Abstract:For 64-Gbaud operation and beyond, we developed a power efficient high-bandwidth coherent driver modulator composed of a linear four-channel ultra-low power CMOS driver IC and an InP-based dual-polarization IQ modulator. The CMOS driver was fabricated in 65-nm CMOS technology and showed power dissipation of <1 W owing to the use of an open-drain configuration and a stacked current-mode architecture. Moreover, by optimizing the temperature of the thermoelectric cooler that controls the modulator operating tempe… Show more
“…So, a semiconductor optical amplifier (SOA) is an ideal optical shutter because the ACT of a laser cavity does not have to be dynamically turned off/on. Furthermore, unlike an electro-absorption (EA) modulator [14,15] and a Mach-Zehnder (MZ) modulator [16][17][18], it is possible to obtain a high extinction ratio (ER) without wavelength-dependent bias control proven in the form of SOA gate switches [19][20]. A residual issue in using an SOA as an optical shutter is thermal crosstalk from the SOA to the laser cavity, which results in a laser frequency drift [21][22][23][24][25].…”
A spurious wavelength (spurious) from a tunable laser during tuning is an issue in optical systems based on dynamically controlled laser wavelengths. Output shuttering synchronized with tunable-laser tuning is promising way to suppress spurious. A semiconductor optical amplifier (SOA) is an ideal shutter for laser outputs with spurious in terms of lowwavelength-independent extinction ratio. We developed an electro-optically tunable reflection-type transversal filter (RTF) laser monolithically integrated with an SOA. Thanks to the nanosecond scale tuning speed of the RTF laser, the required shuttering time of the integrated SOA is also a corresponding nanosecond scale, which leads to little temperature change in the laser cavity. As a result, the laser frequency drift after turning off/on the SOA is suppressed to within +/-2.5 GHz without any additional laser control algorithm to compensate for the thermal crosstalk from the SOA. Using the laser, we demonstrated a "hitless" wavelength-switching subsystem based on a coherent format. Namely, outputs from an SOA-RTF laser coded with 32-GBd dual-polarization quadrature phase-shift keying (128 Gbps) are dynamically switched with spurious eliminated by SOA shuttering. In addition to practical bit error rates (BERs) of wavelength channels from the SOA-RTF laser, we observe no interference with the BER of a wavelength channel from another monitor laser in the wavelength-switching subsystem.
“…So, a semiconductor optical amplifier (SOA) is an ideal optical shutter because the ACT of a laser cavity does not have to be dynamically turned off/on. Furthermore, unlike an electro-absorption (EA) modulator [14,15] and a Mach-Zehnder (MZ) modulator [16][17][18], it is possible to obtain a high extinction ratio (ER) without wavelength-dependent bias control proven in the form of SOA gate switches [19][20]. A residual issue in using an SOA as an optical shutter is thermal crosstalk from the SOA to the laser cavity, which results in a laser frequency drift [21][22][23][24][25].…”
A spurious wavelength (spurious) from a tunable laser during tuning is an issue in optical systems based on dynamically controlled laser wavelengths. Output shuttering synchronized with tunable-laser tuning is promising way to suppress spurious. A semiconductor optical amplifier (SOA) is an ideal shutter for laser outputs with spurious in terms of lowwavelength-independent extinction ratio. We developed an electro-optically tunable reflection-type transversal filter (RTF) laser monolithically integrated with an SOA. Thanks to the nanosecond scale tuning speed of the RTF laser, the required shuttering time of the integrated SOA is also a corresponding nanosecond scale, which leads to little temperature change in the laser cavity. As a result, the laser frequency drift after turning off/on the SOA is suppressed to within +/-2.5 GHz without any additional laser control algorithm to compensate for the thermal crosstalk from the SOA. Using the laser, we demonstrated a "hitless" wavelength-switching subsystem based on a coherent format. Namely, outputs from an SOA-RTF laser coded with 32-GBd dual-polarization quadrature phase-shift keying (128 Gbps) are dynamically switched with spurious eliminated by SOA shuttering. In addition to practical bit error rates (BERs) of wavelength channels from the SOA-RTF laser, we observe no interference with the BER of a wavelength channel from another monitor laser in the wavelength-switching subsystem.
