Mamyshev 2R regenerator

The Mamyshev regenerator can handle return-to-zero signals with ultrahigh data bit rates. Indeed, thanks to the quasi-instantaneous response of the nonlinear Kerr effect, this regenerator does not suffer from the finite recover time of some saturable absorbers.

The interest of the Mamyshev regenerator lies in its ability to regenerate simultaneously the 'ones' and 'zeros' bit of information.

The key effect affecting the pulse evolution in the regenerator is the self-phase modulation that broadens the spectrum in proportion to the intensity of the initial optical pulse. Combined with an output frequency offset OBPF, this constitutes an efficient ultrafast thresholder. In more details, low intensity pulses or noise do not broaden significantly and fall outside of the off-centered BPF and hence the output for the noisy 0's in the data stream are reduced to the zero floor. On the contrary, for the 1's data pulses the intensity is sufficiently strong to broaden the spectra by SPM, and a significant portion of the spectrum falls into the OBPF passband, leading to a generation of the output 1's pulse.

For a careful design of the regenerator and an appropriate combination of filter parameter (spectral offset and bandwidth) / fiber parameter (length, dispersion and nonlinearity values),^[8][9] a reduction of amplitude fluctuations can also be achieved, leading to power equalization of the pulse stream.

The modelling results for the 2R regenerator are shown with the article. In Figure 1, the upper panel shows regenerated pulse from the input (lower panel) for the Mamyshev 2R regenerator. The noisy 1's pulses are boosted to same power levels in the output, while the 0's pulses are reduced to the noise floor.

An important property of a Mamyshev regenerator is its transfer function that links the output peak power to the input peak power. For an efficient operation and power equalization, this transfer function should exhibit a marked plateau at the 1's power level.^[9] Example of a transfer function is provided Figure 2.

The spectral operations of broadening, filtering and regeneration about the central wavelength are shown in Figure 3.

In the design of this nonlinear regenerator, care should be given to avoid the consequences of deleterious Brillouin backscattering^[10] as well as pulse to pulse interaction leading to patterning effects in the output sequence.^[9][10]

Due to the spectral filtering process, the regenerated pulse is intrinsically shifted from the original frequency. This can be beneficial if wavelength conversion is to be achieved simultaneously the regeneration and therefore channel switching can be considered.^[11] However, if one wants to recover an output signal having the initial wavelength, an option of applying another regeneration with the BPF center frequency placed at the original channel center frequency allows to overcome this problem. This can be done in a single fiber using a bidirectional propagation in the nonlinear fiber.^[12]

The Mamyshev regenerator in its standard configuration is limited to single-wavelength operation in order to prevent from cross-phase modulation (XPM) effects from adjacent channels. Several schemes have been proposed to extend its region of operation to multichannel regime.

In their work on Four-wave mixing (FWM) compensation by using a HLNF and its XPM, Michael Vasilyev and co-workers have proposed,^[13] and demonstrated up to 12-channel optical regeneration in 10 Gbit/s systems.^[14]

In other work, taking advantage of counter-propagating scheme, double wavelength regeneration has been demonstrated.^[15] The number of channels that can be handled has been increased up to four thanks to polarization multiplexing.^[16]

Efficient all-optical regeneration based on Mamyshev device has been demonstrated at various repetition rates : 10 Gbit/s, 40 Gbit/s and up to 160 Gbit/s.^[11]

The Mamyshev regenerator may suffer from a poor yield : the spectral filtering of the expanded spectrum induces high intrinsic energy loss. In order to compensate those losses, distributed Raman amplification can be involved.^[17]

The 2R regeneration can be combined with an additional stage of regeneration to provide 3R regeneration.^[11][18]

Mamyshev technique has also been used for OCDMA transmission^[19] and it has been proposed to use the Mamyshev setup in the framework of optical performance monitoring.^[20] The reshaping features of the Mamyshev regenerator have also been combined with a polarization attraction process that enables to simultaneously regenerate thepolarization state and the intensity profile of degraded pulse streams.^[21]

The potential applications of Mamyshev regenerators are not restricted to the field of optical telecommunications. This technique has also been found beneficial in the field of ultrashort and high peak power pulse generation. Indeed, the background improvement and reshaping features of Mamyshev regenerators have opened new perspectives to the use of gain switched lasers and have allowed subpicosecond pulses with peak powers exceeding the megaWatt level to be generated in so-called Mamyshev Oscillators.^[22] Other example has been achieved with the contrast enhancement by several orders of magnitude of mJ femtosecond pulse in Argon-filled hollow core fiber.^[23]

Concatenation of pairs of Mamyshev regenerators has been numerically studied and has shown that well-defined structures could spontaneously emerge from an oscillator architecture,^[24][25] which has then been experimentally confirmed.^[26] Additional investigations have focused on the development of ultrashort high peak power fiber lasers ^[27][28] and other cavity designs have been considered.^[29][30] In 2017, record peak powers well above the MW level have been reached.