Undergrad Double slit particle distribution with convex lens?

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In the discussed double slit experiment, a convex lens is placed before the detector screen, causing individual photons to pass through the lens and reach the focal point. Instead of creating an interference pattern, the photons result in a particle distribution from the two slits. The inquiry centers on whether the focal point alters or destroys the interference pattern. The conversation suggests reviewing a previous answer by mfb for further clarification on this phenomenon. Continuing the discussion in the linked thread is encouraged to maintain focus on the topic.
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In one double slit experiment, one physicist placed a convex lens before the back screen detector. The individual photons passed through the double slit then through the lens. The individual photons then go through the focal point, then a good distance after they reach the focal point they hit the detector screen. However, they don't produce an interference pattern, instead they produce a particle pattern of the two slits.
My question is what happens after the individual photons after the focal point that makes them produce a particle distribution instead of the interference pattern? Does the the focal point after the lens somehow destroy the interference pattern?
 
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Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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