different kinds of lines.
                             Hydrogen lines and fluroescent
                             lines vary quicker, whereas the
                             (most) forbidden lines excited by
                             collisions have a much slower
                             response set by the recombination
                             time scale, i.e. removal of
                             electrons.




                                                              10
L U N D UN I V E R S I T Y




Variations of SiIII] 1892 Å line

maximum                            Spatial scale




minimum




                                           11
L U N D UN I V E R S I T Y




Variations of SiIII] 1892 Å line




                                   12
L U N D UN I V E R S I T Y




RETPI of Si+, enhancing the 1892Å SiIII] line

                             The 2-photon process involving HLyα
                             and HLyγ leaves the atom doubly
                             ionized and in an excited state,
                             producing the 1892 Å radiation as it
                             decays.




                               Johansson & Letokhov, Science (2001)
                               Johansson, Hartman, Letokhov A&A (2006)

                                                                  13
L U N D UN I V E R S I T Y




Estimation of the RETPI rate in the Weigelt blobs




 The 2-photon process involving HLyα
 and HLyγ depends on the difference
 between the real level and the virtual
 level, and in the intensity of the H
 Lyman lines.

 With estimates of the conditions in the
 WB, the observed intensity of the
 1892 Å feature, 7x10-12 erg cm-2 s-1 Å-1,
 can be explained buy the RETPI
 process.




                                                    14
L U N D UN I V E R S I T Y




Ionization balance in the Weigelt blobs




                                          15
L U N D UN I V E R S I T Y




Possibilities for RETPI producing [FeIII]

                             The double H Lyα energy corresponds to
                             the difference between the 3d5(6S) 4s 5S in
                             FeIII and 3d6(5D) 4s 4D in FeII, with the 5p
                             levels in between.




                                                                      16
L U N D UN I V E R S I T Y




    Conclusion and outlook
•    In the Weigelt blobs of Eta Carinae (as in many other astrophysical plasmas),
     fluorescence is an important process for line formation. The temporal variations in the
     incident radiation from the central star allow us to study these processes separate from
     the collisional excitation and ionization.

•    The same HST spectra indicate that RETPI (Resonance Enhanced Two-Photon
     Ionization) can be responsible for the formation of strongly varying lines. During the
     high state (maximum), the RETPI process can control the ionization equilibrium for
     many ions.

•    RETPI often leaves the ions in an excited state. With the RETPI producing strong
     forbidden lines, e.g. Si III] and [FeIII], care must be taken when using simple line
     rations for determination of physical conditions.

•    Forbidden lines are often strong and used for diagnostics in emission line objects like
     stellar winds, AGNs and Quasars. Eta Carinae is an ideal and rare object to study
     these processes, but the importance of these processes are probably much wider.


                                                                                               17

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Fluorescence and resonant ionization in astrophysical plasmas, with emphasis on and examples from the star Eta Carinae

