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Matrix Mechanics and Operator Ideas

Matrix mechanics was the first complete form of modern quantum mechanics. It did not begin by drawing better electron orbits. It reorganized mechanics around transition frequencies, spectral intensities, and arrays of quantities whose multiplication is not generally commutative.

This chapter explains how noncommuting observables entered the theory historically. The formal operator theory belongs in Operators, while this chapter explains why operators were not a decorative notation added after the fact.

All currently planned pages in this chapter have mature drafts. Future expansion can add primary-source annotations, worked source-reading exercises, and deeper connections to later formulations.

This chapter owns the historical route to operator ideas. The modern formal definitions belong elsewhere:

  • W. Heisenberg, “Über quantentheoretische Umdeutung kinematischer und mechanischer Beziehungen,” Zeitschrift für Physik 33, 879-893, 1925, DOI: 10.1007/BF01328377.
  • M. Born and P. Jordan, “Zur Quantenmechanik,” Zeitschrift für Physik 34, 858-888, 1925, DOI: 10.1007/BF01328531.
  • P. A. M. Dirac, “The fundamental equations of quantum mechanics,” Proceedings of the Royal Society A 109, 642-653, 1925, DOI: 10.1098/rspa.1925.0150.
  • B. L. van der Waerden, ed., Sources of Quantum Mechanics, Dover, 1968.
  • M. Jammer, The Conceptual Development of Quantum Mechanics, 2nd ed., American Institute of Physics, 1989.