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Mechanics of Nanowires

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Presentation on theme: "Mechanics of Nanowires"β€” Presentation transcript:

1 Mechanics of Nanowires
Davide Cadeddu Mechanics of Nanowires Introduction to Nanomechanics - Fall 2018

2 Fluctuation-Dissipation Theorem
When limited by thermal fluctuations: Gives a minimum detectable force: mechanics of nanowires

3 Optimal Cantilever Geometry
For a given temperature we need to minimize mechanical dissipation: mechanics of nanowires

4 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

5 MBE-grown GaAs/AlGaAs nanowires
mechanics of nanowires

6 Equation of motion π‘₯ (𝑑)+𝛾 π‘₯ (𝑑)+ πœ” 0 π‘₯(𝑑)=𝐹(𝑑)
Linear Response Equation of motion π‘₯ (𝑑)+𝛾 π‘₯ (𝑑)+ πœ” 0 π‘₯(𝑑)=𝐹(𝑑) mechanics of nanowires

7 π‘₯ 𝑑 +𝛾 π‘₯ 𝑑 + π‘₯ 𝑑 (πœ” 0 +𝛼 π‘₯ 2 (𝑑))=𝐹(𝑑)
Duffing Oscillator Duffing Equation π‘₯ 𝑑 +𝛾 π‘₯ 𝑑 + πœ” 0 π‘₯ 𝑑 +𝛼 π‘₯ 3 (𝑑)=𝐹(𝑑) positive (negative) Ξ± could be seen as a hardening (softening) of the spring constant π‘₯ 𝑑 +𝛾 π‘₯ 𝑑 + π‘₯ 𝑑 (πœ” 0 +𝛼 π‘₯ 2 (𝑑))=𝐹(𝑑) π‘₯ 𝑑 =𝑍 cos⁑(πœ”π‘‘βˆ’πœ“) mechanics of nanowires

8 Duffing Oscillator Duffing Equation 𝑍 2 πœ” 2 βˆ’ πœ” 0 2 βˆ’ 3 4 𝛼 𝑍 𝛾𝑍 πœ” 2 = 𝐹 Bistable solution! The jumping point depends on the history of the resonator mechanics of nanowires

9 Nanowire mode doublet MODE I MODE II Slightly asymmetric nanowire gives two non-degenerate flexural modes Ο‰ 0 = 𝛽 𝑛 5𝐸𝐴 24π‘š d L 2 mechanics of nanowires

10 External Force mechanics of nanowires

11 External Force mechanics of nanowires

12 External Force mechanics of nanowires

13 External Force mechanics of nanowires

14 External Force mechanics of nanowires


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