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3.4 Probability theory and statistics in quantum mechanics

2 min readaugust 9, 2024

Quantum mechanics introduces probability into the heart of physics. It uses mathematical tools like wavefunctions and operators to describe the chances of measuring specific particle properties. This probabilistic nature is a fundamental departure from classical physics.

The connects wavefunctions to probabilities, while concepts like expectation values and help analyze quantum measurements. Understanding these ideas is crucial for grasping how quantum mechanics describes the bizarre world of atomic-scale particles.

Probability in Quantum Mechanics

Probability Density and Born Rule

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  • describes likelihood of finding particle at specific position
  • Born rule connects to probability density
  • Probability density given by square of wavefunction's absolute value: P(x)=Ψ(x)2P(x) = |\Psi(x)|^2
  • Normalization condition ensures total probability equals 1: Ψ(x)2dx=1\int_{-\infty}^{\infty} |\Psi(x)|^2 dx = 1
  • Probability of finding particle in interval [a,b] calculated by integrating probability density: P(axb)=abΨ(x)2dxP(a \leq x \leq b) = \int_a^b |\Psi(x)|^2 dx
  • Born rule applies to other observables (momentum, energy) using appropriate wavefunctions

Wavefunction Collapse and Measurement

  • occurs when measurement performed on quantum system
  • Before measurement, system exists in of possible states
  • Measurement causes wavefunction to collapse into single
  • Probability of collapsing into specific eigenstate determined by Born rule
  • addresses difficulty in reconciling continuous wavefunction evolution with discrete collapse
  • Various interpretations proposed to explain measurement problem (Copenhagen, Many-Worlds)
  • attempts to explain apparent collapse through interaction with environment

Statistical Concepts

Expectation Values and Standard Deviation

  • Expectation value represents average outcome of repeated measurements
  • For position, expectation value calculated as: x=xΨ(x)2dx\langle x \rangle = \int_{-\infty}^{\infty} x|\Psi(x)|^2 dx
  • Generalizes to other observables using appropriate operator: A=Ψ(x)A^Ψ(x)dx\langle A \rangle = \int_{-\infty}^{\infty} \Psi^*(x) \hat{A} \Psi(x) dx
  • Standard deviation measures spread of possible measurement outcomes
  • Calculated using expectation values: ΔA=A2A2\Delta A = \sqrt{\langle A^2 \rangle - \langle A \rangle^2}
  • relates standard deviations of complementary observables (position and momentum)

Quantum Ensembles and Statistical Interpretation

  • represents collection of identically prepared quantum systems
  • Allows statistical analysis of quantum measurements
  • consists of systems in identical quantum states
  • contains systems in different quantum states with associated probabilities
  • formalism used to describe mixed ensembles
  • views quantum mechanics as fundamentally probabilistic
  • Emphasizes role of measurement in determining quantum states
  • Contrasts with deterministic interpretations (hidden variables theories)
  • represents information about system rather than objective reality
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© 2024 Fiveable Inc. All rights reserved.
AP® and SAT® are trademarks registered by the College Board, which is not affiliated with, and does not endorse this website.

© 2024 Fiveable Inc. All rights reserved.
AP® and SAT® are trademarks registered by the College Board, which is not affiliated with, and does not endorse this website.
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