Laser amplifier system and laser amplifier method
A laser amplification arrangement comprising a laser medium for producing an amplified laser emission as output signal from a useful signal to be amplified and a pump source has a switching component for coupling the useful signal into the laser medium. Laser medium and switching component are formed and arranged so that a division of an input signal (ES) into the useful signal and a background signal is effected, the background signal being passed through the laser medium at a time immediately before and/or after the coupling-in of the useful signal to be amplified.
1. A laser amplification arrangement, in particular for amplifying femtosecond and picosecond pulses, comprising at least
a laser medium for producing an amplified laser emission as output signal (AS), in particular having an average power of more than 10 W or more than 100 W, from a useful signal to be amplified,
a pump source, in particular a laser diode source, for pumping the laser medium,
a switching component for coupling the useful signal into the laser medium,
wherein laser medium and switching component are formed and arranged in such a way that a division of the input signal (ES) into the useful signal and a background signal is effected, in particular with the constant sum of useful signal power and background signal power, the background signal being passed through the laser medium at a time immediately before and/or after the coupling-in of the useful signal to be amplified.
2. The laser amplification arrangement as claimed in claim 1 , wherein laser medium and switching component are formed and arranged in such a way that a saturation state of the laser medium is produced by the background signal, the useful signal being coupled into the laser medium when the saturation state is present.
3. The laser amplification arrangement as claimed in claim 1 , wherein the power of the input signal (ES) can be switched back and fourth either completely or in a ratio between useful signal and background signal.
4. The laser amplification arrangement as claimed in claim 1 , wherein useful signal and background signal can be separated from one another on the basis of angle of emergence, beam direction in the laser medium or polarization.
5. The laser amplification arrangement as claimed in claim 1 , wherein the division of the input signal (ES) is effected by the switching component.
6. The laser amplification arrangement as claimed in claim 5 , wherein the switching component is
an electro-optical modulator,
an acousto-optical modulator in which the zeroth and the first order have different polarizations or
an acousto-optical tunable filter, in particular a collinear one,
useful signal and background signal being separable on the basis of their different polarizations.
7. The laser amplification arrangement as claimed in claim 6 , wherein the laser medium is a polarization-preserving optical fiber.
8. The laser amplification arrangement as claimed in claim 6 , wherein the polarization directions of useful signal and background signal in the laser medium are chosen so that both polarization directions produce an identical saturation effect.
9. The laser amplification arrangement as claimed in claim 6 , wherein the laser medium has a polarization-dependent anisotropy direction and consists of at least two components,
the at least two components being oriented rotated relative to one another and/or
a rotation of the polarization directions of useful signal and background signal being effected between the at least two components.
10. The laser amplification arrangement as claimed in claim 1 , wherein the switching component is
an acousto-optical modulator or
an electro-optical deflector
having at least two switching states with different angles of emergence, the switching states being coordinated in each case with the useful signal and with the background signal, in particular with a downstream half-wave plate and a combination of the beam paths of useful signal and background signal.
11. The laser amplification arrangement as claimed in claim 10 , wherein the acousto-optical modulator or the electro-optical deflector has three switching states, a beam path belonging to one of the three switching states being optically interrupted with respect to the laser medium, in particular by an optical trap.
12. A laser amplification method for an input signal (ES) to be amplified, in particular for amplifying femtosecond or picosecond pulses, comprising at least
optical pumping of a laser medium,
coupling of a useful signal to be amplified into the laser medium,
production of an amplified laser emission as output signal (AS), in particular having an average power of more than 10 W or more than 100 W, by the laser medium,
wherein a division of an input signal (ES) into the useful signal and a background signal is effected, in particular with a constant sum of useful signal power and background signal power, the background signal being passed through the laser medium at a time immediately before and/or after the coupling-in of the useful signal to be amplified.
13. The laser amplification method as claimed in claim 12 , wherein a saturation state of the laser medium is produced by the background signal, the useful signal being coupled into the laser medium when the saturation state is present.
14. The laser amplification method as claimed in claim 12 , wherein the power of the input signal (ES) is switched back and forth either completely or in a ratio between useful signal and background signal.
15. The laser amplification method as claimed in claim 12 , wherein useful signal and background signal are separated from one another on the basis of angle of emergence, beam direction in the laser medium or polarization.