Table 1 Fermi-surface parameters.

From: Anomalous high-field magnetotransport in CaFeAsF due to the quantum Hall effect

FS cylinder

α

β

carrier type

Dirac electron

Schrödinger hole

F (T)

19.01 (1)

47.49 (2)

m*/me

0.41 (2)

0.90 (5)

TD (K)

4.7 (3)

2.9 (2)

n (10−3 per Fe)

1.39

1.74

n (1019 cm−3)

2.14

2.68

vF (104 m s−1)

6.8

4.9

EF (meV)

10.7

6.1

Γ (meV)

1.3

0.78

S

0.321

1.61

  1. The first three parameters F, m*, and TD were estimated from the Shubnikov–de Haas oscillations for B∥c in sample D2. The rest except S were derived from these first three: n is the carrier density, vF the Fermi velocity, EF the Fermi energy, and Γ = πkBTD the Landau-level broadening. The value of n for the α cylinder refers to the sum of the carriers of the two cylinders that occur in the Brillouin zone. To derive EF, we used the linear dispersion relation (EF = ℏvFkF) for the α cylinder and a quadratic one (\({E}_{{{{\rm{F}}}}}={\hslash }^{2}{k}_{{{{\rm{F}}}}}^{2}/(2{m}^{* })\)) for β. The spin-splitting parameter S for B∥c is based on11.
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