Novel Energy Scale in the Interacting 2D Electron System Evidenced from Transport and Thermodynamic Measurements

By analyzing the in-plane field magnetoconductivity, zero field transport, and thermodynamic spin magnetization in 2D correlated electron system in high mobility Si-MOS samples, we have revealed a novel high energy scale $T^*$, beyond the Fermi energy. In magnetoconductivity, we found a sharp onset of the novel regime $δσ(B,T) \propto (B/T)^2$ above a density dependent temperature $T_{\rm kink}(n)$, the high-energy behavior that "mimics" the low-temperature diffusive interaction regime. The zero field resistivity temperature dependence exhibits an inflection point $T_{\rm infl}$. In thermodynamic magnetization, the weak field spin susceptibility per electron, $\partial χ/\partial n$ changes sign at $T_{dM/d n}$. All three notable temperatures, $T_{\rm kink}$, $T_{\rm infl}$, and $T_{d M/ d n}$, behave critically $\propto (n-n_c)$, are close to each other, and are intrinsic to high mobility samples only; we therefore associate them with a novel energy scale $T^*$ caused by interactions in the 2DE system.

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