Device for applying a laser pulse delivered by a laser oscillator

Claim 1

A device for amplifying a laser pulse delivered by a laser oscillator, wherein said device comprises: a light-amplifying medium which is pumped by an auxiliary excitation source and comprises a number of energy levels, one or a number of upper reserve levels, an upper laser level, a lower laser level and one or a number of lower reserve levels, the laser transition being intended to correspond to the laser pulse delivered by the oscillator and to take place between the upper laser level and the lower laser level, a series of mirrors placed around the amplifying medium to reflect said laser pulse from one mirror to the following mirror of the series of mirrors, wherein the mirrors are so arranged as to ensure that the time interval Δt 1 which elapses between two successive passes of the pulse within the same volume of the amplifying medium is longer than the time interval Δt 2 which is necessary for population transfer between on the one hand the upper reserve level or levels and the upper laser level and on the other hand the lower laser level and the lower reserve level or levels, with the result that the amplifying medium is regenerated by population exchange at the lower and upper levels between each traversal of the pulse through said amplifying medium, wherein the amplifying medium is placed between two parallel planes which are perpendicular to an axis Oz and wherein said mirrors are oriented so as to ensure that the path of the light pulse between said mirrors is perpendicular to said axis Oz.

Claim 2

A device for amplifying a laser pulse delivered by a laser oscillator, wherein said device comprises: a light-amplifying medium which is pumped by an auxiliary excitation source and comprises a number of energy levels, one or a number of upper reserve levels, an upper laser level, a lower laser level and one or a number of lower reserve levels, the laser transition being intended to correspond to the laser pulse delivered by the oscillator and to take place between the upper laser level and the lower laser level, a series of mirrors placed around the amplifying medium to reflect said laser pulse from one mirror to the following mirror of the series of mirrors, wherein the mirrors are so arranged as to ensure that the time interval Δt 1 which elapses between two successive passes of the pulse within the same volume of the amplifying medium is longer than the time interval Δt 2 which is necessary for population transfer between on the one hand the upper reserve level or levels and the upper laser level and on the other hand the lower laser level and the lower reserve level or levels, with the result that the amplifying medium is regenerated by population exchange at the lower and upper levels between each traversal of the pulse through said amplifying medium, wherein the amplifying medium is placed between two parallel planes which are perpendicular to an axis Oz and wherein said mirrors are oriented so as to ensure that the path of the light pulse between said mirrors is perpendicular to said axis Oz.

Claim 3

A device for amplifying a laser pulse delivered by a laser oscillator, wherein said device comprises: a light-amplifying medium which is pumped by an auxiliary excitation source and comprises a number of energy levels, one or a number of upper reserve levels, an upper laser level, a lower laser level and one or a number of lower reserve levels, the laser transition being intended to correspond to the laser pulse delivered by the oscillator and to take place between the upper laser level and the lower laser level, a series of mirrors placed around the amplifying medium to reflect said laser pulse from one mirror to the following mirror of the series of mirrors, wherein the mirrors are so arranged as to ensure that the time interval Δt 1 which elapses between two successive passes of the pulse within the same volume of the amplifying medium is longer than the time interval Δt 2 which is necessary for population transfer between on the one hand the upper reserve level or levels and the upper laser level and on the other hand the lower laser level and the lower reserve level or levels, with the result that the amplifying medium is regenerated by population exchange at the lower and upper levels between each traversal of the pulse through said amplifying medium, wherein the amplifying medium is in the shape of a cylinder having an axis of revolution Oz, wherein the width of the laser beam in a plane Oxy perpendicular to the axis Oz is approximately equal to the radius of the circular section of the amplifying medium in the same plane Oxy, wherein the series of mirrors includes n mirrors, M 1 , M 2 . . . M i , . . . M n , of substantially rectangular shape which are disposed annularly at a uniform angular interval around the amplifying medium, the planes of said mirrors being parallel to the axis Oz, wherein the amplifying medium is so arranged that the beam issuing from the laser oscillator passes substantially through a first half of the volume of the amplifying medium, wherein the first mirror M 1 is so oriented as to reflect the beam issuing from the oscillator to the mirror M 2 after passing through the second half of the volume of the amplifying medium, the beam being reflected from the mirror M 2 onto the mirror M 3 after passing through another half of the amplifying medium, said beam being reflected from the mirror M i having an order i to the mirror M i+1 onto the mirror M i+2 after passing through a second half of the amplifying medium, the beam which has thus been amplified being reflected to the exterior from the last exit mirror M n after passing through the amplifying medium.

