Optical Phase Locking of Modelocked Lasers for Particle Accelerators
Summary (2 min read)
INTRODUCTION
- Laser-driven acceleration of relativistic particles in vacuum has been proposed and studied on a theoretical basis for many years [1,2,3].
- At present extensive research and development is being carried out on the architecture design of extended laser accelerator structures [8,9] and on efficiency and luminosity considerations [10,11].
- On the other hand little thought has been devoted on the still pending development of the laser architecture that will drive an extended laser driven particle accelerator.
- While it is true that laser-driven particle acceleration profits from progress made in laser power scaling, wallplug efficiency improvements [12], newly developed laser frequency comb stabilization and pulse synchronization techniques [13] there are still laser requirements specific to particle acceleration that will require dedicated research.
- One such aspect is the ability to sustain optical stability between independent modelocked oscillators to within 1 degree of phase for an extended period of time.
Laser Frequency Stabilization Methods
- Single mode continuous wave (CW) lasers require one parameter (the length of the laser cavity) to control the frequency of the laser beam.
- The frequency nν is inversely proportional to the optical path length of the laser cavity l and is given by repn nfl cn ≡= 2 ν 1 repf is the frequency spacing c is the speed of light and n is a large integer representing the mode number.
- Small perturbations in l can be used for active frequency stabilization [14] and for control of the optical phase of the laser beam.
- Since intra-cavity dispersion affects the effective cavity length that each mode observes a modelocked laser requires two parameters to control its pulse structure.
- Comb offset detection and control techniques [16,17,18] as well as techniques for sub-femtosecond pulse stabilization [19].
The Proposed Experimental Approach
- Present frequency comb and pulse envelope stabilization techniques alone are not going to be sufficient to lock the optical phase of two modelocked lasers to within 1degree of optical phase.
- This can be accomplished by a simple interferometric detection scheme that generates a optical phase dependent error signal that actuates on a variable optical delay for one laser beam.
- Figure 1 is a schematic of the proposed twolaser optical phase locking scheme.
- Each modelocked laser has its comb offset stabilized to the same reference frequency offset δ , which does not have to be zero but has to be the same for both lasers.
- A balanced crosscorrelator measures the timing difference of the pulse envelopes between laser 1 and laser 2 and produces an error signal that adjusts the cavity length of laser 2.
Comb Offset Detection and Control
- Initial comb offset detection and control experiments were carried out with a commercial 80 MHz, 1 W, 800 nm, 100 fsec pulse Ti:Sapphire laser.
- To broaden the frequency comb width of the laser beam to a full octave a white light continuum fiber was used.
- Figure 2 shows the electronics employed to extract the comb offset frequency.
- The laser intra-cavity dispersion can be adjusted by control of dispersion compensating prisms in the cavity or more simply by small adjustments in the power of the pump laser beam.
- For convenience the latter method was employed.
Pulse Envelope Timing Monitor
- In essence a balanced crosscorrelator consists of two separate crosscorrelators with optical path lengths set such that the crosscorrelators give an optimum crosscorrelation signal at slightly different relative beam timings.
- The difference of the two signals gives a very steep error signal curve that allows for the sought sub-fsec timing resolution.
- To test the sensitivity of the device the laser beam from the modelocked laser was split into a beam going through a fixed delay and another beam going through a PZT controlled delay arm.
- Figure 4 illustrates the layout and the resulting error signal observed from a 240 attosecond delay.
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References
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"Optical Phase Locking of Modelocked..." refers methods in this paper
...To detect the comb offset the standard self-referencing technique was employed [20]....
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"Optical Phase Locking of Modelocked..." refers background in this paper
...Two elements that have allowed this particle acceleration technology to become feasible are the appearance of tabletop high peak power lasers [ 5 ] and the maturing of micro fabrication technologies [6]....
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264 citations
"Optical Phase Locking of Modelocked..." refers background in this paper
...Laser-driven acceleration of relativistic particles in vacuum has been proposed and studied on a theoretical basis for many years [1,2,3]....
[...]
