Graduate What Happens When Particles Travel in Non-Crystal Directions?

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Particles traveling in non-crystal directions are more likely to experience large-angle scattering, resulting in a shorter mean penetration depth compared to those traveling along specific crystal channels. In crystal structures like silicon, certain directions, such as the 110 direction, provide clear paths with fewer atomic collisions, allowing particles to travel further. Conversely, random directions lack these channels, leading to more frequent encounters with atoms and reduced penetration depth. Figures 1 and 2 illustrate these concepts, highlighting the importance of crystal orientation in particle behavior. Understanding these dynamics is crucial for applications in materials science and particle physics.
aveline de grandpre
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Can someone explain this paragraph especially the bold part in simpler language:

"If it is not in a major crystal direction or plane ("random direction", Fig. 2), it is much more likely to undergo large-angle scattering and hence its final mean penetration depth is likely to be shorter." full article : https://en.wikipedia.org/wiki/Channelling_(physics)

Thank you
 
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Can you be more specific about what you don't understand? Do you know what a mean penetration depth is? Do you understand why it will be shorter in a random direction than along a channel? Do Figs 1 and 2 help you see this?
 
mjc123 said:
Can you be more specific about what you don't understand? Do you know what a mean penetration depth is? Do you understand why it will be shorter in a random direction than along a channel? Do Figs 1 and 2 help you see this?
I don't understand why it will be shorter in a random direction
 
Look again at Figure 1. Can you see that if the particle goes straight along the 110 direction of a silicon crystal, there are "channels" with no atoms down the middle, and the particle can go a relatively long way before being stopped by collision with a silicon atom. These channels only occur in certain specific directions, depending on the crystal structure. If the particle enters the crystal in any old "random" direction, there will be no such clear channels, and the particle is likely to encounter a silicon atom relatively soon along its trajectory.
 
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