27 research outputs found
Magnetic structure and spin dynamics of quasi-one-dimensional spin-chain antiferromagnet BaCo2V2O8
We report a neutron diffraction and muon spin relaxation muSR study of static
and dynamical magnetic properties of BaCo2V2O8, a quasi-one-dimensional
spin-chain system. A proposed model for the antiferromagnetic structure
includes: a propagation vector k_AF = (0, 0, 1), independent of external
magnetic fields for fields below a critical value H_c(T). The ordered moments,
of 2.18 \mu_B per Co ion, are aligned along the crystallographic c-axis. Within
the screw chains, along the c axis, the moments are arranged
antiferromagnetically. In the basal planes the spins are arranged
ferromagnetically (forming zig-zags paths) along one of the axis and
antiferromagnetically along the other. The temperature dependence of the
sub-lattice magnetization is consistent with the expectations of the 3D Ising
model. A similar behavior is observed for the internal static fields at
different muon stopping sites. Muon time spectra measured at weak longitudinal
fields and temperatures much higher than T_N can be well described using a
single muon site with an exponential muon spin relaxation that gradually
changes into an stretched exponential on approaching T_N. The
temperature-induced changes of the relaxation suggest that the Co fluctuations
dramatically slow down and the system becomes less homogeneous as it approaches
the antiferromagnetic state.Comment: 7 pages, 9 figure
Pressure-induced phase transition and band gap decrease in semiconducting β-Cu2V2O7
The understanding of the interplay between crystal structure and electronic structure in semiconductor materials is of great importance due to their potential technological applications. Pressure is an ideal external control parameter to tune the crystal structures of semiconductor materials in order to investigate their emergent piezo-electrical and optical properties. Accordingly, we investigate here the high-pressure behavior of the semiconducting antiferromagnetic material β-Cu2V2O7, finding it undergoes a pressure-induced phase transition to γ-Cu2V2O7 below 4000 atm. The pressure-induced structural and electronic evolutions are investigated by single-crystal X-ray diffraction, absorption spectroscopy and ab initio density functional theory calculations. β-Cu2V2O7 has previously been suggested as a promising photocatalyst for water splitting. Now, these new results suggest that β-Cu2V2O7 could also be of interest with regards to barocaloric effects, due to the low phase -transition pressure, in particular because it is a multiferroic material. Moreover, the phase transition involves an electronic band gap decrease of approximately 0.2 eV (from 1.93 to 1.75 eV) and a large structural volume collapse of approximately 7%.The authors acknowledge financial support from the Spanish Research Agency (AEI) and Spanish Ministry of Science and Investigation (MCIN) under projects PID2019106383GBC41/ C43/C44 (DOI: 10.13039/501100011033), and projects PGC2018-101464−B-I00 and PGC2018-097520-A-I00 (cofinanced by EU FEDER funds). The authors acknowledge financial support from the MALTA Consolider Team network, under project RED2018-102612-T. R.T. acknowledges funding from the Spanish Ministry of economy and competitiveness (MINECO) via the Juan de la Cierva Formación program (FJC2018-036185-I). J.G.P. thanks the Servicios Generales de Apoyo a la Investigación (SEGAI) at the University of La Laguna. A.L. and D.E. would like to thank the Generalitat Valenciana for the Ph.D. fellowship GRISOLIAP/2019/025, and the authors would also like to thank them for funding under the Grant Prometeo/2018/123 (EFIMAT). The authors also thank ALBA synchrotron light source for funded experiment under proposal numbers 2020074389 and 2020074398 at the MSPD-BL04 beamline
