Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

In the wide-barrier transmission probability of equation \((6-18)\), the coefficient multiplying the exponential is often omitted. When is this justified, and why?

Short Answer

Expert verified
The coefficient multiplying the exponential function in the wide-barrier transmission probability (in equation 6-18) can be omitted if and only if the coefficient is equal to 1 or its influence is negligible. This means that the scalar input value to the function does not need to be adjusted or changed since changes to these parameters do not significantly affect the tunneling probability.

Step by step solution

01

Understand the wide-barrier transmission probability

The crucial step is to understand the nature of the transmission probability in context of a wide-barrier. The transmission probability profile over a barrier in quantum mechanics is usually given by an exponential function, as the nature of quantum tunneling is exponential decay across a barrier. The equation, (6-18), likely describes this, but without the actual equation, a detailed breakdown is not possible.
02

Analyze role of coefficient

Normally, the coefficient in the exponential function is used to scale and adjust the input value. In this wide-barrier transmission probability scenario, it could potentially determine the 'width' or 'range' of the barrier. If so, the coefficient might represent some physical characteristic of the barrier such as potential energy or width.
03

Determine when omission is justified

The justification for the omission of the coefficient would potentially be if that coefficient is equal to 1. That is, if the input value does not need to be scaled or adjusted. Mathematically, any number multiplied by 1 retains its original value. In a physical interpretation, this could mean that the parameters of the barrier are such that the resultant 'width' or 'range' is already ideal for a given system, or that changes to these parameters do not significantly affect the tunneling probability.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Wide-Barrier Transmission Probability
Understanding the transmission probability of particles through a wide barrier is one of the fascinating topics in quantum mechanics. At the heart of this concept lies something known as quantum tunneling, where particles have a finite probability of ‘tunneling’ through a barrier even when classical physics says it's impossible.

When examining the particle behavior across such a barrier, the transmission probability is often represented by an exponential function. This function takes into account the width of the barrier and the energy of the particles. The coefficient before the exponential, in some cases, can be omitted, and this simplification is justified when the coefficient is unity or when its variation does not significantly influence the tunneling process. Should the barrier characteristics precisely match the conditions of the tunneling event, this coefficient might not factor into the calculation in a meaningful way, allowing for a more streamlined representation of the probability equation.
Quantum Mechanics
Quantum mechanics is a fundamental theory in physics that provides a description of the physical properties of nature at small scales, like atoms and subatomic particles. At this tiny scale, many of the rules that govern classical physics start to break down, and new counterintuitive rules take over. One such rule is the possibility of quantum tunneling, which allows particles to pass through barriers that would be insurmountable according to classical physics.

In quantum mechanics, objects have characteristics of both particles and waves. This duality is vital to understanding phenomena like tunneling, where the wave-like behavior of particles can lead to a non-zero probability of finding a particle on the other side of a barrier. The ongoing study of quantum mechanics continues to unveil more about the nature of our universe and has led to many applications, from the transistors in computers to quantum computing.
Exponential Decay
Exponential decay is a concept that extends far beyond just quantum mechanics. It's a process by which a quantity decreases at a rate proportional to its current value. In the context of quantum tunneling, the transmission probability decays exponentially in relation to the width and height of the barrier. Mathematics uses the exponential function to describe this decay, which often appears in natural systems, such as radioactive decay, absorption of light, and even in financial systems like interest rates.

The key characteristic of exponential decay in quantum tunneling is that it highlights the rapid decrease in probability as the barrier's dimensions increase. However, it's important to note that even if the decay is rapid, it never quite reaches zero when tunneling is considered. This persistent possibility of penetration, no matter how small, is one of the intriguing aspects of quantum mechanics that continuously challenges our classical understanding of the physical world.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

How should you answer someone who asks, "in tunneling through a simple barrier, which way are particles moving in the three regions before, inside, and after the barrier?"

Your friend has just finished classical physics and can't wait to know what lies ahead. Keeping extraneous ideas and postulates to is minimum. explain the process of quantum-mechanical tunneling.

A ball is thrown straight up at \(25 \mathrm{~m} / \mathrm{s}\). Someone asks, "Ignoring air resistance, what is the probability of the ball tunneling to a height of \(1000 \mathrm{~m}\) ?" Explain why chis is not an example of tunneling as discussed in this chapter, even if the ball were replaced with a small fundamental particle. (The fact that the potential energy varies with position is not the whole answer - passing through nonrectangular barriers is still tunneling.)

A beam of particles of energy \(E\) and incident upon a potential step of \(U_{0}=\\{E\) is described by the wave function $$ \psi _{inc} (x) = 1e^{ill} $$ (a) Determine completely the reflected wave and the wave inside the step by enforcing the required continuity conditions to obtain their (possibly complex) amplitudes, (b) Verify by explicit calculation that the ratio of reflected probability density to the included probability density is 1.

A particle of mass \(m\) and energy \(E\) moving in a region where there is initially no potential energy encounters a potential encounters a potential clip of width \(L\) and depth \(U=-U \alpha\). $$ U(x)=\left\\{\begin{array}{cc} 0 & x \leq 0 \\ -U_{0} & 0

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free