Claim 4

A device for amplifying a laser pulse delivered by a laser oscillator, wherein said device comprises: a light-amplifying medium which is pumped by an auxiliary excitation source and comprises a number of energy levels, one or a number of upper reserve levels, an upper laser level, a lower laser level and one or a number of lower reserve levels, the laser transition being intended to correspond to the laser pulse delivered by the oscillator and to take place between the upper laser level and the lower laser level, a series of mirrors placed around the amplifying medium to reflect said laser pulse from one mirror to the following mirror of the series of mirrors, wherein the mirrors are so arranged as to ensure that the time interval Δt 1 which elapses between two successive passes of the pulse within the same volume of the amplifying medium is longer than the time interval Δt 2 which is necessary for population transfer between on the one hand the upper reserve level or levels and the upper laser level and on the other hand the lower laser level and the lower reserve level or levels, with the result that the amplifying medium is regenerated by population exchange at the lower and upper levels between each traversal of the pulse through said amplifying medium, wherein the amplifying medium is in the shape of a cylinder having an axis of revolution Oz, wherein the width of the laser beam in a plane Oxy perpendicular to the axis Oz is approximately equal to the radius of the circular section of the amplifying medium in the same plane Oxy, wherein the series of mirrors includes n mirrors, M 1 , M 2 . . . M i , . . . M n , of substantially rectangular shape which are disposed annularly at a uniform angular interval around the amplifying medium, the planes of said mirrors being parallel to the axis Oz, wherein the amplifying medium is so arranged that the beam issuing from the laser oscillator passes substantially through a first half of the volume of the amplifying medium, wherein the first mirror M 1 is so oriented as to reflect the beam issuing from the oscillator to the mirror M 2 after passing through the second half of the volume of the amplifying medium, the beam being reflected from the mirror M 2 onto the mirror M 3 after passing through another half of the amplifying medium, said beam being reflected from the mirror M i having an order i to the mirror M i+1 onto the mirror M i+2 after passing through a second half of the amplifying medium, the beam which has thus been amplified being reflected to the exterior from the last exit mirror M n after passing through the amplifying medium.

Claim 5

A device for amplifying a laser pulse delivered by a laser oscillator, wherein said device comprises: a light-amplifying medium which is pumped by an auxiliary excitation source and comprises a number of energy levels, one or a number of upper reserve levels, an upper laser level, a lower laser level and one or a number of lower reserve levels, the laser transition being intended to correspond to the laser pulse delivered by the oscillator and to take place between the upper laser level and the lower laser level, a series of mirrors placed around the amplifying medium to reflect said laser pulse from one mirror to the following mirror of the series of mirrors, wherein the mirrors are so arranged as to ensure that the time interval Δt 1 which elapses between two successive passes of the pulse within the same volume of the amplifying medium is longer than the time interval Δt 2 which is necessary for population transfer between on the one hand the upper reserve level or levels and the upper laser level and on the other hand the lower laser level and the lower reserve level or levels, with the result that the amplifying medium is regenerated by population exchange at the lower and upper levels between each traversal of the pulse through said amplifying medium, wherein the amplifying medium is of cylindrical shape having an axis Oz wherein, in a plane Oxy perpendicular to the axis Oz, the width of the laser beam emitted by the laser oscillator is substantially equal to the diameter of the circular cross-section of the amplifying medium in the same plane Oxy, wherein the device comprises n rectangular mirrors M 1 , M 2 . . . M i , . . . M n disposed at uniform angular intervals around the amplifying medium, the plane of said mirrors being parallel to the axis Oz, wherein the amplifying medium is so arranged that the beam issuing from the laser oscillator passes through the volume of the amplifying medium, wherein the first mirror M 1 is oriented so as to reflect the beam issuing from the oscillator to the mirror M 2 but does not pass through the amplifying medium between the mirrors M 1 and M 2 , the beam being reflected from the mirror M 2 onto the mirror M 3 after passing through practically the entire amplifying medium, said beam being reflected from the mirror M i to the mirror M i+1 after passing through the volume of the amplifying medium and said beam being reflected from the mirror M i+1 onto the mirror M i+2 but does not pass through the amplifying medium between the mirror M i+1 and the mirror M i+2 , the amplified beam being reflected from the last exit mirror M n after a final pass through the amplifying medium.

Claim 6

A device for amplifying a laser pulse delivered by a laser oscillator, wherein said device comprises: a light-amplifying medium which is pumped by an auxiliary excitation source and comprises a number of energy levels, one or a number of upper reserve levels, an upper laser level, a lower laser level and one or a number of lower reserve levels, the laser transition being intended to correspond to the laser pulse delivered by the oscillator and to take place between the upper laser level and the lower laser level, a series of mirrors placed around the amplifying medium to reflect said laser pulse from one mirror to the following mirror of the series of mirrors, wherein the mirrors are so arranged as to ensure that the time interval Δt 1 which elapses between two successive passes of the pulse within the same volume of the amplifying medium is longer than the time interval Δt 2 which is necessary for population transfer between on the one hand the upper reserve level or levels and the upper laser level and on the other hand the lower laser level and the lower reserve level or levels, with the result that the amplifying medium is regenerated by population exchange at the lower and upper levels between each traversal of the pulse through said amplifying medium, wherein the amplifying medium is of cylindrical shape having an axis Oz wherein, in a plane Oxy perpendicular to the axis Oz, the width of the laser beam emitted by the laser oscillator is substantially equal to the diameter of the circular cross-section of the amplifying medium in the same plane Oxy, wherein the device comprises n rectangular mirrors M 1 , M 2 . . . M i , . . . M n disposed at uniform angular intervals around the amplifying medium, the plane of said mirrors being parallel to the axis Oz, wherein the amplifying medium is so arranged that the beam issuing from the laser oscillator passes through the volume of the amplifying medium, wherein the first mirror M 1 is oriented so as to reflect the beam issuing from the oscillator to the mirror M 2 but does not pass through the amplifying medium between the mirrors M 1 and M 2 , the beam being reflected from the mirror M 2 onto the mirror M 3 after passing through practically the entire amplifying medium, said beam being reflected from the mirror M i to the mirror M i+1 after passing through the volume of the amplifying medium and said beam being reflected from the mirror M i+1 onto the mirror M i+2 but does not pass through the amplifying medium between the mirror M i+1 and the mirror M i+2 , the amplified beam being reflected from the last exit mirror M n after a final pass through the amplifying medium.