Abstract:Coherent propagation of supermodes in a multicore fiber is promising for power scaling of fiber laser systems, eliminating the need for the active feedback system to maintain the phases between the channels. We studied the propagation of broadband pulsed radiation at a central wavelength of 1030 nm in a multicore fiber with coupled cores arranged in a square array. We designed and fabricated a silica multicore fiber with a 5 × 5 array of cores. For controllable excitation of a desired supermode, we developed a… Show more
“…This assumption is accurate when the step size of SSF is smaller than or equal to the coupling length 𝐿 𝑐 . In this paper, we utilize the coupling length 𝐿 𝑐 = 1/𝐾 𝑎𝑏 as a parameter to investigate IC-XT influence to submarine cables [16]. Here, we typically investigate the 4-core SC-MCF [13] to compare the 4-core WC-MCF for the trans-Atlantic and Pacific cables.…”
Section: Q Factor Evaluations For the Wc-mcfs And Sc-mcfs Submarine C...mentioning
The practical cable design for optical submarine communications has a limited fiber pair count due to the mechanical considerations of cable weight and size. Consequently, multi-core fibers (MCFs) could exhibit higher capacity than the conventional single-mode fibers (SMFs) thanks to space division multiplexing (SDM). That is because the power supply to a submarine cable is fed by the voltage difference between shores.
Under the power limited condition, SDM improves the cable capacity by using more paths which outperforms the SMF link whose capacity approximately complies with a logarithmic relationship to optical power.
At the same time, fiber nonlinearity can be alleviated by the reduced power density of transmitted light in MCFs, due to the increased spatial diversity and mode coupling among coupled cores. In this work, we theoretically investigate the potentials of MCFs including weakly-coupled mutlicore fiber (WC-MCF) and strongly-coupled multicore fiber (SC-MCF) as the propagation media for submarine communications across the Atlantic and the Pacific. To fairly compare the performances of SMFs- and MCFs-based submarine cables, Gaussian noise (GN) model for SDM links is employed to optimize the systematic settings including modulation format, optical signal-to-noise ratio (OSNR) and single span length. Then, we develop an SDM and wavelength division multiplexing (WDM) fiber transmission model based on coupled nonlinear Schrodinger equations (CNSE) to investigate the optical filed coupling effect in MCFs-based cables. Developed transmission model has been self-examined by measuring the inter-core crosstalk (IC-XT) and spatial mode dispersion (SMD), referring to the set values. As indicated by the theoretical analysis, the WC-MCFs cable exhibits larger capacity than the SMFs cable, when fiber pair count is limited below 32. Moreover, the SC-MCFs cable outperforms the WC-MCFs cable thanks to the reduced fiber nonlinearity due to the random mode coupling and the assitance of multiple-input and multiple-output digital signal processing (MIMO-DSP). At last, the marginal influences of IC-XT, SMD and insertion loss of Fan-in and Fan-out couplers are also analyzed for the MCFs cable.
“…This assumption is accurate when the step size of SSF is smaller than or equal to the coupling length 𝐿 𝑐 . In this paper, we utilize the coupling length 𝐿 𝑐 = 1/𝐾 𝑎𝑏 as a parameter to investigate IC-XT influence to submarine cables [16]. Here, we typically investigate the 4-core SC-MCF [13] to compare the 4-core WC-MCF for the trans-Atlantic and Pacific cables.…”
Section: Q Factor Evaluations For the Wc-mcfs And Sc-mcfs Submarine C...mentioning
The practical cable design for optical submarine communications has a limited fiber pair count due to the mechanical considerations of cable weight and size. Consequently, multi-core fibers (MCFs) could exhibit higher capacity than the conventional single-mode fibers (SMFs) thanks to space division multiplexing (SDM). That is because the power supply to a submarine cable is fed by the voltage difference between shores.
Under the power limited condition, SDM improves the cable capacity by using more paths which outperforms the SMF link whose capacity approximately complies with a logarithmic relationship to optical power.
