Abstract:We report a substantial increase in PMD tolerance in a single-channel ultrahigh-speed transmission using optical Nyquist pulses. We demonstrate both analytically and experimentally a large reduction in depolarization-induced crosstalk with optical Nyquist pulses, which is one of the major obstacles facing polarization-multiplexed ultrashort pulse transmission. By taking advantage of the high PMD tolerance, a low-penalty 1.28 Tbit/s/ch optical Nyquist TDM transmission at 640 Gbaud was achieved over 525 km.
“…Being compared to conventional OTDM systems, long distance transmission of Nyquist OTDM is possible thanks to the improved dispersion and polarization mode dispersion (PMD) tolerances due to the significant reduction of the signal bandwidth through the optical Nyquist filtering [12,13]. Highly accurate dispersion compensation is necessary to maintain the orthogonality of the Nyquist pulses in time domain at the receiver.…”
Section: Transmission and Add-drop Operationsmentioning
confidence: 99%
“…Since the raised cosine waveform causes interference between neighboring tributaries, CR for Nyquist OTDM is hardly possible even by the state-of-the-art ultrafast CR techniques. This issue, however, has not been addressed in the transmission demonstrations [5,6,12,13]. We have carried out a stable CR scheme for Nyquist OTDMs with baudrate up to 344 Gbaud [9] by using the optical null-header insertion [14].…”
Section: Transmission and Add-drop Operationsmentioning
All-optical Nyquist filtering allows generation of coarse-granular, flexible, spectrally-efficient signals. This talk reviews important technologies for applications of Nyquist OTDM-WDM to elastic optical network including transmission, add/drop operations, spectral defragmentation.
“…Being compared to conventional OTDM systems, long distance transmission of Nyquist OTDM is possible thanks to the improved dispersion and polarization mode dispersion (PMD) tolerances due to the significant reduction of the signal bandwidth through the optical Nyquist filtering [12,13]. Highly accurate dispersion compensation is necessary to maintain the orthogonality of the Nyquist pulses in time domain at the receiver.…”
Section: Transmission and Add-drop Operationsmentioning
confidence: 99%
“…Since the raised cosine waveform causes interference between neighboring tributaries, CR for Nyquist OTDM is hardly possible even by the state-of-the-art ultrafast CR techniques. This issue, however, has not been addressed in the transmission demonstrations [5,6,12,13]. We have carried out a stable CR scheme for Nyquist OTDMs with baudrate up to 344 Gbaud [9] by using the optical null-header insertion [14].…”
Section: Transmission and Add-drop Operationsmentioning
All-optical Nyquist filtering allows generation of coarse-granular, flexible, spectrally-efficient signals. This talk reviews important technologies for applications of Nyquist OTDM-WDM to elastic optical network including transmission, add/drop operations, spectral defragmentation.
“…High spectral single-channel transmission has become the target of intensive research as required by the growing demand for network resource. Nyquist optical time-division multiplexing (N-OTDM) [1] has been a research interest due to its capability to achieve fundamental minimum bandwidth, as well as its tolerance to transmission impairments such as chromatic dispersion [2], polarization mode dispersion [3], and self-phase modulation [4]. Combined with other multiplexing techniques, it has been proved to achieve an ultra large transmission capacity of 43 Tbit/s [5].…”
Demultiplexing of high-speed Nyquist optical time-division multiplexed (N-OTDM) signal requires ultra-narrow local sampling pulse to avoid the severe inter-symbolinterference (ISI) between each tributary. Unfortunately, generation of such narrow sampling pulse is difficult or usually need complex setup configure at the receiver side, which would cause ineffective cost in application scenarios such as short-reach optical communication or PON applications. In this paper, we propose and demonstrate demultiplexing of N-OTDM signal based on temporal magnification followed by coherent optical sampling to enable broader sampling pulsewidths while reducing the ISI. The target tributary of the N-OTDM signal is temporally magnified and further demultiplexed through coherent optical sampling using Gaussian-shaped or Nyquist-shaped pulses. With the aid of temporal magnification based on a time-lens, the sampling window can be extended during the coherent detection progress at the receiver side. Gaussian sampling pulses with a pulsewidth up to 10.4 ps are enabled for the demultiplexing of a 160 Gbaud N-OTDM signal. Compared with demultiplexing based on Nyquist pulses (i.e., coherent matched sampling) without temporal magnification, the proposed scheme features a better performance with pulsewidths greater than 6 ps. If temporal magnification is combined with coherent matched sampling, Nyquist sampling pulses with a pulsewidth up to 12.4 ps are made possible for the demultiplexing. Therefore, the proposed scheme based on temporal magnification could significantly release the pulsewidth requirement for N-OTDM demultiplexing while mitigating the ISI.
“…The conventional NRZ-to-RZ format conversion schemes cannot generate the Nyquist-shaped RZ signal. Several approaches have been demonstrated for optical Nyquist pulse generation, such as electrical Nyquist filtering [6], temporal optical pulse-shaping [7] and cascaded Mach À Zehnder modulators (MZMs) [8]. However, these existing Nyquist pulse generation methods cannot be simply adapted for the NRZ-to-RZ format conversion.…”
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