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The entrapment of radiation will make a photon be emitted and resonance-reabsorbed many times inside the laser material.
Suppression of the potential well prevents the free electrons from recombination and, thus, no high-energy photon can be emitted.
The photon counting histogram in fluorescence fluctuation spectroscopy.
However, a significant radiated energy can be achieved since all the electrons scattered in the photon mirror will radiate.
We can see that the photon energy is enlarged greatly in the laboratory frame because of the relativistic effect.
To look at alterations in photon responses, dim flashes of light were presented in the presence or absence of steady background illumination.
Following the injection of such pulses into strongly scattering media, such as tissue, the time dispersion of the photons can be studied.
One detection scheme presently in use requires optical band-pass filters appropriately designed to bin emitted fluorescence photons of desired target molecules.
This mismatch is mainly related to the inability of primary producers to harvest the photons incident on the sea or the land surface.
A small contribution is also obtained from electrons produced by photon interactions in the chamber.
The ridges have compressed enough to be somewhat opaque to backlighter photons.
This process is analogous to treating the photon or plasmon field as particles.
Charged particles will attain relativistic energies close to the pulsar magnetic poles and radiate -ray photons.
The polarization vector of the massive transverse photon hence is perpendicular to the propagation direction, an expected result.
When reflection occurs, we can identify the laser pulse with a photon mirror.