Ultrafast Fiber Lasers Enabled by Highly Nonlinear Pulse Evolutions

ULTRAFAST FIBER LASERS ENABLED BY HIGHLY NONLINEAR PULSE EVOLUTIONS A Dissertation Presented to the Faculty of the Graduate School of Cornell University in Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy by Walter Pupin Fu August 2019 c 2019 Walter Pupin Fu ALL RIGHTS RESERVED ULTRAFAST FIBER LASERS ENABLED BY HIGHLY NONLINEAR PULSE EVOLUTIONS Walter Pupin Fu, Ph.D. Cornell University 2019 Ultrafast lasers have had tremendous impact on both science and applications, far beyond what their inventors could have imagined. Commercially-available solid-state lasers can readily generate coherent pulses lasting only a few tens of femtoseconds. The availability of such short pulses, and the huge peak intensities they enable, has allowed scientists and engineers to probe and manip- ulate materials to an unprecedented degree. Nevertheless, the scope of these advances has been curtailed by the complexity, size, and unreliability of such devices. For all the progress that laser science has made, most ultrafast lasers remain bulky, solid-state systems prone to misalignments during heavy use. The advent of fiber lasers with capabilities approaching that of traditional, solid-state lasers offers one means of solving these problems. Fiber systems can be fully integrated to be alignment-free, while their waveguide structure en- sures nearly perfect beam quality. However, these advantages come at a cost: the tight confinement and long interaction lengths make both linear and nonlinear effects significant in shaping pulses. Much research over the past few decades has been devoted to harnessing and managing these effects in the pur- suit of fiber lasers with higher powers, stronger intensities, and shorter pulse durations. This thesis focuses on less quantitative metrics of fiber laser performance, with an emphasis on furthering the versatility and practicality of ultrafast sources. Much of this work relies on the calculated use of strong fiber nonlinear- ities, turning conventionally-undesirable phenomena into crucial tools for en- abling new capabilities. First, the generation of femtosecond-scale pulses from much slower, more robust sources is investigated, conferring not only reliabil- ity advantages but also a fundamentally greater scope for repetition rate tun- ing. Next, prospects for fiber lasers operating at wavelengths far from any gain media are explored. By leveraging optical parametric gain alongside chirped- pulse evolutions, energy and bandwidth generated at one wavelength can be efficiently converted to another, while keeping the pulse’s phase and compress- ibility intact. Both the scaling properties and the underlying theoretical considerations of this approach are discussed. Prospects for realizing optical parametric sources in birefringent step-index fibers are then studied. By using the po- larization modes in a telecom-grade fiber to obtain phase-matching, new wavelengths can be generated while eschewing photonic crystal fiber and its inherent practical disadvantages. Finally, more speculative ideas for future work along these themes are discussed. BIOGRAPHICAL SKETCH Various figures are commonly cited as a measure of the dedicated effort required to become an expert at a given task. Notwithstanding the accuracy or precision of these metrics, Walter has spent an estimated 36,000 hours of his life as a student of some kind–13,000 in grade school (first in his birth city of St. Louis, and later in Philadelphia); another 5,000 as an undergraduate, after returning to St. Louis to earn his B.A. in Physics from Washington University in St. Louis; and now another 18,000 as a graduate student at Cornell University. It is a safe assumption that being a student is now one of his most finely-honed skills. Unfortunately, upon reaching the end of his time at Cornell, Walter found studenthood not to be a particularly employable skill in and of itself. He therefore turned to his secondary area of focus: physics. He had discovered his love of physics as an undergraduate, after spending just enough time in a chem- istry classroom to encounter quantum mechanics. This had eventually led him to Frank Wise’s group at Cornell’s School of Applied Physics, having become drawn to optics due to its intersection of complex physics and clearly-visible applications. He had subsequently spent his graduate years immersing himself in laser science and nonlinear wave equations, gradually coming to appreciate the myriad ways a differential equation could be instantiated into a real, phys- ical laser. He has therefore decided to continue designing new types of laser systems at Advanced Optowave Corporation, casting aside his studentship in favor of industrial research. After over 20 years as a student, Walter is now a person. We shall see how that works out for him. iii To my family and