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Review Article

All-optical XOR gates based on dual semiconductor optical amplifiers

, & | (Reviewing editor)
Article: 1660495 | Received 16 Oct 2018, Accepted 04 Aug 2019, Published online: 05 Sep 2019

Figures & data

Figure 1. Schematic diagram of the dual SOA-MZI-based XOR gate. BPF: bandpass filter centered at λ2. Two phase shifters are used to induce a π phase difference at two arms.

Figure 1. Schematic diagram of the dual SOA-MZI-based XOR gate. BPF: bandpass filter centered at λ2. Two phase shifters are used to induce a π phase difference at two arms.

Figure 2. (a) The QD-SOA density of state as a function of transition energy. (b) A schematic of carrier dynamics in an InAs/GaAs QD-SOA. Quantum dots are embedded in the wetting layer.

Figure 2. (a) The QD-SOA density of state as a function of transition energy. (b) A schematic of carrier dynamics in an InAs/GaAs QD-SOA. Quantum dots are embedded in the wetting layer.

Figure 3. Simulation results of XOR gates operating at 250 Gb/s from a dual QD-SOA MZI scheme.

Figure 3. Simulation results of XOR gates operating at 250 Gb/s from a dual QD-SOA MZI scheme.

Figure 4. Calculated 250 Gb/s operation quality factor Q at different single pulse energy and transition lifetime from QD excited state to ground state. Injected current density is set to 1.8 kA/cm2. (a): Q factor dependence on single pulse energy, τe-g = 1 ps. (b): Q factor dependence on ES to GS transition lifetime, single pulse energy is 0.5 pJ. Q > 6 is typically needed for bit-error-rate of <10−9. The above figure shows Q > 6 is obtained at 250 Gb/s for pulse width of ~1 ps.

Figure 4. Calculated 250 Gb/s operation quality factor Q at different single pulse energy and transition lifetime from QD excited state to ground state. Injected current density is set to 1.8 kA/cm2. (a): Q factor dependence on single pulse energy, τe-g = 1 ps. (b): Q factor dependence on ES to GS transition lifetime, single pulse energy is 0.5 pJ. Q > 6 is typically needed for bit-error-rate of <10−9. The above figure shows Q > 6 is obtained at 250 Gb/s for pulse width of ~1 ps.

Figure 5. Calculated gain and phase change in an SOA due to a series of pulses shown in (a). (b) Gain modulation as a function of time, (c) phase modulation due to gain modulation as a function of time. The gain plotted is the value of G. (d) total phase modulation including two-photon absorption as a function of time. Note the periodic total phase change is primarily due to two-photon absorption in (d).

Figure 5. Calculated gain and phase change in an SOA due to a series of pulses shown in (a). (b) Gain modulation as a function of time, (c) phase modulation due to gain modulation as a function of time. The gain plotted is the value of G. (d) total phase modulation including two-photon absorption as a function of time. Note the periodic total phase change is primarily due to two-photon absorption in (d).

Figure 6. Simulation results of XOR gates operating at 250 Gb/s from a TPA based dual SOA MZI scheme. Data A and Data B are shown on the left. XOR and an eye pattern (after 100 pseudo-random A and B bits) are shown on the right.

Figure 6. Simulation results of XOR gates operating at 250 Gb/s from a TPA based dual SOA MZI scheme. Data A and Data B are shown on the left. XOR and an eye pattern (after 100 pseudo-random A and B bits) are shown on the right.

Figure 7. The calculated quality factor Q at different operating bit-rates and different input data stream average powers. Q > 6 is typically needed for bit-error-rate of <10−9. The above figure shows Q > 6 is obtained at 250 Gb/s for input powers of 24 dBm.

Figure 7. The calculated quality factor Q at different operating bit-rates and different input data stream average powers. Q > 6 is typically needed for bit-error-rate of <10−9. The above figure shows Q > 6 is obtained at 250 Gb/s for input powers of 24 dBm.

Figure 8. A schematic of carrier dynamics with TPA in an InAs/GaAs QD-SOA.

Figure 8. A schematic of carrier dynamics with TPA in an InAs/GaAs QD-SOA.

Figure 9. Simulation results of XOR gates operating at 320 Gb/s without the consideration of TPA. The input single pulse energy is 0.5 pJ and pulse width is 1 ps.

Figure 9. Simulation results of XOR gates operating at 320 Gb/s without the consideration of TPA. The input single pulse energy is 0.5 pJ and pulse width is 1 ps.

Figure 10. Simulation results of XOR gates operating at 320 Gb/s with the effects of TPA. The input single pulse energy is 0.5 pJ and pulse width is 1 ps.

Figure 10. Simulation results of XOR gates operating at 320 Gb/s with the effects of TPA. The input single pulse energy is 0.5 pJ and pulse width is 1 ps.

Figure 11. The dependence of Q factor on single pulse energy. The injected current is fixed at 250 mA and pulse width is 1 ps. (b) The dependence of Q factor on injected current. The input single pulse energy is fixed at 0.5 pJ and pulse width is 1 ps. (c) The dependence of Q factor on pulse width/bit period ratio at 320 Gb/s. Note that Q > 6 (needed for bit-error-rate < 10−9) can be obtained. The injected current is fixed at 250 mA and single pulse energy is set at 0.5 pJ. (d) The dependence of Q factor on data rate. The single pulse energy is 0.5 pJ and injected current is 250 mA. The ratio of the pulse width to bit period is fixed.

Figure 11. The dependence of Q factor on single pulse energy. The injected current is fixed at 250 mA and pulse width is 1 ps. (b) The dependence of Q factor on injected current. The input single pulse energy is fixed at 0.5 pJ and pulse width is 1 ps. (c) The dependence of Q factor on pulse width/bit period ratio at 320 Gb/s. Note that Q > 6 (needed for bit-error-rate < 10−9) can be obtained. The injected current is fixed at 250 mA and single pulse energy is set at 0.5 pJ. (d) The dependence of Q factor on data rate. The single pulse energy is 0.5 pJ and injected current is 250 mA. The ratio of the pulse width to bit period is fixed.