Abstract:Due to the continuous increase in data traffic, it is becoming imperative to develop communication systems capable of meeting the throughput requirements. Monolithic Opto-Electronic Integrated Circuits (OEICs) are ideal candidates to meet these demands. With that in mind, we propose a compact and computationally efficient model for Uni-Traveling Carrier Photodiodes (UTC-PDs) which are a key component of OEICs because of their high bandwidth and RF output power. The developed compact model is compatible with ex… Show more
“…We previously reported an equivalent circuit model of our UTC-PDs, showing a resistive and capacitive behavior of the devices up to 67 GHz. The CPW pads are designed so that the elements of the equivalent circuits of the OPEN and SHORT test structures are independent of the frequency up to 67 GHz and, thus, do not affect the normalized RF device response below 67 GHz [19]. However, for higher frequencies, the On completion of the measurements, both measured and fitted photoresponses are normalized to the near DC (0.2 GHz) value to obtain the normalized response curves plotted in Fig.…”
Section: B 110 Ghz Small-signal Equivalent Circuitmentioning
confidence: 99%
“…In parallel to the junction capacitance, the transconductance of the voltage-controlled-current-source (VCCS) is used to tune the absolute response (power) level for different device sizes. To model the behavior of the pad parasitics up to 110 GHz, three different LC sections were added to the circuit model, as shown in Fig.4(b)[19]. The first section, L ab and C ab , represents the parasitic behavior of the mesa bridge with Teflon underneath.…”
We report the wideband performance of uniform Type-II GaInAsSb/InP UTC-PDs for optical data communications near 300 Gbps. A wide bandwidth of >110 GHz is achieved for a device area of 50 µm 2 . In signal transmission measurements, the present UTC-PDs show a low Bit-Error Rate (BER) and a high Signal-to-Noise Ratio (SNR) of more than 18 dB at data rates as high as 288 Gbps (96 GBd, PAM-8) without postamplification electronics. The work demonstrates the suitability of GaInAsSb/InP UTC-PDs for optical data transmission at bit rates approaching 300 Gbps.
“…We previously reported an equivalent circuit model of our UTC-PDs, showing a resistive and capacitive behavior of the devices up to 67 GHz. The CPW pads are designed so that the elements of the equivalent circuits of the OPEN and SHORT test structures are independent of the frequency up to 67 GHz and, thus, do not affect the normalized RF device response below 67 GHz [19]. However, for higher frequencies, the On completion of the measurements, both measured and fitted photoresponses are normalized to the near DC (0.2 GHz) value to obtain the normalized response curves plotted in Fig.…”
Section: B 110 Ghz Small-signal Equivalent Circuitmentioning
confidence: 99%
“…In parallel to the junction capacitance, the transconductance of the voltage-controlled-current-source (VCCS) is used to tune the absolute response (power) level for different device sizes. To model the behavior of the pad parasitics up to 110 GHz, three different LC sections were added to the circuit model, as shown in Fig.4(b)[19]. The first section, L ab and C ab , represents the parasitic behavior of the mesa bridge with Teflon underneath.…”
We report the wideband performance of uniform Type-II GaInAsSb/InP UTC-PDs for optical data communications near 300 Gbps. A wide bandwidth of >110 GHz is achieved for a device area of 50 µm 2 . In signal transmission measurements, the present UTC-PDs show a low Bit-Error Rate (BER) and a high Signal-to-Noise Ratio (SNR) of more than 18 dB at data rates as high as 288 Gbps (96 GBd, PAM-8) without postamplification electronics. The work demonstrates the suitability of GaInAsSb/InP UTC-PDs for optical data transmission at bit rates approaching 300 Gbps.
“…Moreover, the simplicity of the existing equivalent circuit models limit their accuracy compared to analytic equations describing the physics of UTC-PDs [10][11][12]. In an effort to bring SPICE models closer to the physical transport mechanisms, a comprehensive SPICE model in Verilog-A, which accounts for both static and dynamic behavior of UTC-PDs, was presented in [13] and further detailed in [14][15]. However, due to the inherent complexity in implementing the analytical equations describing the photoresponse in Verilog-A, behavioral approximations were used that limit the model's physical basis as well as its accuracy at higher frequencies.…”
Section: Introductionmentioning
confidence: 99%
“…The photocurrent is controlled by the input optical power and is modelled by the photo-generation rate and the transfer functions in the absorber and collector regions. While the Verilog-A model presented in [13][14][15], captured both the static and dynamic behavior of UTC-PDs quite well, the dynamic photocurrent modeling remained rather simplified. This is because the implementation of the complete analytical form is not straightforward due to the complex sinc and exponential functions representing its frequency dependence.…”
Section: Introductionmentioning
confidence: 99%
“…3-dB cut-off frequency. To take this into account for model validation, we leveraged the UTC-PD SPICE compact model and associated parameter set without illumination (detailed in [14][15]) for the simulation of dynamic photo-response. Results are shown in Figs.…”
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