friends, for supporting me throughout this thesis. Also to the Wise group floppy drive: may your whirring never still and your mechanism never jam. iv ACKNOWLEDGEMENTS First and foremost, I would like to thank Frank Wise. I owe much of my growth as a researcher to Frank–both for his patient and insightful mentorship, as well as for the habits he ingrained of always asking where the greatest impact can be had. Special thanks go out to my committee members, Chris Schaffer and Steve Strogatz. Chris pushed me to expand my views beyond that of a typical laser scientist, both in his science policy class and during our longstanding biomedi- cal collaborations. Steve, too, helped show me a unique appreciation for nonlinear dynamics that will continue to inform how I think about dynamical systems. I consider myself incredibly lucky to have benefited from both of their teaching and guidance. I would also like to thank my colleagues, former and present alike, labmates or otherwise: Erin Lamb, Zhanwei Liu, Yuxing Tang, Logan Wright, Zimu Zhu, Pavel Sidorenko, Michael Buttolph, Yi-Hao Chen, Hamed Pourbeyram, Michel Olivier, Dylan Heberle, and Noah Flemens, all of whom helped me grow and learn over the course of innumerable stimulating conversations. In addition to my academic friends and colleagues, I have had the privi- lege of collaborating with a number of industrial scientists, whose technical ex- pertise, loans of equipment, and insight into how lasers can have real impact have been invaluable: Sterling Backus, from KMLabs; Robert Herda and Adam Heiniger, from Toptica Photonics; Timothy McComb, formerly from nLIGHT; and Tyson Lowder, from nLIGHT. v TABLE OF CONTENTS Biographical Sketch . iii Dedication . iv Acknowledgements . .v Table of Contents . vi List of Tables . viii List of Figures . ix 1 Introduction 1 1.1 Organization of thesis . .3 1.2 Nonlinear pulse propagation in optical fibers . .5 1.3 Four-wave-mixing in optical fibers . .6 1.4 Modelocked oscillators . .8 1.5 Gain-switching . 10 1.6 Application spaces for ultrafast lasers . 11 BIBLIOGRAPHY 14 2 Femtosecond pulses from a gain-switched diode 15 2.1 Introduction . 15 2.2 Numerical simulations . 17 2.3 Experimental results . 20 2.4 Noise behavior . 23 2.4.1 Noise measurement . 23 2.4.2 Nature of the noise . 25 2.5 Repetition rate tunability . 27 2.6 Conclusions . 29 BIBLIOGRAPHY 30 3 Normal-dispersion fiber optical parametric chirped-pulse amplifica- tion 34 3.1 Introduction . 34 3.2 CW-seeded FOPCPA . 36 3.3 Scaling FOPCPA in the time domain . 41 3.4 Conclusions . 44 BIBLIOGRAPHY 45 4 Theoretical considerations for FOPCPA 50 4.1 Introduction . 50 4.2 Types of FOPCPAs . 51 4.3 Theory of CW-seeded FOPCPA . 52 4.3.1 Overview . 52 vi 4.3.2 Pump evolution . 53 4.3.3 Phase dynamics . 55 4.3.4 Nonlinear distortions . 57 4.3.5 Parametric gain chirp . 62 4.4 Theory of continuum-seeded FOPCPA . 71 4.4.1 Overview . 71 4.4.2 Gain chirp revisited . 72 4.5 Conclusions . 77 BIBLIOGRAPHY 79 5 Parametric sources without photonic crystal fiber 83 5.1 Introduction . 83 5.2 Vector fiber OPOs . 86 5.3 Gain chirp in vector four-wave-mixing . 87 5.4 Other pulse propagation considerations . 90 5.5 Conclusions . 92 BIBLIOGRAPHY 93 6 Future directions 95 6.1 Alternatives to modelocked oscillators . 95 6.1.1 Generating pulses without modelocking . 95 6.1.2 Compressing pulses from non-modelocked sources . 98 6.1.3 Multi-stage compression . 101 6.1.4 Compression using extreme dispersion engineering . 104 6.1.5 Noise reduction . 106 6.1.6 Conclusions . 107 6.2 Prospects for vector fiber optical parametric devices . 108 6.2.1 Introduction . 108 6.2.2 In-amplifier vector four-wave-mixing . 109 6.2.3 Extension to higher-order modes . 110 6.2.4 Tunable birefringence . 110 6.2.5 Conclusions . 112 BIBLIOGRAPHY 114 vii LIST OF TABLES 4.1 Simulation parameters corresponding to Figure 4.8. The gain chirp factor will be introduced later. 63 viii LIST OF FIGURES 1.1 Cartoons illustrating typical four-wave-mixing gain for pump- ing in (a) anomalous dispersion and (b) normal dispersion. .8 2.1 Simulation results (a) at the output of the GSD, (b-c) before and after the filter, (d-e) after parabolic shaping, (f-g) after amplifica- tion, and (h) after dechirping. 19 2.2 Schematic of the experimental system. Labels correspond to pan- els in Figure 2.1. 20 2.3 (a) Spectra (scaled for visibility) and (b) autocorrelations of the pulses at the GSD output, after spectral broadening, and after filtering. Inset: logarithmic scale. 21 2.4 (a) Spectrum and (b) interferometric autocorrelation of the output pulses (inset: measured intensity autocorrelation and its transform-limited counterpart). 23 2.5 Measured RF spectra at the system output using (a) a linear detector and (b) a two-photon detector. Both spectra are centered at 1 MHz, and have a resolution bandwidth of 200 Hz.

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