93 research outputs found
Pressure-induced Superconductivity in a Ferromagnet UGe -- Resistivity Measurements in Magnetic Field --
The electrical resistivity measurements in the magnetic field are carried out
on the pressure-induced superconductor UGe. The superconductivity is
observed from 1.06 to 1.44 GPa. The upper critical field of is
anisotropic where exhibits positive curvature for and
-axis. The characteristic enhancement of is reconfirmed for
-axis. In the temperature and field dependence of resistivity at where the ferromagnetic ordering disappears, it is observed that the
application of the external field along the {\it a}-axis increases the
coefficient of Fermi liquid behavior correspondingly to the
metamagnetic transition.Comment: To be published in the proceeding of the International Conference on
High Pressure Science and Technology(AIRAPT-18),Beijing,China,23-27 July 200
Magnetic measurements at pressures above 10 GPa in a miniature ceramic anvil cell for a superconducting quantum interference device magnetometer
A miniature ceramic anvil high pressure cell (mCAC) was earlier designed by
us for magnetic measurements at pressures up to 7.6 GPa in a commercial
superconducting quantum interference (SQUID) magnetometer [N. Tateiwa et al.,
Rev. Sci. Instrum. 82, 053906 (2011)]. Here, we describe methods to generate
pressures above 10 GPa in the mCAC. The efficiency of the pressure generation
is sharply improved when the Cu-Be gasket is sufficiently preindented. The
maximum pressure for the 0.6 mm culet anvils is 12.6 GPa when the Cu-Be gasket
is preindented from the initial thickness of 0.30 to 0.06 mm. The 0.5 mm culet
anvils were also tested with a rhenium gasket. The maximum pressure attainable
in the mCAC is about 13 GPa. The present cell was used to study YbCu2Si2 which
shows a pressure induced transition from the non-magnetic to magnetic phases at
8 GPa. We confirm a ferromagnetic transition from the dc magnetization
measurement at high pressure. The mCAC can detect the ferromagnetic ordered
state whose spontaneous magnetic moment is smaller than 1 mB per unit cell. The
high sensitivity for magnetic measurements in the mCAC may result from the the
simplicity of cell structure. The present study shows the availability of the
mCAC for precise magnetic measurements at pressures above 10 GPa
Normal metal to ferromagnetic superconductor tunneling
We study the point-contact tunneling between normal metal and ferromagnetic
superconductor. In the case of magnon-induced pairing the tunneling conductance
is continuous and smooth function of the applied voltage. For small values of
the applied voltage the Ohm law holds. We show that one can obtain the
magnetization and the superconducting order parameter from the tunneling
conduc- tance. In the case of paramagnon-induced superconductivity the
tunneling does not depend on the magnetization. We argue that tunneling
experiment can unambiguously determine the correct pairing mechanism in the
ferromagnetic superconductors.Comment: 6 pages, 4 figur
Pressure-temperature phase diagram of the heavy-electron superconductor URu2Si2
The pressure-temperature phase diagram of the heavy-electron superconductor
URu2Si2 has been reinvestigated by ac-susceptibility and elastic
neutron-scattering (NS) measurements performed on a small single-crystalline
rod (2 mm in diameter, 6 mm in length) in a Cu-Be clamp-type high-pressure cell
(P < 1.1 GPa). At ambient pressure, this sample shows the weakest
antiferromagnetic (AF) Bragg reflections reported so far, corresponding to the
volume-averaged staggered moment of mord ~ 0.011 mB/U. Under applied pressure,
the AF scattering intensity exhibits a sharp increase at P ~ 0.7 GPa at low
temperatures. The saturation value of the AF scattering intensity above 0.7 GPa
corresponds to mord ~ 0.41 mB/U, which is in good agreement with that (~ 0.39
mB/U) observed above 1.5 GPa in our previous NS measurements. The
superconductivity is dramatically suppressed by the evolution of AF phase,
indicating that the superconducting state coexists only with the hidden order
phase. The presence of parasitic ferro- and/or antiferromagnetic phases with
transition temperatures T1star =120(5) K, T2star = 36(3) K and T3star = 16.5(5)
K and their relationship to the low-T ordered phases are also discussed.Comment: 6 pages, 7 figures, submitted to J. Magn. Magn. Mater. (ICM2006
High-field phase diagram of the Haldane-gap antiferromagnet
We have determined the magnetic phase diagram of the quasi-one-dimensional
1 Heisenberg antiferromagnet by
specific heat measurements to 150 mK in temperature and 32 T in magnetic field.
