Total Reflection of a Classical Particle off a Two-Dimensional Potential

Your Name]In summary, the classical trajectory of a particle traveling towards a two dimensional potential of the form V(x,y) = V if x>0 and V(x,y)=0 if x<0, with an oblique angle of incidence and kinetic energy less than V, will experience a lateral shift upon reflection depending on the angle of incidence and the height of the potential barrier. This is due to the conservation of y-component of momentum and energy.
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Homework Statement


This question is motivated by Problem 8, Ch 1 of Cohen-Tannoudji's "Quantum Mechanics". Suppose that you are given a two dimensional potential of the form V(x,y) = V if x>0 and V(x,y)=0 if x<0. A particle travels toward the the potential obliquely, i.e. neither parallel to the x-axis nor to the y-axis, and its kinetic energy is less than V. Describe the classical trajectory of the particle upon reflection.

Homework Equations



Presumably, conservation of the y-component of momentum and conservation of energy.

The Attempt at a Solution


The classical trajectory is described as a "lateral shift upon reflection." I assume that the answer will somehow depend on the angle \theta between the trajectory and the normal to the surface. Thanks!
 
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Hello there,

Thank you for bringing this problem to our attention. I can offer you some insights into this problem.

First, let's consider the classical trajectory of a particle traveling towards the potential obliquely. As you mentioned, the conservation of the y-component of momentum and conservation of energy must be taken into account. This means that the particle's y-component of momentum and energy remain constant throughout its motion.

Now, when the particle reaches the potential barrier, it will experience a change in direction due to the potential. The angle of reflection will depend on the angle of incidence and the potential barrier's shape. In this case, the potential barrier is a step function, so the angle of reflection will depend on the angle of incidence and the height of the potential barrier.

If the particle's kinetic energy is less than the potential barrier, it will be reflected back in the opposite direction. However, due to the oblique angle of incidence, the reflected particle's trajectory will be shifted laterally, as you mentioned. The amount of lateral shift will depend on the angle of incidence and the height of the potential barrier.

I hope this helps you understand the classical trajectory of the particle upon reflection in this scenario. Let me know if you have any further questions or need clarification.
 

FAQ: Total Reflection of a Classical Particle off a Two-Dimensional Potential

What is total reflection of a classical particle off a two-dimensional potential?

Total reflection refers to the phenomenon where a classical particle, such as a light ray or an electron, is completely reflected upon encountering a two-dimensional potential barrier. This means that the particle does not penetrate the barrier and instead bounces off of it.

How does total reflection occur?

Total reflection occurs when the energy of the particle is lower than the potential barrier it encounters. In this case, the particle does not have enough energy to overcome the barrier and is therefore reflected back in the opposite direction.

What factors can affect total reflection?

The main factors that can affect total reflection are the energy of the particle and the height and width of the potential barrier. As the energy of the particle increases, the likelihood of total reflection decreases. Additionally, a higher and wider potential barrier will also decrease the likelihood of total reflection.

How is total reflection different from partial reflection?

In total reflection, the particle is completely reflected and does not penetrate the potential barrier. In contrast, in partial reflection, the particle has enough energy to partially penetrate the barrier before being reflected back.

What are the applications of total reflection?

Total reflection has many applications in various fields, such as optics, electronics, and quantum mechanics. For example, it is used in optical fibers to transmit light signals without loss, and in quantum computing to control the behavior of electrons. It also plays a role in understanding the behavior of particles in potential wells and barriers, which is important in the development of new materials and technologies.

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