P. Monceau

Dielectric response of the charge-induced correlated state in the quasi-one-dimensional conductor ( TMTTF ) 2 PF 6

Conductivity and permittivity of the quasi-one-dimensionsional organic transfer salt

Dielectric Response of the Charge Ordered State in Quasi-One-Dimensional Organic Conductors

(\mathrm{TMTTF}{)}_{2}{\mathrm{PF}}_{6}

Transition of charge-density-wave conductors into a glassy-like state

have been measured at low frequencies

Low temperature specific heat of the spin-density-wave compound (TMTSF)2PF6

{(10}^{3}\char21{}{10}^{7}\mathrm{Hz})

Charge ordering phase transition in the quasi-one-dimensional conductor (TMTTF)2AsF6

between room temperature down to below the temperature of transition into the spin-Peierls state. We interpret the huge real part of the dielectric permittivity (up to

An ultrasonic and thermal expansion study of the quasi-one-dimensional compound

{10}^{6})

Spontaneous breaking of isotropy observed in the electronic transport of rare-earth tritellurides.

in the localized state as the realization in this compound of a charge ordered state of Wigner crystal type due to long-range Coulomb interaction.

Heat capacity of CuGeO3 : Sensitivity to crystalline quality

We present a survey of the recent experimental results which provide the evidence for the formation in quasi-one-dimensional (Q1D) conductors of a charge ordered (CO) state corresponding to an elec...

Surface charge density wave phase transition in NbSe3.

Abstract We have found that the real part of the dielectric constant of the quasi-one-dimensional conductors with a charge density wave (CDW) shows a peak in the low temperature range ( T

Hall effect in the pinned and sliding charge density wave state of NbSe3

Abstract We report on specific heat measurements of the SDW compound (TMTSF)2PF6 between 2 and 25 K, performed by two different techniques. We discuss the two successive transitions which occur in this T-range: the SDW ordering transition at T = 12.1 K, and a glass transition around 3–3.5 K. The latter is very dependent on the kinetics of measurements, and has all characteristic features of freezing of supercooled liquids.