Fig. 3From: A novel high accuracy finite-difference time-domain methodSpatial profiles of magnetic field \(B_{z}\) in two dimensions at \(t=200\Delta t/C\), where C is the dimensionless Courant number: a Sekido23 with \(C=0.5\); b Sekido23 with \(C=1\); c scheme 1 with \(C=0.5\); d scheme 1 with \(C=1\); e scheme 2 with \(C=0.5\); f scheme 2 with \(C=1\)Back to article page