Ultrashort seed-pulse generating laser with integral pulse shaping
View Patent ↗An ultrafast laser for delivering ultra-short duration seed-pulses for further amplification has a resonator including negative group delay dispersion (NGDD) mirrors for minimizing increases in the duration of the pulses due to positive group delay dispersion effects inherent in the resonator. The NGDD mirrors could be configured such that the pulses had a Gaussian spectrum. Instead, however, the NGDD mirrors are configured and arranged such the pulses have a non-Gaussian spectrum. The non-Gaussian spectrum has a FWHM bandwidth significantly greater than that of the Gaussian spectrum.
1. A laser comprising:
a laser resonator terminated by first and second mirrors;
a gain-element located in the laser resonator;
an arrangement for optically pumping the gain-element, the optical pumping causing fundamental radiation to circulate in the laser-resonator;
the laser resonator being folded by a plurality of fold-mirrors on which the circulating radiation is incident at a non-normal angle of incidence, selected ones of the fold-mirrors being coated with one of a plurality of multilayer coating designs, each thereof arranged to impart a predetermined group delay dispersion (GDD) as a function of wavelength to the fundamental radiation incident thereon at a predetermined angle of incidence thereon, the fundamental radiation having a spectrum dependent on the resonator configuration, the gain-element, and the GDD imparted by each of the selected ones of the fold-mirrors; and
wherein the GDD as a function of wavelength of each of the selected ones of the fold-mirrors and the angle of incidence of circulating radiation on each of the selected ones of the fold-mirrors are selected such that the spectrum of the circulating radiation has one of first and second non-Gaussian forms, the first form characterized as having one of a region of about uniform intensity with intensity falling to zero on either side of the region, and the second form characterized as having at least two intensity peaks with an intensity trough therebetween.
2. The laser of claim 1 , wherein the GDD as a function of wavelength of each of the selected ones of the fold-mirrors and the angle of incidence of circulating radiation on each of the selected ones of the fold-mirrors could be selected such that the spectrum of the circulating radiation had an about Gaussian form, but are not so selected, and wherein the non-Gaussian forms of the spectrum of the circulating radiation have a FWHM bandwidth at least about 25% greater than the about Gaussian form.
3. The laser of claim 1 , wherein the spectrum of the circulating radiation is of the first form.
4. The laser of claim 3 , wherein the spectrum of the circulating radiation approximates a super-Gaussian of order two or greater.
5. The laser of claim 1 , wherein the spectrum of the circulating radiation is of the second form and has only two intensity peaks having an intensity trough therebetween.
6. The laser of claim 1 , wherein the gain-element is a Ti:sapphire gain-element.
7. The laser of claim 6 , wherein there are twelve fold mirrors, nine of which are coated with one of the plurality of GDD-imparting multilayer coating designs.
8. The laser of claim 7 , wherein there are first and second GDD-imparting multilayer coating designs, each thereof designed to provide a nominal GDD of about −55 femtoseconds squared, at normal incidence, in a wavelength range between about 900 nm, wherein the GDD in each thereof fluctuates about the nominal value between maximum and minimum values of about −40 femtoseconds squared and −75 femtoseconds squared respectively, and wherein the first design has fluctuation maxima at wavelengths of about 760 nm, about 820 nm, and about 875 nm, and the second design has fluctuation maxima at about 730 nm, about 790 nm, about 850 nm, and about 890 nm.
9. The laser of claim 8 wherein the angles of incidence first thorough the ninth GDD-imparting mirrors are respectively 31.5° , 24.0° , 14.5° , 12.5° , 12.5° , 4.0° , 17.0° , 24.0° , and 4.0° , and wherein the designs on the mirrors are respectively the second, first, first, second, second, first, first, first, and second.
10. The laser of claim 9 , wherein the spectrum of circulating radiation has only two intensity peaks with an intensity trough therebetween.
