Fig. B.3.

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Temporal evolution of the longitudinally-averaged magnetic fields and horizontal velocities for the dynamo simulation with deeper Babcock-Leighton α-effect (Δrbmr = 0.12 R⊙). (a) Azimuthally-averaged radial field ⟨Br⟩ at the surface r = 0.985 R⊙. (b) Azimuthally-averaged toroidal field ⟨Bϕ⟩ near the base of the convection zone r = 0.715 R⊙. Black solid lines are the contours of the emerged BMRs at each time. (c) Torsional oscillation pattern δ⟨Ω⟩ at the surface. (d) Azimuthally-averaged latitudinal velocity ⟨vθ⟩ near the base of the convection zone.
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