Carrier envelope phase stabilization of an optical amplifier
View Patent ↗A laser and amplifier combination delivers a sequence of optical pulses. Pulses from the laser are temporally stretched by a pulse stretcher before amplification and temporally compressed by a pulse compressed after amplification. The pulse stretcher includes a diffraction grating on which pulses being compressed are incident. An arrangement is provided for measuring the carrier-envelope phase of the pulses and adjusting the incidence angle of pulses on the grating cooperative with the measurement such that the carrier envelope phase of the pulses in the sequence is about constant.
1. Optical apparatus, comprising:
an oscillator for generating a sequence of optical pulses;
a pulse stretcher for temporally stretching the optical pulses, the pulse-stretcher including a first diffraction grating, the pulses being incident on the diffraction grating at a first incidence angle;
an optical amplifier arranged to amplify the temporally stretched optical pulses; and
a pulse compressor for temporally compressing the amplified temporally stretched pulses, the pulse compressor including a second diffraction grating, the amplified temporally stretched pulses being incident on the second diffraction grating at a second incidence angle; and
a detector for periodically measuring a carrier envelope phase (CEP) of the temporally compressed amplified pulses and with the output from the detector being used to adjust one of the first and second incidence angles cooperative with the CEP measurement such that the CEP of the temporally compressed amplified pulses remain about constant.
2. The apparatus of claim 1 , wherein the second incidence angle is adjusted.
3. The apparatus of claim 2 , wherein the pulses are incident on the second diffraction grating in an incidence plane and the second incidence angle is adjusted by tilting the second diffraction grating in the incidence plane.
4. The apparatus of claim 1 , wherein the first incidence angle is adjusted.
5. The apparatus of claim 4 , wherein the pulses are incident on the first diffraction grating in an incidence plane and the first incidence angle is adjusted by tilting the first diffraction grating in the incidence plane.
6. The apparatus of claim 1 , wherein the first diffraction grating is cooperative with an optical arrangement for imaging the first grating back onto itself to provide an effect similar to a grating-pair pulse-stretcher.
7. The apparatus of claim 1 , wherein the second diffraction grating is cooperative with an optical arrangement for imaging the second grating back onto itself to provide an effect of a grating-pair pulse compressor.
8. The apparatus of claim 1 , wherein the carrier envelope phase measurement arrangement includes an f-2f interferometer.
9. Optical apparatus, comprising:
an oscillator for generating a sequence of optical pulses having a wavelength λ;
a pulse stretcher for temporally stretching the optical pulses;
an optical amplifier arranged to amplify the temporally stretched optical pulses; and
a pulse compressor for temporally compressing the amplified temporally stretched pulses, the pulse compressor including a diffraction grating having a groove density d and being cooperative with optical elements which cause that each of the temporally stretched pulses to be incident repeatedly on the diffraction grating at a predetermined nominal incidence angle α in an incidence plane, following a path having a length G between the repeated incidences; and
a detector for periodically measuring a carrier envelope phase (CEP) of the temporally compressed amplified pulses and with the output from the detector being used to adjust the nominal incidence angle of the pulses on the diffraction grating cooperative with the CEP measurement such that the CEP of the temporally compressed amplified pulses is about constant.
10. The apparatus of claim 9 , wherein the nominal incidence angle is adjusted by tilting the diffraction grating in the incidence plane.
11. The apparatus of claim 10 , wherein adjustment of the CEP as a function of the adjustment of the incidence angle is approximated by an equation
δφ
=
2
*
4
π
d
G
cos
α
1
-
(
d
λ
-
sin
α
)
2
δα
where δα is the incidence angle adjustment and δφ is about the resulting CEP adjustment.
12. A method of controlling the carrier envelope phase (CEP) of laser pulses, said pulses being generated by an oscillator and supplied to an amplifier for amplifying the pulses, and wherein prior to entering the amplifier, the pulses are passed through a pulse stretcher for stretching the pulses and after leaving the amplifier, the pulses are passed through pulse compressor for compressing the pulses and wherein at least one of the stretcher and the compressor include a diffraction grating, said method comprising the steps of:
monitoring the CEP of the pulses after they have been compressed;
generating a feedback signal indicative of the CEP; and
varying the angle of the incidence of the pulses on said grating in response to the feedback signal in order to adjust the CEP to a desired value.
13. A method as recited in claim 12 , wherein said grating is supported on an angularly adjustable mount and wherein said step of varying the angle of the incidence of the pulses on said grating is performed by adjusting the angle of the mount.
14. A method as recited in claim 12 , wherein angle of incidence of the pulses on said grating is adjusted in order to drive the CEP towards a constant value during the generation of a plurality of pulses in a train.
15. A method as recited in claim 12 , wherein said grating is in the compressor.
16. A method as recited in claim 12 , wherein the diffraction grating is cooperative with an optical arrangement for imaging the grating back onto itself to provide an effect similar to a grating-pair pulse-stretcher.