Physics:Quantum many-body problem: Difference between revisions

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{{Short description|Problem of describing interacting systems with many quantum particles}}
{{Short description|Problem of describing interacting systems with many quantum particles}}
{{Quantum book backlink|Mathematical structure and systems}}
{{Quantum book backlink|Mathematical structure and systems}}
{{Quantum article nav|previous=Physics:Quantum Exactly solvable quantum systems|previous label=Exactly solvable quantum systems|next=Physics:Quantum Formulas Collection|next label=Formulas Collection}}


[[File:Quantum_many_body_problem_yellow.png|thumb|280px|Many interacting particles generate a rapidly growing quantum state space.]]
[[File:Quantum_many_body_problem_yellow.png|thumb|280px|Many interacting particles generate a rapidly growing quantum state space.]]

Revision as of 21:58, 20 May 2026



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Many interacting particles generate a rapidly growing quantum state space.

The quantum many-body problem is the challenge of describing systems containing many interacting quantum particles. Because the state space grows extremely rapidly with particle number, exact solutions are usually impossible except for small or specially structured systems.[1]

Many-body physics appears in atoms, molecules, nuclei, solids, quantum fluids, plasmas, and quantum information systems. It connects microscopic quantum laws with collective behavior such as magnetism, superconductivity, phase transitions, and emergent quasiparticles.

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

References


Author: Harold Foppele


Source attribution: Physics:Quantum many-body problem