Ultrafast fiber lasers with broad bandwidth and short pulse duration have a variety of applications, such as ultrafast time-resolved spectroscopy and supercontinuum generation. We report a simple and compact all-fiber thulium-doped femtosecond laser mode-locked by carbon nanotubes. The oscillator operates in slightly normal cavity dispersion at 0.055 ps2 and delivers 152 fs pulses with 52.8 nm bandwidth and 0.19 nJ pulse energy. This is the shortest pulse duration and the widest spectral width demonstrated from Tm-doped all-fiber lasers based on 1 or 2 dimensional nanomaterials, underscoring their growing potential as versatile saturable absorber materials.
Ultrafast fiber lasers have been extensively studied and developed over the past decades1,2. Their continuous improvements have started to challenge other laser technologies due to their compact design, inherently high beam quality and alignment-free format1,2. In recent years, ultrafast lasers at 2 μm spectral region are attracting growing attention due to their various applications, including remote gas sensing, bio-medical treatment, mid-infrared (IR) supercontinuum generation and mid-IR frequency comb. Thulium- (Tm) and holmium- (Ho) doped gain fibers are known to have lasing spectrum in this spectral region. In particular, Tm-doped fibers offer a broad gain bandwidth ranging from 1.8 to 2.1 μm3, enabling ultrashort (e. g. < 200 fs) pulse generation from oscillators based on these fibers. Such ultrashort pulses are highly demanding for ultrafast time resolved spectroscopy, which can be used to monitor dynamic relaxation processes of materials4. In addition, highly efficient nonlinear mid-IR frequency conversion can be enabled with ultrashort pulses at 2 μm region due to their high peak power5.
It is widely accepted that cavity group delay dispersion (GDD) control is of critical importance for ultrashort pulse generation. In general, a fiber cavity with negative GDD can generate soliton pulses, due to the balance of negative dispersion and self-phase modulation. Soliton duration is typically determined by the cavity dispersion such that τ∝|GDD|1/2 2. Pulses as short as 58 fs at 1.9 μm have been obtained by designing a short fiber cavity with only −0.017 ps2 GDD6. However, bulk optics is employed in this cavity, eliminating the advantage offered by the all-fiber configuration. To date, the shortest soliton duration reported from an all-fiber Tm-doped oscillator is 190 fs7, however, with a limited (20 pJ) pulse energy. An effective way to generate shorter pulses with moderate pulse energy is to utilize intracavity dispersion management that typically set total cavity GDD close to zero8 or slightly normal9,10. Combining dispersion management with nonlinear polarization evolution (NPE) technique, sub-200 fs pulses have been successfully achieved in Tm-doped11,12,13,14,15 and Ho-doped fiber lasers16. However, they all require the use of bulk optics to realize NPE. Dispersion management technology has also been employed in many reports on all-fiber, ultrashort Tm-doped oscillators17,18,19,20,21. For example, ref.  used a chirped Bragg fiber grating to manage dispersion, both soliton and dissipative soliton regimes can be achieved in a semiconductor saturable absorber mirror (SESAM)-based Tm oscillator. Ref.  combined SESAM and nonlinear amplifying loop mirror (NALM) mechanisms to mode-lock an all-fiber Tm laser and directly achieved 2 nJ pulses with 230 fs duration. Ref.  reported the highest single pulse energy (4.9 nJ) from an all-fiber laser cavity at 2 μm regime. Recently, Sobon et al. used the NPE technique to directly generate dissipative solitons with >100 nm bandwidth. This is thus far the broadest spectrum directly generated from a normal dispersion mode-locked Tm-doped fiber laser21. To date, the shortest pulse directly generated from an all-fiber Tm-doped oscillator is 140 fs, mode-locked by SESAM18.
