Abstract:In this paper, we demonstrate that forward bias (+0.9V) of a high-speed silicon (Si) optical Mach-Zehnder modulator (MZM) increases the radio-frequency (RF) link gain by 30 dB when compared to reverse bias operation (-8V). RF applications require tunable, narrowband electro-optic conversion with high gain to mitigate noise of the optical receiver and realize high RF spur-free dynamic range. Compared to reverse bias, the forward bias gain rolls off more rapidly but offers higher RF link gain improvement of more… Show more
“…It can be clearly seen that under 3-port operation the device can not only provide us with a smaller RAM (0.18 vs. 1.6 dB) but also a smaller V π (0.18 vs. 0.22 V). The achieved RAM number (0.18 dB) is also much smaller than that reported for Si-photonic MZI under forward bias operation, where the RAM is usually as high as 2 dB [4], [5]. The smaller RAM of our device can be mainly attributed to the corresponding sweeping current (I peak − I valley ) for V π being as small as 2 mA.…”
Section: Device Structurementioning
confidence: 55%
“…linking gain is difficult on the SiP platform due to the fact that the required driving voltage for the π phase-shift at the reverse bias regime of Silicon based modulators is usually large (nearly ten volts) [3]- [5]. Increasing the p-type doping density in the active volume is one of the most effective ways to reduce the driving-voltage, but this leads to a significant optical insertion loss [3], [4].…”
Section: Introductionmentioning
confidence: 99%
“…Thermo-optics resistive phase-shifters are popular because of their simple structure and small footprint [7]- [12], but device performance has been constrained by large power consumption (>12mW) and longer than µs scale switching/response time. On the other hand, the more conventional Mach-Zehnder interferometers (MZI) require high driving voltages (>6V; under reverse bias) for the π phase shift [4], [5], [13]. This impedes their application in optical phase arrays (OPA), which usually need to have hundreds of optical phase-shifters inside with a lowdriving voltage for >2π phase shifting [10]- [12].…”
Section: Introductionmentioning
confidence: 99%
“…This has been the most effective method to reduce the 2π driving-voltage but at the expense of lower modulation speed and higher power consumption [4], [5] as compared to MZIs operated under a reverse bias. Although the forward bias gain rolls off more rapidly with the increase of operating frequency, it offers a higher RF link gain improvement of more than 10 dB from nearly DC to 25 GHz [5]. Furthermore, forward bias operation is shown to result in a comparable spurious-free dynamic range [5].…”
Section: Introductionmentioning
confidence: 99%
“…Although the forward bias gain rolls off more rapidly with the increase of operating frequency, it offers a higher RF link gain improvement of more than 10 dB from nearly DC to 25 GHz [5]. Furthermore, forward bias operation is shown to result in a comparable spurious-free dynamic range [5]. Nevertheless, large (>2 dB) residual-amplitude-modulation (RAM), which leads to undesirable AM noise during phase modulation, usually happens in these forward-bias based p-n junction phase-shifters due to the free-carrier absorption loss induced by the high level injection carriers [4], [5].…”
A three-port optical phase-shifter and Mach-Zehnder modulator (MZM) based on PNP-type bipolar junction transistor (BJT) is demonstrated. Significant plasma (injected carrier) induced changes of the refractive index for the optical waveguide become possible with an extremely small driving-voltage and a compact device size during operation of this BJT between the saturation and forward active modes. Devices with a standard MZM structure and a small footprint (0.5 mm) exhibit a moderate optical insertion loss (2 dB), extremely small V π (0.18V) and P π (0.21mW), fast rise/fall time (∼1ns), and a residue-amplitudemodulation (RAM) as small as 0.18 dB. Furthermore, thanks to the ultra-high modulation efficiency characteristic of our device, a +4.0 dB net RF-linking gain can be obtained under dynamic operation. Compared to 2-port (base-collector) forward bias operation, under three-port operation, the extra bias current from the base-emitter junction provides a lower V π (0.18 vs. 0.22 V), a smaller RAM (0.18 vs. 0.6 dB), and a larger RF-linking gain (+4 vs. −3.2 dB). The superior performances of the three-port to two-port operations can be attributed to the additional forward bias BE junction being able to provide more injected carriers to induce stronger plasma effects for optical phase-shifting. INDEX TERMS Optical phase shifter, photonics integrated circuits, RF-linking gain, silicon photonics.
