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Physical Review B - Condensed Matter and Materials Physics

Volumn 91, Issue 12, 2015, Pages

Coupling between electrons and optical phonons in suspended bilayer graphene

(6) Laitinen, Antti a Kumar, Manohar a Oksanen, Mika a Plaçais, Bernard a,b Virtanen, Pauli a Hakonen, Pertti a

a AALTO UNIVERSITY (Finland)

b UNIVERSITÉ PARIS DESCARTES (France)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 84926435547 PISSN: 10980121 EISSN: 1550235X Source Type: Journal
DOI: 10.1103/PhysRevB.91.121414 Document Type: Article

Times cited : (34)

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- According to the electrostatic contact analysis of Ref. [42], applicable also for a bilayer, the contact capacitance amounts to (Equation presented) for Au/Cr/Au contacts similar to ours. Hence, we may estimate the real part (Equation presented) of the impedance at the contact; (Equation presented) in parallel with contact capacitance (Equation presented). Using the above value for (Equation presented) and a contact area of 4 (Equation presented), we obtain (Equation presented) at (Equation presented) 1 GHz, which yields about 100 (Equation presented) instead of 1 (Equation presented) for the high-frequency contact resistance
- According to the electrostatic contact analysis of Ref. [42], applicable also for a bilayer, the contact capacitance amounts to (Equation presented) for Au/Cr/Au contacts similar to ours. Hence, we may estimate the real part (Equation presented) of the impedance at the contact; (Equation presented) in parallel with contact capacitance (Equation presented). Using the above value for (Equation presented) and a contact area of 4 (Equation presented), we obtain (Equation presented) at (Equation presented) 1 GHz, which yields about 100 (Equation presented) instead of 1 (Equation presented) for the high-frequency contact resistance.

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