Optical system having aberrations for transforming a Gaussian laser-beam intensity profile to a quasi-flat-topped intensity profile in a focal region of the optical system
View Patent ↗An optical system is configured for projecting an image having a quasi-flat-topped intensity profile from a laser-beam having a Gaussian intensity profile. The optical system includes a diffraction limited lens for focusing the laser beam and one or more optical elements that introduce aberration into the beam before the beam is focused. The aberration introduced causes the Gaussian intensity profile to be changed to the quasi-flat-topped intensity profile at some position in a focal region of the diffraction-limited lens.
1. Optical apparatus, comprising:
an optical system arranged to receive a laser-beam, said laser-beam having a substantially Gaussian intensity profile, said optical system including a substantially diffraction-limited lens having a longitudinal optical axis and arranged to focus said laser-beam into a focal region having a depth extending parallel to said optical axis, wherein said focal region extends axially plus and minus four Rayleigh ranges of the focused laser beam from a nominal focal plane of said diffraction-limited lens; and
wherein said optical system further includes one or more optical elements configured to introduce one or more optical aberrations into said laser-beam before said laser-beam is focused into the focal region by the diffraction-limited lens, the extent of said one or more optical aberrations introduced by said one or more aberration-introducing elements being arranged such that the intensity profile of the focused laser-beam is quasi-flat-topped at one or more paraxial positions in said focal region.
2. The apparatus of claim 1 , wherein none of said one or more aberration-introducing optical elements is an aspheric optical element.
3. The apparatus of claim 1 , wherein said one optical element has a spherical surface.
4. The apparatus of claim 1 , wherein said one or more aberration-introducing optical elements introduce third-order spherical aberration.
5. The apparatus of claim 1 , wherein said laser beam received by said optical system is a substantially collimated laser-beam.
6. The apparatus of claim 5 , wherein there are first and second aberration-introducing optical elements arranged to afocally increase the diameter of the laser-beam, said elements being numbered in the direction of propagation of the laser-beam.
7. The apparatus of claim 6 , wherein said first optical element has negative optical power and said second optical element has positive optical power.
8. The apparatus of claim 7 , wherein said first optical element has a plane first surface and a concave second surface and the other of said elements has a convex first surface and a plane second surface said surfaces of said elements being numbered in the direction of propagation of the laser-beam.
9. Optical apparatus, comprising:
an optical system arranged to receive a substantially collimated laser-beam, said laser-beam having a substantially Gaussian intensity profile, said optical system including a substantially diffraction-limited lens having a longitudinal optical axis and arranged to focus said laser-beam into a focal region having a depth extending parallel to said optical axis; and
wherein said optical system further includes at least two optical elements configured to introduce one or more optical aberrations into said laser-beam before said laser-beam is focused into the focal region by the diffraction-limited lens, the extent of said one or more optical aberrations introduced by said at least two aberration-introducing elements being arranged such that the intensity profile of the focused laser-beam is quasi-flat-topped at one or more paraxial positions in said focal region,
wherein there are first and second aberration-introducing optical elements arranged to afocally increase the diameter of the laser-beam, said elements being numbered in the direction of propagation of the laser-beam, and
wherein each of said first and second optical elements has positive optical power, the power of said first optical element being greater than the power of said second optical element, and wherein said first and second optical elements are axially spaced apart such that the laser-beam has an intermediate focus therebetween.
10. The apparatus of claim 9 , wherein said first optical element has a plane first surface and a convex second surface and said second optical element has a convex first surface and a plane second surface, said surfaces being numbered in the direction of propagation of the laser-beam.
11. Optical apparatus, comprising:
an optical system arranged to receive a substantially collimated laser-beam, said laser-beam having a substantially Gaussian intensity profile, said optical system including a substantially diffraction-limited lens having a longitudinal optical axis and arranged to focus said laser-beam into a focal region having a depth extending parallel to said optical axis;
wherein said optical system further includes at least two optical elements configured to introduce one or more optical aberrations into said laser-beam before said laser-beam is focused into the focal region by the diffraction-limited lens, the extent of said one or more optical aberrations introduced by said at least two aberration-introducing elements being arranged such that the intensity profile of the focused laser-beam is quasi-flat-topped at one or more paraxial positions in said focal region, and
wherein there are first and second aberration-introducing optical elements arranged to afocally decrease the diameter of the laser-beam, said elements being numbered in the direction of propagation of the laser-beam.
12. The apparatus of claim 11 , wherein said first optical element has positive optical power and said second optical element has negative optical power.
13. The apparatus of claim 12 wherein said first optical element has a plane first surface and a convex second surface and the other of said elements has a concave first surface and a plane second surface, said surfaces of said elements being numbered in the direction of propagation of the laser-beam.
14. Optical apparatus, comprising:
an optical system arranged to receive a substantially collimated laser-beam, said laser-beam having a substantially Gaussian intensity profile, said optical system including a substantially diffraction-limited lens having a longitudinal optical axis and arranged to focus said laser-beam into a focal region having a depth extending parallel to said optical axis;
wherein said optical system further includes at least two optical elements configured to introduce one or more optical aberrations into said laser-beam before said laser-beam is focused into the focal region by the diffraction-limited lens, the extent of said one or more optical aberrations introduced by said at least two aberration-introducing elements being arranged such that the intensity profile of the focused laser-beam is quasi-flat-topped at one or more paraxial positions in said focal region,
wherein there are first and second aberration-introducing optical elements arranged to afocally increase the diameter of the laser-beam, said elements being numbered in the direction of propagation of the laser-beam, and
wherein each of said first and second optical elements has positive optical power, the power of said first optical element being less than the power of said second optical element, and wherein said first and second optical elements are axially spaced apart such that the laser-beam has an intermediate focus therebetween.
