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Trans., MAG-19, 6 (1983), pp. 2450-3.

[F1] K. Fujiwara, T. Nakata, H. Ohashi: "Improvement of Convergence Characteristic of ICCG Method for the A-ϕ  Method Using Edge Elements", IEEE Trans.,MAG-32, 3 (1996), pp. 804-7.

[F2] K. Fujiwara, N. Takahashi, T. Nakata: "Effect of Gauge Condition for Edge Elementon Convergence Characteristic of ICCG Method", Int. J. Appl. Electromagn.

in Materials, Supplement to No 6 (1995), pp. 259-62.

[Lo] L. Lorenz: "On the identity of the vibrations of light with electrical currents",Philos. Mag., 34 (1867), pp. 287-301.

[NC]9

R.D. Nevels, K.J. Crowell: “A Coulomb gauge analysis of a wire scatterer”, IEEProc.-H, 137, 6 (1990), pp. 384-8.

[PB&] K. Preis, I. Bardi, O. Biro, C. Magele, G. Vrisk, K.R. Richter: "Different FiniteElement Formulations of 3D Magnetostatic Fields", IEEE Trans., MAG-28, 2(1992), pp. 1056-9.

[Re] Z. Ren: "Autogauging of vector potential by iterative solver—Numerical evidence",in  3

dInt. Workshop on  Electric and Magnetic Fields (Proc., Liège, 6-9 May

1996), A.I.M. (31 Rue St-Gilles, Liège), 1996, pp. 119-24.

Some call the classical Lorenz gauge the "radiation gauge" (E = iωA and B = ik ×  A, inFourier space, with wavevector k). See

J.F. Nieves, P.B. Pal: "Third electromagnetic constant of an isotropic medium", Am. J.Phys., 62, 3 (1994), pp. 207-16.

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9They quote Whittaker in a footnote, but write "Lorentz gauge", notwithstanding.