Difference between revisions of "Wave packet"

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A '''wave packet''' is a localized wavelike perturbation.
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A '''wave packet''' is a localized wavelike perturbation, which appears frequently in [[Quantum Mechanics|quantum]] descriptions of particles. For instance, incident [[x-ray]]s during [[scattering]] experiments can be thought of as wave-packets.
  
[[File:Wave packet (dispersion).gif|right|thumb|300px|A 1D wave packet (with dispersion), propagating over time.]]
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[[File:Wave packet (dispersion).gif|center|thumb|300px|A 1D wave packet (with dispersion), propagating over time.]]
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[[File:2dpack.jpg|center|thumb|300px|A snapshot of a 2D wave packet.]]
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==Position-momentum tradeoff==
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The wave-packet can be described as a wavefunction in either [[realspace|position-space]] or [[reciprocal-space|momentum-space]]:
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:<math> \psi(x) = \frac{1}{\sqrt{2 \pi}} \int \tilde{\psi}(k) e^{i k x } \mathrm{d}k </math>
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:<math> \tilde{\psi}(k) = \frac{1}{\sqrt{2 \pi}} \int {\psi}(x) e^{-i k x } \mathrm{d}x </math>
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Note that these two descriptions are [[Fourier transform]]s of one another. Thus, there is an inherent tradeoff between the 'spread' of a wave-packet in position-space vs. momentum-space.
  
[[File:2dpack.jpg|right|thumb|300px|A snapshot of a 2D wave packet.]]
 
  
 
==Wave-particle duality==
 
==Wave-particle duality==

Revision as of 08:22, 13 October 2014

A wave packet is a localized wavelike perturbation, which appears frequently in quantum descriptions of particles. For instance, incident x-rays during scattering experiments can be thought of as wave-packets.

A 1D wave packet (with dispersion), propagating over time.
A snapshot of a 2D wave packet.

Position-momentum tradeoff

The wave-packet can be described as a wavefunction in either position-space or momentum-space:

Note that these two descriptions are Fourier transforms of one another. Thus, there is an inherent tradeoff between the 'spread' of a wave-packet in position-space vs. momentum-space.


Wave-particle duality

In the context of quantum mechanics, particles can be thought of as wave-packets. That is, quantum particles are neither ideal point-like particles, nor ideal plane-waves. They are instead intermediate objects, which are certainly wave-like (e.g. can undergo interference), but also somewhat localized. The classical concepts of 'particle' (perfectly localized; mathematically a delta-function), and 'wave' (oscillation with a single well-defined wavelength, spread infinitely over all space) can be viewed as limited cases of the general wave-packet. These limiting cases are only conceptual: in reality neither can exist.


See Also