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By the end of this section, you will be able to:
  • Describe the statistical interpretation of the wave function
  • Use the wave function to determine probabilities
  • Calculate expectation values of position, momentum, and kinetic energy

In the preceding chapter, we saw that particles act in some cases like particles and in other cases like waves. But what does it mean for a particle to “act like a wave”? What precisely is “waving”? What rules govern how this wave changes and propagates? How is the wave function used to make predictions? For example, if the amplitude of an electron wave is given by a function of position and time, Ψ ( x , t ) , defined for all x , where exactly is the electron? The purpose of this chapter is to answer these questions.

Using the wave function

A clue to the physical meaning of the wave function Ψ ( x , t ) is provided by the two-slit interference of monochromatic light ( [link] ). (See also Electromagnetic Waves and Interference .) The wave function    of a light wave is given by E ( x , t ), and its energy density is given by | E | 2 , where E is the electric field strength. The energy of an individual photon depends only on the frequency of light, ε photon = h f , so | E | 2 is proportional to the number of photons. When light waves from S 1 interfere with light waves from S 2 at the viewing screen (a distance D away), an interference pattern is produced (part (a) of the figure). Bright fringes correspond to points of constructive interference of the light waves, and dark fringes correspond to points of destructive interference of the light waves (part (b)).

Suppose the screen is initially unexposed to light. If the screen is exposed to very weak light, the interference pattern appears gradually ( [link] (c), left to right). Individual photon hits on the screen appear as dots. The dot density is expected to be large at locations where the interference pattern will be, ultimately, the most intense. In other words, the probability (per unit area) that a single photon will strike a particular spot on the screen is proportional to the square of the total electric field, | E | 2 at that point. Under the right conditions, the same interference pattern develops for matter particles, such as electrons.

Part a shows monochromatic light of wavelength lambda emitted from a source, arriving as plane waves at a single slit, S. The waves pass through the slit ad form circular waves that arrive at a double slit, S sub 1 and S sub 2. The light rays emerge from two slits as semicircles overlapping one another. The interacting waves spread out and end on a screen where points of maximum, where the crests or troughs overlap, and minimum, where the crests from one slit overlap the troughs from the other, are marked. The pattern appears on the screen as a series of alternating bright and dark fringes. The fringes separation, y, is the distance between adjacent maxima. In part b, a photograph of the fringe pattern is shown. Part c shows how the pattern develops in time. Photos of the image at five times are shown. At first, only a few scattered bright points appear, apparently randomly, against a dark background. In the second image, we see more dots but not yet any discernible pattern. In the third image, we start to see that there are more dots in some parts of the image and fewer elsewhere. Vertical stripes of dense bright dots separated are clearly seen in the fourth image, and even more clearly in the fifth.
Two-slit interference of monochromatic light. (a) Schematic of two-slit interference; (b) light interference pattern; (c) interference pattern built up gradually under low-intensity light (left to right).

Visit this interactive simulation to learn more about quantum wave interference.

The square of the matter wave | Ψ | 2 in one dimension has a similar interpretation as the square of the electric field | E | 2 . It gives the probability that a particle will be found at a particular position and time per unit length, also called the probability density    . The probability ( P ) a particle is found in a narrow interval ( x , x + dx ) at time t is therefore

P ( x , x + d x ) = | Ψ ( x , t ) | 2 d x .

(Later, we define the magnitude squared for the general case of a function with “imaginary parts.”) This probabilistic interpretation of the wave function is called the Born interpretation    . Examples of wave functions and their squares for a particular time t are given in [link] .

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Source:  OpenStax, University physics volume 3. OpenStax CNX. Nov 04, 2016 Download for free at http://cnx.org/content/col12067/1.4
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