Pytanie |
Odpowiedź |
rozpocznij naukę
|
|
this energy is emitted in the form of a photon
|
|
|
non-radiative recombination rozpocznij naukę
|
|
it is passed on to one or more phonons and in the case of Auger recombination it is given off in the form of kinetic energy to another electron
|
|
|
Band-to-band recombination rozpocznij naukę
|
|
electron moves from its conduction band state into the empty valence band state associated with the hole
|
|
|
Trap-assisted recombination an energy level within the bandgap caused by the presence of a foreignatom or a structural defect rozpocznij naukę
|
|
occurs when an electron falls into a "trap"
|
|
|
rozpocznij naukę
|
|
a process in which an electron and a hole recombine in a band-to band transition
|
|
|
rozpocznij naukę
|
|
When the number of particles in the excited state is greater than the number of particlesin the ground state the material is in a state of
|
|
|
rozpocznij naukę
|
|
The low energy part of the spectral
|
|
|
characteristics will be related to transitions between dopant levels and edge bands. The maximum of LED’s output power refers to the photon’s energy which is a little smaller rozpocznij naukę
|
|
characteristics will be related to transitions between dopant levels and edge bands. The maximum of LED's output power refers to the photon's energy which is a little smaller
|
|
|
than the width of the energy gap. The phenomenon of "fill-band" is rozpocznij naukę
|
|
than the width of the energy gap. The phenomenon of "fill-band" is
|
|
|
responsible for the high energy part of the spectral characteristics rozpocznij naukę
|
|
|
|
|
increasing of the current flowing through the diode. rozpocznij naukę
|
|
increasing of the current flowing through the diode.
|
|
|
rozpocznij naukę
|
|
contains a coherent beam of light
|
|
|
between reflective surfaces-mirrors so that the light passes through the gain medium more rozpocznij naukę
|
|
between reflective surfaces-mirrors so that the light passes through the gain medium more
|
|
|
than once before it is emitted from the output aperture or lost to diffraction or absorption rozpocznij naukę
|
|
than once before it is emitted from the output aperture or lost to diffraction or absorption
|
|
|
rozpocznij naukę
|
|
in each passage through the active material the intensity gains
|
|
|
rozpocznij naukę
|
|
reached when the optical gain of the laser medium is exactly
|
|
|
balanced by the sum of all the losses experienced by light in one round trip of the laser's rozpocznij naukę
|
|
balanced by the sum of all the losses experienced by light in one round trip of the laser's
|
|
|
rozpocznij naukę
|
|
|
|
|
rozpocznij naukę
|
|
obtained when the phase of the signal in cavity is equal the phase
|
|
|
of the signal after transition through whole resonator rozpocznij naukę
|
|
of the signal after transition through whole resonator
|
|
|
rozpocznij naukę
|
|
current at which optical gain of the laser medium equals the
|
|
|
rozpocznij naukę
|
|
|
|
|