Are fundamental particles like electrons and protons truly matter waves?

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Discussion Overview

The discussion revolves around the nature of fundamental particles, specifically electrons and protons, and their characterization as matter waves. Participants explore the implications of wave-particle duality, the concept of wave packets, and the mathematical representation of these phenomena, touching on both theoretical and experimental aspects.

Discussion Character

  • Exploratory
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • Some participants propose that fundamental particles can be represented as waves, with their wavelength depending on the particle's momentum, as evidenced by experiments like electron diffraction.
  • There is a suggestion that the waves associated with particles can be described by their displacement and amplitude as functions of time and space, governed by quantum equations.
  • Participants discuss the concept of wave packets, indicating that these may represent the particle nature of waves and may be localized forms of wave functions.
  • A mathematical representation of a wave packet is provided, illustrating a solution to the Schrödinger equation for a free particle, with emphasis on the wave function as a probability amplitude.
  • There is a question regarding whether the wave function indeed represents the state of a particle as a localized wave packet, with a later reply noting that localization depends on the function used in the representation.

Areas of Agreement / Disagreement

The discussion presents multiple viewpoints on the nature of matter waves and wave packets, with no consensus reached on specific interpretations or implications of these concepts.

Contextual Notes

Participants express varying assumptions about the nature of wave packets and their localization, which depend on the mathematical functions used in their descriptions. The discussion also reflects a reliance on experimental evidence without resolving the complexities involved in the interpretations of wave-particle duality.

Jianphys17
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Hi at all, I've the following question:
How the fondamental particles (electrons, protons) are seen as matter waves, what shape and size should be these waves? They are wave-packets?
 
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Jianphys17 said:
How the fundamental particles (electrons, protons) are seen as matter waves, what shape and size should be these waves? They are wave-packets?

a fundamental particle can be represented as a wave and its wavelength depends on the momentum of the particle and such conclusions were drawn from definite experiments where the particles interfered like waves. or in other situations waves acted like particles...so one will have to go to the initial descriptions and analysis of effects like electron diffraction experiments when a beam of electrons showed diffraction pattern as produced by electromagnetic waves i.e. light.

The waves and its nature can be given by the variation of its displacement/amplitude as a function of time and space and they are solution of the equation governing the state of the particle. the picture is of 'quantum nature' therefore new equations govern the relationship between its time varying characteristics.

The second part of your question talks about wave packets...which shows that you wish to prepare packets of waves...leading to possible representation of particle nature of waves.
Kindly elaborate on your question so that we may understand further.
 
drvrm said:
The second part of your question talks about wave packets...which shows that you wish to prepare packets of waves...leading to possible representation of particle nature of waves.
Kindly elaborate on your question so that we may understand further.
therefore the waves of matter should be represented as localized waveforms of wave packets right ?
 
Jianphys17 said:
therefore the waves of matter should be represented as localized waveforms of wave packets right ?

A wave packet, for example, is a normalisable solution to Schroedinger equation for a free particle (of mass ##m##), and can be represented by a wave function of the form:

$$\Psi(x, t) = \frac{1}{\sqrt{2\pi}} \int_{-\infty}^{+\infty} f(k) \exp[i(kx - \frac{\hbar k^2}{2m}t)] dk$$

Where ##f(k)## represents the weighting of the underlying eigenstates. Note that ##\Psi(x, t)## is a probability amplitude.
 
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PeroK said:
A wave packet, for example, is a normalisable solution to Schroedinger equation for a free particle (of mass ##m##), and can be represented by a wave function of the form:

$$\Psi(x, t) = \frac{1}{\sqrt{2\pi}} \int_{-\infty}^{+\infty} f(k) \exp[i(kx - \frac{\hbar k^2}{2m})] dk$$

Where ##f(k)## represents the weighting of the underlying eigenstates. Note that ##\Psi(x, t)## is a probability amplitude.
so , correct me if I'm wrong, the wave-function represents the state of the particle as a localized wave packet..
 
Jianphys17 said:
so , correct me if I'm wrong, the wave-function represents the state of the particle as a localized wave packet..

It might be localised. That depends on ##f(k)##.
 

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