Order Maxima under the Fraunhofer Envelope

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    Fraunhofer Maxima
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SUMMARY

The discussion focuses on the interpretation of the order spectrum observed through a spectrometer when analyzing mercury and hydrogen as polychromatic sources. It clarifies that each Fraunhofer envelope corresponds to a specific diffraction order (m = 1, 2, 3, ...), with the central line in the first envelope representing the central maxima. Additionally, it explains that the increasing separation of spectral lines in higher orders is due to the interaction between the single slit diffraction pattern and the double slit interference pattern, a concept referred to as the array theorem.

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Zibi04
Let's say we are using a spectrometer to observe the order spectrum of mercury, a polychromatic source.
Each order contains a an array of colour bands.
In the case of the following image: http://imgur.com/a/bnm9r , I was wondering if each Fraunhofer envelope represented one order, (m = 1 , 2 , 3 ...) or if each line under the envelopes represent each order, where the central line in the first envelope is the central maxima.

Also, the following picture is the order spectrum of hydrogen http://imgur.com/a/DkrJC
Why is it that after each order, the spectral lines separate further away from each other?
 
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In a double interference with finite width of the slits, it's useful to distinguish between diffraction order and interference order. The reason is that the intensity pattern as seen in the screen is a product between the single diffraction pattern from a slit with non-zero width and the double slit (but zero slit width) interference pattern. Some books called this product rule the array theorem. The envelope is the diffraction pattern from a single slit, therefore the peaks of the envelope correspond to a given diffraction order.
 
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