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Quantum effects of gravity
The only neutrons that will survive absorption at A are those that cannot cross H. Their turning points will be below H. So that, for a neutron entering to the cavity at height z with vertical velocity vz , conservation of energy implies
T
The cavity should be long enough to ensure the absorption of all neutrons with velocities outside the allowed range. Therefore, neutrons have to reach its maximum height at least once within the cavity. The longest required length corresponds to neutrons that enter at z = H with vz = 0 (see the figure). Calling tf to their time of fall
The rate of transmitted neutrons entering at a given height z, per unit height, is proportional to the range of allowed velocities at that height, r being the proportionality constant
The total number of transmitted neutrons is obtained by adding the neutrons entering at all possible heights. Calling
T
For a neutron falling from a height H, the action over a bouncing cycle is twice the action during the fall or the ascent
Using the BS quantization condition
T
The corresponding energy levels (associated to the vertical motion) are
T
Numerical values for the first level:
Note that H1 is of the same order than the given cavity height, H = 50 μm. This opens up the possibility for observing the spatial quantization when varying H.
The uncertainty principle says that the minimum time and the minimum energy satisfy the relation . During this time, the neutrons move to the right a distance
Now, the minimum neutron energy allowed in the cavity is E1, so that . Therefore, an estimation of the minimum time and the minimum length required is
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