Laser system

Claim 3

A method according to claim 1 wherein said generating of said laser beam is carried out in said laser oscillator further comprising a first optical means compensating the thermally-induced optical power of the first solid-state medium.

Claim 4

A laser system comprising in combination a solid state active medium located within an optical resonator, pumping means for exciting said active medium thereby generating laser radiation within said optical resonator, means for coupling out of the resonator part of said radiation as oscillator beam; and a second solid state active medium positioned external to said optical resonator, pumping means for exciting the said second active medium thereby amplifying said oscillator beam to an amplified output beam and means for operating said system over a range of varying pumping power and in a range of repetition rates whereby the pumping by said pumping means induces optical lensing in both active media, of optical power varying between a minimum value φ o min and a maximum value φ o max in the first medium, and a minimum value φ a min and a maximum value φ a max in the second medium; said optical power being a function of the average pumping power which is the product of pulse repetition rate and pumping energy per pulse, depending on pumping power and repetition rate, there being provided compensating means for balancing said lensing, said compensating means comprising a first optical means with an optical power of minus φ o min within said optical resonator, and a second optical means with an optical power of minus φ a max external said optical resonator; the amplified output beam being of essentially constant divergence over the range of pumping power and repetition rates at which the system is operated.

Claim 5

A laser system comprising in combination a solid state active medium located within an optical resonator, pumping means for exciting said active medium thereby generating laser radiation within said optical resonator, means for coupling out of the resonator part of said radiation as oscillator beam; and a second solid state active medium positioned external to said optical resonator, pumping means for exciting the said second active medium thereby amplifying said oscillator beam to an amplified output beam and means for operating said system over a range of varying pumping power and in a range of repetition rates whereby the pumping by said pumping means induces optical lensing in both active media, of optical power varying between a minimum value φ o min and a maximum value φ o max in the first medium, and a minimum value φ a min and a maximum value φ a max in the second medium; said optical power being a function of the average pumping power which is the product of pulse repetition rate and pumping energy per pulse, depending on pumping power and repetition rate, there being provided compensating means for balancing said lensing, said compensating means comprising a first optical means with an optical power of minus φ o min within said optical resonator, and a second optical means with an optical power of minus φ a max external said optical resonator; the amplified output beam being of essentially constant divergence over the range of pumping power and repetition rates at which the system is operated.

Claim 6

A laser system according to claim 3, wherein said oscillator beam passes more than once through said second active medium thereby achieving more amplification and higher output energy.

Claim 7

A laser system according to claim 3, wherein said pumping energies E o and E a of first and second active media respectively are designed to approximately satisfy the condition E.sub.o /E.sub.a.sup.2 ≃(KL/D.sub.o.sup.2)(R.sup.max -R.sup.min) where L is the length of said optical resonator D o is the diameter of said oscillator beam K is a constant characteristic to said active media R min and R max are respectively the lowest and highest repetition rates at which said system is designed to operate.

Claim 8

A laser system according to claim 3, wherein the optical means in the resonator is a lens or a beam expander.

Claim 9

A laser system according to claim 3, wherein optical means external the resonator is a lens or a beam expander.

Claim 10

A laser system according to claim 3, wherein said first and second active media are identical.

Claim 11

A laser system according to claim 8, wherein said first and second active media are enclosed in a common pump cavity using common pumping means for both active media.

Claim 12

A laser system according to claim 9, wherein said first and second optical means approximately satisfy the condition (D.sub.o /D.sub.a).sup.4 ≃L(φ.sup.max -φ.sup.min) where D o is the diameter of said oscillator beam in said first active medium. D a is the diameter of said amplified beam, φ min and φ max are respectively the minimal and maximal values of the optical power induced in said first and second active media.

Claim 13

A laser system according to claim 3, wherein said first and second active media are different regions in a single excited solid-state medium.

Claim 14

A laser system according to claim 4, wherein said first active medium is the central core of said single excited medium and said second active medium is the surrounding annular region of said single excited medium.

Claim 15

A laser system according to claim 11, wherein said first and second optical means approximately satisfy the condition (D.sub.o /D.sub.a).sup.4 ≃L(φ.sup.max -φ.sup.min) where D o is the diameter of said oscillator beam in said first active medium, D a is the diameter of said amplified beam, φ min and φ max are respectively the minimal and maximal values of the optical power induced in said first and second active media.

Claim 16

A laser system comprising in combination a solid state active medium located within an optical resonator, pumping means for exciting said active medium thereby generating laser radiation within said optical resonator, means for coupling out of the resonator part of said radiation as oscillator beam; and a second solid state active medium positioned external to said optical resonator, pumping means for exciting the said second active medium thereby amplifying said oscillator beam to an amplified output beam and means for operating said system over a range of varying pumping power and in a range of repetition rates whereby the pumping by said pumping means induces optical lensing in both active media, of optical power varying between a minimum value φ o min and a maximum value φ o max in the first medium, and φ a min a minimum value φ a max in the second medium; said optical power being a function of the average pumping power which is the product of pulse repetition rate and pumping energy per pulse, depending on pumping power and repetition rate, there being provided compensating means for balancing said lensing, said compensating means comprising a first optical means with an optical power of minus φ a max external said optical resonator; the amplified output beam being of essentially constant divergence over the range of pumping power and repetition rates at which the system is operated.

Claim 17

A laser system comprising in combination a solid state active medium located within an optical resonator, pumping means for exciting said active medium thereby generating laser radiation within said optical resonator, means for coupling out of the resonator part of said radiation as oscillator beam; and a second solid state active medium positioned external to said optical resonator, pumping means for exciting the said second active medium thereby amplifying said oscillator beam to an amplified output beam and means for operating said system over a range of varying pumping power and in a range of repetition rates whereby the pumping by said pumping means induces optical lensing in both active media, of optical power varying between a minimum value φ o min and a maximum value φ o max in the first medium, and φ a min a minimum value φ a max in the second medium; said optical power being a function of the average pumping power which is the product of pulse repetition rate and pumping energy per pulse, depending on pumping power and repetition rate, there being provided compensating means for balancing said lensing, said compensating means comprising a first optical means with an optical power of minus φ a max external said optical resonator; the amplified output beam being of essentially constant divergence over the range of pumping power and repetition rates at which the system is operated.