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Lecture 4 - Coulomb blockade & SET Fulton TA and Dolan GJ, Phys. Rev. Lett. 59 (1987) 109.
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Circuit for SET transistor 1 V1V1 VgVg V2V2 CgCg C1C1 C2C2 R1R1 R2R2 nanocluster tunnelling junction VCVC Q When an electron tunnels onto or off the cluster already containing n excess electrons, the change in electrostatic energy is: Algebra – first calculate charge on middle island: Rearrange- 1 2
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Circuit for SET transistor 2 Electrostatic energy Only term that varies as the charge on the cluster varies. Consider process when 1 charge tunnels onto or off the cluster. 3
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Circuit for SET transistor V1V1 VgVg V2V2 CgCg C1C1 C2C2 R1R1 R2R2 nanocluster tunnelling junction VCVC Q When an electron tunnels onto or off the cluster already containing n excess electrons, the change in electrostatic energy is: The work done by the voltage sources when an electron tunnels through the j th junction is:
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Circuit for SET transistor 0 VgVg V CgCg C1C1 C2C2 R1R1 R2R2 nanocluster tunnelling junction VCVC Q e-e-
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Enthalpy change
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Coulomb staircase Electrons fill island until Tunnelling current
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Single electron transistor blockade
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Experimental Coulomb staircase Wilkins R et al., Phys. Rev. Lett. 63 (1989) 801.
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