A New One-Dimensional Spin Chain System Co<sub>3</sub>(BPO<sub>4</sub>)<sub>2</sub>(PO<sub>4</sub>)(OH)<sub>3</sub> Showing 1/3 Magnetization Plateau
A new
borophosphate Co<sub>3</sub>(BPO<sub>4</sub>)<sub>2</sub>(PO<sub>4</sub>)(OH)<sub>3</sub> was synthesized by a conventional hydrothermal
method. The titled compound crystallizes in the monoclinic system
with space group <i>Cc</i>, which exhibits a typical spin-chain
structure. In the structural framework, Co<sup>2+</sup> ions form
a zigzag chain via edge-sharing oxygen atoms, and further the zigzag
Co-chains are separated by linear [B<sub>2</sub>P<sub>2</sub>O<sub>8</sub>]<sub>∞</sub> chains. Magnetic measurements confirm
that Co<sub>3</sub>(BPO<sub>4</sub>)<sub>2</sub>(PO<sub>4</sub>)(OH)<sub>3</sub> possesses an antiferromagnetic ordering at <i>T</i><sub>N</sub> = 12 K, while a 1/3 plateau is observed in
the magnetization curve at 2 K. The possible spin arrangements for
antiferromagnetic, ferrimagnetic, and ferromagnetic states are also
suggested
Layered Cu<sub>7</sub>(TeO<sub>3</sub>)<sub>2</sub>(SO<sub>4</sub>)<sub>2</sub>(OH)<sub>6</sub> with Diluted Kagomé Net Containing Frustrated Corner-Sharing Triangles
The half-spin Kagomé
antiferromagnet is one of the most promising candidates for the realization
of a quantum spin liquid state because of its inherent frustration
and quantum fluctuations. The search for candidates for quantum spin
liquids with novel spin topologies is still a challenge. Herein, we
report a new diluted Kagomé lattice in Cu<sub>7</sub>(TeO<sub>3</sub>)<sub>2</sub>(SO<sub>4</sub>)<sub>2</sub>(OH)<sub>6</sub>,
showing a 9/16-depleted triangle lattice, where the corner-sharing
triangle units [Cu<sub>5</sub>(OH)<sub>6</sub>O<sub>8</sub>] are separated
by CuO<sub>2</sub>(OH)<sub>2</sub>. Magnetic measurements show that
the title compound does not exhibit long-range antiferromagnetic order
down to 2 K, suggesting strong spin frustration with <i>f</i> > 19
Layered Cu<sub>7</sub>(TeO<sub>3</sub>)<sub>2</sub>(SO<sub>4</sub>)<sub>2</sub>(OH)<sub>6</sub> with Diluted Kagomé Net Containing Frustrated Corner-Sharing Triangles
The half-spin Kagomé
antiferromagnet is one of the most promising candidates for the realization
of a quantum spin liquid state because of its inherent frustration
and quantum fluctuations. The search for candidates for quantum spin
liquids with novel spin topologies is still a challenge. Herein, we
report a new diluted Kagomé lattice in Cu<sub>7</sub>(TeO<sub>3</sub>)<sub>2</sub>(SO<sub>4</sub>)<sub>2</sub>(OH)<sub>6</sub>,
showing a 9/16-depleted triangle lattice, where the corner-sharing
triangle units [Cu<sub>5</sub>(OH)<sub>6</sub>O<sub>8</sub>] are separated
by CuO<sub>2</sub>(OH)<sub>2</sub>. Magnetic measurements show that
the title compound does not exhibit long-range antiferromagnetic order
down to 2 K, suggesting strong spin frustration with <i>f</i> > 19
K<sub>4</sub>Fe<sub>4</sub>P<sub>5</sub>O<sub>20</sub>: A New Mixed Valence Microporous Compound with Elliptical Eight-Ring Channels
A new small-pore compound K<sub>4</sub>Fe<sub>4</sub>P<sub>5</sub>O<sub>20</sub> was obtained by conventional solid-state
reaction
in a closed crucible. The crystal structure is constructed by Fe<sub>4</sub>P<sub>5</sub>O<sub>20</sub> units forming chains along the <i>c</i> axis and elliptical eight-ring channels on the <i>a</i>–<i>b</i> plane in which K cations locate
inside. Such structural characteristics seem to be quite similar to
those seen in the natrolite family. However, Fe ions in K<sub>4</sub>Fe<sub>4</sub>P<sub>5</sub>O<sub>20</sub> have trigonal–bipyramidal
instead of common tetrahedral coordination. Furthermore, our experimental
results combined from magnetic susceptibility and <sup>57</sup>Fe
Mössbauer spectrum measurements show mixed valence Fe<sup>3+</sup>/Fe<sup>2+</sup> in the titled material. To the best
of our knowledge, this is the first example that contains mixed valence
iron ions in a so-called natrolite framework