“…as a coherent driver modulator (CDM) [4][5][6] and an intradyne coherent receiver (ICR) [6][7][8], are key components for highspeed multi-level operation. These components integrate optical and electrical devices in one package to reduce the RF loss, footprint and cost.…”
Section: Introductionmentioning
confidence: 99%
“…InP modulator chips have been commonly used for CDMs [5,6] because they can achieve high bandwidth with a low driving voltage and a small footprint [9,10]. Recently, novel CDM using a thin-film LiNbO3 (TFLN) modulator was demonstrated [11].…”
We developed an InP-based coherent driver modulator (CDM) with a flexible printed circuit (FPC) RF interface. The CDM has a 3-dB electro-optic (EO) bandwidth of over 85 GHz, including the evaluation board loss, which is sufficient for 1-Tb/s/-class operation. Furthermore, we obtained good back-to-back bit-error-rate (BER) performance in modulations up to 144-Gbaud dual-polarization 16-QAM, and we confirmed the CDM's capability for operation over the 150-Gbaud class. With the FPC RF interface, a package's roll-off frequency above 100 GHz was demonstrated in both measured and simulated results. The CDM includes an InP-based n-i-p-n heterostructure modulator chip with a differential capacitively loaded travelingwave electrode (CL-TWE) and a 4-channel linear SiGe BiCMOS driver IC with an open-collector configuration and low wire inductance. The modulator chip has an EO 3-dB bandwidth of over 70 GHz, which is an improvement of about 30 GHz over that of a conventional p-i-n structure. In addition, to facilitate future 200-Gbaud-class operation, a simulation with a reduced GND via diameter confirmed that the package's roll-off frequency can be improved to more than 120 GHz. Moreover, by reducing the CL-TWE period and the metal's DC resistance, the n-i-p-n modulator chip achieve an EO 3-dB bandwidth of 90 GHz or more.
“…Regarding optical IQ modulator chips that are assembled in the HB-CDM, InP-based IQ modulators have been used for their superior material properties that enable them to achieve high speeds and low driving voltages with a small footprint [4,5]. An InP IQ modulator with 3-dB electro-optic (EO) bandwidth of 80 GHz and half-wave voltage (Vπ) of 1.5 V has J. Ozaki, Y. Ogiso, Y. Hashizume, and M. Ishikawa are with NTT Device Innovation Center, Nippon Telegraph and Telephone Corporation, Atsugi, Kanagawa 243-0198, Japan (e-mail: josuke.ozaki.mp@hco.ntt.co.jp; yoshihiro.ogiso.uv@hco.ntt.co.jp; yasuaki.hashizume.ph@hco.ntt.co.jp; mitsuteru.ishikawa.pe@hco.ntt.co.jp).…”
We developed a flexible printed circuit (FPC) RF interface InP-based high-bandwidth coherent driver modulator (CDM) for 128-Gbaud class operations. To increase the bandwidth of the CDM, an FPC RF interface was introduced to the CDM package, which significantly improved the roll-off frequency by about 40 GHz compared with a conventional package with a surface-mount-type RF interface. The FPC package has a 3-dB bandwidth of about 75 GHz and roll-off frequency above 110 GHz. These are the best characteristics among the CDM packages reported so far. By integrating a modulator with an electro-optic (EO) 3-dB bandwidth of >67 GHz and a driver IC with an electrical 3-dB bandwidth of >75 GHz in this package, the CDM had an EO 3-dB bandwidth of >72 GHz. This EO 3-dB bandwidth is sufficient for 128 Gbaud-class operations. Furthermore, we performed 128-Gbaud dual polarization 16QAM modulations and confirmed good back-to-back bit-error-rate characteristics.
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