J.C. Dias

Suppression of a charge-density-wave ground state in high magnetic fields: Spin and orbital mechanisms

The charge density wave (CDW) transition temperature in the quasi-one-dimensional (Q1D) organic material

Evolution of superconductivity from a charge-density-wave ground state in pressurized (Per)2[Au(mnt)2]

(\mathrm{Per}{)}_{2}\mathrm{Au}(\mathrm{mnt}{)}_{2}

Magnetic Field Dependence of CDW Phases in (Per)2M(mnt)2 (M = Pt, Au)

is relatively low

Geometrical and orbital effects in a quasi-one-dimensional conductor

{(T}_{\mathrm{CDW}}\ensuremath{\sim}12\mathrm{K}).

Searching for switchable molecular conductors : Salts of [M(dcbdt)2] (M = Ni, Au) anions with [Fe(sal2-trien)]+ and [Fe(phen)3]2+

Hence in a mean field BCS model, the CDW state should be completely suppressed in magnetic fields of order 30\char21{}40 T. To explore this possibility, the magnetoresistance of

Magnetic Field Dependent Behavior of the CDW ground state in Per2M(mnt)2 (M = Au, Pt)

(\mathrm{Per}{)}_{2}\mathrm{Au}(\mathrm{mnt}{)}_{2}

The low and high temperature phase transitions in the family of compounds (DT-TTF)4[M(L)2]3, M = Au, Cu and L = pds, pdt

was investigated in magnetic fields to 45 T for

Infrared investigation of the charge ordering pattern in the organic spin ladder candidate (DTTTF)2Cu(mnt)2

0.5\mathrm{K}lTl12\mathrm{K}.

Structural and electrical properties of (DT-TTF)2[ Cu(mnt)2]

For fields directed along the Q1D molecular stacking direction,

Quantum interference in the quasi-one-dimensional organic conductor "Per…2Au"mnt…2

{T}_{\mathrm{CDW}}