Semiconductor laser device
The invention relates to a semiconductor laser devcie, including a semiconductor laser element, or a number of individual lasers mounted parallel to each other, with a number of output surfaces, from which laser light can escape, having a treater divergence in a first direction (Y) than in a second direction parallel to the above and at least one reflecting means, at a distance from the output surfaces, outside the semiconductor laser element or the individual laser, with at least one reflective surface which reflects at least a part of the laser light escaping from the semiconductor laser element or the individual lasers through the output surfaces back into the semiconductor laser element or the individual lasers, such that the mode spectrum of the semiconductor laser element or the individual lasers is influenced. The at least one reflective surface of the reflecting means has a concave curve.
1 . A semiconductor laser device comprising a semiconductor laser element or a plurality of individual lasers mounted in parallel with a plurality of exit surfaces from which laser light can emerge which in a first direction (Y) has greater divergence than in the second direction which is perpendicular to it; and at least one reflection means which is located spaced apart from the exit surfaces outside of the semiconductor laser element or of the plurality of individual lasers, with at least one reflecting surface which can reflect back at least parts of the laser light which has emerged from the semiconductor laser element or the plurality of individual lasers through the exit surfaces into the semiconductor laser element or the plurality of individual lasers such that the mode spectrum of the semiconductor laser element or of the individual lasers is influenced thereby; wherein at least one reflecting surface of the reflection means is concavely curved.
2 . The semiconductor laser device as claimed in claim 1 , wherein at least one reflecting surface can reflect back component beams of laser light onto the exit surfaces such that they are used as an aperture.
3 . The semiconductor laser device as claimed in claim 1 , wherein the semiconductor laser device comprises a lens means which is located between the reflection means and the semiconductor laser element or the plurality of individual lasers and which can at least partially reduce the divergence of the laser light at least in the first direction (Y).
4 . The semiconductor laser device as claimed in claim 1 , wherein the at least one reflection means has a reflecting surface on which component beams emerging from different exit surfaces can be reflected.
5 . The semiconductor laser device as claimed in claim 1 , wherein the at least one reflection means has a host of reflecting surfaces which can each reflect the component beams ( 2 a , 2 c ; 3 a , 3 c ; 4 a , 4 c ; 5 a , 5 c ) emerging from the individual exit surfaces ( 2 , 3 , 4 , 5 , 22 , 23 , 24 ).
6 . The semiconductor laser device as claimed in claim 1 , wherein the semiconductor laser device comprises a beam transformation unit which is a beam rotation unit and can rotate individual ones of the component beams at one time, by roughly 90°.
7 . The semiconductor laser device as claimed in claim 6 , wherein the beam transformation unit is located between the at least one reflection means and the semiconductor laser element or the Plurality of individual lasers, between the at least one reflection means and the lens means.
8 . The semiconductor laser device as claimed in claim 1 , wherein the semiconductor laser device further comprises a frequency-doubling element which is located between the at least one reflection means and the semiconductor laser element or the plurality of individual lasers, between the at least one reflection means and the lens means.
9 . The semiconductor laser device as claimed in claim 1 , wherein the semiconductor laser element is exposed to a voltage and is supplied with current for producing electron-hole pairs only in partial areas which correspond to the three-dimensional extension of the desired mode of the laser light.