Quantum mechanics describes a quantum system using a quantum state, with observables represented by self-adjoint operators. For a single particle in one dimension, a pure state can be described by a wavefunction : its squared modulus gives the probability density for position. The Schrödinger equation predicts how this probability amplitude evolves between interventions; measurement in quantum mechanics connects it to experimental outcomes through the Born rule. A wavefunction therefore predicts a distribution of possible positions rather than a single trajectory as in classical mechanics.
The infinite square well makes three central ideas visible with elementary sine functions. Confinement selects discrete energy eigenvalues; wavefunction normalization converts a shape into quantitative probabilities; and a quantum superposition can have a changing probability density even when each constituent energy eigenstate has a stationary one. This combination explains why quantum mechanics uses both linear algebra and differential equations: eigenfunctions describe the building blocks, while quantum phases determine how they interfere. The same tools help explain the discrete energies of chemical atoms and molecules, although their Quantum Hamiltonians require different potentials and often many particles.
In his first 1926 paper, Erwin Schrödinger formulated quantization as an eigenvalue problem for a hydrogen atom in nonrelativistic quantum mechanics. On its opening page he compared the emergence of integers with the number of nodes of a standing wave on a vibrating string. The infinite square well below realizes that appealing idea especially transparently: the allowed integers follow from the boundary conditions. This historical analogy concerns the origin of discrete energies; the Born rule supplies the statistical interpretation of the modern wavefunction. [ref].
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Daniel Gottesman. External portrait supplied by the University of Maryland Department of Computer Science; photographer and licence are not specified on the verified profile.
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Portrait of Avshalom Elitzur
. Avishag Shaar-Yashuv. CC BY-SA 4.0, via Wikimedia Commons. Source.

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A physicist who proposed a unitary relative-state account of quantum measurement, developed in the many-worlds interpretation.
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Hugh Everett III in 1964; Hugh Everett III papers, University of California, Irvine; photographer unrecorded in the Wikimedia file record; non-free historical portrait hosted by English Wikipedia
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Coauthor of work on the GRW flash ontology and its relation to other quantum theories.

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Coauthor of an ontological model of a quantum system classification distinguishing psi-ontic models and psi-epistemic models.

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Coauthor of an ontological model of a quantum system classification distinguishing psi-ontic models and psi-epistemic models.

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Coauthor of work on Bohmian mechanics and the GRW model.

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Coauthor of work on Bohmian mechanics and the GRW model.

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Portrait of Detlef Dürr
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Coauthor of the original Ghirardi-Rimini-Weber theory.

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Coauthor of the original Ghirardi-Rimini-Weber theory.

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Coauthor of the original Ghirardi-Rimini-Weber theory and work on its interpretation.

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Author of the 1964 Bell theorem argument.
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Portrait of John Stewart Bell
. CERN, portrait of John Bell, June 1982; CERN archive record 1823937. CC BY 4.0, via Wikimedia Commons. Source.

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A physicist who coauthored a 2022 experimental demonstration of programmable neutral-atom quantum algorithms and multipartite entanglement using Rydberg blockade.

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A theoretical physicist whose work includes geometric phases in quantum mechanics.
Figure 1. . Vahram Mekhitarian, photograph; Jakob Gottfried, derivative crop. CC BY-SA 4.0, via Wikimedia Commons. Source.

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Lucien Hardy; portrait hosted by Perimeter Institute
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Portrait of Boris Podolsky
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A physicist who developed matrix mechanics and held a professorship in theoretical physics at Hamburg.[ref]
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Portrait of Pascual Jordan
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A physicist, Professor of theoretical physics at Birkbeck from 1961 to 1987.[ref]

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Portrait of Anton Zeilinger
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A physicist who holds an experimental quantum-physics chair at LMU Munich.[ref]
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Portrait of Harald Weinfurter
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Portrait of Dirk Bouwmeester in 2014
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A physicist researching quantum optics and the foundations of quantum mechanics.[ref]
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Portrait of Alain Aspect
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A physicist who performed experimental tests of Bell inequalities.[ref]
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Portrait of John Clauser
. Peter Lyons, photograph; Adem, existing portrait crop. CC BY-SA 4.0, via Wikimedia Commons. Source.

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A physicist who researched nuclear physics and experimentally tested Bell inequalities.[ref]
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Portrait of Stuart Freedman
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Portrait of Wolfgang Pauli
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Quantum mechanics is quite a broad term. Perhaps it is best to start approaching it from the division into:
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