The basic setup of the double slit experiment is illustrated in Figure 1. Red filtered light derived from sunlight is first passed through a slit to achieve a coherent state. Light waves exiting the first slit are then made incident on a pair of slits positioned close together on a second barrier. A screen is placed in the region behind the slits to capture overlapped light rays that have passed through the twin slits, and a pattern of bright red and dark interference bands becomes visible on the screen. The key to this type of experiment is the mutual coherence between the light waves diffracted from the two slits at the barrier. Although Young achieved this coherence through the diffraction of sunlight from the first slit, any source of coherent light (such as a laser) can be substituted for light passing through the single slit.
The coherent wavefront of light impacting on the twin slits is divided into two new wavefronts that are perfectly in step with each other. Light waves from each of the slits must travel an equal distance to reach point A on the screen illustrated in Figure 1, and should reach that point still in step or with the same phase displacement. Because the two waves reaching point A possess the necessary requirements for constructive interference, they should add together to produce a bright red interference fringe on the screen.
In contrast, neither of the points B on the screen is positioned equidistant from the two slits, so light must travel a greater distance from one slit to reach point B than from the other. The wave emanating from the slit closer to point B (take for example the slit and point B on the left-hand side of Figure 1) does not have as far to travel to reach its destination, as does a wave traveling from the other slit. As a consequence, the wave from the closest slit should arrive at point B slightly ahead of the wave from the farthest slit. Because these waves will not arrive at point B in phase (or in step with each other), they will undergo destructive interference to produce a dark region (interference fringe on the screen. Interference fringe patterns are not restricted to experiments having the double slit configuration, but can be produced by any event that results in the splitting of light into waves that can be canceled or added together.
The success of Young's experiment was strong testimony in favor of the wave theory, but was not immediately accepted by his peers. The events in place behind phenomena such as the rainbow of colors observed in soap bubbles and Newton's rings (to be discussed below), although explained by this work, were not immediately obvious to those scientists who firmly believed that light propagated as a stream of particles. Other types of experiments were later devised and conducted to demonstrate the wave-like nature of light and interference effects. Most notable are the single mirror experiment of Humphrey Lloyd and the double mirror and bi-prism experiments devised by Augustin Fresnel for polarized light in uniaxial and birefringent crystals. Fresnel concluded that interference between beams of polarized light could only be obtained with beams having the same polarization direction. In effect, polarized light waves having their vibration directions oriented parallel to each other can combine to produce interference, whereas those that are perpendicular do not interfere.