In this thesis, the author investigates hidden-order phase
transition at" T"0 = 17.5 K in the heavy-fermion URu2Si2. The
four-fold rotational symmetry breaking in the hidden order phase,
which imposes a strong constraint on the theoretical model, is
observed through the magnetic torque measurement. The
translationally invariant phase with broken rotational symmetry is
interpreted as meaning that the hidden-order phase is an electronic
"nematic" phase. The observation of such nematicity in URu2Si2
indicates a ubiquitous nature among the strongly correlated
electron systems.
The author also studies the superconducting state of URu2Si2
below" T"c = 1.4 K, which coexists with the hidden-order phase. A
peculiar vortex penetration in the superconducting state is found,
which may be related to the rotational symmetry breaking in the
hidden-order phase. The author also identifies a vortex lattice
melting transition. This transport study provides essential clues
to the underlying issue of quasiparticle dynamics as to whether a
quasiparticle Bloch state is realized in the periodic vortex
lattice.
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