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Contact Developer. Register a free business account. Developer info admin doublewin This type of experiment was first performed, using light, by Thomas Young in , as a demonstration of the wave behavior of light.
At that time it was thought that light consisted of either waves or particles. With the beginning of modern physics, about a hundred years later, it was realized that light could in fact show behavior characteristic of both waves and particles.
In , Davisson and Germer demonstrated that electrons show the same behavior, which was later extended to atoms and molecules.
He believed it demonstrated that the wave theory of light was correct, and his experiment is sometimes referred to as Young's experiment  or Young's slits.
The experiment belongs to a general class of "double path" experiments, in which a wave is split into two separate waves that later combine into a single wave.
Changes in the path lengths of both waves result in a phase shift , creating an interference pattern. Another version is the Mach—Zehnder interferometer , which splits the beam with a mirror.
In the basic version of this experiment, a coherent light source , such as a laser beam, illuminates a plate pierced by two parallel slits, and the light passing through the slits is observed on a screen behind the plate.
These results demonstrate the principle of wave—particle duality. Other atomic-scale entities, such as electrons , are found to exhibit the same behavior when fired towards a double slit.
The experiment can be done with entities much larger than electrons and photons, although it becomes more difficult as size increases. The largest entities for which the double-slit experiment has been performed were molecules that each comprised atoms whose total mass was over 10, atomic mass units.
The double-slit experiment and its variations has become a classic thought experiment , for its clarity in expressing the central puzzles of quantum mechanics.
Because it demonstrates the fundamental limitation of the ability of the observer to predict experimental results, Richard Feynman called it "a phenomenon which is impossible […] to explain in any classical way , and which has in it the heart of quantum mechanics.
In reality, it contains the only mystery [of quantum mechanics]. If light consisted strictly of ordinary or classical particles, and these particles were fired in a straight line through a slit and allowed to strike a screen on the other side, we would expect to see a pattern corresponding to the size and shape of the slit.
However, when this "single-slit experiment" is actually performed, the pattern on the screen is a diffraction pattern in which the light is spread out.
The smaller the slit, the greater the angle of spread. The top portion of the image shows the central portion of the pattern formed when a red laser illuminates a slit and, if one looks carefully, two faint side bands.
More bands can be seen with a more highly refined apparatus. Diffraction explains the pattern as being the result of the interference of light waves from the slit.
If one illuminates two parallel slits, the light from the two slits again interferes. Here the interference is a more pronounced pattern with a series of alternating light and dark bands.
The width of the bands is a property of the frequency of the illuminating light. When Thomas Young — first demonstrated this phenomenon, it indicated that light consists of waves, as the distribution of brightness can be explained by the alternately additive and subtractive interference of wavefronts.
However, the later discovery of the photoelectric effect demonstrated that under different circumstances, light can behave as if it is composed of discrete particles.
These seemingly contradictory discoveries made it necessary to go beyond classical physics and take the quantum nature of light into account.
Feynman was fond of saying that all of quantum mechanics can be gleaned from carefully thinking through the implications of this single experiment.
The Englert—Greenberger duality relation provides a detailed treatment of the mathematics of double-slit interference in the context of quantum mechanics.
A low-intensity double-slit experiment was first performed by G. A double-slit experiment was not performed with anything other than light until , when Claus Jönsson of the University of Tübingen performed it with electron beams.
In , Stefano Frabboni and co-workers eventually performed the double-slit experiment with electrons and real slits, following the original scheme proposed by Feynman.
In , single particle interference was demonstrated for antimatter by Marco Giammarchi and coworkers. An important version of this experiment involves single particles or waves—for consistency, they are called particles here.
Sending particles through a double-slit apparatus one at a time results in single particles appearing on the screen, as expected.
Remarkably, however, an interference pattern emerges when these particles are allowed to build up one by one see the adjacent image.
This demonstrates the wave—particle duality , which states that all matter exhibits both wave and particle properties: the particle is measured as a single pulse at a single position, while the wave describes the probability of absorbing the particle at a specific place on the screen.
The probability of detection is the square of the amplitude of the wave and can be calculated with classical waves see below. The particles do not arrive at the screen in a predictable order, so knowing where all the previous particles appeared on the screen and in what order tells nothing about where a future particle will be detected.
Ever since the origination of quantum mechanics, some theorists have searched for ways to incorporate additional determinants or " hidden variables " that, were they to become known, would account for the location of each individual impact with the target.
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