Short-pulse laser device with a preferably passive mode coupling and multiple reflection telescope therefor
The invention relates to a short-pulse laser device ( 11 ) with a preferably passive mode coupling. Said device comprises a resonator ( 12 ) which contains a laser crystal ( 14 ) in addition to several mirrors (M 1 -M 7 , OC) that define a long resonator arm ( 17 ) and a short resonator arm ( 16 ), one (M 1 ) of said mirrors forming a pump beam coupling-in mirror and another (OC) forming a laser beam output coupler and comprising a multiple reflection telescope ( 18 ) that increases the length of the resonator and is allocated to the resonator arms ( 16, 17 ). Said telescope is constructed using mirrors ( 25, 26 ), in order to reflect a laser beam ( 15 ) that is coupled into the space between them back and forth several times, prior to being decoupled back into the other resonator, whereby sequential eccentric reflection points ( 1 to 8; 1 ′ to 8 ′) on the mirrors ( 25, 26 ) are offset in relation to one another. The telescope ( 18 ) comprises only one curved mirror ( 26 ), in addition to a planar mirror ( 25 ), whose position corresponds at least substantially to the center ( 25 ′) of an imaginary multiple reflection assembly comprising two curved mirrors ( 26 a, 26 b ), whereby the one curved mirror ( 26 ) of the telescope ( 18 ) also contains the reflection points of the other imaginary curved mirror. The invention also relates to a multiple reflection telescope ( 18 ) for said device.
1. A short pulse laser device with mode-locking, comprising:
a resonator containing a laser crystal as well as several mirrors which define a long resonator arm as well as a short resonator arm, one of said several mirrors being a pump beam in-coupling mirror, and another of said several mirrors being a laser beam out-coupler, and
a multiple reflection telescope increasing the resonator length and associated with one of the long resonator arm and the short resonator arm, said multiple reflection telescope being constructed using mirrors in order to reflect a laser beam coupled into the space between them back and forth between the mirrors several times before the laser beam is out-coupled back into the remaining resonator, sequential eccentric reflection points on the mirrors being offset relative to one another, wherein the telescope has only one curved mirror and a plane mirror, the position of the plane mirror being substantially midway between a first imaginary curved mirror and a second imaginary curved mirror forming an imaginary multiple reflection arrangement, the one curved mirror of the telescope being located in the position of the first imaginary curved mirror and containing the reflection points of the second imaginary curved mirror.
2. A short pulse laser device according to claim 1 , wherein the curved mirror is a concave mirror.
3. A short-pulse laser device according to claim 1 , wherein on the one curved mirror, reflection points of the one curved mirror and reflection points of the second imaginary curved mirror are alternately arranged on an imaginary circle, each pair of adjacent reflection points being separated by equal arcuate distances on the imaginary circle.
4. A short-pulse laser device according to claim 1 , wherein a total of eight reflection points are provided on the one curved mirror.
5. A short-pulse laser device according to claim 1 , wherein the distance between the one curved mirror and the plane mirror and the radius of curvature of the one curved mirror correspond to a relation L/R=1±√{square root over ((1+cos α)/2)}, wherein
L is twice the distance between the one curved mirror and the plane mirror,
R is the radius of curvature of the one curved mirror, and
α is the central angle between two respective sequential reflection points actually associated to the one curved mirror and located on an imaginary circle.
6. A short-pulse laser device according to claim 5 , wherein the one curved mirror is a concave mirror, for which the relation is:
L/R =1−√{square root over ((1+cos α)/2)}.
7. A short-pulse laser device according to claim 1 , wherein substantially midway between the one curved mirror and the plane mirror, in- and out-coupling mirrors for the laser beam are provided in one of the beam paths between respective reflection points on the one curved mirror and the plane mirror.
8. A short-pulse laser device according to claim 1 , wherein the telescope is associated with the long resonator arm.
9. A short-pulse laser device according to claim 1 , wherein said mode-locking is passive mode-locking.
10. A multiple reflection telescope for a short-pulse laser device, said multiple reflection telescope increasing a resonator length of said short-pulse laser device, said telescope reflecting a laser beam back and forth between the mirrors several times before the laser beam is out-coupled into the short-pulse laser device, sequential eccentric reflection points on the mirrors being offset relative to each other,
wherein said mirrors include only one curved mirror and a plane mirror, the position of the plane mirror being substantially midway between a first imaginary curved mirror and a second imaginary curved mirror forming an imaginary multiple reflection arrangement, the one curved mirror of the telescope being located in the position of the first imaginary curved mirror and also containing the reflection points of the second imaginary curved mirror.
11. A multiple-reflection telescope according to claim 10 , that wherein the curved mirror is a concave mirror.
12. A telescope according to claim 10 , wherein on the one curved mirror reflection points of the one curved mirror and reflection points of the second imaginary curved mirror are alternately arranged on an imaginary circle, each pair of adjacent reflection points being separated by equal arcuate distances on the imaginary circle.
13. A telescope according to claim 10 , wherein a total of eight reflection points are provided on the one curved mirror.
14. A telescope according claim 10 , wherein the distance between the one curved mirror and the plane mirror and the radius of curvature of the one curved mirror correspond to a relation
L/R =1±√{square root over (1+cos α)/2)},
wherein
L is twice the distance between the one curved mirror and the plane mirror,
R is the radius of curvature of the one curved mirror, and
α is the central angle between two respective sequential reflection points actually associated to the one curved mirror and located on an imaginary circle.
15. A telescope according to claim 14 , wherein the one curved mirror is a concave mirror for which the relation is:
L/R =1−√{square root over ((1+cos α)/2)}.
16. A telescope according to claim 13 , wherein substantially midway between the one curved mirror and the plane mirror, in- and out-coupling mirrors for the laser beam are provided in one of the beam paths between respective reflection points on the one curved mirror and the plane mirror.