Abstract:We
demonstrate a straightforward construction of MoTe2 PN
homojunction on a silicon photonic crystal cavity, which promises
the realizations of cavity-enhanced optoelectronic devices integrated
on silicon photonic chips. The employed silicon photonic crystal cavity
has an air-slot in the middle to split it into two parts, which directly
function as two individual back-gate electrodes of the top-coated
few-layer MoTe2. Beneficial from MoTe2’s
ambipolar property, reconfigured (PN, NN, PP, NP) homojunctions are
r… Show more
“…The photodetection performance of the device is comparable to other p-n homojunction photodiodes based on 2D semiconductors, such as WSe 2 and MoTe 2 . [17,18,22] In Figure S3 (Supporting Information), we present the short-circuit current I sc , open-circuit voltage V oc , power conversion efficiency γ, and fill factor FF of the InSe p-n diode as a function of incident laser power. The conversion efficiency of γ ≈ 2.3% and the fill factor of FF ≈ 0.38 are obtained, respectively.…”
Section: Resultsmentioning
confidence: 99%
“…[ 8–12 ] Gate‐tunable polarity has been implemented with a few 2D semiconductors such as black phosphorus and some transition metal dichalcogenides, [ 13–16 ] which enable reconfigurable field‐effect transistors (FETs) and p–n diodes with a simple dual‐gate structure that boost the development of digital technology and complementary electronics. [ 17–22 ]…”
Section: Introductionmentioning
confidence: 99%
“…[8][9][10][11][12] Gatetunable polarity has been implemented with a few 2D semiconductors such as black phosphorus and some transition metal dichalcogenides, [13][14][15][16] which enable reconfigurable field-effect transistors (FETs) and p-n diodes with a simple dual-gate structure that boost the development of digital technology and complementary electronics. [17][18][19][20][21][22] Indium selenide (InSe) is a layered metal-chalcogenide semiconductor assembled by van der Waals (vdW) interactions. Atoms in each InSe layer (≈0.8 nm thick) are close-packed in the Se-In-In-Se atomic sequence.…”
As a 2D semiconductor, indium selenide (InSe) has shown great potentials in electronic and optoelectronic applications attributed to high carrier mobility and moderately large bandgap. However, switchable doping polarity of intrinsic InSe by electrical gating is not yet demonstrated, which is essential for applications in complementary electronics. In this work, the ambipolarity of InSe is realized and exploited through the van der Waals (vdW) integration with metal electrodes, which gets rid of the Fermi‐level pinning at the metal/semiconductor interfaces. On this basis, InSe field‐effect transistors (FETs) with controllable polarities are reconfigured with a dual‐gate structure, functioning as both unipolar FETs and p–n diodes. The p‐ and n‐type operations of the unipolar FETs are dynamically switched with on–off ratios of 106 and 109, respectively. Meanwhile, p–n diodes with a rectification ratio of 106 and high photodetection performance are also demonstrated. This work paves a promising way for InSe‐based reconfigurable complementary electronics and optoelectronics.
“…The photodetection performance of the device is comparable to other p-n homojunction photodiodes based on 2D semiconductors, such as WSe 2 and MoTe 2 . [17,18,22] In Figure S3 (Supporting Information), we present the short-circuit current I sc , open-circuit voltage V oc , power conversion efficiency γ, and fill factor FF of the InSe p-n diode as a function of incident laser power. The conversion efficiency of γ ≈ 2.3% and the fill factor of FF ≈ 0.38 are obtained, respectively.…”
Section: Resultsmentioning
confidence: 99%
“…[ 8–12 ] Gate‐tunable polarity has been implemented with a few 2D semiconductors such as black phosphorus and some transition metal dichalcogenides, [ 13–16 ] which enable reconfigurable field‐effect transistors (FETs) and p–n diodes with a simple dual‐gate structure that boost the development of digital technology and complementary electronics. [ 17–22 ]…”
Section: Introductionmentioning
confidence: 99%
“…[8][9][10][11][12] Gatetunable polarity has been implemented with a few 2D semiconductors such as black phosphorus and some transition metal dichalcogenides, [13][14][15][16] which enable reconfigurable field-effect transistors (FETs) and p-n diodes with a simple dual-gate structure that boost the development of digital technology and complementary electronics. [17][18][19][20][21][22] Indium selenide (InSe) is a layered metal-chalcogenide semiconductor assembled by van der Waals (vdW) interactions. Atoms in each InSe layer (≈0.8 nm thick) are close-packed in the Se-In-In-Se atomic sequence.…”
As a 2D semiconductor, indium selenide (InSe) has shown great potentials in electronic and optoelectronic applications attributed to high carrier mobility and moderately large bandgap. However, switchable doping polarity of intrinsic InSe by electrical gating is not yet demonstrated, which is essential for applications in complementary electronics. In this work, the ambipolarity of InSe is realized and exploited through the van der Waals (vdW) integration with metal electrodes, which gets rid of the Fermi‐level pinning at the metal/semiconductor interfaces. On this basis, InSe field‐effect transistors (FETs) with controllable polarities are reconfigured with a dual‐gate structure, functioning as both unipolar FETs and p–n diodes. The p‐ and n‐type operations of the unipolar FETs are dynamically switched with on–off ratios of 106 and 109, respectively. Meanwhile, p–n diodes with a rectification ratio of 106 and high photodetection performance are also demonstrated. This work paves a promising way for InSe‐based reconfigurable complementary electronics and optoelectronics.