15. The apparatus of claim 14 , wherein said first optical element has a plane first surface and a convex second surface and said second optical element has a convex first surface and a plane second surface, said surfaces being numbered in the direction of propagation of the laser-beam.
16. The apparatus of claim 5 , wherein there are first and second optical elements numbered in the direction of propagation of the laser beam and said first and second optical elements have equal positive optical power and are axially spaced apart to form a unit-magnification optical relay.
17. The apparatus of claim 16 wherein said first optical element has a plane first surface and a convex second surface and said second optical element has a convex first surface and a plane second surface, said surfaces being numbered in the direction of propagation of the laser-beam.
18. The apparatus of claim 1 , wherein said laser-beam is received as a diverging laser beam and there is only one aberration introducing optical element configured and arranged to collimate the laser beam before the laser-beam is focused by said diffraction limited-lens.
19. Optical apparatus, comprising:
an optical system arranged to receive a laser-beam, said laser-beam having a substantially Gaussian intensity profile, said optical system including a substantially diffraction-limited lens having a longitudinal optical axis and arranged to focus said laser-beam into a focal region having a depth extending parallel to said optical axis;
wherein said optical system further includes one or more optical elements configured to introduce one or more optical aberrations into said laser-beam before said laser-beam is focused into the focal region by the diffraction-limited lens, the extent of said one or more optical aberrations introduced by said one or more aberration-introducing elements being arranged such that the intensity profile of the focused laser-beam is quasi-flat-topped at one or more paraxial positions in said focal region; and
a beam displacing device located between said one or more aberration-introducing elements and said diffraction-limited lens for selectively directing said laser-beam into said diffraction-limited lens such that said laser-beam can be provided at selectively different positions transverse to said optical axis of said diffraction-limited lens.
20. The apparatus of claim 19 , wherein said beam displacing device is a tiltable mirror arranged to turn the laser beam from the aberration elements through a range of angles about the optical axis of said diffraction-limited lens.
21. Optical apparatus, comprising:
an optical system arranged to receive a laser-beam, said optical system including a substantially diffraction-limited lens having a longitudinal optical axis and arranged to focus said laser-beam to form an image in a focal region having a depth extending parallel to said optical axis of said diffraction-limited lens;
said optical system further including one or more optical elements configured to introduce one or more optical aberrations into said laser-beam before said laser-beam is focused into the focal region by the diffraction-limited lens, the extent of said one or more optical aberrations introduced by said one or more aberration-introducing elements being arranged such that said image has a quasi-flat-topped radial intensity profile; and
a beam displacing device located between said one or more aberration-introducing elements and said diffraction-limited lens for selectively directing said laser-beam into said diffraction-limited lens such that said image can be provided at selectively different positions in said focal region transverse to said optical axis of said diffraction-limited lens.
22. The apparatus of claim 21 , wherein said beam displacing device is a tiltable mirror arranged to turn the laser beam from the aberration elements through a range of angles about the optical axis of said diffraction-limited lens.
23. The apparatus of claim 21 , wherein said focal region extends axially plus and minus four Rayleigh ranges of the focused laser beam from a nominal focal plane of said diffraction-limited lens.
24. Optical apparatus, comprising:
an optical system arranged to receive a substantially collimated laser-beam, said laser-beam having a substantially Gaussian intensity profile;
said optical system including a substantially diffraction-limited lens having a longitudinal optical axis and arranged to focus said laser-beam into a focal region having a depth extending parallel to said optical axis; and first and second optical elements configured to introduce one or more optical aberrations into said laser-beam before said laser-beam is focused into the focal region by the diffraction-limited lens;
said first and second optical elements being numbered in the direction of propagation of said laser beam and each including first and second surfaces said first and second surfaces being numbered in the direction of propagation of said laser beam; and
wherein said first and second surfaces of said first element are respectively plane and spherical convex, said first and second surfaces of said second element are respectively spherical concave and plane and, and the extent of said one or more optical aberrations introduced by said first and second optical elements is arranged such that the intensity profile of the focused laser-beam is quasi-flat-topped at one or more paraxial positions in said focal region.
25. The apparatus of claim 24 , wherein said aberrations include third-order spherical aberration.
26. Optical apparatus, comprising:
an optical source of a diverging laser-beam having a substantially Gaussian intensity profile;
an optical system arranged to receive the diverging laser-beam;
said optical system including a substantially diffraction-limited lens having a longitudinal optical axis and arranged to focus said laser-beam into a focal region having a depth extending parallel to said optical axis; an optical element configured to collimate the diverging laser beam and to introduce one or more optical aberrations into said laser-beam before said laser-beam is focused into the focal region by the diffraction-limited lens; and
wherein said laser-beam-collimating and aberration-introducing optical element does not include an aspheric surface and said one or more optical aberrations are arranged such that the intensity profile of the focused laser-beam is quasi-flat-topped at one or more paraxial positions in said focal region.
27. The apparatus of claim 26 , wherein said aberrations include third-order spherical aberration.
28. The apparatus of claim 26 wherein said laser-beam-collimating and aberration-introducing optical element has one plane surface and one convex surface.
29. The apparatus of claim 26 wherein said diverging laser beam is delivered from a laser via an optical fiber.
30. The apparatus of claim 26 wherein said diverging laser beam is delivered by a fiber laser.