Although NPE3 and SESAMs7 are the two most widely studied mechanisms for mode-locking Tm-doped fiber lasers, they still suffer from some fundamental drawbacks. For example, NPE requires polarization optimization at all times due to its environmental sensitivity. SESAMs generally have a limited bandwidth which results from their resonant design and require complex semiconductor fabrication processes, packaging and integration22. Recently, a new generation of saturable absorber (SA) based on 1D (carbon nanotubes, CNTs) or 2D (such as graphene, MoS2 and black phosphorous) nanomaterials have come into prominence23,24,25,26,27,28,29,30,31,32,33,34,35,36,37,38. These nanomaterial-based SAs have the advantages through easy and economic fabrication and when in composite form, transmission-type operation for simple integration into all-fiber ring cavities33,39. Among these nanomaterials, CNTs possess ultrafast recovery time, large modulation depth and wide operation bandwidth when samples with large diameter distribution are used24. Such diameter distribution are inherent in most CNT production techniques40. Thus, fiber lasers mode-locked by CNTs have been widely demonstrated in the 1 41,42,43, 1.5 23,44,45,46 and 2 μm25,30,47,48,49 region. However, because of the large negative dispersion of SMF fiber at 2 μm, CNT-mode-locked Tm-doped fiber oscillators typically emit picosecond pulses25,29,47. Recently, a section of germanium-silicate (GeO2/SiO2) fiber was used to control the intracavity dispersion, 450 fs pulses with 15.8 nm bandwidth were directly achieved in a CNTs/NALM hybrid mode-locked Tm-doped fiber laser19. This is thus far the shortest pulse duration with the broadest bandwidth directly generated from a Tm-doped fiber oscillator mode-locked by CNTs or other 2D nanomaterials.
In this letter, we demonstrate a robust and compact Tm-doped all-fiber femtosecond oscillator mode-locked by CNTs. The oscillator operates in a slightly normal GDD after intracavity dispersion management. 152 fs pulses with 52.8 nm bandwidth are directly produced from our oscillator without any free-space components. Both the pulse duration and spectral bandwidth are ~3 times shorter and wider, respectively, than previous CNT-based Tm-doped fiber lasers19 and demonstrate an improvement on graphene or other 2D material-based Tm-doped fiber oscillators50,51,52,53,54.
CNTs preparation and characterization
We use CNTs grown by arc discharge on Ni/Y catalyst (P2, Carbon Solutions, Inc., 0.5–1.5 μm in length, 4–8% catalyst metal content)55. The CNTs, with diameters ranging from 1.3–1.6 nm, are embedded into carboxymethyl cellulose via solution processing to form polymer composite40. After 4 or 5 days of slow evaporation at room temperature, we obtain a free-standing polymer composite SA with ~30 μm thickness. Such composites can be used in transmission-type configurations through simple and easy integration into all-fiber format. These CNTs exhibit optical absorption in the 1.75 to 2 μm range centered at ~1.85 μm (see Fig. 1(a)) due to S11 excitonic absorption of the semiconducting tubes. This absorption band fits well with the operating wavelength of the Tm gain fiber (see dashed line in Fig. 1(a)). Power-dependent absorption at 1.9 μm of the CNT-SA are measured with an optical parametric oscillator (Coherent Chameleon Ultra II) producing ~260 fs pulses. The experimental data is then fitted by a nonlinear function of fast SA that describes its transmittance9, giving ~10% modulation depth and ~18 μJ/cm2 saturation fluence (corresponding to ~68 MW/cm2 saturation intensity); Fig. 1(b).
