The Implications of a High Cosmic-Ray Ionization Rate in Diffuse Interstellar Clouds PowerPoint PPT Presentation

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Title: The Implications of a High Cosmic-Ray Ionization Rate in Diffuse Interstellar Clouds


1
The Implications of a High Cosmic-Ray Ionization
Rate in Diffuse Interstellar Clouds
  • Nick Indriolo, Brian D. Fields, Benjamin J. McCall

University of Illinois at Urbana-Champaign
2
Cosmic Ray Basics
  • Charged particles (e-, e, p, a, etc.)
    with high energy (103-1019 eV)
  • Galactic cosmic rays are primarily accelerated in
    supernovae remnants

3
Background
  • Cosmic rays have several impacts on the
    interstellar medium, all of which produce some
    observables
  • Ionization molecules
  • CR H2 ? H2 e- CR
  • H2 H2 ? H3 H
  • Spallation light element isotopes
  • p, a C, N, O ? 6Li, 7Li, 9Be, 10B, 11B
  • Nuclear excitation gamma rays
  • p, a C, O ? C, O ? ? (4.4, 6.13 MeV)

4
Motivations
  • Many astrochemical processes depend on ionization
  • Cosmic rays are the primary source of ionization
    in cold interstellar clouds
  • Low-energy cosmic rays (2-10 MeV) are the most
    efficient at ionization
  • The cosmic ray spectrum below 1 GeV cannot be
    directly measured at Earth

5
Example Cosmic Ray Spectra
1 - Herbst, E., Cuppen, H. M. 2006, PNAS, 103,
12257 2 - Spitzer, L.,
Jr., Tomasko, M. G. 1968, ApJ, 152, 971
3 - Kneller, J. P., Phillips, J.
R., Walker, T. P. 2003, ApJ, 589, 217 Shading
Mori, M. 1997, ApJ, 478, 225
4 - Valle, G., Ferrini, F., Galli, D., Shore,
S. N. 2002, ApJ, 566, 252 5 - Hayakawa, S.,
Nishimura, S., Takayanagi, T. 1961, PASJ, 13,
184 6 - Nath, B. B., Biermann, P. L. 1994,
MNRAS, 267, 447 Points AMS
Collaboration, et al. 2002, Phys. Rep., 366, 331
6
Motivations
  • Recent results from H3 give an ionization rate
    of ?2410-16 s-1
  • Given a cosmic ray spectrum and cross section,
    the ionization rate can be calculated
    theoretically

Indriolo, N., Geballe, T. R., Oka, T., McCall,
B. J. 2007, ApJ, 671, 1736
7
Results from Various Spectra
a Indriolo, N., Geballe, T. R., Oka, T.,
McCall, B. J. 2007, ApJ, 671, 1736 b van der
Tak, F. F. S., van Dishoeck, E. F. 2000, AAL,
358, L79
8
Add Flux at Low Energies
9
High Flux Results
  • This is no surprise, as these spectra were
    tailored to reproduce the diffuse cloud
    ionization rate results

10
Carrot Construction
11
Light Element Results
a Anders, E. Grevesse, N. 1989 Geochim.
Cosmochim. Acta, 53, 197
12
Gamma-Ray Results
13
Energy Constraints
  • There are approximately 32 supernovae per
    century, each releasing about 1051 erg of
    mechanical energy
  • The carrot spectrum requires 0.181051 erg per
    century, while the broken power law requires
    0.171051 erg per century
  • Both are well within constraints

14
Acceleration Mechanism
  • Carrot spectrum shape does not match acceleration
    by supernovae remnants
  • Voyager 1 observations at the heliopause show a
    steep slope at low energies
  • Possible that astropauses are accelerating
    cosmic rays throughout the Galaxy

Fig. 2 - Stone, E. et al. 2005, Science, 309, 2017
15
Conclusions
  • Carrot spectrum explains high ionization rate,
    and is broadly consistent with various
    observables
  • p-4.3 power law is inconsistent with acceleration
    from SNR
  • Perhaps weak shocks in the ISM are responsible
    for the vast majority of low-energy cosmic rays

16
Acknowledgments
17
Cross Sections
Bethe, H. 1933, Hdb. d Phys. (Berlin J.
Springer), 24, Pt. 1, 491 Read, S. M., Viola,
V. E. 1984, Atomic Data Nucl. Data, 31, 359
Meneguzzi, M. Reeves, H. 1975, AA, 40, 91
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