Generation of self-pulsating source based on regenerative SPM and realizing high-quality-pulse source.
Self-pulsating fiber lasers have become a topic of interest for their ability to combine a high beam quality, stability and compactness. In such lasers, the generation of short pulses enables imaging, spectroscopy or metrology as well as industrial application when operating at watt levels. To generate pulses, a nonlinear transfer function favoring pulses over continuous wave (CW) operation must be added in the laser cavity.
we have presented a self-pulsating laser source based on cascaded optical regeneration working at a wavelength of 1550 nm [2,3]. In 2008, pulsed lasers based on a pair of complementary regenerators of type self-phase modulation (SPM) and offset filtering (SPM-OF) regenerators was demonstrated . Pulsed lasers based on a pair of complementary regenerators of type self-phase modulation (SPM) and offset filtering (SPMOF) regenerators was demonstrated .
Sources of that kind, referred to as SPM-soliton self-frequency shift (SPM-SSFS) sources, are composed of two distinct regeneration stages. A particular feature of SPM-SSFS sources is that they provide a broadband SC at one of their output, along with a tunable temporal burst duration which can be extended up to several hundreds of nanoseconds when the pump power is increased.
Because of the presence of multiple and varying pump pulses, the SC generated by this type of sources may be compared to supercontinnum emanating from noise bursts , or noise like pulses . SPM-SSFS sources therefore provide a flexible platform for ultrashort pulse generation, which results in a tunable output energy and SC width, without active optical elements such as optical modulators. Results provide the optimal filter bandwidth that maximizes the output SC bandwidth as well as the total output power.
Self-pulsating sources based on cascaded regeneration rely on two or more nonlinear stages whose function is to convert the propagating signal from one wavelength to another. When there are two nonlinear stages, the initial signal is shifted from the wavelength to the wavelength [[lambda].sub.2,1] via nonlinear wavelength converters (NWCs). This setup is composed of two HNLFs of length L = 1007 m, two adjustable and tunable BPFs, centered at the wavelengths [[lambda].sub.1,2], and with tunable 3 dB bandwidths [[OMEGA].sub.1,2], respectively.
The filter offset is defined as [DELTA[lambda]] = [absolute value of [lambda]1] - [lambda]2]]. The spectral components, SPM broadening occurs in the first few meters of the fiber, thereby shifting some energy towards the shorter wavelengths and resetting the central wavelength.
Pulses propagating in HNLF1 at [lambda]2 undergo spectral broadening by the conjugated effects of SPM and dispersion. After filtering at BPF1 and reamplification a similar spectral broadening is experienced by pulses in HNLF2, and finally BPF2 reestablished [lambda]2 as the central wavelength for the next cavity round-trip. Dispersive waves are also emitted as a result of these interactions, and the observed spectrum is similar to spectra arising from supercontinuum seeded by pico second pulses.
[gamma] = 2[pi][[pi].sub.2]/([lambda][A.sub.eff])
Solitons resulting of the propagation in HNLF2 experience a significant amount of SPM when propagating in HNLF1. Low-pass filtering at BPF1 do not extinct the significantly shifted solitons. However, they do not benefit from the gain of EDFA1, nor pass through BPF2. For other spectral components, SPM broadening occurs in the first few meters of the fiber, thereby shifting some energy towards the shorter wavelengthsand resetting the central wavelength.
Effect Of The Filter Bandwidths:
The output properties of SPM-SSFS sources were studied in  for fixed filter spectral positions and bandwidths. The source was started from ASE, as the pump power of EDFA1,2 was increased beyond a given power threshold. At one limiting case, BPF1 is a low-pass filter, and BPF2 is a high-pass filter. Self-pulsation occurs for a fixed EDFA pump power, by reducing the spectral separation between the BPFs, by red-shifting BPF2. For a BPF2 bandwidth of 3.5 nm, the continuum generated at the coupler is maximized, and reaches wavelengths past 1900 nm. For larger and smaller bandwidths, less energy is transferred towards the long wavelengths. Hence, there exist an optimal spectral bandwidth of BPF2 for which the captured spectral power density contributes optimally to sustain the existing pulses in the cavity.
In such a situation, the pulses filtered at BPF2 exhibit long temporal duration due to the accumulated dispersion, or contain a broad pedestal if compression is achieved by chirp compensation. The pulse energy is high due to the large amount of spectral components captured by the BPF, but it is spread over a long duration, which is non optimal for SC generation. BPF2 is first shifted towards the longer wavelengths to trigger selfpulsation, and the output power at the coupler is recorded at that moment.
Then, BPF2 is shifted in the opposite direction, and the wavelength at which the source stops pulsating is recorded. For filter bandwidths of 4.7 nm, pulses are sustained in the cavity up to a filter offset of [DELTA][lambda] = 3 nm. Spectrally, the continuum at the coupler shows insignificant changing when altering the filters bandwidth. Optimal filter bandwidths maximize the source efficiency by blocking the spectral content which does not contribute to the pulses.
Noise bins represent the noise by the average spectral density in two polarizations using a coarse spectral resolution. The main advantage of using noise bins is to cover the wide spectrum of the optical signals or to represent the noise outside the sample signal bandwidths.
Pulse Compression Stage:
In this paper, a remarkable pulse compression is realized through utilizing soliton pulse. Fig. 2 represents the general block diagram of pulse compression stage. The comb-like dispersion profile fiber (CDPF) structure is used by SMF and DSF. In this work, and after an optimization, around 30 dBm launch into ten parts are chosen of alternately arranged 140 m SMF segments with (a GVD value of D=17ps/nm/km at 1550 nm) as high-dispersion segments with a 140 m DSF segments with negligible low dispersion have zero dispersion at 1547 nm as low-dispersion segments with total length 1.4 km. Pulses in the CDPF are influenced alternatively by nonlinear effect and group velocity dispersion (GVD) effect in space and adiabatic optical soliton transmission can be maintained and evolved in anomalous dispersion region.
