Photon Detectors: How Do They Work?

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Photon detectors operate by converting incoming photons into measurable signals, with solid-state semiconductor detectors generating electron-hole pairs in a crystal to produce a current proportional to photon energy. Scintillation detectors function by emitting new photons when struck by incoming photons, which are then detected by photomultiplier tubes to create a current. Detectors are typically designed for specific energy ranges, meaning a detector for visible light may not effectively detect gamma radiation without specialized instrumentation. The discussion highlights the complexity and variety of photon detection methods, emphasizing their application in different energy ranges. Understanding these principles is essential for exploring quantum physics and photon detection technologies.
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Hey, I'm new to these forums and am just learning about quantum physics.

I was wondering about the detectors used to pick up on photons. How exactly do these detectors work? What about the ones described which detect a photon but allow it pass through?

Also, if a detector were designed to detect a photon of visible light radiation, would it also pick up a photon of gamma radiation?
 
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There's a bunch of ways to detect photons. Your average camera has a photon detector, film. Here's a couple of ways that are used atleast at the X-ray energies.

Solid state semiconductor detectors detect photons via the electron-hole pairs the incoming photons create in a semiconducting crystal. In an applied electric field that produces a current which is propotional to the incoming photons' energies. Then there's scintillation detectors in which the incoming photon makes the detecting element emit new photons which create a current via a photomultiplier tube.

I don't know about your last question. The detectors are usually designed to work at a certain photon energy range. For something to work at ev and MeV photon energies would take some exceptional instrumentation.
 
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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