Abstract

We analyze energy consumption in optical modulators operated in depletion and intended for low-power interconnect applications. We include dynamic dissipation from charging modulator capacitance and net energy consumption from absorption and photocurrent, both in reverse and small forward bias. We show that dynamic dissipation can be independent of static bias, though only with specific kinds of bias circuits. We derive simple expressions for the effects of photocurrent on energy consumption, valid in both reverse and small forward bias. Though electroabsorption modulators with large reverse bias have substantial energy penalties from photocurrent dissipation, we argue that modulator diodes with thin depletion regions and operating in small reverse and/or forward bias could have little or no such photocurrent energy penalty, even conceivably being more energy-efficient than an ideal loss-less modulator.

Highlights

  • Because of the quantum nature of optical detection [1], optics could reduce the energy for transmitting information even at short distances inside computers and information switching and processing machines [1,2,3]

  • / e) ), so any photocurrent in this state is fed back into the bias supply. Such a scheme is conceivably viable for Ge quantum well modulators driven from low voltage CMOS

  • Optical modulators are attractive compared to lasers for low-energy dense optical interconnects because they offer threshold-less operation and easier integration with Si

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Summary

Introduction

Because of the quantum nature of optical detection [1], optics could reduce the energy for transmitting information even at short distances inside computers and information switching and processing machines [1,2,3]. Because the absorption edge can remain quite abrupt even with large bias [23, 36], such bias allows the modulator’s operating wavelength to be voltage-tuned while still allowing low drive swing [19, 23, 36] Such static bias can, lead to additional dissipation from photocurrent and to some consequences for the dynamic dissipation of the modulator that we discuss below. Fixed capacitance is a substantial approximation for some silicon carrier depletion modulators that may not use p-i-n diodes, but our model should allow reasonable comparisons This model covers electrorefractive (electro-optic) devices in the form of either biased insulating materials, such as electro-optic polymers [26], or diodes; presumably these would have little if any photocurrent. After summarizing dissipation results, we discuss implications for device design

Dissipation from capacitive charging and discharging
Model drive circuit
Dynamic energy calculation
Adiabatic operation
Energy dissipation from photocurrent
Reverse bias dissipation
Forward bias dissipation
Indirect gap semiconductors
Expression for energy dissipation
Energy per bit from absorption and photocurrent dissipation
Example limiting cases
Low energy operating modes for electroabsorptive modulators
Total energy dissipation
Conclusions
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