“…It can be clearly seen that under 3-port operation the device can not only provide us with a smaller RAM (0.18 vs. 1.6 dB) but also a smaller V π (0.18 vs. 0.22 V). The achieved RAM number (0.18 dB) is also much smaller than that reported for Si-photonic MZI under forward bias operation, where the RAM is usually as high as 2 dB [4], [5]. The smaller RAM of our device can be mainly attributed to the corresponding sweeping current (I peak − I valley ) for V π being as small as 2 mA.…”
Section: Device Structurementioning
confidence: 55%
“…linking gain is difficult on the SiP platform due to the fact that the required driving voltage for the π phase-shift at the reverse bias regime of Silicon based modulators is usually large (nearly ten volts) [3]- [5]. Increasing the p-type doping density in the active volume is one of the most effective ways to reduce the driving-voltage, but this leads to a significant optical insertion loss [3], [4].…”
Section: Introductionmentioning
confidence: 99%
“…Thermo-optics resistive phase-shifters are popular because of their simple structure and small footprint [7]- [12], but device performance has been constrained by large power consumption (>12mW) and longer than µs scale switching/response time. On the other hand, the more conventional Mach-Zehnder interferometers (MZI) require high driving voltages (>6V; under reverse bias) for the π phase shift [4], [5], [13]. This impedes their application in optical phase arrays (OPA), which usually need to have hundreds of optical phase-shifters inside with a lowdriving voltage for >2π phase shifting [10]- [12].…”
Section: Introductionmentioning
confidence: 99%
“…This has been the most effective method to reduce the 2π driving-voltage but at the expense of lower modulation speed and higher power consumption [4], [5] as compared to MZIs operated under a reverse bias. Although the forward bias gain rolls off more rapidly with the increase of operating frequency, it offers a higher RF link gain improvement of more than 10 dB from nearly DC to 25 GHz [5]. Furthermore, forward bias operation is shown to result in a comparable spurious-free dynamic range [5].…”
Section: Introductionmentioning
confidence: 99%
“…Although the forward bias gain rolls off more rapidly with the increase of operating frequency, it offers a higher RF link gain improvement of more than 10 dB from nearly DC to 25 GHz [5]. Furthermore, forward bias operation is shown to result in a comparable spurious-free dynamic range [5]. Nevertheless, large (>2 dB) residual-amplitude-modulation (RAM), which leads to undesirable AM noise during phase modulation, usually happens in these forward-bias based p-n junction phase-shifters due to the free-carrier absorption loss induced by the high level injection carriers [4], [5].…”
A three-port optical phase-shifter and Mach-Zehnder modulator (MZM) based on PNP-type bipolar junction transistor (BJT) is demonstrated. Significant plasma (injected carrier) induced changes of the refractive index for the optical waveguide become possible with an extremely small driving-voltage and a compact device size during operation of this BJT between the saturation and forward active modes. Devices with a standard MZM structure and a small footprint (0.5 mm) exhibit a moderate optical insertion loss (2 dB), extremely small V π (0.18V) and P π (0.21mW), fast rise/fall time (∼1ns), and a residue-amplitudemodulation (RAM) as small as 0.18 dB. Furthermore, thanks to the ultra-high modulation efficiency characteristic of our device, a +4.0 dB net RF-linking gain can be obtained under dynamic operation. Compared to 2-port (base-collector) forward bias operation, under three-port operation, the extra bias current from the base-emitter junction provides a lower V π (0.18 vs. 0.22 V), a smaller RAM (0.18 vs. 0.6 dB), and a larger RF-linking gain (+4 vs. −3.2 dB). The superior performances of the three-port to two-port operations can be attributed to the additional forward bias BE junction being able to provide more injected carriers to induce stronger plasma effects for optical phase-shifting. INDEX TERMS Optical phase shifter, photonics integrated circuits, RF-linking gain, silicon photonics.
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