Setup of mode-locked fiber laser
The schematic of the laser setup is shown in Fig. 2. The CNT-SA is sandwiched between two fiber connectors (see inset of Fig. 2). The gain medium is a 17.5 cm long, highly-doped Tm fiber (Nufern SM-TSF-5/125) with −20 ps2/km dispersion at 1.9 μm estimated from numerical calculation. The pump is provided by a commercial Er fiber laser that emits at ~1570 nm and is coupled into the cavity via a 1570/1940 nm wavelength division multiplexer (WDM). The pigtails of the WDM amount to 1.14 m SMF-28e fiber. A polarization insensitive isolator, consisting of 0.91 m SMF-28e pigtail is spliced after the gain fiber and ensures unidirectional operation of the oscillator. An in-line polarization controller (PC) is employed to optimize the polarization state to compensate for the intrinsic weak birefringence of the passive and active fibers. 20% intracavity light is coupled out through a 20/80 coupler with 0.985 m long SMF-28e fiber in the cavity. The dispersion of the SMF-28e fiber is −71 ps2/km at 1.9 μm15.
Since the gain fiber and SMF exhibit negative dispersion at 1.9 μm, a component with normal dispersion, is required to realize dispersion management Ultra-high NA fibers, such as normal dispersion fiber (NDF). have been demonstrated to have normal dispersion at long wavelength, due to their much stronger waveguide dispersion than material dispersion15,48,56,57. We thus add a 3.75 m long fiber (Nufern UHNA4) as the NDF. The dispersion of UHNA4 fiber is measured to be 93 ps2/km at 1.9 μm48. Thus, the cavity length depicted in Fig. 2 is 6.96 m with a total GDD of 0.13 ps2. By changing the passive fiber between PC and CNT-SA via adding SMF-28e or NDF fibers and without changing other fiber segments, the net cavity GDD could be either normal or anomalous, within a range of 0.385 ps2 to −0.265 ps2. The total cavity length is varied between 6.96 m and 12.5 m.
Mode-locking operation and characteristics
When the pump power is increased to an appropriate level, stable oscilloscope traces could always be achieved by adjusting the PC in this dispersion range. We note that no pulse trace could be observed in the oscilloscope without the CNTs. This suggests that the CNT-SA plays a major role in starting and stabilizing the pulses. Figure 3(a–g) show the evolution of the pulse spectrum with different net cavity GDDs. Similar to previously reported 2 μm pulsed lasers12,25,56, sharp dips are observed due to the absorption of atmospheric molecules58. We experimentally find that the dips become significant when the wavelength is below 1940 nm, further confirming such dips are predominantly caused by the absorption of CO2 and water molecules58. Moreover, the central emission wavelength is usually blue-shifted from the peak emission wavelength of the gain fiber (1950~1970 nm) to ~1915 nm. This could be predominantly caused by the cavity loss. For example, the two splicing points between UHNA4 and SMF induce large insertion losses (~54% measured). Also, to get stable mode-locking operation, we sometimes bent a small segment of SMF-28e fiber to finely tune intra-cavity loss during the experiments. In addition, we note that the automatic balance between the intra-cavity dispersion and nonlinearity could play a role in the wavelength shift since it is sensitive to the wavelength and the setting of PC, respectively.
Initially, a wide FWHM bandwidth of up to 48.07 nm is achieved with net cavity GDD of 0.055 ps2, accompanied by narrowing of the spectrum bandwidth on both sides of this dispersion value, see Fig. 3(a–g). On one hand, the steep spectral edges, expected as a signature of dissipative solitons1, are observed when the net GDD is larger than 0.055 ps2; Fig. 3(a–c). On the other hand, the absence of spectral sidebands in Fig. 3(d–f) show that these cavities work in the dispersion-managed soliton regime2. Finally, Kelly sidebands of soliton spectrum appears when the negative dispersion increases to −0.265 ps2; Fig. 3(g). We then use a radio-frequency (RF) spectrum analyzer (Agilent N9010) and a 12.5 GHz photodiode (EOT-5000) to verify the pulse stability of these cases by measuring their wideband RF spectra to up to 3.6 GHz; Fig. 3(h–n). RF spectra in high-order harmonics exhibit fluctuations in the dispersion-managed soliton regime (Fig. 3(k–m)), indicating a noise-like regime. This is confirmed by the autocorrelation (AC) trace/interferometric AC (IAC) trace measurements of three operating regimes (i.e. dissipative soliton regime, dispersion-managed soliton regime and soliton regime) since no stable pulse is generated in the dispersion-managed soliton regime, see Fig. 4(a–c). The noise-like operation could be caused by the limited modulation depth (~10%) of our CNT-SA59. Figure 4(d) summarizes the dechirped pulse duration and time-bandwidth product (TBP) as a function of net cavity dispersion. The shortest pulse duration of ~170 fs could be achieved as soon as the net dispersion is slightly normal. When the cavity works in the dissipative soliton regime, the TBP is >0.66 (i.e. >1.5 times of Fourier limit), indicating incomplete compression. Such imperfect compression could be caused by uncompensated high-order dispersion, in particular, the third-order dispersion induced by intra-cavity fibers (e.g., the NDF fiber)15.
