Lorenz gauge condition

In electromagnetism, the Lorenz gauge condition or Lorenz gauge (after Ludvig Lorenz) is a partial gauge fixing of the electromagnetic vector potential by requiring ⁠ ∂ μ A μ = 0 {\displaystyle \partial _{\mu }A^{\mu }=0} ⁠. The name is frequently confused with Hendrik Lorentz, who has given his name to many concepts in this field.

Source: Wikipedia — Lorenz gauge condition (CC BY-SA 4.0)

Lorenz gauge condition

In electromagnetism, the Lorenz gauge condition or Lorenz gauge (after Ludvig Lorenz) is a partial gauge fixing of the electromagnetic vector potential by requiring ⁠ ∂ μ A μ = 0 {\displaystyle \partial _{\mu }A^{\mu }=0} ⁠. The name is frequently confused with Hendrik Lorentz, who has given his name to many concepts in this field.

Source: Wikipedia "Lorenz gauge condition" · CC BY-SA 4.0

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