2.4 Operators and Observables in Quantum Mechanics

Quantum mechanics relies heavily on operators and observables to describe physical systems. These mathematical tools allow us to extract information about particles and waves, connecting the abstract world of wave functions to measurable quantities.

Operators act on wave functions, while observables represent physical quantities we can measure. Understanding their relationship is crucial for grasping how quantum mechanics predicts experimental outcomes and describes the behavior of particles at the atomic scale.

Operators in Quantum Mechanics

Definition and Properties

Top images from around the web for Definition and Properties

• 

  Quantum Numbers | Introduction to Chemistry View original

  Is this image relevant?

• 

  Circuits of space and time quantum channels – Quantum View original

  Is this image relevant?

• 

  Hermitian matrix - Knowino View original

  Is this image relevant?

• 

  Quantum Numbers | Introduction to Chemistry View original

  Is this image relevant?

• 

  Circuits of space and time quantum channels – Quantum View original

  Is this image relevant?

1 of 3

Top images from around the web for Definition and Properties

• 

  Quantum Numbers | Introduction to Chemistry View original

  Is this image relevant?

• 

  Circuits of space and time quantum channels – Quantum View original

  Is this image relevant?

• 

  Hermitian matrix - Knowino View original

  Is this image relevant?

• 

  Quantum Numbers | Introduction to Chemistry View original

  Is this image relevant?

• 

  Circuits of space and time quantum channels – Quantum View original

  Is this image relevant?

1 of 3

• Operators are mathematical entities that act on wave functions to extract information or transform them in quantum mechanics
• Linear operators satisfy the linearity property: $Â(αψ₁ + βψ₂) = αÂψ₁ + βÂψ₂$, where $α$ and $β$ are complex numbers, and $ψ₁$ and $ψ₂$ are wave functions
  • Nonlinear operators do not satisfy this property
• Hermitian operators have real eigenvalues and orthogonal eigenfunctions
  • They satisfy the condition $⟨ψ₁|Âψ₂⟩ = ⟨Âψ₁|ψ₂⟩*$, where $*$ denotes the complex conjugate
• Unitary operators preserve the inner product between wave functions
  • They satisfy the condition $ÛÛ† = Û†Û = Î$, where $Û†$ is the adjoint of $Û$, and $Î$ is the identity operator

Expectation Values

• The expectation value of an operator $Â$ for a given state $ψ$ is calculated as $⟨Â⟩ = ⟨ψ|Âψ⟩$
  • Represents the average value of the observable associated with the operator
  • For example, the expectation value of the position operator $x̂$ gives the average position of a particle in a given state
• Expectation values are crucial for making predictions and comparing theoretical results with experimental measurements in quantum mechanics

Operators and Observables

Relationship between Operators and Observables

• Observables are physical quantities that can be measured in quantum mechanics
  • Examples include position, momentum, energy, and angular momentum
• Each observable is associated with a Hermitian operator that acts on the wave function to extract the observable's value
• The eigenvalues of an operator represent the possible outcomes of a measurement of the corresponding observable
  • For instance, the eigenvalues of the energy operator (Hamiltonian) give the possible energy levels of a quantum system
• The eigenfunctions of an operator form a complete set of basis states for the Hilbert space
  • Any state can be expressed as a linear combination of these eigenfunctions

Uncertainty Principle

• The uncertainty principle states that certain pairs of observables cannot be simultaneously measured with arbitrary precision
  • This is related to the non-commutative nature of their corresponding operators
• The most well-known example is the Heisenberg uncertainty principle for position and momentum: $ΔxΔp ≥ ħ/2$
  • $Δx$ is the uncertainty in position, $Δp$ is the uncertainty in momentum, and $ħ$ is the reduced Planck's constant
• The uncertainty principle imposes fundamental limitations on the precision of simultaneous measurements of incompatible observables

Commutation Relations of Operators

Definition and Properties

• The commutator of two operators $Â$ and $B̂$ is defined as $[Â, B̂] = ÂB̂ - B̂Â$
  • If the commutator is zero, the operators are said to commute
• Commutation relations are essential for determining the compatibility of observables and the uncertainty relations between them

Examples of Commutation Relations

• The position and momentum operators in one dimension satisfy the canonical commutation relation: $[x̂, p̂] = iħ$
  • This commutation relation leads to the Heisenberg uncertainty principle for position and momentum
• The angular momentum operators $L̂ₓ$, $L̂ᵧ$, and $L̂ₓ$ satisfy the cyclic commutation relations:
  • $[L̂ₓ, L̂ᵧ] = iħL̂ₓ$
  • $[L̂ᵧ, L̂ₓ] = iħL̂ₓ$
  • $[L̂ₓ, L̂ₓ] = iħL̂ᵧ$
• These commutation relations are crucial for understanding the properties of angular momentum in quantum mechanics, such as quantization and conservation laws

Eigenfunctions and Eigenvalues of Operators

Eigenvalue Equation

• Eigenfunctions $ψₙ$ of an operator $Â$ satisfy the eigenvalue equation: $Âψₙ = aₙψₙ$
  • $aₙ$ is the corresponding eigenvalue
• To find the eigenfunctions and eigenvalues, one solves the eigenvalue equation by applying the operator to a general wave function and solving the resulting differential or algebraic equation

Significance of Eigenfunctions and Eigenvalues

• The eigenvalues of an operator represent the possible outcomes of a measurement of the associated observable
• The eigenfunctions of an operator form a complete set of basis states for the Hilbert space
  • Any state can be expressed as a linear combination of these eigenfunctions
• Eigenfunctions and eigenvalues play a central role in determining the energy levels, angular momentum states, and other properties of quantum systems

Examples of Operators and Their Eigenfunctions

• The position operator $x̂$ has eigenfunctions $δ(x - x₀)$ with eigenvalues $x₀$
  • These eigenfunctions represent states with a definite position $x₀$
• The momentum operator $p̂$ has eigenfunctions $exp(ipx/ħ)$ with eigenvalues $p$
  • These eigenfunctions represent states with a definite momentum $p$
• The Hamiltonian operator $Ĥ$ has eigenfunctions $ψₙ$ with eigenvalues $Eₙ$
  • The eigenfunctions represent the stationary states of the system, and the eigenvalues give the corresponding energy levels