Illumination device and its use
View Patent ↗To provide an illumination beam ( 5 ) which is essentially homogeneous in cross-section, in particular for a laser scanning microscope ( 15 ), an illumination device is used which provides an original beam which is essentially rotationally symmetric in cross-section and is incident at a converting unit which then transmits the desired illumination beam ( 5 ) and which comprises, for this purpose, an aspherical, convex mirror ( 1 ) which is more strongly curved in the area of the point of incidence of the original beam ( 3 ) than in the areas removed from the point of incidence.
1. An illumination device for use in a laser scanning microscope to provide a profiled illumination beam that is essentially homogeneous in at least one cross-sectional direction, the illuminating device comprising:
means for transmitting an original beam which is inhomogeneous in cross-section and which has a point of incidence, and
a mirror for expanding the original beam, the mirror being more strongly curved in the area of the point of incidence of the original beam than in the areas removed from the point of incidence to provide a profiled illumination beam that is essentially homogeneous in at least one cross-sectional direction,
wherein the surface of the mirror has a top and the surface satisfies in Cartesian (x, y, z)-coordinates y 2 /[c+(c 2 −(1+Q)y 2 ) 1/2 ], where c is a radius of curvature of the top and Q is the conical constant, and
wherein the mirror satisfies the equation f(x,y)=√{square root over ((a(y)−r x ) 2 −x 2 )}−r x , where r x is the radius of curvature along the longitudinal axis of the top and a(y) is the function of y 2 /[c+(c 2 −(1+Q)y 2 ) 1/2 ].
2. The illumination device according to claim 1 wherein the inhomogeneneous cross-section is Gaussian-shaped.
3. The illumination device according to claim 1 , wherein the mirror has an axis of symmetry that lies at an angle between 4° and 20° to the axis of incidence (OA) of the original beam.
4. The illumination device according to claim 1 , wherein the mirror is one of an aspherical mirror, a convex mirror, and a concave mirror.
5. The illumination device according to claim 4 , wherein the mirror is an aspherical mirror and is formed as a wedge and with a rounded top.
6. The illumination device according to claim 5 , wherein the surface of the mirror is curved in addition along the longitudinal axis of the top.
7. The illumination device according to claim 4 , wherein the mirror is an aspherical mirror and a second mirror is disposed behind the aspherical mirror.
8. The illumination device according to claim 7 , wherein the second mirror is one of cylindrical and toroidal.
9. The illumination device according to claim 7 , wherein the second mirror in the x-direction has a radius of curvature equal to (r x +2·d), where d is the distance between the aspherical mirror and the second mirror.
10. Use of the illumination device of claim 1 for at least one of:
studying dynamic processes in the range of a tenth of a second up to 1 hour range, at the level of united cell structures and entire organisms;
representing small motile structures with high speed;
representing very small structures with high speed for the resolution of submolecular structures; and
studying neurophysiological processes with high temporal resolution within muscle or nerve systems.
11. Use of the illumination device according to claim 10 , wherein the very small structures are represented using FRET with region of interest bleaching.
12. A laser scanning microscope comprising:
means for transmitting an original beam which is inhomogeneous in cross-section and which has a point of incidence, and
a mirror for expanding the original beam, the mirror being more strongly curved in the area of the point of incidence of the original beam than in the areas removed from the point of incidence to provide a profiled illumination beam that is essentially homogeneous in at least one cross-sectional direction,
wherein the surface of the mirror has a top and the surface satisfies in Cartesian (x, y, z)-coordinates y 2 /[c+(c 2 −(1+Q)y 2 ) 1/2 ], where c is a radius of curvature of the top and Q is the conical constant, and
wherein the mirror satisfies the equation f(x,y)=√{square root over ((a(y)−r x ) 2 −x 2 )}−r x , where r x is the radius of curvature along the longitudinal axis of the top and a(y) is the function of y 2 /[c+(c 2 −(1+Q)y 2 ) 1/2 ].
13. The laser scanning microscope according to claim 12 , wherein the microscope has sampling in the form of a line.
14. An illumination device for use in a laser scanning microscope with sampling in the form of a line, comprising:
means for transmitting an original beam which is inhomogeneous in cross-section, and
a mirror for expanding the original beam, the mirror being more strongly curved in the area of the point of incidence of the original beam than in the areas removed from the point of incidence to provide a profiled illumination beam that is essentially homogeneous in at least one cross-sectional direction,
wherein the surface of the mirror has a top and the surface satisfies in Cartesian (x, y, z)-coordinates y 2 /[c+(c 2 −(1+Q)y 2 ) 1/2 ], where c is a radius of curvature of the top and Q is the conical constant, and
wherein the mirror satisfies the equation f(x,y)=√{square root over ((a(y)−r x ) 2 −x 2 )}−r x , where r x is the radius of curvature along the longitudinal axis of the top and a(y) is the function of y 2 /[c+(c 2 −(1+Q)y 2 ) 1/2 ].
15. The illumination device according to claim 14 , wherein the inhomogeneneous cross-section is Gaussian-shaped.
16. The illumination device according to claim 14 , wherein the mirror has an axis of symmetry that lies at an angle between 4° and 20° to the axis of incidence (OA) of the original beam.
17. Use of the illumination device of claim 14 for at least one of:
studying dynamic processes in the range of a tenth of a second up to 1 hour range, at the level of united cell structures and entire organisms;
representing small motile structures with high speed;
representing very small structures with high speed for the resolution of submolecular structures; and
studying neurophysiological processes with high temporal resolution within muscle or nerve systems.
18. Process for studying internal cellular transport processes, comprising the steps of:
utilizing the illumination device of claim 14 to represent small motile structures with high speed.
19. The illumination device according to claim 14 , wherein the mirror is one of an aspherical mirror, a convex mirror, and a concave mirror.
20. The illumination device according to claim 19 , wherein the mirror is an aspherical mirror and is formed as a wedge and with a rounded top.
21. The illumination device according to claim 20 , wherein the surface of the mirror is curved in addition along the longitudinal axis of the top.
22. The illumination device according to claim 19 , wherein the mirror is an aspherical mirror and a second mirror is disposed behind the aspherical mirror.
23. The illumination device according to claim 22 , wherein the second mirror is one of cylindrical and toroidal.
24. The illumination device according to claim 22 , wherein the second mirror in the x-direction has a radius of curvature equal to (r x +2·d), where d is the distance between the aspherical mirror and the second mirror.