Nuclear Radius and Diffraction

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Discussion Overview

The discussion revolves around the concept of electron diffraction when high-energy electrons interact with atomic nuclei. Participants explore the implications of diffraction in relation to the size of nuclei, the nature of the interaction between electrons and nuclei, and the conditions under which diffraction occurs.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants question whether electrons are diffracted by the nuclei themselves or by the gaps between them, raising concerns about the implications for understanding nuclear size.
  • It is suggested that the de Broglie wavelength of electrons being similar to the size of the nucleus indicates that diffraction occurs due to the nucleus acting as an obstacle.
  • Some argue that the density of the nucleus complicates the notion of electrons diffracting through it, leading to confusion about the nature of the interaction.
  • A participant mentions that higher energy electrons can provide insights into the structure of the nucleus through deep inelastic scattering, while longer wavelengths may simply result in diffraction patterns.
  • References are made to differential cross-section plots and specific calculations of de Broglie wavelengths to illustrate the relationship between electron energy and nuclear size.
  • Participants discuss the overall diffraction pattern resulting from multiple nuclei and how it relates to individual nuclei and their arrangement.

Areas of Agreement / Disagreement

Participants express differing views on whether the diffraction is due to the nuclei themselves or the spaces between them, and there is no consensus on the interpretation of how electrons interact with the dense nuclear material. The discussion remains unresolved regarding the exact nature of the diffraction process.

Contextual Notes

There are limitations in understanding the assumptions regarding the interaction between electrons and nuclei, particularly concerning the density of nuclei and the implications for diffraction patterns. The discussion also highlights unresolved mathematical steps in relating electron energy to nuclear size.

esmeralda4
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Hi there,

My textbook says "When a beam of high energy electrons is directed at a thin solid sample of an element, the incident electrons are diffracted by the nuclei of the atoms in the foil."

What does this mean exactly? Are the atoms diffracted by the gap between different nuclei?

It goes on to say they are diffracted because the de broglie wavelength of the electrons is similar to the diameter of the nuclei - but I thought the wavelength had to be similar to the gap width, i.e the distance between two nuclei. This gap width wouldn't necessary by the same as the diameter of the nucleus would it?

Thanks in advance!
 
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It is true that waves can be diffracted around obstacles as well as through apertures.
This partly explains how you can hear sound behind an obstacle.
The effects of diffraction are apparent when the wavelength of the wave is of the same order as the dimensions of the obstacle.
 
Thanks for your reply but I'm still confused.

I understand the principle of diffraction. What I don't understand is what is actually diffracting the electrons in this case? Is it the gap between the nuclei or the nucleus itself? If it is the gap between the nuclei then how does that give an approximation for the diameter of a nucleus?

If the beam are diffracted by traveling through the nucleus itself then what is that all about?!

Thanks
 
From the wording I would say that the electrons are diffracted by the nucleus. The nucleus is behaving as an obstacle and the details of the diffraction pattern will indicate the size of the nucleus.
I would not say the beams are "travelling through the nucleus itself"
 
The distance between nuclei of atoms is far larger than the nuclei themselves. If the de broglie wavelength is approximately the size of the nucleus then it is being diffracted by the nucleus itself.
 
Thanks Drakkith - That's what I think it is suggesting but what does that mean to say the electron is being diffracted by traveling through the nucleus?

Aren't nuclei relatively dense? 6x10 to the 16 kg per metre cubed. (more dense than a neutron star).

If electrons are firing into this dense object and diffracting then, well, how is this happening!? This doesn't sound like diffraction to me. The electrons are not traveling through a gap or passing an edge - and if they are passing an edge then it will be of something inside the nucleus (a quark possibly)- how would that than tell us the diameter of the nucleus?

Help!
 
esmeralda4 said:
Thanks Drakkith - That's what I think it is suggesting but what does that mean to say the electron is being diffracted by traveling through the nucleus?

Aren't nuclei relatively dense? 6x10 to the 16 kg per metre cubed. (more dense than a neutron star).

If electrons are firing into this dense object and diffracting then, well, how is this happening!? This doesn't sound like diffraction to me. The electrons are not traveling through a gap or passing an edge - and if they are passing an edge then it will be of something inside the nucleus (a quark possibly)- how would that than tell us the diameter of the nucleus?

Help!

The nucleus has an "outer edge" if you want to call it that. Since the electron has wave-like properties, it diffracts off of it just like a sound wave does when it passes over an object. Higher energy electrons have a smaller wavelength and can actually tell us what's in the nucleus through deep inelastic scattering, but longer wavelength ones simply diffract off of it as if it were one object. As to how that tells you the diameter of the nucleus, that is beyond my knowledge and ability to explain. I only know that it does.
 
See the differential cross section plots of electron-nuclear scattering in

http://www.jpoffline.com/physics_docs/y3s6/nuclearphysics_ln.pdf

See the obvious "diffraction" shape in Fig, 6 on page 8. This is due to the electron deBroglie wavelength and the nuclear size, See the discussion in Section 1.4. For a E = 100 MeV electron, the deBroglie wavelength is λ = hc/(2πE) = 197 MeV-fermi / 100 MeV = 1.97 fermi (1.97 x 10-13 cm). So it is similar to nuclear sizes.

This article shows rings fron optical diffraction around a circular dark spot

http://en.wikipedia.org/wiki/Arago_spot
 
Last edited:
The term diffraction refers to the whole thing. The individual diffracting centres and the pattern in which they are arranged (as in the 'array factor' of antenna arrays). The same happens with the 'two slits' experiment, you have the broad beam pattern from the slit width and the banded pattern from the 'array' of two, spaces, slits.
The overall pattern is given by the product of the two patterns but one will often dominate.

In the case of the array of nuclei and fast, diffracting electrons, the pattern is dominated by the individual nuclei. For a longer wavelength (X rays or slow electrons) the array factor will dominate and you get an array of spots for a single crystal or rings (as with the School Electron diffraction through a graphite target).

Btw. The shape of diffraction patterns for a circular obstacle is the same as for a circular hole - the dark areas being replaced by light areas etc.
 

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