11. A laser comprising:
a laser resonator terminated by first and second mirrors;
a gain-element located in the laser resonator;
an arrangement for optically pumping the gain-element, the optical pumping causing fundamental radiation to circulate in the laser-resonator;
the laser resonator being folded by a first plurality of fold-mirrors on which the circulating radiation is incident at a non-normal angle of incidence, selected ones of the fold-minors being coated with one of a plurality of multilayer coating designs, each thereof arranged to impart a predetermined group delay dispersion (GDD) as a function of wavelength to the fundamental radiation incident thereon at a predetermined angle of incidence thereon, the fundamental radiation having a spectrum dependent on the resonator configuration, the gain-element and the GDD imparted by each of the selected ones of the fold-minors; and
wherein the GDD as a function of wavelength of each of the selected ones of the fold-minors and the angle of incidence of circulating radiation on each of the selected ones of the fold-minors could be selected such that the spectrum of the circulating radiation had an about Gaussian form, but are not so selected, and are instead selected such that the spectrum of the circulating radiation has a non-Gaussian form having a FWHM bandwidth at least about 25% greater than the about Gaussian form.
12. The laser of claim 11 , wherein the spectrum of the circulating radiation has one of first and second non-Gaussian forms, the first form characterized as having one of a region of about uniform intensity with intensity falling to zero on either side of the region, and the second form characterized as having at least two intensity peaks with an intensity trough therebetween.
13. The laser of claim 12 , wherein the spectrum of the circulating radiation is of the first form.
14. The laser of claim 13 , wherein the spectrum of the circulating radiation approximates a super-Gaussian of order two or greater.
15. The laser of claim 11 , wherein the spectrum of the circulating radiation has only two intensity peaks having an intensity trough therebetween.
16. The laser of claim 11 , wherein the gain-element is a Ti:sapphire gain-element.
17. The laser of claim 16 , wherein there are twelve fold mirrors, nine of which are coated with one of the plurality of GDD-imparting multilayer coating designs.
18. The laser of claim 17 , wherein there are first and second GDD-imparting multilayer coating designs, each thereof designed to provide a nominal GDD of about −55 femtoseconds squared, at normal incidence, in a wavelength range between about 900 nm, wherein the GDD in each thereof fluctuates about the nominal value between maximum and minimum values of about −40 femtoseconds squared and −75 femtoseconds squared respectively, and wherein the first design has fluctuation maxima at wavelengths of about 760 nm, about 820 nm, and about 875 nm, and the second design has fluctuation maxima at about 730 nm, about 790 nm, about 850 nm, and about 890 nm.
19. The laser of claim 18 , wherein the angles of incidence first thorough the ninth GDD-imparting mirrors are respectively 31.5° , 24.0° , 14.5° , 12.5° , 12.5° , 4.0° , 17.0° , 24.0° , and 4.0° , and wherein the designs on the mirrors are respectively the second, first, first, second, second, first, first, first, and second.
20. The laser of claim 19 , wherein the spectrum of the circulating radiation includes two intensity peaks having an intensity trough therebetween.
21. A laser comprising:
a laser resonator terminated by first and second mirrors;
a gain-element located in the laser resonator;
an arrangement for optically pumping the gain-element, the optical pumping causing fundamental radiation to circulate in the laser-resonator;
the laser resonator being folded by a plurality of fold-mirrors on which the circulating radiation is incident at a non-normal angle of incidence, selected ones of the fold-mirrors being coated with one of a plurality of multilayer coating designs, each thereof arranged to impart a predetermined group delay dispersion (GDD) as a function of wavelength to the fundamental radiation incident thereon at a predetermined angle of incidence thereon, the fundamental radiation having a spectrum dependent on the resonator configuration, the gain-element, and the GDD imparted by each of the selected ones of the fold-mirrors; and
wherein the GDD as a function of wavelength of each of the selected ones of the fold-mirror and the angle of incidence of circulating radiation on each of the selected ones of the fold-mirrors are selected such that the spectrum of the circulating radiation has at least two intensity peaks with an intensity trough therebetween.