2015
DOI: 10.1002/lpor.201500101
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Fundamental limits on the losses of phase and amplitude optical actuators

Abstract: Amplitude and phase are the basic properties of all wave phenomena; as far as optical waves are concerned, the ability to act on these variables is at the root of a wealth of switching devices. To quantify the performance of an optical switching device, an essential aspect is to determine the tradeoff between the insertion loss and the amplitude or phase modulation depth. Here it is shown that every optical switching device is subject to such a tradeoff, intrinsically connected to the dielectric response of th… Show more

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Cited by 18 publications
(19 citation statements)
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“…Still, decreasing the optical mode volume, V m , introduces adverse effects, such as bending-and ohmic losses for polaritonic modes. It is therefore not straightforward to predict modulator performance scaled into sub-micron size regime [42], leading to a rigorous analysis of fundamental scaling laws for nanophotonics as a function of critical device length [38]. In this scaling analysis, we assume three types of optical cavities, (a) a traveling-wave ring resonator (RR) [43], (b) a metal-mirror based FP cavity [39], and (c) a plasmonic metal nano-particle (MNP) [44] (figure 2(b)), that enhance the fundamentally weak interaction between light and matter via the ratio of Q/V m , where Q is the cavity quality factor, V m is the effective volume of electromagnetic energy of a resonant mode.…”
Section: Modulator Scaling Lawsmentioning
confidence: 99%
“…Still, decreasing the optical mode volume, V m , introduces adverse effects, such as bending-and ohmic losses for polaritonic modes. It is therefore not straightforward to predict modulator performance scaled into sub-micron size regime [42], leading to a rigorous analysis of fundamental scaling laws for nanophotonics as a function of critical device length [38]. In this scaling analysis, we assume three types of optical cavities, (a) a traveling-wave ring resonator (RR) [43], (b) a metal-mirror based FP cavity [39], and (c) a plasmonic metal nano-particle (MNP) [44] (figure 2(b)), that enhance the fundamentally weak interaction between light and matter via the ratio of Q/V m , where Q is the cavity quality factor, V m is the effective volume of electromagnetic energy of a resonant mode.…”
Section: Modulator Scaling Lawsmentioning
confidence: 99%
“…The following points arise from Figure 2. First, the resonator’s total loss is always smaller (blue curve < red curve) due to the bypassing mechanism28 . The IL increases with L SPP (i.e.…”
mentioning
confidence: 99%
“…However, decreasing the optical mode volume, V m , introduces adverse effects, for example, bending losses, and ohmic losses for polaritonic modes. It is therefore not straightforward to predict optoelectronic performance for device scaling into the nanoscale1314, and a rigorous analysis of fundamental scaling laws for nanophotonics as a function of critical device length is warranted. Here, we investigate the performances of four actively-controlled (electrically or optically) devices with respect to their scaling behavior: a light source, an electrical-to-optical (EO) data encoder typically in form of an electro-optic modulator, and a photodetector for the inverse OE conversion, along with a fourth device, which is a purely optical switch for all-optical information processing (Fig.…”
mentioning
confidence: 99%