“…Two Au electrodes with a thickness of 100 nm were then transferred on the ReS2 flake acting as the drain and source electrodes. [25][26][27][28][29] The heavily doped Si substrate could function as a bottom electrical gate. By applying an electrical voltage between the heavily doped Si substrate and the source electrode, i.e.…”
Electrical tuning of second-order nonlinearity in optical materials is attractive to strengthen and expand the functionalities of nonlinear optical technologies, though its implementation remains elusive. Here, we report the electrically tunable second-order nonlinearity in atomically thin ReS2 flakes benefiting from their distorted 1T crystal structure and interlayer charge transfer. Enabled by the efficient electrostatic control of the few-atomiclayer ReS2, we show that second harmonic generation (SHG) can be induced in odd-numberlayered ReS2 flakes which are centrosymmetric and thus without intrinsic SHG. Moreover, the SHG can be precisely modulated by the electric field, reversibly switching from almost zero to an amplitude more than one order of magnitude stronger than that of the monolayer MoS2. For the even-number-layered ReS2 flakes with the intrinsic SHG, the external electric field could be leveraged to enhance the SHG. We further perform the first-principles calculations which suggest that the modification of in-plane second-order hyperpolarizability by the redistributed interlayer-transferring charges in the distorted 1T crystal structure underlies the electrically tunable SHG in ReS2. With its active SHG tunability while using the facile electrostatic control, our work may further expand the nonlinear optoelectronic functions of two-dimensional materials for developing electrically controllable nonlinear optoelectronic devices.
“…[3][4][5] Recently, two-dimensional (2D) materials with layered structures have emerged as an attractive active medium for constructing optoelectronic devices. [6][7][8][9][10][11][12][13][14] It has been reported that versatile single-elementary and compound materials have layered stacking forms, which could be exfoliated into a 2D material with a thickness of few-atom layer. Therefore, plentiful electrical, optical, magnetic, and mechanical properties could be acquired from 2D materials.…”
Two-dimensional (2D) materials with layered structures have a variety of exceptional electronic and optical attributes for potentially developing basic functions of light wave technology from light-emitting to -modulating and -sensing. Here, we present state-of-the-art 2D materials-enabled optical intensity modulators according to their operation spectral ranges, which are mainly determined by the optical bandgaps of the 2D materials. Leveraging rich electronic structures from different 2D materials and the governed unique light–matter interactions, the working mechanisms and device architectures for the enabled modulators at specific wavelength ranges are discussed. For instance, the tunable excitonic effect in monolayer transition metal dichalcogenides allows the modulation of visible light. Electro-absorptive and electro-refractive graphene modulators could be operated in the telecom-band relying on their linear dispersion of the massless Dirac fermions. The bendable electronic band edge of the narrow bandgap in few-layer black phosphorus promises the modulation of mid-infrared light via the quantum-confined Franz–Keldysh or Burstein–Moss shift effect. Electrically and magnetically tunable optical conductivity in graphene also supports the realizations of terahertz modulators. While these modulators were demonstrated as proof of concept devices, part of them have great potential for future realistic applications, as discussed with their wavelength coverage, modulation depth, insertion loss, dynamic response speed, etc. Specifically, benefiting from the well-developed technologies of photonic chips and optical fibers in telecom and datacom, the 2D materials-based modulators integrated on these photonic structures are expected to find applications in fiber and chip optical communications. The free-space mid-infrared and terahertz modulators based on 2D materials can expect application in chemical bond spectroscopy, free-space communications, and environment/health sensing.
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