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Table 2.

Energetic particle timing results and shock height at the particle release times.

Spacecraft/Instrument/ Effective path length Estimated Shock height θBn at the
Particle species or IMF length (a) solar release time from Sun centre cobpoint
(au) (UT) (b) (R) (c)
(deg) (d)
Parker ENLIL Parker ENLIL
(1) (2) (3) (4) (5) (6) (7)
STA/SEPT/HET (e) 3.55 ± 0.50 (VDA) 23:28 ± 15 min 6.0 ± 2.0 5.7 ± 2.0 22 ± 2 26 ± 3

STA/SEPT/ 65–105 keV e 1.14 ± 0.03 (TSA) 00:15 ± 10 min 9.5 ± 1.0 10.2 ± 1.0 19 ± 2 20 ± 2

STB/HET/0.7-1.4 MeV e 1.26 ± 0.03 (TSA) 02:57 ± 15 min (27.5 ± 2.0) (f)

MESS/EPPS/71–112 keV e 0.31 ± 0.01 (TSA) 23:22 ± 5 min (g) 5.9 ± 0.6 5.1 ± 0.6 5 ± 1 8 ± 1

SOHO/EPHIN/0.25–0.70 MeV e 1.09 ± 0.03 (TSA) 00:58 ± 60 min (15.6 ± 6.0) (f)

Notes.

(a)

Magnetic field lines length for TSA analysis from ENLIL modelling.

(b)

Solar release times late on 2013 August 19 and early on August 20, shifted by light propagation time to 1 au in order to compare with electromagnetic observations.

(c)

CME-driven shock heliospheric height at the cobpoint (Sanahuja et al. 1995) for STEREO-A and MESSENGER (calculated for Parker spiral and ENLIL), and at the shock nose for STEREO-B and SOHO. The range of heights includes the uncertainty in the estimated SEP release time, as discussed in Lario et al. (2016).

(d)

θBn: The angle between the shock normal vector and the magnetic field lines at the cobpoint (estimated using Parker spiral and ENLIL, which are radially extended from 21.5 R). The given uncertainties are rounded to one degree. They are based on the shock height deviation due to the uncertainty in the particle release time (the fluctuations in the magnetic field lines, due to waves and turbulence, or in the shock front geometry are not considered).

(e)

Energies used in VDA analysis: 0.065–2.8 MeV e & 13.6–60 MeV p.

(f)

STEREO-B is not connected to the shock until later in time, and SOHO is never connected to the shock.

(g)

MESSENGER was pointing in the anti-Sun direction, thus the solar release time should be interpreted as an upper limit.

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