2018
DOI: 10.1126/sciadv.aao6653
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Electrically tunable single- and few-layer MoS 2 nanoelectromechanical systems with broad dynamic range

Abstract: Atomically thin semiconductor resonators vibrating at radio frequencies with exceptional tunability and broad dynamic range.

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Cited by 142 publications
(176 citation statements)
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“…For the same characteristic length and built-in strain, the circular device gives higher resonance frequency than the doubly clamped device does, since its circumference-clamped structure provides higher spring constant and smaller effective mass. These correlations for both cases agree with the results from previous models [ 6 , 9 , 10 , 19 , 20 , 21 , 22 , 23 , 24 ] at gate voltage V g = 0 V. To enable resonance frequency above gigahertz, f res > 1 GHz, built-in strain ≈0.25% with length smaller than 0.4 μm or built-in strain ≈0.05% with length smaller than 0.18 μm are required for doubly clamped graphene resonators. For circular drumhead resonators to achieve f res > 1 GHz, it needs a built-in strain ≈0.05% with a diameter smaller than 0.22 μm or a built-in strain ≈0.25% with a diameter smaller than 0.6 μm.…”
Section: Resultssupporting
confidence: 91%
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“…For the same characteristic length and built-in strain, the circular device gives higher resonance frequency than the doubly clamped device does, since its circumference-clamped structure provides higher spring constant and smaller effective mass. These correlations for both cases agree with the results from previous models [ 6 , 9 , 10 , 19 , 20 , 21 , 22 , 23 , 24 ] at gate voltage V g = 0 V. To enable resonance frequency above gigahertz, f res > 1 GHz, built-in strain ≈0.25% with length smaller than 0.4 μm or built-in strain ≈0.05% with length smaller than 0.18 μm are required for doubly clamped graphene resonators. For circular drumhead resonators to achieve f res > 1 GHz, it needs a built-in strain ≈0.05% with a diameter smaller than 0.22 μm or a built-in strain ≈0.25% with a diameter smaller than 0.6 μm.…”
Section: Resultssupporting
confidence: 91%
“…For convenience, we use a polar coordinate for the circular drumhead that closely matches the device geometry. The elastic energy stored in the stretched membrane U el,c can be obtained by [ 19 , 25 ] where R , ν , ε 0, r , ε 0, θ are radius, Poisson’s ratio, initial radial strain, initial tangential strain, respectively. Similar to the doubly clamped case, we assume that the curvature of the static deflection forms the parabolic shape, and it has the maximum static deflection at its center due to symmetry.…”
Section: Analytical Model and Computational Methodsmentioning
confidence: 99%
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“…Few-layer MoS 2 were fabricated into two-dimensional nanoelectromechanical systems (NEMS) as ultralow-power, high-frequency tunable oscillators and ultrasensitive resonant transducers [152]. These devices can operate in the very high frequency band (up to ∼120 MHz).…”
Section: Microwave Irradiationmentioning
confidence: 99%
“…[15][16][17][18] Two-dimensional materials offer the capability to alter the surface dielectric function by electronic tuning of the free carrier concentration in a fast, controllable, and reversible manner without restrictions in operating temperature. [19][20][21][22][23][24][25] Despite this capability, achieving even modest modulation of far-field radiative flux is challenging as thermal radiation is broadband. In the near-field, however, thermal radiation is primarily due to resonant coupling of narrowband surface modes, such as plasmons or phonon-polaritons.…”
mentioning
confidence: 99%