The hidden vector that defines the magnetic field

The hidden vector that defines the magnetic field
Image: Intellect (generated)

In short: We often think of magnetic fields as the primary actors in physics. However, a deeper mathematical layer exists: the magnetic vector potential. This quantity does more than just describe fields; it serves as the fundamental language for the most advanced theories in quantum mechanics.

Within classical electromagnetism, the magnetic field, B, is defined as the curl of the vector quantity A, known as the magnetic vector potential. This relationship allows physicists to describe the electric field using both the electric potential (φ) and the magnetic vector potential (A). By using these potentials, many electromagnetic equations can be rewritten, providing a different perspective on the same physical reality.

The historical development of this concept occurred in the mid-19th century. Franz Ernst Neumann introduced the idea in 1845, followed by Wilhelm Eduard Weber in 1846, both while discussing Ampère's circuital law. A contemporary formulation of the vector potential, including the precise mathematical link to the magnetic field, was presented by William Thomson in 1847. The SI units for A are V·s·m⁻¹ or Wb·m⁻¹, both of which represent Weber per metre.

The significance of the vector potential extends far beyond classical mechanics. In advanced theories like quantum mechanics, most equations rely on potentials rather than fields. For instance, the vector potential is essential when studying the Schrödinger equation for charged particles, the Dirac equation, and the Aharonov–Bohm effect. Furthermore, the vector potential is physically interpreted as 'potential momentum,' forming a part of the canonical momentum.

By describing fields via these potentials, two Maxwell's equations—Faraday's law and Gauss's law for magnetism—are inherently fulfilled. Specifically, if the vector potential is continuous and well-defined everywhere, it guarantees the absence of magnetic monopoles. This mathematical structure also allows for a formal analogy between the vector potential and current density, similar to the relationship between electric potential and charge density.

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