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For a given container made of an extremely reflective surface, is it possible to shine a beam of light in, and with no 'fiddling' (i.e. closing the hole, tilting the object) to contain the beam for an infinite amount of time (not a very long time, but such that it will never escape). Consider the following

here

Something like this. Except I feel like the light will escape given enough time. Also, the object has to be finite in size (infinite is cheating). If there's a proof that no such container exists then that's fine too.

Ignore factors such as dissipation by heat, or quantum tunneling, and just assume a perfect environment with perfect materials.

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    $\begingroup$ In practice, the Q of your container is going to be limited to $\leq 10^7$, so it will take $10^7$ round trips of the beam in a resonator to drop to $e^{-1}$ of its input power. If the resonator's characteristic dimension is $L$ (a "diameter"), then the beam is going to last a time that is of the order $Q\,L/c$; with $L=0.1{\rm m}$ you might get a beam lifetime of $10^7\times 0.1/(3\times 10^8)$ or about three milliseconds. $\endgroup$ Commented Jan 1, 2015 at 10:25
  • $\begingroup$ physics.stackexchange.com/q/95217 $\endgroup$
    – Sensebe
    Commented Jan 1, 2015 at 10:40
  • $\begingroup$ That question regards total internal reflection, in my case I'm using a reflective surface, so it's not really the same situation. $\endgroup$ Commented Jan 1, 2015 at 10:43
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    $\begingroup$ Asking for anything "infinite" in physics is just plain nonsensical. $\endgroup$
    – CuriousOne
    Commented Jan 1, 2015 at 11:04
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    $\begingroup$ aren't you basically describing a (model of a) black body? $\endgroup$
    – glS
    Commented Jan 1, 2015 at 11:13

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I don't think there is any problem with this as a thought experiment. The container does not have to be infinite and when you close-off the container it will contain a radiation field with a finite energy density.

However in practice, even the best reflectors have a finite conductivity and a less than perfect reflectivity, so the radiation field would dissipate by heating the walls of the container.

You could also think about construcing your container out of a solid dielectric block, such that the light was totally internally reflected at each interface (an optical fibre). But again, there is no perfect dielectric and no perfectly smooth surface for ideal specular reflection. Eventually there will be absorption, scattering and even losses to the exterior through evanescent wave coupling.

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  • $\begingroup$ I agree: for more "thought design", send a pulse of light 1 ns long (that's about a foot, for those who never met Admiral Hopper :-) ) into a chamber maybe 1 km cubed. That gives you plenty of time to close the door before the photons can get back up. Given the perfect reflectivity of the unobtanium coating, the light will bounce around forever -- oh, and you'll need a perfect vacuum too so that air molecules don't absorb. $\endgroup$ Commented Jan 1, 2015 at 14:14
  • $\begingroup$ I did mention in my question statement that the capturing was to be done without fiddling, like closing the hole. $\endgroup$ Commented Jan 1, 2015 at 22:39
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With classical ray optics, yes. For example, it is possible to trap a ray between two reflecting spheres. Here are two pictures I created with one of my old computer programs (actually this was a teamwork project).

enter image description here enter image description here

On these two pictures, the incident ray was directed at slightly different angles. It is quite clear, that there exists some limiting case between these two angles, in which the light will not escape either downwards nor upwards. Obviously, we could also use such a system in a bottle.

However, it should be noted that the path of the ray is unstable. If we had taken account also wave-optics, the wave would have "leaked" away very fast from he unstable equilibrium. It turns out, that taking into account quantum mechanics, such a system could be used to heat a hotter body (inside to bottle) with a colder body (outside), which is a contradiction. Thus in real life, this is impossible.

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    $\begingroup$ Are you sure? For this case you seem to imply that the light can enter an infinite loop from which it never escapes. But if it is an infinite loop, that means that the entrance ray must be a part of this loop, which means at some point in time the light must return to the starting position, ie escaping the trap. Or is my logic flawed? $\endgroup$ Commented Jan 1, 2015 at 12:25
  • $\begingroup$ @JoshuaLin: It does not enter an infinite loop. However, in the limiting case, ray's path would converge between the spheres, in a similar way as the sequence given by the relations x[0] = 1 and x[i + 1] = x[i]/2 would converge to 0: 1, 1/2, 1/4, 1/8, ... , even though it never reaches 0. $\endgroup$
    – kristjan
    Commented Jan 1, 2015 at 12:33
  • $\begingroup$ So that means that given enough time the light would leak out anyways? $\endgroup$ Commented Jan 1, 2015 at 12:36
  • $\begingroup$ @JoshuaLin Using ray optics, there would exist a single real-valued angle, for which the beam would converge and not leak out. Using wave-optics (what would happen in real world), the beam would always leak out quite fast, whatever the initial conditions are. $\endgroup$
    – kristjan
    Commented Jan 1, 2015 at 12:43
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Seems like they've found a way to do it!

http://phys.org/news/2015-11-device-theoretically-bit-infinite-amount.html

The problem with my initial idea about using an ordinary container is described succinctly in the above article:

When light is put inside a cavity, it basically interacts with the matter that surrounds it (e.g., glass or metal), and this gives rise to microscopic charge oscillations, so that, similar to the Rutherford atom, the energy of the system is eventually radiated away.

The actual paper is here, I'll need a bit of extra reading to fully understand it. Seems really cool though.

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