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Show that if you attempt to detect a particle while tunneling, your experiment must render its kinetic energy so uncertain that it might well be "over the top."

Short Answer

Expert verified

The order of magnitude of uncertainty makes up for difference between U0鈥塧苍诲鈥E.

Step by step solution

01

Concept involved

Tunnelingis a phenomenon when particles penetrate through a potential barrier which is higher than their kinetic energy.

According to the uncertainty principle, it鈥檚 impossible to calculate the momentum of a particle together with its position simultaneously with absolute accuracy.

螖虫.螖辫/2

Where, 螖虫= Change in position of the particle

螖辫 = Change in momentum of the particle

= modified form of plank鈥檚 constant

02

Explain the reasoning

From the above equation, you get that, uncertainty in x and Pare inversely proportional.

If the particle lies in the barrier, the uncertainty in xneeds to be greater than the wave number- such that pcan be no less than /.

Kinetic energy is given by ( p2/2m), it needs to be greater than or equal to22尘未2=22m2m(U0E)2=U0E .

Thus, the order of magnitude of uncertainty in the Kinetic Energy obtained by the experiment, makes up for difference between the potential energy barrier - U0and the total energy - E.

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Most popular questions from this chapter

As we learn in physical optics, thin-film interference can cause some wavelengths of light to be strongly reflected while others not reflected at all. Neglecting absorption all light has to go one way or the other, so wavelengths not reflected are strongly transmitted. (a) For a film, of thickness t surrounded by air, what wavelengths 位 (while they are within the film) will be strongly transmitted? (b) What wavelengths (while they are 鈥渙ver鈥 the barrier) of matter waves satisfies condition (6-14)? (c) Comment on the relationship between (a) and (b).

Given the situation of exercise 25, show that

(a) as Uo, reflection probability approaches 1 and

(b) as L0, the reflection probability approaches 0.

(c) Consider the limit in which the well becomes infinitely deep and infinitesimally narrow--- that is Uoand data-custom-editor="chemistry" L0but the product U0L is constant. (This delta well model approximates the effect of a narrow but strong attractive potential, such as that experienced by a free electron encountering a positive ion.) Show that reflection probability becomes:

R=[1+2h2EmUoL2]-1

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

Exercise 39 gives the condition for resonant tunneling through two barriers separated by a space of width 2 s, expressed in terms of a factor given in Exercise 30. (a) Suppose that in some system of units, k and are both2. Find two values of 2s that give resonant tunneling. What are these distances in terms of wavelengths of? Is the term resonant tunneling appropriate?(b) Show that the condition has no solution if s = 0 and explain why this must be so. (c) If a classical particle wants to surmount a barrier without gaining energy, is adding a second barrier a good solution?

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Make the crude approximation that this is a rectangular barrier of widthm and approximate height of4X108j/kg. Your mass is 65 kg, and you launch your-self from Earth at an impressive 4 m/s. What is the probability that you can jump to Jupiter?

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