Difference between revisions of "Quantum Mechanics"
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:<math>\Delta_{E}\Delta_{t} \geq \frac{\hbar}{2}</math> | :<math>\Delta_{E}\Delta_{t} \geq \frac{\hbar}{2}</math> | ||
| + | ==Superposition== | ||
| + | If <math>\psi_1(x)</math> and <math>\psi_2(x)</math> are both allowed states for a given system, then the following state is also allowed: | ||
| + | :<math> | ||
| + | \psi(x) = \alpha \psi_1(x) + \beta \psi_2(x) | ||
| + | </math> | ||
| + | This leads to a notable consequence: | ||
| + | :<math> | ||
| + | \begin{alignat}{2} | ||
| + | \Pr(x) & = | \alpha \psi_1(x) + \beta \psi_2(x) |^2 \\ | ||
| + | & = 1 | ||
| + | \end{alignat} | ||
| + | </math> | ||
==See Also== | ==See Also== | ||
* [http://en.wikipedia.org/wiki/Quantum_mechanics Wikipedia: Quantum Mechanics] | * [http://en.wikipedia.org/wiki/Quantum_mechanics Wikipedia: Quantum Mechanics] | ||
Revision as of 18:40, 12 October 2014
Quantum mechanics is a theory that describes the interactions of all particles and systems. It underlies all physical phenomena, including scattering.
Contents
Wavefunction
A quantum system is completely specified by its Wave Function:
The wavefunction is typically normalized:
| Integral Notation | Dirac Notation |
|---|---|
The distribution of the particle described by is given by:
| Integral Notation | Dirac Notation |
|---|---|
In the Copenhagen Interpretation, is the probability of finding the particle at location . In Universal Wave Function interpretations (e.g. MWI), can be thought of as the spatial distribution of the particle. The wavefunction contains all the information one can know about a system. It can thus be thought of as 'being' the particle/system in question. However, the wavefunction can be described in an infinite number of different ways. That is, there is not a unique basis for describing the wavefunction. So, for instance, one can describe the wavefunction using position-space or momentum-space:
These representations can be inter-related (c.f. Fourier transform):
Wave packet
TBD
Heisenberg Indeterminacy Relations
(Also known as Heisenberg Uncertainty Principle.)
Superposition
If and are both allowed states for a given system, then the following state is also allowed:
This leads to a notable consequence: