Non-return optical faraday effect system and application to a laser amplifier

Claim 2

In a non-return optical system, comprising: a number of plates having parallel faces made of a material having a Verdet constant, and means for setting up a magnetic field crossing the faces of these plates with a first plate directed, in relation to a laser beam, such that the angle of incidence be close to the Brewster angle, the improvement wherein: the planes of the various other plates are set in directions such that, on the one hand, the angle of incidence of the laser beam received on each plate is close to the Brewster angle and that, on the other hand, the angle between the normal to the plane of that plate and the normal to the plane of the plate situated upstream thereof is equal to the angle of rotation of the vector of polarization of said laser beam in crossing said upstream plate owing to the Faraday effect, and wherein; the number of plates, the material of which they are made, their thickness and the value of the magnetic field is chosen such that the total rotation angle undergone by the laser beam polarization vector between the input of the system and the output is approximately 45°.

Claim 3

In a laser amplifier including a non-return optical device comprising: a number of plates having parallel faces made of a material having a Verdet constant and means for setting up a magnetic field crossing the faces of these plates with a first plate directed, in relation to a laser beam such that the angle of incidence be close to the Brewster angle, the improvement wherein: the planes of the various other plates are set in such directions that, on the one hand, the angle of incidence of the beam received on each plate is close to the Brewster angle and that, on the other hand, the angle between the normal to the plane of that plate and the normal to the plane of the plate situated upstream thereof, be equal to the angle through which the laser beam polarization vector has been rotated owing to the Faraday effect of the laser beam crossing said upstream plate; and wherein, the number of plates, the material of which they are made, their thickness and the value of the magnetic field is such that the total rotation undergone by the polarization vector of the light between the input of the system and the output is approximately 45°; and wherein said plates are made of an active laser material and said system is provided with means for exciting said active material.

Claim 4

In a laser amplifier including a non-return optical device comprising: a number of plates having parallel faces made of a material having a Verdet constant and means for setting up a magnetic field crossing the faces of these plates with a first plate directed, in relation to a laser beam such that the angle of incidence be close to the Brewster angle, the improvement wherein: the planes of the various other plates are set in such directions that, on the one hand, the angle of incidence of the beam received on each plate is close to the Brewster angle and that, on the other hand, the angle between the normal to the plane of that plate and the normal to the plane of the plate situated upstream thereof, be equal to the angle through which the laser beam polarization vector has been rotated owing to the Faraday effect of the laser beam crossing said upstream plate; and wherein, the number of plates, the material of which they are made, their thickness and the value of the magnetic field is such that the total rotation undergone by the polarization vector of the light between the input of the system and the output is approximately 45°; and wherein said plates are made of an active laser material and said system is provided with means for exciting said active material.