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Frequently Asked Questions (19)
Q2. What are the future works in "Optical phase locking of modelocked lasers for particle accelerators*" ?
Furthermore the authors plan to develop and characterize amplifiers for modelocked lasers. Although aimed for optical phase locking, these experiments provide an opportunity to test other important aspects such as reliability, wallplug efficiency and compactness that will ultimately help determine the future laser architecture for an extended laser driven particle accelerator.
Q3. What can be used for the control of the optical phase of the laser beam?
Small perturbations in l can be used for active frequency stabilization [14] and for control of the optical phase of the laser beam.
Q4. What is the optical phase stability of a laser beam?
Optical phase stability of one degree of optical phase will manifest as a stable fringe pattern observable by a CCD between lasers beams 1 and 2 that is stable to 1/360th of a fringe.
Q5. How can a balanced crosscorrelation technique detect optical phase shifts?
While balanced cross-correlation techniques can detect pulse envelope timing to within ~1/10 of an optical cycle an additional higher resolution timing monitor is required to detect optical phase shifts to within 1 degree.
Q6. What is the motivation for this effort?
A strong motivation for this effort has been the potential ~ 1 GeV/m sustained energy gradient that laser-driven particle accelerators could deliver [4].
Q7. What is the physics principle for modelocked lasers?
Since intra-cavity dispersion affects the effective cavity length that each mode observes a modelocked laser requires two parameters to control its pulse structure.
Q8. What are the main objectives of the experiments?
Although aimed for optical phase locking, these experiments provide an opportunity to test other important aspects such as reliability, wallplug efficiency and compactness that will ultimately help determine the future laser architecture for an extended laser driven particle accelerator.
Q9. What is the phase of the laser?
An optical interferometer placed downstream detects optical phase drifts between laser beams 1 and 2 and produces an error signal that controls a PZT driven variable delay arm for laser beam 2.
Q10. What is the frequency of the laser cavity?
The frequency nν is inversely proportional to the optical path length of the laser cavity l and is given byrepn nfl cn ≡= 2 ν 1repf is the frequency spacing c is the speed of light and n is a large integer representing the mode number.
Q11. What are the two elements that have allowed this particle acceleration technology to become feasible?
Two elements that have allowed this particle acceleration technology to become feasible are the appearance of tabletop high peak power lasers [5] and the maturing of micro fabrication technologies [6].
Q12. What is the result of the comb offset?
In the frequency domain the dispersion causes the modes to shift by a uniform frequency comb offset δ [15]δν += l cnn 2 2The consequence of the comb offset on the carrier-to-envelope relationship is a pulse-to-pulse phase slip φ∆repf⋅∆= φπδ2 3Thus, in order to phase lock two separate modelocked lasers the pulse repetition rate repf and the comb offset δ of the two lasers have to be matched.
Q13. How are the authors preparing to build a second fiber modelocked laser?
The authors are presently setting up the comb offset detection apparatus and are preparing to build a second fiber modelocked laser that will allow us to carry out the phase locking experiment for modelocked lasers.
Q14. What is the current phase locking technique?
For the next phase of experiments the authors are switching to a home built Yb:glass modelocked fiber laser that is more suitable for particle acceleration.
Q15. What is the frequency of a CW laser?
Single mode continuous wave (CW) lasers require one parameter (the length of the laser cavity) to control the frequency of the laser beam.
Q16. What is the important aspect of the research that is currently underway?
One such aspect is the ability to sustain optical stability between independent modelocked oscillators to within 1 degree of phase for an extended period of time.
Q17. What is the comb offset of the laser?
The cavity length of the laser controls the pulse envelope repetition raterepf , and the dispersion in the cavity controls the carrierto-envelope optical phase relationship.
Q18. What was the sensitivity of the comb offset?
The two beams were sent into the balanced crosscorrelator whose sensitivity was tested as a0-7803-8859-3/05/$20.00 c©2005 IEEE 1390function of delay changes caused by the PZT.
Q19. What was the purpose of the experiment?
To test the sensitivity of the device the laser beam from the modelocked laser was split into a beam going through a fixed delay and another beam going through a PZT controlled delay arm.