Optical emissions from sprite streamers are used to estimate peak electric fields and electron
energies [e.g., Kuo et al., GRL, 32, L19103, 2005; Adachi et al., GRL, 33, L17803, 2006]. It
has been shown that significant correction factors need to be used to account for the spatial
shift between distributions of optical emissions in streamers and peak electric fields in their
heads [Celestin and Pasko, GRL, 37, L07804, 2010]. The latter study involved the excited
species N2(C3Πu) and N2+(B2Σu+), whose populations are considered to be in
steady state. The species N2(C3Πu) and N2+(B2Σu+) are responsible for the
second positive (2PN2) and first negative (1NN2+) band systems of N2 and N2+,
respectively.
In this work, we show how this technique can be extended to non-steady state optical
emissions, such as those produced by N2(a1Πg) and N2(B3Πg) in the form of
Lyman-Birge-Hopfield (LBH) and first positive (1PN2) band systems, respectively.
Additionally, we simulate numerically downward propagating sprite streamers and their
optical emissions for the following band systems: 1PN2, 2PN2, LBH, and 1NN2+, and
show how they relate to specific physical properties. This study particularly focuses on
improving analysis of observational results from the future missions ASIM (ESA) and
TARANIS (CNES) that will detect various optical emissions produced by transient luminous
events in the nadir. |