Simple Zero-Q-transforming (ZQT) multi-pass cells for optical applications
This invention comprises a Zero-Q-Transforming (ZQT) multi-pass cell (MPC) of a defined type, comprising a pair of concave high-reflectivity mirrors facing each other and separated by a specified distance. The defined cell is of the type such that the circulating beam forms a closed path inside the cell. A means of coupling light in and out of the cell is defined that uses a single mirror in an arrangement that delivers a beam to the output which has the same properties as the input beam and is aligned along the same path as the input beam. The defined coupling method allows the creation of an MPC where the exact path of the light inside the cell has no effect on the properties of the output beam making it highly tolerant of alignment.
1 . A method for coupling light in and out of a Herriott-type multi-pass optical cell, wherein the Herriott-type multi-pass optical cell comprises a pair of end mirrors, an input Gaussian beam into the Herriott-type multi-pass optical cell, an internal beam path, an output beam out of the Herriott-type multi-pass optical cell, and a single coupling mirror:
wherein the Herriott-type multi-pass optical cell is Zero-Q-Transforming for the input Gaussian laser beam so that the Herriott-type multi-pass cell is now a Zero-Q-Transforming Herriott-type multi-pass cell, such that a phase front of the output beam has a same size and radius of curvature as the input Gaussian beam;
wherein the Zero-Q-Transforming Herriott-type multi-pass cell is of a Complete type, such that the internal beam path circulating inside the Zero-Q-Transforming Herriott-type multi-pass cell forms a closed path; and
wherein the output beam emerges from the Zero-Q-Transforming Herriott-type multi-pass cell in the same direction and in substantially the same position as the input Gaussian beam.
2 . The method of claim 1 , wherein the coupling mirror is located approximately ¼ or ¾ of the distance between the end mirrors of the Zero-Q-Transforming Herriott-type multi-pass cell.
3 . The method of claim 1 , wherein the properties of the output beam emerging from the Zero-Q-Transforming Herriott-type multi-pass cell is indistinguishable from the input Gaussian beam.
4 . The method of claim 1 , wherein the exact beam path inside the Zero-Q-Transforming Herriott-type multi-pass cell does not change the position, direction or properties of the output beam.
5 . The method of claim 1 , wherein the exact direction that the coupling mirror directs the input Gaussian beam into the Zero-Q-Transforming Herriott-type multi-pass cell does not affect the position, direction or properties of the output beam.
6 . The method of claim 1 , further comprising the step wherein a correct separation of the end mirrors of the Zero-Q-Transforming Herriott-type multi-pass cell can be ascertained by adjusting the end mirror separation until the output beam is aligned to the direction defined by the input Gaussian beam were the coupling mirror to be removed.
7 . The method of claim 1 , wherein the Zero-Q-Transforming Herriott-type multi-pass cell is used for long path spectroscopy.
8 . The method of claim 1 , wherein the Zero-Q-Transforming Herriott-type multi-pass cell is used to extend a length of a laser resonator.
9 . The method of claim 1 , wherein the Zero-Q-Transforming Herriott-type multi-pass cell is used in an optical delay line.
10 . The method of claim 1 , wherein the Zero-Q-Transforming Herriott-type multi-pass cell is used in a nonlinear optical pulse compressor for ultrashort pulse lasers.