To further decrease the achievable pulse duration. We therefore increase the pump power and carefully optimize the polarization state of the cavity which can emit pulses with much wider bandwidth than other cavities (see Fig. 3(c)). The cavity has a length of 8.01 m, corresponding to 25.76 MHz pulse repetition rate. At 660 mW pump power, the oscillator delivers pulses with a 52.83 nm bandwidth, centered at 1927 nm, see Fig. 5(a). The output power is 4.85 mW, corresponding to 0.19 nJ pulse energy. A higher pump power results in multi-pulse operation or instability. This could be caused by over saturation of the CNT-SA. Normal net GDD of this oscillator is expected to produce positively chirped pulse1. Fig. 5(b) shows the AC trace of the pulse compressed with ~10.2 m long SMF-28e fiber. The AC FWHM is 216 fs. Assuming a Gaussian profile, the deconvoluted pulse width is ~152 fs, ~1.5 times of Fourier-limit. Considering the large bandwidth of 52.8 nm, we note that transform-limited <100 fs pulse is possible after compression, with appropriate high-order dispersion compensation (e.g., prisms). Figure 5(c) shows the RF spectrum at the fundamental repetition rate. The SNR is as high as 73 dB, comparable to those previously reported pulsed lasers at 2 μm12,15,48, indicating stable mode-locking operation.
In summary, we have demonstrated a simple and compact all-fiber Tm-doped laser delivering 152 fs pulses with a 52.8 nm bandwidth. These are by far the shortest pulses with the broadest bandwidth, directly from CNT mode-locking Tm-doped fiber lasers, constituting a 3-fold improvement both in pulse duration and spectral bandwidth compared to previous reports. Such pulses have a great potential as low-cost light sources for mid-IR supercontinuum generation and pump-probe technique which typically requires ultrashort and wide bandwidth pulses. In addition, these pulses may also find applications as ideal seed pulse for chirped pulse amplification (CPA) because of its clean sidebands.
How to cite this article: Wang, J. et al. 152 fs nanotube-mode-locked thulium-doped all-fiber laser. Sci. Rep. 6, 28885; doi: 10.1038/srep28885 (2016).
Wise, F. W., Chong, A. & Renninger, W. H. High-energy femtosecond fiber lasers based on pulse propagation at normal dispersion. Laser Photon. Rev. 2, 58–73 (2008).
Fermann, M. E. & Hartl, I. Ultrafast fiber laser technology. IEEE J. Sel. Top. Quantum Electron. 15, 191–206 (2009).
Nelson, L. E., Ippen, E. P. & Haus, H. A. Broadly tunable sub-500 fs pulses from an additive-pulse mode-locked thulium-doped fiber ring laser. Appl. Phys. Lett. 67, 19–21 (1995).
Stolow, A., Bragg, A. E. & Neumark, D. M. Femtosecond time-resolved photoelectron spectroscopy. Chem. Rev. 104, 1719–1758 (2004).
Rudy, C. W., Digonnet, M. J. F. & Byer, R. L. Advances in 2-μm Tm-doped mode-locked fiber lasers. Opt. Fiber Technol. 20, 642–649 (2014).
