Phase matching of high order harmonic generation using dynamic phase modulation caused by a non-collinear modulation pulse
View Patent ↗Phase matching high harmonic generation (HHG) uses a single, long duration non-collinear modulating pulse intersecting the driving pulse. A femtosecond driving pulse is focused into an HHG medium (such as a noble gas) to cause high-harmonic generation (HHG), for example in the X-ray region of the spectrum, via electrons separating from and recombining with gas atoms. A non-collinear pulse intersects the driving pulse within the gas, and modulates the field seen by the electrons while separated from their atoms. The modulating pulse is low power and long duration, and its frequency and amplitude is chosen to improve HHG phase matching by increasing the areas of constructive interference between the driving pulse and the HHG, relative to the areas of destructive interference.
1. The method of generating coherent x-ray emissions comprising the steps of:
(a) providing a medium for high harmonic generation (HHG);
(b) focusing a femtosecond driving pulse into the medium to cause high-harmonic generation (HHG) upconversion of the light to shorter wavelengths;
(c) focusing a long duration modulating pulse, non-collinear to the driving pulse, into the medium such that the driving pulse and the modulating pulse interact within the medium; and
(d) selecting the propagation direction, frequency and amplitude of the modulating pulse such that the modulating pulse modulates the phase of the high harmonic emission and improves the phase matching of the HHG by increasing areas of constructive interference between the driving pulse and the generated HHG.
2. The method of claim 1 , wherein the step of providing a medium comprises the step of providing a gas within an enclosed volume.
3. The method of claim 2 , wherein the step of providing a medium comprises the step of providing a noble gas within an enclosed volume.
4. The method of claim 2 wherein the enclosed volume is a waveguide.
5. The method of claim 4 wherein the enclosed volume is a cylindrical waveguide.
6. The method of claim 5 wherein the enclosed volume is a preformed cylindrical plasma waveguide.
7. The method of claim 4 wherein the enclosed volume is a planar waveguide.
8. The method of claim 1 wherein the driving pulse and the modulating pulse interact over a distance of many coherence lengths of the HHG process.
9. The method of claim 8 wherein the modulating pulse is at least a millimeter.
10. The method of claim 8 wherein the intensity of the modulating pulse is on the order of 10 −6 of the intensity of the driving pulse.
11. The method of claim 8 wherein step (d) further includes the step of varying the amplitude of the modulating pulse over the duration of the pulse in order to improve the phase matching.
12. The method of claim 8 wherein step (d) further includes the step of varying the phase of the modulating pulse over the duration of the pulse in order to improve the phase matching.
13. The method of claim 8 wherein step (d) further includes the step of varying the frequency of the modulating pulse over the duration of the pulse in order to improve the phase matching.
14. The method of claim 8 wherein the energy in the modulating pulse is on the order of 1/10 the energy of the driving pulse.
15. The method of claim 8 wherein the driving pulse is on the order of 20 fs, with a wavelength of about 0.8 μm, and peak intensity of about 5.5×10 15 W/cm 2 .
16. The method of claim 8 wherein the medium is doubly ionized Ne ions at a pressure of about 70 Torr.
17. The method of claim 8 , wherein the modulating pulse has a wavelength on the order of 1.6 μm and a peak intensity on the order of 2.35×10 9 W/cm 2 .
18. The method of claim 1 where the modulating pulse consists of a combination of pulses.
19. The method of claim 1 wherein a periodic interference intensity grating between the driving laser and the modulating pulse is formed, and wherein spatial period (measured along the propagation direction of the driving laser) of this interference intensity grating approximately corresponds to an integer multiple of twice a coherence length of a high-harmonic generation process in the absence of the modulating pulse.
20. The method of claim 1 further including the step of tuning the intensity of the modulating pulse over the duration of the modulating pulse such that the absolute value of an mth-order Bessel function of the amplitude of the phase modulation is maximized.
21. Apparatus for generating coherent x-ray emissions comprising:
an enclosed volume filled with a gas;
means for producing a femtosecond driving pulse;
means for focusing the driving pulse into the gas to cause high-harmonic generation (HHG), in the X-ray region of the spectrum;
means for generating a long-duration modulating pulse;
means for focusing the modulating pulse into the gas, not collinear with the driving pulse, such that it interacts with the driving pulse within the gas; and
means for selecting the propagation direction, frequency and amplitude of the modulating pulse such that the modulating pulse modulates the phase of the high harmonic emission and improves the phase matching of the HHG by increasing areas of constructive interference between the driving pulse and the HHG.
22. The apparatus of claim 21 , wherein the gas is a noble gas.
23. The apparatus of claim 21 wherein the enclosed volume is a waveguide.
24. The apparatus of claim 22 wherein the enclosed volume is a preformed cylindrical plasma waveguide.
25. The apparatus of claim 21 wherein the means for generating the modulating pulse includes means for modifying one of the following aspects of the modulating pulse over the duration of the pulse:
amplitude;
phase; or
frequency.