Physics:Quantum many-body problem

From ScholarlyWiki
Revision as of 23:02, 23 May 2026 by WikiHarold (talk | contribs) (Expand short Quantum intro)
(diff) ← Older revision | Latest revision (diff) | Newer revision → (diff)
Jump to navigation Jump to search
← Previous : Exactly solvable quantum systems
Next : Formulas Collection →


Many interacting particles generate a rapidly growing quantum state space.

The quantum many-body problem is a Book I topic in the Quantum Collection. It is the challenge of describing systems made of many interacting quantum particles, where the size of the Hilbert space grows rapidly with particle number. Exact solutions are rare, so the field uses approximations, effective theories, numerical methods, and emergent collective descriptions. The problem appears in atoms, nuclei, solids, quantum fluids, plasmas, and quantum information. It explains why simple microscopic rules can produce phases, quasiparticles, correlations, and complex macroscopic behavior.

State-space growth

For a single particle, a wavefunction may be described over ordinary space. For many particles, the wavefunction depends on all particle coordinates and internal degrees of freedom. The number of amplitudes needed to represent the state can grow exponentially.

This growth makes approximation methods central. Mean-field theory, perturbation theory, density functional theory, tensor networks, Monte Carlo methods, and effective models are all ways to reduce or reorganize the complexity.

Collective behavior

Many-body systems often display properties not obvious from individual particles alone. Examples include superconductivity, spin liquids, Fermi liquids, and topological phases.

The many-body problem is therefore both a technical challenge and a source of new physical phenomena.

See also

Table of contents (217 articles)

Index

Full contents

References


Author: Harold Foppele


Source attribution: Physics:Quantum many-body problem