Next revision | Previous revision | ||
equations:pauli_equation [2017/10/21 15:29] jakobadmin created |
equations:pauli_equation [2018/04/16 09:09] (current) jakobadmin [Intuitive] |
||
---|---|---|---|
Line 1: | Line 1: | ||
- | ====== Pauli Equation ====== | + | <WRAP lag>$\left( \frac{1}{2m}(\vec \sigma ( \vec p - q\vec A))^2 + q\phi \right) \Psi = i \hbar \partial_t \Psi $</WRAP> |
- | <tabbox Why is it interesting?> | + | ====== Pauli Equation ====== |
- | <note tip>The Pauli equation is the correct non-relativistic equation to describe spin 1/2 particles. | ||
- | </note> | ||
- | <tabbox Layman> | ||
- | <note tip> | ||
- | Explanations in this section should contain no formulas, but instead colloquial things like you would hear them during a coffee break or at a cocktail party. | ||
- | </note> | ||
- | | ||
- | <tabbox Student> | ||
- | The Pauli equation is the non-relativistic limit of the [[equations:dirac_equation|Dirac equation]]. | ||
- | |||
- | <tabbox Researcher> | ||
- | * Nonrelativistic particles and wave equations by Jean-Marc Lévy-Leblond | + | <tabbox Intuitive> |
- | --> Common Question 1# | + | The Pauli equation describes how the state of a quantum system with [[basic_notions:spin|half-integer spin]] changes in time. |
+ | In contrast, the [[equations:schroedinger_equation|Schrödinger equation]] describes the time evolution of systems without spin. | ||
+ | <tabbox Concrete> | ||
+ | |||
+ | The Pauli equation is the non-relativistic limit of the [[equations:dirac_equation|Dirac equation]]. | ||
- | <-- | + | <tabbox Abstract> |
- | --> Common Question 2# | + | * Nonrelativistic particles and wave equations by Jean-Marc Lévy-Leblond |
- | |||
- | <-- | ||
- | | ||
- | <tabbox Examples> | ||
- | --> Example1# | + | <tabbox Why is it interesting?> |
- | + | The Pauli equation is the correct __non-relativistic__ equation to describe spin 1/2 particles. | |
- | <-- | + | |
- | --> Example2:# | + | <tabbox Definitions> |
- | + | * Ψ is the wave function, | |
- | <-- | + | * m the mass of the particle, |
- | + | * q the charge of the particle, | |
- | <tabbox History> | + | * →σ the Pauli matrices, |
+ | * →p the momentum, | ||
+ | * →A the vector potential, | ||
+ | * ϕ the electric scalar potential and | ||
+ | * ℏ the reduced Planck constant. | ||
+ | Take note that →σ, a "vector of matrices" is only used as a convenient short-hand notation for the sums that appear in the equation. For example, →σ→p=σ1p1+σ2p2+σ3p3. | ||
</tabbox> | </tabbox> | ||