Jiang, J. et al. 500 MHz, 58 fs highly coherent Tm fiber soliton laser. Presented at Conference on Lasers and Electro-Optics: Science and Innovations, San Jose, USA. OSA Technical Digest (online) (Optical Society of America). (doi: 10.1364/CLEO_SI.2012.CTh5D.7) (May 6–11) (2012).
Sharp, R. C., Spock, D. E., Pan, N. & Elliot, J. 190-fs passively mode-locked thulium fiber laser with a low threshold. Opt. Lett. 21, 881–883 (1996).
Tamura, K., Ippen, E. P., Haus, H. A. & Nelson, L. E. 77-fs pulse generation from a stretched-pulse mode-locked all-fiber ring laser. Opt. Lett. 18, 1080–1082 (1993).
Wang, J. et al. Pulse dynamics in carbon nanotube mode-locked fiber lasers near zero cavity dispersion. Opt. Express 23, 9947–9958 (2015).
Tamura, K., Ippen, E. P. & Haus, H. A. Pulse dynamics in stretched-pulse fiber lasers. Appl. Phys. Lett. 67, 158–160 (1995).
Haxsen, F. et al. Stretched-pulse operation of a thulium-doped fiber laser. Opt. Express 16, 20471–20476 (2008).
Wienke, A. et al. Ultrafast, stretched-pulse thulium-doped fiber laser with a fiber-based dispersion management. Opt. Lett. 37, 2466–2468 (2012).
Nomura, Y. & Fuji, T. Sub-50-fs pulse generation from thulium-doped ZBLAN fiber laser oscillator. Opt. Express 22, 12461–12466 (2014).
Gebhardt, M. et al. Sub-200 fs, nJ-level stretched-pulse thulium-doped fiber oscillator at 23MHz repetition rate. Presented at Advanced Solid State Lasers, Shanghai, China. OSA Technical Digest (online) (Optical Society of America). (doi: 10.1364/ASSL.2014.AM5A.43) (2014, Nov. 16–21).
Tang, Y., Chong, A. & Wise, F. W. Generation of 8 nJ pulses from a normal-dispersion thulium fiber laser. Opt. Lett. 40, 2361–2364 (2015).
Li, P., Ruehl, A., Grosse-Wortmann, U. & Hartl, I. Sub-100 fs passively mode-locked holmium-doped fiber oscillator operating at 2.06 μm. Opt. Lett. 39, 6859–6862 (2014).
Gumenyuk, R., Vartiainen, I., Tuovinen, H. & Okhotnikov, O. G. Dissipative dispersion-managed soliton 2 μm thulium/holmium fiber laser. Opt. Lett. 36, 609–611 (2011).
Wang, Q., Geng, J., Luo, T. & Jiang, S. Ultrashort Pulse 2 Micron Fiber Lasers. Presented at Advanced Solid-State Lasers Congress: Mid-Infrared Coherent Sources, Paris, France. OSA Technical Digest (online) (Optical Society of America). (doi: 10.1364/MICS.2013.MTh1C.1) (Oct. 27-Nov. 1) (2013).
Chernysheva, M. A. et al. SESAM and SWCNT mode-locked all-fiber thulium-doped lasers based on the nonlinear amplifying loop mirror. IEEE J. Sel. Top. Quantum Electron. 20, 448–455 (2014).
Huang, C. et al. Developing high energy dissipative soliton fiber lasers at 2 micron. Sci. Rep. 5, 13680 (2015).
Sobon, G., Sotor, J., Martynkien, T. & Abramski, K. M. Ultra-broadband dissipative soliton and noise-like pulse generation from a normal dispersion mode-locked Tm-doped all-fiber laser. Opt. Express 24, 6156–6161 (2016).
Okhotnikov, O. G. Fiber Lasers. 294 (Wiley-VCH, 2012).
