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Low Cost Ultrafast Optics with a Fiber Laser
Immersion participants will build and characterize a connector-based, mode-locked erbium fiber laser. We will carefully align a polarizer and a series of wave plates in a free-space segment of the cavity (see figure below) to optimize conditions for pulses. Output pulses from such a laser can be on the level of 100 fs and are strongly influenced by the cavity dispersion properties. The Fourier transform of a train of pulses is a relatively broad spectrum (tens of nanometers) of individual frequencies separated by the cavity pulse repetition rate. When stabilized and broadened, this comb of frequencies acts like millions of stable lasers and can be used for applications such as frequency metrology. (The steps to make the mode-locked erbium fiber laser in this Immersion into a frequency comb will be the subject of another concurrent Immersion.) Participants will align and use an auto-correlation device to characterize the temporal profile and chirp of output pulses. The auto-correlator uses the nonlinear response of a silicon photodetector at the lasing wavelength of 1.5 micrometers, which helps make it affordable.
Mode-locked fiber lasers have emerged as a relatively low-cost, high performance tool. The list of ultrafast fiber laser applications is long and growing: multi-photon spectroscopy, frequency combs, pump-probe experiments, precision atomic and molecular spectroscopy, pulse shaping, astronomical measurements, precise length measurement, absolute frequency measurements, and microwave photonics. Fiber lasers have a small footprint (<1 m2) and use common telecommunications equipment such as high-power diode lasers that pump amplifiers and lasers. These factors mean that ultrafast fiber lasers can be efficiently brought into the important educational domains of the undergraduate and graduate-level advanced laboratory. Ultrafast technology is becoming increasingly important and yet is often not introduced until advanced and specialized graduate courses.
Skills that will be acquired during this Immersion include fiber connector epoxying, polishing, cleaving and splicing, optical alignment and design, and familiarity with optical and RF spectrum analyzers. Participants will become familiar with Matlab and Mathematica routines that model ultrafast optical phenomena.
Participants will epoxy angled-face connectors (FC/APC) to single mode fiber and polish their faces. After careful connections with index matching fluid, connection losses will be measured and minimized. We will measure the laser oscillator slope efficiency (Pout vs. pump diode current) in continuous wave operation. Free-space polarization optics will be inserted into the cavity and adjusted to observe mode-locking. Mode-locked pulses will be characterized using an oscilloscope, timer/counter, a power meter and a home-built auto-correlation device. The pulse spectrum before and after mode-locking will be recorded on an optical spectrum analyzer. An external, parallel grating dispersion compensation apparatus will allow us to vary pulse chirp and compress it temporally. We will use a suite of Matlab and Mathematica routines to analyze the pulses and their spectra. If time allows, participants will substitute a length of carbon nanotube-coated tapered fiber into the laser cavity to induce modelocking, followed by full characterization of the laser output.
Participants are encouraged to bring a notebook. A laptop computer would be helpful to view, store and possibly analyze data. We will provide the coffee.
Laser safety glasses for laser light at 980 nm and 1550 nm will be provided.
A connector-based, 100 fs-level, mode-locked erbium fiber laser can be constructed for $3400. This includes fibers, telecom components such as output couplers and WDMs, pump diodes and drivers, detectors and polarization optics. This price does not include an oscilloscope, power meter, timer/counter, or spectrum analyzers. The auto-correlation apparatus can be built for ∼$2000, which includes precision retro-reflectors. The parallel grating dispersion compensation apparatus can be built for ∼$1600.
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