  • 1. L U N D UN I V E R S I T Y Fluorescence and resonant ionization in Eta Carinae - an astrophysical laboratory Henrik Hartman, Lund University, Sweden Current Development in Atomic, Molecular and Optical Physics, Delhi 2011 1
  • 2. L U N D UN I V E R S I T Y Laboratory Astrophysics @ Lund University - Stellar high resolution spectroscopy (VLT; HST) - High-resolution FTS measurements of dishcarges (Edlén lab) - Lifetime measurements: LIF on laser produced plasmas (LLC) 2
  • 3. L U N D UN I V E R S I T Y Collaborators Lund/Malmö: H.Nilsson, H.Lundberg, L.Engström, S.Huldt, T.Lennartsson, T.Brage, P.Jönsson, N.Ryde, (S.Johansson & V.Letokhov) Eta Carinae: T.Gull (NASA), M.Bautista, V.Fivet (U Mich), J.Groh(MPIfI) Lifetimes: E.Biemont group (th, Liege), S.Mannervik group (exp, Stockholm) Thanks to: CDAMOP2011 organizers Swedish Science Council (VR), Swedish National Space Board (SNSB) Johansson & Letokhov (deceased 2009) 3
  • 4. L U N D UN I V E R S I T Y Outline - Introduction, Eta Carinae - Fluorescence - Selective ionization (RETPI – Resonance Enhanced Two-Photon Ionization) for SiIII and FeIII - Outlook 4
  • 5. L U N D UN I V E R S I T Y Eta Carinae Homunculus Central stars Strontium filament Weigelt blobs 10” 1” HST / WFPC2 image 5
  • 6. L U N D UN I V E R S I T Y 5.54 year periodicity observed in X-ray RXTE-obsverations, courtesy of M.Corcoran. K. Nielsen 6
  • 7. L U N D UN I V E R S I T Y Eta Carinae Maximum state – the radiation from the central star is driving the photoprocesses in the Weigelt condensation. Minimum state – the radiation from the central star is blocked for several months. The transition into the minimum is referred to as the spectroscopic event. 7
  • 8. L U N D UN I V E R S I T Y The Bowen mechanism (fluorescence) 8
  • 9. L U N D UN I V E R S I T Y Fluorescence lines in HST spectra of WB 9
  • 10. L U N D UN I V E R S I T Y Temporal variations of HI and FeII lines The temporal variations during the spectroscopic event is different for different kinds of lines. Hydrogen lines and fluroescent lines vary quicker, whereas the (most) forbidden lines excited by collisions have a much slower response set by the recombination time scale, i.e. removal of electrons. 10
  • 11. L U N D UN I V E R S I T Y Variations of SiIII] 1892 Å line maximum Spatial scale minimum 11
  • 12. L U N D UN I V E R S I T Y Variations of SiIII] 1892 Å line 12
  • 13. L U N D UN I V E R S I T Y RETPI of Si+, enhancing the 1892Å SiIII] line The 2-photon process involving HLyα and HLyγ leaves the atom doubly ionized and in an excited state, producing the 1892 Å radiation as it decays. Johansson & Letokhov, Science (2001) Johansson, Hartman, Letokhov A&A (2006) 13
  • 14. L U N D UN I V E R S I T Y Estimation of the RETPI rate in the Weigelt blobs The 2-photon process involving HLyα and HLyγ depends on the difference between the real level and the virtual level, and in the intensity of the H Lyman lines. With estimates of the conditions in the WB, the observed intensity of the 1892 Å feature, 7x10-12 erg cm-2 s-1 Å-1, can be explained buy the RETPI process. 14
  • 15. L U N D UN I V E R S I T Y Ionization balance in the Weigelt blobs 15
  • 16. L U N D UN I V E R S I T Y Possibilities for RETPI producing [FeIII] The double H Lyα energy corresponds to the difference between the 3d5(6S) 4s 5S in FeIII and 3d6(5D) 4s 4D in FeII, with the 5p levels in between. 16
  • 17. L U N D UN I V E R S I T Y Conclusion and outlook • In the Weigelt blobs of Eta Carinae (as in many other astrophysical plasmas), fluorescence is an important process for line formation. The temporal variations in the incident radiation from the central star allow us to study these processes separate from the collisional excitation and ionization. • The same HST spectra indicate that RETPI (Resonance Enhanced Two-Photon Ionization) can be responsible for the formation of strongly varying lines. During the high state (maximum), the RETPI process can control the ionization equilibrium for many ions. • RETPI often leaves the ions in an excited state. With the RETPI producing strong forbidden lines, e.g. Si III] and [FeIII], care must be taken when using simple line rations for determination of physical conditions. • Forbidden lines are often strong and used for diagnostics in emission line objects like stellar winds, AGNs and Quasars. Eta Carinae is an ideal and rare object to study these processes, but the importance of these processes are probably much wider. 17