At the same time, fiber nonlinearity can be alleviated by the reduced power density of transmitted light in MCFs, due to the increased spatial diversity and mode coupling among coupled cores. In this work, we theoretically investigate the potentials of MCFs including weakly-coupled mutlicore fiber (WC-MCF) and strongly-coupled multicore fiber (SC-MCF) as the propagation media for submarine communications across the Atlantic and the Pacific. To fairly compare the performances of SMFs- and MCFs-based submarine cables, Gaussian noise (GN) model for SDM links is employed to optimize the systematic settings including modulation format, optical signal-to-noise ratio (OSNR) and single span length. Then, we develop an SDM and wavelength division multiplexing (WDM) fiber transmission model based on coupled nonlinear Schrodinger equations (CNSE) to investigate the optical filed coupling effect in MCFs-based cables. Developed transmission model has been self-examined by measuring the inter-core crosstalk (IC-XT) and spatial mode dispersion (SMD), referring to the set values. As indicated by the theoretical analysis, the WC-MCFs cable exhibits larger capacity than the SMFs cable, when fiber pair count is limited below 32. Moreover, the SC-MCFs cable outperforms the WC-MCFs cable thanks to the reduced fiber nonlinearity due to the random mode coupling and the assitance of multiple-input and multiple-output digital signal processing (MIMO-DSP). At last, the marginal influences of IC-XT, SMD and insertion loss of Fan-in and Fan-out couplers are also analyzed for the MCFs cable.
“…We studied a silica-based MCF consisting of a square array of 5 × 5 cores with diameters of about 6 µm, numerical aperture (NA) = 0.12, and the distance between the nearest cores of 8.5 µm (figures 1(b) and (c)). Details of the fibre design and manufacturing technology are presented in [12]. To measure the dispersion for the fundamental and highest supermodes, we used an interferometric scheme based on a Mach-Zehnder interferometer with a 67 cm MCF located in the 1st arm and a free-space motorized delay line located in the 2nd arm for the compensation of a group delay.…”
Section: Experimental Studymentioning
confidence: 99%
“…In our experiment >90% of the pulse power was contained in the respective supermode. The experimental details can be found in [12]. The spatial phase distributions of selectively excited in-phase and out-of-phase supermodes are presented in figures 2 (a) and (b), respectively.…”
Section: Experimental Studymentioning
confidence: 99%
“…paid to studies of the fundamental in-phase supermode with the same spatial phases in all cores [9]. At the same time, the recent works demonstrated that the highest out-of-phase supermode (with the spatial phase difference of π in the nearest cores) is also of great importance due to its stability in nonlinear regimes [10][11][12]. Group velocity dispersion (GVD) impacts significantly on the nonlinear dynamics of ultrashort optical pulses with high peak powers, so its analysis is highly important for MCFs.…”
In-phase and out-of-phase supermodes were selectively excited (with modal content >90%) in the wavelength range near 1030 nm in a silica multicore fibre with 5 × 5 coupled cores using a spatial light modulator. Group velocity dispersion (GVD) parameters of 21 ps2 km−1 and 14 ps2 km−1 at 1030 nm were measured for in-phase and out-of-phase supermodes, respectively, using an interferometric scheme. The numerically simulated GVD values agree with the experimental results. The calculated zero-dispersion wavelengths (ZDWs) of 1360 nm and 1180 nm for in-phase and out-of-phase supermodes are red-shifted and blue-shifted, respectively, compared to the ZDW of silica glass. The anomalous dispersion for the out-of-phase supermode is predicted in the telecommunication O-band near 1300 nm. The theoretical explanation of the difference in the wavelength-dependence of GVD for in-phase and out-of-phase supermodes is given.
“…In recent years, the propagation of laser radiation in multicore fibers (MCF) with weak coupling between the cores has attracted much attention. [1][2][3][4][5][6] Thanks to the use of such fibers, it becomes possible to amplify coherently high-power laser pulses with the maintaining of radiation characteristics, 7,8 and it also becomes possible to combine radiation from different laser sources into one beam with minimal power loss. 9 Powerful ultrashort laser pulses can further be used for material processing, medicine, spectroscopy, etc.…”
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