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Mechanics of Nanowires
Davide Cadeddu Mechanics of Nanowires Introduction to Nanomechanics - Fall 2018
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Fluctuation-Dissipation Theorem
When limited by thermal fluctuations: Gives a minimum detectable force: mechanics of nanowires
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Optimal Cantilever Geometry
For a given temperature we need to minimize mechanical dissipation: mechanics of nanowires
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Bottom-up NWs are ideal force sensors:
Bottom-up Nanowires Bottom-up NWs are ideal force sensors: nearly perfect crystalline structure singly-clamped cantilever geometry high aspect ratio and nanometer-scale dimensions high resonance frequencies mechanics of nanowires
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MBE-grown GaAs/AlGaAs nanowires
mechanics of nanowires
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Equation of motion π₯ (π‘)+πΎ π₯ (π‘)+ π 0 π₯(π‘)=πΉ(π‘)
Linear Response Equation of motion π₯ (π‘)+πΎ π₯ (π‘)+ π 0 π₯(π‘)=πΉ(π‘) mechanics of nanowires
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π₯ π‘ +πΎ π₯ π‘ + π₯ π‘ (π 0 +πΌ π₯ 2 (π‘))=πΉ(π‘)
Duffing Oscillator Duffing Equation π₯ π‘ +πΎ π₯ π‘ + π 0 π₯ π‘ +πΌ π₯ 3 (π‘)=πΉ(π‘) positive (negative) Ξ± could be seen as a hardening (softening) of the spring constant π₯ π‘ +πΎ π₯ π‘ + π₯ π‘ (π 0 +πΌ π₯ 2 (π‘))=πΉ(π‘) π₯ π‘ =π cosβ‘(ππ‘βπ) mechanics of nanowires
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Duffing Oscillator Duffing Equation π 2 π 2 β π 0 2 β 3 4 πΌ π πΎπ π 2 = πΉ Bistable solution! The jumping point depends on the history of the resonator mechanics of nanowires
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Nanowire mode doublet MODE I MODE II Slightly asymmetric nanowire gives two non-degenerate flexural modes Ο 0 = π½ π 5πΈπ΄ 24π d L 2 mechanics of nanowires
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External Force mechanics of nanowires
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External Force mechanics of nanowires
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External Force mechanics of nanowires
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External Force mechanics of nanowires
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External Force mechanics of nanowires
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