When field is applied along the spin-chain direction, a new phase appears at
T. For the previously known phases of field-induced order,
accurate determination is made of the power-law exponents of the ordering
temperature near the zero-temperature critical field , owing to the
four-fold improvement of the minimum temperature over the previous work. The
results are compared with the predictions based on the Bose-Einstein
condensation of triplet excitations. Substituting deuterium for hydrogen is
found to slightly reduce the interchain exchange.Comment: 6 pages, 6 figure
Tuning Low Temperature Physical Properties of CeNiGe by Magnetic Field
We have studied the thermal, magnetic, and electrical properties of the
ternary intermetallic system CeNiGe by means of specific heat,
magnetization, and resistivity measurements. The specific heat data, together
with the anisotropic magnetic susceptibility, was analyzed on the basis of the
point charge model of crystalline electric field. The \,=\,5/2 multiplet of
the Ce is split by the crystalline electric field (CEF) into three
Kramers doublets, where the second and third doublet are separated from the
first (ground state) doublet by 100\,K and
170\,K, respectively. In zero field CeNiGe exhibits an
antiferromangeic order below = 5.0\,K. For
\textbf{H}\,\,\textbf{a} two metamagnetic transitions are clearly
evidenced between 2\,\,4\,K from the magnetization isotherm and extended
down to 0.4\,K from the magnetoresistance measurements. For
\textbf{H}\,\,\textbf{a}, shifts to lower temperature as
magnetic field increases, and ultimately disappears at
32.5\,kOe. For , the electrical resistivity shows the quadratic
temperature dependence (). For , an
unconventional -dependence of with emerges, the
exponent becomes larger as magnetic field increases. Although the
antiferromagnetic phase transition temperature in CeNiGe can be
continuously suppressed to zero, it provides an example of field tuning that
does not match current simple models of Quantum criticality.Comment: accepted PR
Diamagnetic susceptibility of spin-triplet ferromagnetic superconductors
We calculate the diamagnetic susceptibility in zero external magnetic field
above the phase transition from ferromagnetic phase to phase of coexistence of
ferromagnetic order and unconventional superconductivity. For this aim we use
generalized Ginzburg-Landau free energy of unconventional ferromagnetic
superconductor with spin-triplet electron pairing. A possible application of
the result to some intermetallic compounds is briefly discussed.Comment: 7 pages, 1 figur
Effects of Randomness on the Field-Induced Phase Transition in the S=1 Bond-Alternating Spin Chain NTENP
We report novel effects of randomness in the S=1 bond-alternating
antiferromagnetic chain compound with a dimer-singlet ground state
[Ni(N,N'-bis(3-aminopropyl)propane-1,3-diamine(mu-NO2]ClO4 abbreviated as
NTENP. The 15N NMR spectra develop a continuum with sharply peaked edges at low
temperatures, indicating an inhomogeneous staggered magnetization induced by
magnetic field. We attribute this to random anisotropic interactions due to
disorder of NO2 groups in the chains. The field-induced antiferromagnetic
transition exhibits remarkably anisotropic behavior. We propose that a
field-induced incoherent magnetization is transformed into a coherent
antiferromagnetic moment with spatially fluctuating amplitude.Comment: 4pages, 5 figues, submitted to J. Phys. Soc. Jp
Coupled CDW and SDW Fluctuations as an Origin of Anomalous Properties of Ferromagnetic Superconductor UGe_2
It is shown that anomalous properties of UGe_2 can be understood in a unified
way on the basis of a single assumption that the superconductivity is mediated
by the coupled SDW and CDW fluctuations induced by the imperfect nesting of the
Fermi surface with majority spins at T=T_x(P) deep in the ferromagnetic phase.
Excess growth of uniform magnetization is shown to develop in the temperature
range T<T_x(P) as a mode-coupling effect of coupled growth of SDW and CDW
orderings, which has been observed by two different types of experiments. The
coupled CDW and SDW fluctuations are shown to be essentially ferromagnetic spin
fluctuations which induce a spin-triplet p-wave attraction. These fluctuations
consist of two modes, spin and charge fluctuations with large momentum transfer
of the nesting vector. An anomalous temperature dependence of the upper
critical field H_c2(T) such as crossing of H_c2(T) at P=11.4 kbar and P=13.5
kbar, can be understood by the strong-coupling-superconductivity formalism.
Temperature dependence of the lattice specific heat including a large shoulder
near T_x is also explained quite well as an effect of a kind of Kohn anomaly
associated with coupled SDW-CDW transition.Comment: (12 pages, 10 eps figures) submitted to J. Phys. Soc. Jp
Improved sensitivity of magnetic measurements under high pressure in miniature ceramic anvil cell for a commercial SQUID magnetometer
Two modifications have been made to a miniature ceramic anvil high pressure
cell (mCAC) designed for magnetic measurements at pressures up to 12.6 GPa in a
commercial superconducting quantum interference (SQUID) magnetometer [N.
Tateiwa et al., Rev. Sci. Instrum. 82, 053906 (2011)., ibid. 83, 053906
(2012)]. Replacing the Cu-Be piston in the former mCAC with a composite piston
composed of the Cu-Be and ceramic cylinders reduces the background
magnetization significantly smaller at low temperatures, enabling more precise
magnetic measurements at low temperatures. A second modification to the mCAC is
the utilization of a ceramic anvil with a hollow in the center of the culet
surface. High pressures up to 5 GPa were generated with the "cupped ceramic
anvil" with the culet size of 1.0 mm.Comment: Rev. Sci. Instrum. 84, 046105 (2013
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