TY - JOUR
T1 - In situ spectroscopy of the solar corona
AU - Morgan, H.
AU - Fineschi, S.
AU - Habbal, Shadia Rifai
AU - Li, B.
PY - 2008/3/4
Y1 - 2008/3/4
N2 - Context: Future spacecraft missions, such as the proposed Solar Probe
mission, will venture close to the Sun, allowing spectrometers measuring
emission from heavy ions or neutrals in the solar wind to have radial
lines of sight (LOS) pointing away from the Sun, or indeed in any
direction other than sunwards. Aims: We show that a radial LOS
gives excellent solar wind diagnostics, with tight constraints on ion
density, outflow velocity, and effective temperature parallel to the
coronal magnetic field. In addition, we present the concept that a
spectrometer onboard a spacecraft reaching the solar corona can yield
measurements somewhat similar to an in situ sampling instrument, in that
the 3D velocity distribution and density of the emitting ions can be
measured. Methods: The well-studied O VI doublet at 1031.96 and
1037.6 Å and the H Ly-α line at 1215.67 Å are chosen
as examples. Solar wind parameters obtained from a 2D three-fluid
magnetohydrodynamic (MHD) model, and formulations for collisional and
radiative emission along a radial LOS, are used to calculate spectral
line profiles for these lines at various heights within a streamer and
coronal hole. Results: For O VI, the collisional line profiles
directly measure the ion velocity distribution in the radial direction,
with the general Doppler shift of the profiles related to the bulk ion
outflow velocity and the width of the line related to the effective ion
temperature parallel to the magnetic field. An obvious skew in the
collisional profiles is seen in regions with a high gradient in outflow
velocity and/or temperature. The resonant (or radiative) line profiles
behave very differently from those currently observed in 90°
scattering. They are more closely related to the profile and
distribution of the exciting chromospheric spectrum: the lines are
narrow and are centered at wavelengths mirrored around the rest
wavelength of the ion emission, allowing easy separation of the
collisional and radiative components. Despite the Ly-α line being
much more intense than the O VI lines, the large width and high
intensity of the Ly-α radiative component in comparison to the
collisional component is such that these two components cannot be
separated. The Ly-α line is therefore less suitable for solar wind
diagnostics. Conclusions: The prospect of coronal in situ
spectral observations, combined with simultaneous in situ sampling
measurements of the solar wind and magnetic field will give unsurpassed
constraints on models of solar wind heating and acceleration.
AB - Context: Future spacecraft missions, such as the proposed Solar Probe
mission, will venture close to the Sun, allowing spectrometers measuring
emission from heavy ions or neutrals in the solar wind to have radial
lines of sight (LOS) pointing away from the Sun, or indeed in any
direction other than sunwards. Aims: We show that a radial LOS
gives excellent solar wind diagnostics, with tight constraints on ion
density, outflow velocity, and effective temperature parallel to the
coronal magnetic field. In addition, we present the concept that a
spectrometer onboard a spacecraft reaching the solar corona can yield
measurements somewhat similar to an in situ sampling instrument, in that
the 3D velocity distribution and density of the emitting ions can be
measured. Methods: The well-studied O VI doublet at 1031.96 and
1037.6 Å and the H Ly-α line at 1215.67 Å are chosen
as examples. Solar wind parameters obtained from a 2D three-fluid
magnetohydrodynamic (MHD) model, and formulations for collisional and
radiative emission along a radial LOS, are used to calculate spectral
line profiles for these lines at various heights within a streamer and
coronal hole. Results: For O VI, the collisional line profiles
directly measure the ion velocity distribution in the radial direction,
with the general Doppler shift of the profiles related to the bulk ion
outflow velocity and the width of the line related to the effective ion
temperature parallel to the magnetic field. An obvious skew in the
collisional profiles is seen in regions with a high gradient in outflow
velocity and/or temperature. The resonant (or radiative) line profiles
behave very differently from those currently observed in 90°
scattering. They are more closely related to the profile and
distribution of the exciting chromospheric spectrum: the lines are
narrow and are centered at wavelengths mirrored around the rest
wavelength of the ion emission, allowing easy separation of the
collisional and radiative components. Despite the Ly-α line being
much more intense than the O VI lines, the large width and high
intensity of the Ly-α radiative component in comparison to the
collisional component is such that these two components cannot be
separated. The Ly-α line is therefore less suitable for solar wind
diagnostics. Conclusions: The prospect of coronal in situ
spectral observations, combined with simultaneous in situ sampling
measurements of the solar wind and magnetic field will give unsurpassed
constraints on models of solar wind heating and acceleration.
KW - Sun: corona
KW - Sun: particle emission
KW - Sun: solar wind
UR - http://hdl.handle.net/2160/9126
U2 - 10.1051/0004-6361:20079202
DO - 10.1051/0004-6361:20079202
M3 - Article
SN - 0004-6361
VL - 482
SP - 981
EP - 987
JO - Astronomy and Astrophysics
JF - Astronomy and Astrophysics
IS - 3
ER -