5: Multi-Particle Systems
- Page ID
- 15756
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In this chapter, we shall extend the single particle, one-dimensional formulation of non-relativistic quantum mechanics, introduced in the previous chapters, in order to investigate one-dimensional systems containing multiple particles.
- 5.1: Fundamental Concepts of Multi-Particle Systems
- This page covers the quantum mechanical description of non-relativistic particle systems through wavefunctions, \(\psi(x,t)\), which determine particle location probabilities and require normalization. For multiple particles, the wavefunction expands to \(\psi(x_1, x_2, \ldots, x_N,t)\) and must also be normalized.
- 5.2: Non-interacting Particles
- This page describes the Hamiltonian for multi-particle systems, highlighting its components of kinetic and potential energy. It explains that for non-interacting particles, the Hamiltonian can be simplified to a sum of independent single-particle Hamiltonians. This leads to the multi-particle wavefunction being expressed as a product of single-particle wavefunctions, allowing the Schrödinger equation to be factored into independent equations.
- 5.3: Two-Particle Systems
- This page explores a two-particle system with masses \(m_1\) and \(m_2\) that interact through a position-dependent potential. It explains how to transform the Hamiltonian using center of mass and relative coordinates, allowing for wavefunction factorization. Key equations show conservation of the total momentum and time-dependent Schrödinger equations.
- 5.4: Identical Particles
- This page explores the wavefunctions of systems with identical particles, distinguishing between bosons and fermions based on their symmetrical properties. It delineates the construction of wavefunctions for two identical non-interacting particles and underscores the Pauli exclusion principle that prevents identical fermions from occupying the same state.
- 5.E: Multi-Particle Systems (Exercises)
- This page explores the behavior and theoretical constructs of two non-interacting particles in various quantum states, focusing on distinguishable particles, indistinguishable bosons, and fermions. It details state counting differences and calculates expectation values like \(\langle (x_1-x_2)^{\,2}\rangle\), as well as energy levels and degeneracies in a 1D box, emphasizing the impact of quantum statistics arising from particle indistinguishability.


