Difference between revisions of "Quantum Mechanics"
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A quantum system is completely specified by its '''Wave Function''': | A quantum system is completely specified by its '''Wave Function''': | ||
:<math> | :<math> | ||
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:<math> \psi(x) = \frac{1}{\sqrt{2 \pi}} \int \tilde{\psi}(k) e^{i k x } \mathrm{d}k </math> | :<math> \psi(x) = \frac{1}{\sqrt{2 \pi}} \int \tilde{\psi}(k) e^{i k x } \mathrm{d}k </math> | ||
:<math> \tilde{\psi}(k) = \frac{1}{\sqrt{2 \pi}} \int {\psi}(x) e^{-i k x } \mathrm{d}x </math> | :<math> \tilde{\psi}(k) = \frac{1}{\sqrt{2 \pi}} \int {\psi}(x) e^{-i k x } \mathrm{d}x </math> | ||
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+ | ==[[Wave packet]]== | ||
+ | TBD | ||
==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 15:56, 12 October 2014
Quantum mechanics is a theory that describes the interactions of all particles and systems. It underlies all physical phenomena, including scattering.
Wavefunction
A quantum system is completely specified by its Wave Function:
The wavefunction is typically normalized:
Integral Notation | Dirac Notation |
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The distribution of the particle described by is given by:
Integral Notation | Dirac Notation |
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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