Open Access

Table A.1

GP hyper-parameters for DS Leo (Gl 410).

DS Leo Value Prior
GP fit on 〈B
μ (kG) 0.900.02+0.02$0.90^{+0.02}_{-0.02}$ 𝒰(−10, 10)
σ (kG) 0.010.01+0.01$0.01^{+0.01}_{-0.01}$ 𝒰(0, 1000)
α (kG) 0.080.01+0.01$0.08^{+0.01}_{-0.01}$ 𝒰(0, 10)
l (d) 547+8$54^{+8}_{-7}$ 𝒰(10, 500)
β 0.570.08+0.10$0.57^{+0.10}_{-0.08}$ 𝒰(0, 20)
Prot (d) 13.9530.086+0.088$13.953^{+0.088}_{-0.086}$ 𝒰(5, 20)
χ2r 0.72
RMS 0.02 (kG)
GP fit on B
μ (G) 0.603.28+3.24$-0.60^{+3.24}_{-3.28}$ 𝒰(−500, 500)
σ (G) 1.941.16+0.94$1.94^{+0.94}_{-1.16}$ 𝒰(0, 1000)
α (G) 15.191.60+1.92$15.19^{+1.92}_{-1.60}$ 𝒰(0, 1000)
l (d) 577+9$57^{+9}_{-7}$ 𝒰(10, 500)
β 0.450.05+0.06$0.45^{+0.06}_{-0.05}$ 𝒰(0, 5)
Prot,ℓ (d) 14.0010.075+0.077$14.001^{+0.077}_{-0.075}$ 𝒰(5, 20)
χ2r, ℓ 0.66
RMS 3.93 (G)
GP fit on 〈B〉 and B
μ (kG) 0.900.02+0.02$0.90^{+0.02}_{-0.02}$ 𝒰(−10, 10)
σ (kG) 0.010.01+0.01$0.01^{+0.01}_{-0.01}$ 𝒰(0, 1000)
α (kG) 0.080.01+0.01$0.08^{+0.01}_{-0.01}$ 𝒰(0, 10)
l (d) 547+8$54^{+8}_{-7}$ 𝒰(10, 500)
β 0.570.08+0.10$0.57^{+0.10}_{-0.08}$ 𝒰(0, 20)
Prot (d) 13.9800.058+0.059$13.980^{+0.059}_{-0.058}$ 𝒰(5, 20)
μ (G) 0.763.34+3.31$-0.76^{+3.31}_{-3.34}$ 𝒰(−500, 500)
σ (G) 1.901.14+0.97$1.90^{+0.97}_{-1.14}$ 𝒰(0, 1000)
α (G) 15.481.61+1.98$15.48^{+1.98}_{-1.61}$ 𝒰(0, 1000)
l (d) 587+9$58^{+9}_{-7}$ 𝒰(10, 500)
β 0.450.05+0.06$0.45^{+0.06}_{-0.05}$ 𝒰(0, 20)
χ2r 0.72
χ2r, ℓ 0.66
RMS 0.02 (kG)
RMS 3.94 (G)
GP fit on dTemp
μdTemp (K) 1.181.61+1.57$-1.18^{+1.57}_{-1.61}$ 𝒰(−50, 50)
σdTemp (K) 0.710.12+0.13$0.71^{+0.13}_{-0.12}$ 𝒰(0, 1000)
αdTemp (K) 7.460.81+0.93$7.46^{+0.93}_{-0.81}$ 𝒰(0, 100)$
ldTemp (d) 383+3$38^{+3}_{-3}$ 𝒰(10, 500)
βdTemp 0.630.06+0.07$0.63^{+0.07}_{-0.06}$ 𝒰(0, 20)
Prot, dTemp (d) 14.2140.102+0.106$14.214^{+0.106}_{-0.102}$ 𝒰(3, 200)
χ2r, dTemp 0.98
RMSdTemp 0.58 (K)

Notes. Hyper-parameters obtained when applying our process to the small-scale magnetic field measurements (〈B〉), the longitudinal magnetic field (Bt), or 〈B〉 and Bt simultaneously. Error bars on 〈B〉 and dTemp measurements were adjusted to ensure a minimum reduced χ2 close to one for the best fit.

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