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Method Article

Low-cost Custom Fabrication and Mode-locked Operation of an All-normal-dispersion Femtosecond Fiber Laser for Multiphoton Microscopy

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DOI:

10.3791/60160

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November 22nd, 2019

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In This Article

Summary

A method is presented to build a custom low-cost, mode-locked femtosecond fiber laser for potential applications in multiphoton microscopy, endoscopy, and photomedicine. This laser is built using commercially available parts and basic splicing techniques.

Abstract

A protocol is presented to build a custom low-cost yet high-performance femtosecond (fs) fiber laser. This all-normal-dispersion (ANDi) ytterbium-doped fiber laser is built completely using commercially available parts, including $8,000 in fiber optic and pump laser components, plus $4,800 in standard optical components and extra-cavity accessories. Researchers new to fiber optic device fabrication may also consider investing in basic fiber splicing and laser pulse characterization equipment (~$63,000). Important for optimal laser operation, methods to verify true versus apparent (partial or noise-like) mode-locked performance are presented. This system achieves 70 fs pulse duration with a center wavelength of approximately 1,070 nm and a pulse repetition rate of 31 MHz. This fiber laser exhibits the peak performance that may be obtained for an easily assembled fiber laser system, which makes this design ideal for research laboratories aiming to develop compact and portable fs laser technologies that enable new implementations of clinical multiphoton microscopy and fs surgery.

Introduction

Solid state femtosecond (fs) pulsed lasers are widely used for microscopy and biological research. One typical example is the usage of multiphoton excitation (MPE) fluorescence microscopy, where high peak power and low average power are desired to facilitate the MPE process while minimizing photodamage mechanisms. Many high-performance solid-state lasers are commercially available, and when combined with an optical parametric oscillator (OPO), the laser wavelength can be tuned over a wide range1. For example, commercial oscillator-OPO systems generate <120 fs pulse durations (typically with an 80 MHz pulse repetition rate) and >1 W aver....

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Protocol

1. Splice single mode fibers (SMF)

NOTE: Section 1 consists of general steps to splice SMFs. This is a non-essential, but recommended, step for practicing fiber splices using inexpensive fiber. This step ensures proper performance of the splicing equipment before using more valuable fiber optic materials.

  1. Cleave the first fiber.
    1. Strip approximately 30 mm of the fiber with a fiber stripping tool. For fragile fibers (e.g., double clad fibers), a razor blade can be used to carefully peel off the buffer.
    2. Use lint-free tissue with ethanol or isopropanol to clean the stripped fiber. A buzzing sound when wiping t....

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Results

It is critical to verify mode-locked operation upon completion of the fiber laser fabrication procedures. Signatures of optimal fs pulse generation and laser stability are as follows: First, the output pulse may be sufficiently characterized by the instrumentation outlined in step 6. The pulse spectrum output from the laser oscillator should be centered near 1,070 nm with the characteristic cat-ear or Batman shape that indicates mode-locking as predicted by numerical simulation of ANDi pu.......

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Discussion

The protocols outlined here synthesize know-how and expertise that have been common practice in the laser physics laboratory for decades, but which is frequently unfamiliar to many biomedical researchers. This work attempts to make this ultrafast fiber laser technology more accessible to the broader community. The ANDi fiber laser design is well-established, as first developed in seminal works by Wise and colleagues3. However, implementations of this technology by other groups have sometimes resul.......

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Disclosures

The authors declare no competing interests.

Acknowledgements

We thank Drs. E. Cronin-Furman and M. Weitzman (Olympus Corporation of the Americas Scientific Solutions Group) for assistance in acquiring images. This work was supported by National Institutes of Health Grant K22CA181611 (to B.Q.S.) and the Richard and Susan Smith Family Foundation (Newton, M.A.) Smith Family Award for Excellence in Biomedical Research (to B.Q.S.).

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Materials

List of materials used in this article
NameCompanyCatalog NumberComments
Adapters, mirrors, posts, mounts, and translational stage (optomechanics)ThorlabsTR6-P5 (3x), AD12NT (2x), PFSQ20-03-M01, PFSQ05-03-M01, KMS, KM100C, KM100CL, KM200S, LT1, LT101, UPH2-P5, UPH3-P5 (2x)Standard optical components
Advanced optical fiber cleaverAFLCT-100
AutocorrelatorFemtochromeFR-103XL/IR/FA/CDA
Beamsplitter mountThorlabsBSH1/M
Factory fusion splicerAFLFSM-100P
Fiber collimatorsOZ Optics (Canada)LPC-08-1064-6/125-S-1.6-7.5AS-60-X-1-2-HPC3x
Fiber-coupled,high-speed photodiode detectorThorlabsDET08CFC
Free-space isolatorThorlabsIO-5-1050-HP
Free-space isolatorThorlabsIO-3D-1050-VLP
Half waveplateUnion Optics (China)WPZ23122x
High power multimode fiber pump moduleGauss Lasers (China)Pump-MM-976-10
High power pump and signal combinerITF Technology (Canada)MMC02112DF1
Index matching gelThorlabsG608N3
Optical spectrum analyzerKeysightAgilent 70951B
OscilloscopeKeysightAgilent 54845A
Passive double clad fiber(5/130 μm)ITF Technology (Canada)MMC02112DF13m, Included with combiner
Polarizing beamsplitterThorlabsPBS253
Quarter waveplatesUnion Optics (China)WPZ43122x
Quartz birefringent filter plateNewlight (Canada)BIR1060
RF spectrum analyzerTektronixRSA306B
Single mode fiber (6/125 μm)OZ Optics (Canada)LPC-08-1064-6/125-S-1.6-7.5AS-60-X-1-2-HPC1m, Included with collimators
Single mode fiber couplerAFW (Australia)FOSC-2-64-30-L-1-H64-2
Transmission diffraction grating 1LightSmythT-1000-1040-3212-94For compressor
Transmission diffraction grating 2LightSmythT-1000-1040-60x12.3-94For compressor
Waveplate rotation mountThorlabsRSP1/M4x
Ytterbium-doped single mode double clad fiberThorlabsYB1200-6/125DC3m

References

  1. Savage, N. Optical parametric oscillators. Nature Photonics. 4, 124(2010).
  2. Xu, C., Wise, F. Recent advances in fibre lasers for nonlinear microscopy. Nature Photonics. 7, 875(2013).
  3. Kieu, K., Wise, F.

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