Set, S. Y., Yaguchi, H., Tanaka, Y. & Jablonski, M. Ultrafast fiber pulsed lasers incorporating carbon nanotubes. IEEE J. Sel. Top. Quantum Electron. 10, 137–146 (2004).
Wang, F. et al. Wideband-tuneable, nanotube mode-locked, fibre laser. Nat. Nanotechnol. 3, 738–742 (2008).
Kieu, K. & Wise, F. W. Soliton thulium-doped fiber laser with carbon nanotube saturable absorber. IEEE Photon. Technol. Lett. 21, 128–130 (2009).
Bao, Q. et al. Atomic-layer graphene as a saturable absorber for ultrafast pulsed lasers. Adv. Funct. Mater. 19, 3077–3083 (2009).
Sun, Z. et al. Graphene mode-locked ultrafast laser. ACS Nano 4, 803–810 (2010).
Popa, D. et al. Sub 200 fs pulse generation from a graphene mode-locked fiber laser. Appl. Phys. Lett. 97, 203106 (2010).
Zhang, M. et al. Mid-infrared Raman-soliton continuum pumped by a nanotube-mode-locked sub-picosecond Tm-doped MOPFA. Opt. Express 21, 23261–23271 (2013).
Hasan, T. et al. Double-wall carbon nanotubes for wide-band, ultrafast pulse generation. ACS Nano 8, 4836–4847 (2014).
Zhao, J., Yan, P. & Ruan, S.-C. Observations of three types of pulses in an erbium-doped fiber laser by incorporating a graphene saturable absorber: erratum. Appl. Opt. 53, 458–458 (2014).
Huang, S. S. et al. High order harmonic mode-locking in an all-normal-dispersion Yb-doped fiber laser with a graphene oxide saturable absorber. Laser Phys. 24, 015001 (2014).
Woodward, R. I. & Kelleher, E. J. 2D saturable absorbers for fibre lasers. Appl. Sci. 5, 1440–1456 (2015).
Guo, Z. et al. From black phosphorus to phosphorene: basic solvent exfoliation, evolution of Raman scattering and applications to ultrafast photonics. Adv. Funct. Mater. 25, 6996–7002 (2015).
Sobon, G. et al. 260 fs and 1 nJ pulse generation from a compact, mode-locked Tm-doped fiber laser. Opt. Express 23, 31446–31451 (2015).
Luo, Z. et al. Two-dimensional material-based saturable absorbers: towards compact visible-wavelength all-fiber pulsed lasers. Nanoscale 8, 1066–1072 (2016).
Sun, Z., Martinez, A. & Wang, F. Optical modulators with 2D layered materials. Nat. Photon. 10, 238 (2016).
Sotor, J. et al. All-fiber Ho-doped mode-locked oscillator based on a graphene saturable absorber. Opt. Lett. 41, 2592–2595 (2016).
Yamashita, S. A tutorial on nonlinear photonic applications of carbon nanotube and graphene. J. Lightwave Technol. 30, 427–447 (2012).
Hasan, T. et al. Nanotube–polymer composites for ultrafast photonics. Adv. Mater. 21, 3874–3899 (2009).
Nicholson, J. W., Windeler, R. S. & DiGiovanni, D. J. Optically driven deposition of single-walled carbon-nanotube saturable absorbers on optical fiber end-faces. Opt. Express 15, 9176–9183 (2007).
Kieu, K. & Wise, F. W. All-fiber normal-dispersion femtosecond laser. Opt. Express 16, 11453–11458 (2008).
Pedersen, M. E. V. et al. Stable gain-guided soliton propagation in a polarized Yb-doped mode-locked fiber laser. IEEE Photonics J. 4, 1058–1064 (2012).
Sun, Z. et al. A compact, high power, ultrafast laser mode-locked by carbon nanotubes. Appl. Phys. Lett. 95, 253102 (2009).
Martinez, A. & Yamashita, S. Multi-gigahertz repetition rate passively modelocked fiber lasers using carbon nanotubes. Opt. Express 19, 6155–6163 (2011).