CR = [FWHM.sub.outputpulse]/[FWHM.sub.inputpulse] x 100
An optimal filter bandwidth leads to a broad SC extending beyond 1900 nm. A BPF2 bandwidth of 3.5 nm, the continuum generated at Coupler is maximized, and reaches wavelengths past 1900 nm. For larger and smaller bandwidths, less energy is transferred towards the long wavelengths. Hence, there exist an optimal spectral bandwidth of BPF2 for which the captured spectral power density contributes optimally to sustain the existing pulses in the cavity.
A remarkable performance is achieved having a low pulse CR (8 %).
CR = 0.9/10.6 x 100% = 8%
The operation of self-pulsating sources based on SPM regenerators as well as SSFS followed by offset filtering is characterized temporally and spectrally. An optimal filter bandwidth leads to a broad SC which extends past 1900 nm, and potentially the HNLF pumped closer to the zero dispersion wavelength. All-optical pulse compression and reshaping are key stages for realizing a remarkable high-quality pulse source. Several techniques were proposed to realize effective pulse compression stage. Among all, recently a soliton based pulse compression stage and a self-phase modulation (SPM) based pulse reshaping stage become an optimum choice. This work presents a simple design for a soliton based pulse compression stage. A remarkable performance is achieved having a low pulse CR(8 %). This design is a suitable candidate for realizing a remarkable pulse source for OTDM applications. Using soliton based compression, a very small pulse width can be produced but with pedestal which can be removed by an SPM based reshaping stage in future.
[1.] Sibbett, W., A.A. Lagatsky and C.T.A. Brown, 2012. "The development and application of femtosecond laser systems," Opt. Exp., 20(7): 6989-7001.
[2.] Sala, K., M. Richardson and N.R. Isenor, 1977. "Passive mode locking of lasers with the optical Kerr effect modulator," IEEE J. Quantum Electron., vol. QE-13, 11: 915-924.
[3.] Doran,N.J.and D.Wood, 1988. "Nonlinear-optical loop mirror," Opt. Lett., 13(1): 56-58.
[4.] Rochette, M., L.R. Chen, K. Sun and J. Hernandez-Cordero, 2008. "Multiwavelength and tunable selfpulsating fiber cavity based on regenerative SPM spectral broadening and filtering," IEEE Photon. Technol. Lett., 20(17): 1497-1499.
[5.] North, T. and M. Rochette, 2012. "Broadband self-pulsating fiber laser based on soliton self-frequency shift and regenerative self-phase modulation," Opt.Lett., 37(14): 2799-2801.
[6.] Nicholson, J.W., A.K. Abeeluck, C. Headley, M.F. Yan and C.G. Jorgensen, 2013. "Pulsed and continuouswave supercontinuum generation in highly nonlinear, dispersion-shifted fibers," Appl. Phys. B, 77(2-3): 211-218.
[7.] Takushima, Y., 2005. "High average power, depolarized supercontinuum generation using a 1.55-nm ASE noise source," Opt. Exp.,13(15): 5871-5877.
[8.] Hernandez-Garcia, J.C., O. Pottiez, J.M. Estudillo-Ayala and R. Rojas- Laguna, 2012. "Numerical analysis of a broadband spectrum generated in a standard fiber by noise-like pulses from a passively mode-locked fiber laser," Opt. Commun., 285(7): 1915-1919.
[9.] Runge, A.F.J., C. Aguergaray, N.G.R. Broderick and M. Erkintalo, 2013. "Coherence and shot-to-shot spectral fluctuations in noise-like ultrafast fiber lasers," Opt. Lett., 38(21): 4327-4330.
(1) B.Selva priya and (2) C.Mahendran
(1) Department of Electronics and Communication Engineering
(2) Alagappa Chettiar College of Engineering and Technology,Karaikudi,Tamilnadu,India.
Received 28 February 2017; Accepted 29 April 2017; Available online 2 May 2017
Address For Correspondence:
B. Selva priya, Department of Electronics and Communication Engineering
Caption: Fig. 1: Self-pulsating source based on cascaded regeneration.
Caption: Fig. 2: Pulse compression stage and structure of CDPF
Caption: Fig. 3: Generation of Supercontinuum
Caption: Fig. 4: Sampled signal spectrum
Caption: Fig. 5: Input optical pulse
Caption: Fig. 5: Pulse compression
Caption: Fig. 6: Pulse compression in 3D view
Edfa: erbium-doped fiber amplifier Highly Non linear fiber(HNLF) [gamma] 12.5 [w.sup.-1] [km.sup.-1] [D.sub.1] -0.71 ps/(nm.km) [D.sub.2] 2.09 ps/(nm.km) [S.sub.1] 0.0074 ps/([nm.sup.2].km) [S.sub.2] 0.002 ps/([nm.sup.2].km) [A.sub.eff] 6.3933 [micro]m Insertion losses [BPF.sub.1] 8 dBm [BPF.sub.2] 5.5 dBm EDFA [P.sub.sat] 15 dBm Table I:Output Powers For Various Bpf [BPF.sub.1] [BPF.sub.2] OUTPUT POWER OUTPUT POWER B/W in nm B/W in nm Max in dB Min in dB 6 5 -40.9815 -102.81 0.2 1.5 -47.7304 -102.48 2.5 3.5 -42.4711 -102.73 4 6 -40.4233 -102.83 7 12 -41.7679 -102.77
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|Author:||Priya, B. Selva; Mahendran, C.|
|Publication:||Advances in Natural and Applied Sciences|
|Date:||May 1, 2017|
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