Abstract
Landauer’s formula discussed in Sect. 1.3.3 gives the quantized conductance in an ideal quantum wire without impurities,
where N is the number of subbands which cross the Fermi energy EF. This formula was derived in noninteracting case. In one-dimensional systems, it has long been known that the mutual interaction has strong effects. In fact, each order of perturbation calculations has a divergence and thus the ground state is a non-perturbative one. Such a state is described as a Tomonaga—Luttinger liquid [1], which differs from the conventional Fermi liquid. It exhibits several anomalous behaviors such as a power-law decay of physical quantities and a spin-charge separation [2–5]. It is thus very interesting and important to study quantum wires and to find out such anomalous phenomena characteristic of the Tomonaga—Luttinger liquid.
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Ogata, M., Fukuyama, H. (1998). Tomonaga—Luttinger Liquid in Quantum Wires. In: Ando, T., Arakawa, Y., Furuya, K., Komiyama, S., Nakashima, H. (eds) Mesoscopic Physics and Electronics. NanoScience and Technology. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-71976-9_7
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