# Interference pattern and slit

Three questions about interference pattern and slit.

(i) In the 1-slit experiment, an interference pattern is observed if the slit is wide enough (a narrow slit gives a rather blurred interference pattern). In theory, if we widen the slit more and more but keep the source of light narrow (constant narrow source), the interference pattern will remain sharp or get even sharper. In the limiting case, one can take away the barrier altogether and the slit can become infinitely wide while the source of light is kept narrow (constant narrow source). In this limiting case, the interference pattern will still remain or become the sharpest. Has people done an experiment with no barrier and therefore no slit but with a very narrow source of light to see what interference pattern emerges?

(ii) According to http://web.mit.edu/viz/EM/visualizations/coursenotes/modules/guide14.pdf, in the 2-slit experiment, the distance of the first minimum (with m=0) from the centre of the central fringe is inversely proportional to the distance between the two slits, i.e., d in eqn. 14.2.9. Using this expression, if we let d decreases towards zero which amounts to the 2-slit experiment becoming a wide 1-slit experiment, the first minimum will be infinitely far away from the central fringe. That would mean that effectively there will be no first minimum and there will be no interference pattern for this 1-slit experiment. But this is contrary to what is observed where we find 1-slit experiment still produces interference pattern. Hence, we have to conclude that there is something wrong with this expression for the position of the first minimum and other minimums. Can someone provide us with a better formula than the one given in eqn. 14.2.9? For that matter, the expression for the maximums in eqn. 14.2.8 also looks suspect.

(iii) According to eqn. 14.2.9, the first minimum and other minimums depend linearly on the distance between the slits and the detecting screen (L). I wonder if people have done experiment by varying L and keep everything else the same, and have observed this linear dependence on L. Since the expression in 14.2.9 seems to be suspect by the argument in (ii), this dependence on L may also be suspect.For that matter, the dependence on L in the expression for the maximums in eqn. 14.2.8 also looks suspect.

I think that the formalism of Fourier transforms and Fraunhofer diffraction will be able to answer all your questions. Indeed, when we place ourselves in the case where the distance $$L$$ between the slit of size $$d$$ and the screen is very large ($$L >> d/\lambda$$, where $$\lambda$$ is the wavelength of the light source), we know that the intensity profile $$A(x,y)$$ on the screen is related to the Fourier transform $$\mathcal{F}$$ of the intensity profile $$a(x,y)$$ at the slit, to be exact $$A(x,y)=\mathcal{F}(\frac{kx}{2},\frac{ky}{2})$$, where $$k=\frac{2 \pi}{\lambda}$$ is the wave number. This is the Fraunhofer diffraction.
In the case of the 1-slit experiment, if the slit is infinitely wide in $$y$$ and of size $$d$$ in $$x$$, $$a(x,y)$$ is a rectangular window function i.e. $$a(x,y)=1$$ if $$x and $$a(x,y)=0$$ elsewhere. The Fourier transform of a rectangular function of size $$d$$ is given by $$d \frac{\sin(\alpha d)}{\alpha d}$$, which give the correct single-slit profile (sine cardinal function). When you take a function and its Fourier transform, a wider function gives a tiner Fourier transform and vice-versa, it explains why it becomes narrow when you increase the size of the slit.