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A commonly used device to achieve this is a saturable absorber.
The option of non-linear (saturable) protein binding is also included.
Once saturated, the inductance of the saturable reactor drops dramatically.
In particular, as it has no bandgap, its saturable absorption is wavelength independent.
Saturable reactor amplifiers were used for control of power to industrial furnaces.
Then, the saturable absorption can be written as follows:
A saturable absorber is an optical device that exhibits an intensity-dependent transmission.
Saturable absorber is widely used in passively mode locking lasers.
Of others, their awake-consciousness is aware of more than one entity and obtain ecstasy by saturable desire.
Saturable absorption has been demonstrated for X-rays.
As enzyme-catalysed reactions are saturable, their rate of catalysis does not show a linear response to increasing substrate.
Most materials show some saturable absorption, but often only at very high optical intensities (close to the optical damage).
In this case, the Q-switch is a saturable absorber, a material whose transmission increases when the intensity of light exceeds some threshold.
Saturable absorbers are useful in laser cavities.
The limited availability of CYP2D6 means perhexiline metabolism is a saturable process.
Free pantothenic acid is absorbed into intestinal cells via a saturable, sodium-dependent active transport system.
This nonlinear optical behavior is termed saturable absorption and the threshold value is called the saturation fluency.
Saturable absorbers are commonly liquid organic dyes, but they can also be made from doped crystals and semiconductors.
This terminal phase probably represents saturable binding to ACE and is not proportional to dose.
Reset of the saturable reactor usually places a minimum off time requirement on GTO based circuits.
Saturable absorption is a property of materials where the absorption of light decreases with increasing light intensity.
In rolled-up graphene sheets (carbon nanotubes), saturable absorption is dependent on diameter and chirality.
When placed in a laser cavity, a saturable absorber will attenuate low-intensity constant wave light (pulse wings).
However, this assumption is sometimes modified to include a saturable response that follows Michaelis-Menten kinetics or a related model called a Hill equation.
The pulse repetition rate can only indirectly be controlled, e.g. by varying the laser's pump power and the amount of saturable absorber in the cavity.