| 21. | The vector potential changes the phase of the quanta produced by the field when they move from point to point.
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| 22. | Where is the particle's electric charge, is the vector potential, and is the speed of light.
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| 23. | Where \ mathbf { \ Phi } is a harmonic vector potential and \ chi is a harmonic scalar potential.
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| 24. | Moreover, the TM field can be derived from a purely longitudinal Lorentz vector potential \ underline { A }.
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| 25. | This is also true in electrodynamics since you can do a gauge transformation which will only affect the vector potential tomorrow.
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| 26. | This is why sometimes the electric potential is called the scalar potential and the magnetic potential is called the vector potential.
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| 27. | These four polarizations seemed to correspond to the four components of the relativistically covariant vector potential A ^ { \ mu }.
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| 28. | In the potential formulation, there are only four components : the electric potential and the three components of the vector potential.
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| 29. | Sharper upper limits on the speed of light have been obtained in experiments designed to detect effects caused by the galactic vector potential.
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| 30. | Just as the phase of the wave function depends upon the magnetic vector potential, it also depends upon the scalar electric potential.
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