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Extracting information from the wavefunction

Peter Joshua Atkins, Julio de Paula, Ronald Friedman

Contents Postulate III: quantum mechanical operators 47 Brief illustration 6.1: The kinetic energy operator in two dimensions 49 Postulate IV: eigenvalues and eigenfunctions 50 Example 6.1: Identifying an eigenfunction 50 Brief illustration 6.2: The wavefunction as an eigenfunction 51 Checklist of concepts 52...

Oxford University Press eBooksDec 12, 20130 citations

CHAPTER 3. The Wavefunction and the Quantum State

Tim Maudlin

Princeton University Press eBooksMar 23, 20190 citations

Wavefunctions

Peter Joshua Atkins, Julio de Paula, James Keeler

This chapter examines the interpretation of the wavefunction, and specifically what it reveals about the location of a particle. In quantum mechanics, all the properties of a system are expressed in terms of a wavefunction, which is obtained by solving the equation proposed by Erwin Schrödinger. Indeed, wavefunctions provide the essential foundation for understanding the properties of electrons in atoms and molecules, and are central to explanations in chemistry. The chapter then considers how, according to the Born interpretation, the probability density at a point is proportional to the square of the wavefunction at that point. A wavefunction is normalized if the integral over all space of its square modulus is equal to 1. Ultimately, a wavefunction must be single-valued, continuous, not infinite over a finite region of space, and have a continuous slope. The quantization of energy stems from the constraints that an acceptable wavefunction must satisfy.This chapter examines the interpretation of the wavefunction, and specifically what it reveals about the location of a particle. In quantum mechanics, all the properties of a system are expressed in terms of a wavefunction, which is obtained by solving the equation proposed by Erwin Schrödinger. Indeed, wavefunctions provide the essential foundation for understanding the properties of electrons in atoms and molecules, and are central to explanations in chemistry. The chapter then considers how, according to the Born interpretation, the probability density at a point is proportional to the square of the wavefunction at that point. A wavefunction is normalized if the integral over all space of its square modulus is equal to 1. Ultimately, a wavefunction must be single-valued, continuous, not infinite over a finite region of space, and have a continuous slope. The quantization of energy stems from the constraints that an acceptable wavefunction must satisfy.

Oxford University Press eBooksDec 5, 20220 citations

Chapter 20. The wave function and its interpretation

R. Shankar

Yale University Press eBooksMay 1, 20200 citations

Chapter 1 The wave function and Schrodinger equation

EDP Sciences eBooksApr 30, 20260 citations

On a Constraint–Theoretical Reinterpretation of Quantum Measurement

Kevin Shepheard

Quantum measurement theory traditionally introduces probabilities axiomatically, most notably through the Born rule and projection postulates. In this work, I introduce Constraint Mechanics (CM), a framework in which quantum probabilities arise as conditional statistics over dynamically generated constraint fields acting on configuration space, without modifying unitary Schrödinger evolution or introducing dynamical collapse. A detector-scale conditional measurement operator is defined using soft viability weights that do not alter the wavefunction. I prove that the Born rule is recovered exactly as a theorem in the limit of spatially homogeneous constraints, while structured deviations emerge under heterogeneous constraint profiles with exact norm preservation. Numerical validation using a double-slit geometry confirms unitary evolution, exact normalization, and controlled deviation behavior. CM reframes quantum measurement as conditioning on dynamically viable configuration-space regions and provides a unifying interpretational link between interference, measurement, and selection.Quantum measurement theory traditionally introduces probabilities axiomatically, most notably through the Born rule and projection postulates. In this work, I introduce Constraint Mechanics (CM), a framework in which quantum probabilities arise as conditional statistics over dynamically generated constraint fields acting on configuration space, without modifying unitary Schrödinger evolution or introducing dynamical collapse. A detector-scale conditional measurement operator is defined using soft viability weights that do not alter the wavefunction. I prove that the Born rule is recovered exactly as a theorem in the limit of spatially homogeneous constraints, while structured deviations emerge under heterogeneous constraint profiles with exact norm preservation. Numerical validation using a double-slit geometry confirms unitary evolution, exact normalization, and controlled deviation behavior. CM reframes quantum measurement as conditioning on dynamically viable configuration-space regions and provides a unifying interpretational link between interference, measurement, and selection.

Feb 6, 20260 citations

The wavefunction

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The wavefunction

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