Mou, C., Rozhin, A. G., Arif, R., Zhou, K. & Turitsyn, S. Polarization insensitive in-fiber mode-locker based on carbon nanotube with N-methyl-2-pryrrolidone solvent filled fiber microchamber. Appl. Phys. Lett. 100, 101110 (2012).
Solodyankin, M. A. et al. Mode-locked 1.93 μm thulium fiber laser with a carbon nanotube absorber. Opt. Lett. 33, 1336–1338 (2008).
Wang, Q. et al. All-fiber ultrafast thulium-doped fiber ring laser with dissipative soliton and noise-like output in normal dispersion by single-wall carbon nanotubes. Appl. Phys. Lett. 103, 011103 (2013).
Chernysheva, M. A. et al. Thulium-doped mode-locked all-fiber laser based on NALM and carbon nanotube saturable absorber. Opt. Express 20, B124–B130 (2012).
Sobon, G. et al. All-polarization maintaining, graphene-based femtosecond Tm-doped all-fiber laser. Opt. Express 23, 9339–9346 (2015).
Zhang, M. et al. Tm-doped fiber laser mode-locked by graphene-polymer composite. Opt. Express 20, 25077–25084 (2012).
Sotor, J. et al. Ultrafast thulium-doped fiber laser mode locked with black phosphorus. Opt. Lett. 40, 3885–3888 (2015).
Tian, Z. et al. Mode-locked thulium fiber laser with MoS2 . Laser Phys. Lett. 12, 065104 (2015).
Ren, Y. et al. 7.8-GHz graphene-based 2-μm monolithic waveguide laser. IEEE J. Sel. Top. Quantum Electron. 21, 395–400 (2015).
Carbon Solutions Inc., P2-SWNT. Available at: http://www.carbonsolution.com/products/p2-swnt. (Date of access: 10/01/2016).
Haxsen, F., Wandt, D., Morgner, U., Neumann, J. & Kracht, D. Monotonically chirped pulse evolution in an ultrashort pulse thulium-doped fiber laser. Opt. Lett. 37, 1014–1016 (2012).
Kadel, R. & Washburn, B. R. Stretched-pulse and solitonic operation of an all-fiber thulium/holmium-doped fiber laser. Appl. Opt. 54, 746–750 (2015).
Stark, A. et al. Intracavity absorption spectroscopy with thulium-doped fibre laser. Opt. Commun. 215, 113–123 (2003).
Herda, R. & Okhotnikov, O. G. Dispersion compensation-free fiber laser mode-locked and stabilized by high-contrast saturable absorber mirror. IEEE J. Quantum Electron. 40, 893–899 (2004).
We acknowledge funding from the Science and Technology Projects of Shenzhen City (JCYJ20150324140036862, JCYJ20140418095735546), the Natural Science Foundation of Guangdong Province (2015A030310464, 2016A030310049), the Scientific Research Foundation of Shenzhen City (827-000118), the Teknologiateollisuus TT-100, the European Union’s Seventh Framework Programme (REA grant agreement No. 631610), the Academy of Finland (No. 284548), Tekes (OPEC) and Aalto University (Finland). TH acknowledges funding from the Royal Academy of Engineering through a research fellowship (Graphlex).
The authors declare no competing financial interests.
About this article
Cite this article
Wang, J., Liang, X., Hu, G. et al. 152 fs nanotube-mode-locked thulium-doped all-fiber laser. Sci Rep 6, 28885 (2016). https://doi.org/10.1038/srep28885
Journal of the European Optical Society-Rapid Publications (2021)
Scientific Reports (2020)
Generation of multi-solitons and noise-like pulses in a high-powered thulium-doped all-fiber ring oscillator
Scientific Reports (2019)
CNT-based saturable absorbers with scalable modulation depth for Thulium-doped fiber lasers operating at 1.9 μm
Scientific Reports (2017)
Scientific Reports (2017)