Effect of magnetic field on the intermediate phase in Mn1-xFexSi: spin-liquid vs. fluctuations scenario
S. V. Demisheva,b, I. I. Lobanovaa,b, A. V. Bogacha, V. V. Glushkova,b, V. Yu. Ivanova, T. V. Ischenkoa, N. A. Samarina, N. E. Sluchankoa, S. Gabanic, E. Cizmárd, K. Flachbartc, N. M. Chubovae, V. A. Dyadkine,f, S. V. Grigorieve
aProkhorov General Physics Institute of RAS, 119991 Moscow, Russia
bMoscow Institute of Physics and Technology, 141700 Dolgoprudny, Russia
cInstitute of Experimental Physics SAS, 040 01 Kosice, Slovak Republic
dP.J. Safárik Univesity in Kosice, SK-04001 Kosice, Slovak Republic
ePetersburg Nuclear Physics Institute, 188300 Gatchina, Russia
fSwiss-Norwegian Beamlines at the European Synchrotron Radiation Facility, 38000 Grenoble, France
Abstract
We report results of the magnetic field influence on the chiral
spin liquid state in Mn1-xFexSi single crystal with iron content
x=0.108 in proximity of a hidden quantum critical point. The use of small
angle neutron scattering data together with magnetic susceptibility
measurements down to 0.4 K and precise magnetoresistance measurements in the
temperature range 2-20 K in magnetic field up to 5 T allowed us to construct
the magnetic phase diagram of this compound in which at low magnetic fields
B<0.15 T an intermediate phase with short-range magnetic order exists
in a wide temperature range 0.62<T<9.1 K. It was found that the
increase of magnetic field first results in a suppression
of transition into
spiral phase with long-range magnetic order at very low temperatures, and
then induces a transition of the intermediate phase into a
spin-polarized
(ferromagnetic) phase with lowering temperature. The temperature of this
transition TSP increases with magnetic field logarithmically,
, and results in formation of a singular point on the
magnetic phase diagram located at T 8.5 K and B 3.5 T,
which may be either a triple or a critical point. The possible spin-liquid
nature of the intermediate phase is discussed.