Abstract: The present invention relates to a device for generating laser radiation. A problem addressed by the present invention is that of specifying a device for generating laser radiation using a nonlinear crystal, which device has a simple construction and low optical losses. The device according to the invention comprises an optical amplifier having an active zone, wherein the optical amplifier has a front facet and a rear facet, between which the active zone extends; and a resonator having a first resonator element and a second resonator element, between which the optical amplifier extends, wherein the first resonator element is arranged on a side of the active zone facing away from the front facet and the second resonator element is arranged on a side of the active zone facing the front facet, and wherein the second resonator element comprises a nonlinear crystal having periodic poling.

Abstract: The inventive waveguide structure comprises a first waveguide region having a constant first width adapted to guide electromagnetic waves mode sustainably along its longitudinal axis; a second waveguide region adapted to guide electromagnetic waves mode sustainably along its longitudinal axis, wherein the longitudinal axis of the first waveguide region and the longitudinal axis of the second waveguide region form a common longitudinal axis of the waveguide structure, wherein a first end face of the first waveguide region and a first end face of the second waveguide region are aligned with each other, the width of the first end face of the second waveguide region corresponding to the first width, and the width of the second waveguide region along its longitudinal axis widens from the first end face to a second end face to a second width greater than the first width.

Abstract: The inventive waveguide structure comprises a first waveguide region having a constant first width adapted to guide electromagnetic waves mode sustainably along its longitudinal axis; a second waveguide region adapted to guide electromagnetic waves mode sustainably along its longitudinal axis, wherein the longitudinal axis of the first waveguide region and the longitudinal axis of the second waveguide region form a common longitudinal axis of the waveguide structure, wherein a first end face of the first waveguide region and a first end face of the second waveguide region are aligned with each other, the width of the first end face of the second waveguide region corresponding to the first width, and the width of the second waveguide region along its longitudinal axis widens from the first end face to a second end face to a second width greater than the first width.

Abstract: The invention relates to an optical bank (1) comprising a carrier (10) for receiving optical components (60, 70) and a crystal (30) that is mechanically connected to the carrier, for changing the frequency of the light irradiated into the crystal (30) from a light source (50). Two rails (12) are arranged essentially in parallel on the carrier (10). The crystal (30) and the carrier (10) are mechanically connected by a surface of the rails (12), facing away from the carrier (10). A heat conducting element (20) is arranged on the crystal, said heat conducting element being applied to the surfaces of the rails (12), that face away from the carrier (10).

Abstract: The invention relates to an optical bank (1) comprising a carrier (10) for receiving optical components (60, 70) and a crystal (30) that is mechanically connected to the carrier, for changing the frequency of the light irradiated into the crystal (30) from a light source (50). Two rails (12) are arranged essentially in parallel on the carrier (10). The crystal (30) and the carrier (10) are mechanically connected by a surface of the rails (12), facing away from the carrier (10). A heat conducting element (20) is arranged on the crystal, said heat conducting element being applied to the surfaces of the rails (12), that face away from the carrier (10).