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Electrical conduction in ultra-high purity quantum transistors

Figure 1: (a) Resistivity as a function of temperature for a high quality hole transistor at different carrier densities, (b) the same data scaled along the x-axis by a parameter T0, highlighting that all the data collapses onto two separate branches: insulating and metallic behaviour. (Taken from a paper by M.Y. Simmons, A.R. Hamilton et al., to appear in Phys. Rev. Letters, March 13, 2000).

THIS YEAR A NEW research program into the nature of electrical conduction in quantum semiconductor transistors has been initiated. These transistors, which form the basis of many high-speed electronic systems from computers to mobile telephones, rely on the ability to conduct electricity, controllably and reproducibly, such that they can switch between metallic (ON) and insulating (OFF) states. However, the fundamental question of whether the highly mobile two dimensional (2D) sheet of charge carriers in a quantum semiconductor transistor behaves like a metal or an insulator and, what drives it between these two states, remains unanswered.

The discovery of a metallic state of matter in exceptionally high quality 2D silicon transistors, and more recently in high quality GaAs hole transistors, has sparked intense international interest into the method of conduction in semiconductor systems. Early, well-established theoretical works, supported by experimental evidence, predicted that there could be no metallic state in 2D systems. Its unexpected discovery therefore challenges our basic understanding of conduction in highly pure quantum transistors. At present there is no consensus as to the nature of the metallic state.

It is important to be clear about the difference between a metal and an insulator. The distinction is only properly made at the absolute zero of temperature, since thermal excitations can permit an insulator to carry a current. If the resistance is finite at T=0 then the system is metallic, otherwise it is insulating.

The importance of phase coherent effects had not previously been recognised because the mean free path in these high quality systems is so large that weak localisation is only observable at very low, often inaccessible, temperatures. We directly measured weak localisation effects in the metallic state and found that they moved to lower temperatures as we went further into the metallic regime. These results suggest that the metallic behaviour is a finite temperature effect and that there is no true quantum phase transition. However, much work remains to be done before we can answer the apparently simple question is it possible for a two-dimensional system to be a metal?

Alex Hamilton &
Michelle Simmons

Figure 2: A phase diagram for the metallic state for two different electric fields, where increasing the electric field has the same effect as increasing the temperature. [A.R. Hamilton, M.Y. Simmons et al., Phys. Rev. Letters 82, 1542 (1999).]

 

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