Nonlinear conduction in charge-ordered Pr0.63Ca0.37MnO3: Effect of magnetic fields

Nonlinear conduction in a single crystal of charge-ordered Pr0.63Ca0.37MnO3 has bren investigated in an applied magnetic field. In zero field, the nonlinear conduction, which starts at T< T-CO, can give rise to a region of negative differential resistance (NDR) which shows up below the Neel temperature. Application of a magnetic field Inhibits the appearance of NDR and makes the nonlinear conduction strongly hysteritic on cycling of the bias current. This is most severe in the temperature range where the charge-ordered state melts in an applied magnetic field. Our experiment strongly suggests that application of a magnetic field in the charge-ordering regime causes a coexistence of two phases.

Magnetic properties of rare earth nickelates of the Ln(2)BaNiO(5) family

Rare-earth nickelates Ln(2)BaNi(1-x)Cu(2)O(5), Ln = Nd and Dy, and Dy2-xYxBaNiO5 have been synthesized in order to investigate the effect of substitution of Ni by Cu and Dy by nonmagnetic Y on the magnetic properties of the nickelates. In Ln(2)BaNi(1-x)Cu(x)O(5), the nickelate structure (x=0.0) changes to the cuprate structure (x=1.0) at a specific composition (x=0.3). The Neel temperature of Nd2BaNi1-xCuxO5 decreases continuously with increase in x upto x=0.3 (T-N = 18K); when x > 0.3, the materials are paramagnetic down to 20K. The mu(eff) in Nd2BaNi1-xCxO5 essentially corresponds to the contribution of the Nd ions. In Dy2-xYxBaNiO5, the Neel temperature decreases from 40K when x=0.0 to 24K when x=1.5. The compositions with 1.5 less than or equal to x less than or equal to 2 (including the x=1.95 composition) are paramagnetic down to 20K, unlike Y2BaNiO5 (x=2.0) which exhibits a T-N of 370K. Even the smallest concentration of paramagnetic Dy seems to destroy the antiferromagnetic Ni-O-Ni chains in Y2BaNiO5.

Density-matrix renormalization-group studies of the spin-1/2 Heisenberg system with dimerization and frustration

Using the density-matrix renormalization-group technique, we study the ground-state phase diagram and other low-energy properties of an isotropic antiferromagnetic spin-1/2 chain with both dimerization and frustration, i.e., an alternation delta of the nearest-neighbor exchanges and a next-nearest-neighbor exchange J(2). For delta = 0, the system is gapless for J(2) < J(2c) and has a gap for J(2) > J(2c) where J(2c) is about 0.241. For J(2) = J(2c) the gap above the ground state grows as delta to the power 0.667 +/- 0.001. In the J(2)-delta plane, there is a disorder line 2J(2) + delta = 1. To the left of this line, the peak in the static structure factor S(q) is at q(max) = pi (Neel phase), while to the right of the line, q(max) decreases from pi to pi/2 as J(2) is increased to large values (spiral phase). For delta = 1, the system is equivalent to two coupled chains as on a ladder and it is gapped for all values of the interchain coupling.

Low-temperature specific heat of antiferromagnetic EuNi5P3 and mixed-valent EuNi2P2 in magnetic fields to 7 T

he specific heats of EUNi(5)P(3), an antiferromagnet, and EuNi2P2, a mixed-valence compound, have been measured between 0.4 and 30 K in magnetic fields of, respectively, 0, 0.5, 1, 1.5, 2.5, 5, and 7 T, and 0 and 7 T. In zero field the specific heat of EuNi5P3 shows a h-like anomaly with a maximum at 8.3 K. With increasing field in the range 0-2.5 T, the maximum shifts to lower temperatures, as expected for an antiferromagnet. In higher fields the antiferromagnetic ordering is destroyed and the magnetic part of the specific heat approaches a Schottky anomaly that is consistent with expectations for the crystal-field/Zeeman levels. In low fields and for temperatures between 1.5 acid 5 K the magnetic contribution to the specific heat is proportional to the temperature, indicating a high density of excited states with an energy dependence that is very unusual for an antiferromagnet. The entropy associated with the magnetic ordering is similar to R In8, confirming that only the Eu2+-with J=7/2, S=7/2, L=0-orders below 30 R. In zero field approximately 20% of the entropy occurs above the Neel temperature, consistent. with the usual amount of short-range order observed in antiferromagnets. The hyperfine magnetic field at the Eu nuclei in EUNi(5)P(3) is 33.3 T, in good agreement with a value calculated from electron-nuclear double resonance measurements. For EuNi2P2 the specific heat is nearly field independent and shows no evidence of magnetic ordering or hyperfine fields. The coefficient of the electron contribution to the specific heat is similar to 100 mJ/mol K-2.

Synthesis and properties of La1-xSrxFeO3

Fine particle strontium substituted lanthanum ferrites La1-xSrxFeO3, where x = 0.0-1.0, have been synthesized by the solution combustion method using corresponding metal nitrates, oxalyl dihydrazide (ODH) or tetra formal tris azine (TFTA). Formation of La1-xSrxFeO3 was confirmed by the XRD and the fine particle nature of the ferrites investigated using SEM, particle size analysis and BET surface area measurements. La1-xSrxFeO3 (up to x = 0-0.4) exhibited low resistivity near the Neel temperatures. La1-xSrxFeO3 with x greater than or equal to 0.8 when used as bifunctional electrodes, showed oxygen evolution and reduction activity comparable with the orthoferrites prepared by the conventional solid state method. (C) 1999 Elsevier Science B.V. All rights reserved.

Evidence of nanoscale structural phase separation in large bandwidth La0.2Sr0.8MnO3

We have investigated the structural evolution of La0.2Sr0.8MnO3 using temperature dependent high resolution synchrotron x-ray diffraction technique. In a wide temperature range, La0.2Sr0.8MnO3 reveals nanoscale structural inhomogeneity consisting of cubic and tetragonal phases. The present results suggest that domains of nanometer size of the tetragonal (low temperature) phase start nucleating in the cubic (high temperature) phase even above the Neel temperature (T-N). The tetragonal phase fraction increases substantially below T-N. Detailed analysis suggests that the twinned phase is tetragonal, orbital ordered, and insulating. At temperatures below 170 K, a small amount of the cubic phase is retained. The present results reveal the significance of the connectivity between the nanoscale structural phase separation with the physical properties.

Study of ground state phases for spin-1/2 Falicov-Kimball model on a triangular lattice

The spin dependent Falicov-Kimball model (FKM) is studied on a triangular lattice using numerical diagonalization technique and Monte-Carlo simulation algorithm. Magnetic properties have been explored for different values of parameters: on-site Coulomb correlation U, exchange interaction J and filling of electrons. We have found that the ground state configurations exhibit long range Neel order, ferromagnetism or a mixture of both as J is varied. The magnetic moments of itinerant (d) and localized U) electrons are also studied. For the one-fourth filling case we found no magnetic moment from d- and f-electrons for U less than a critical value. `.2014 Elsevier Ltd. All rights reserved.

Magneto-structural study of the multiferroic BiFeo(3)-SrTiO3

The structural and magnetic study of the pseudo-binary multiferroic (1 x)BiFeO3 (x)SrTiO3 has been investigated as a function of composition and temperature. In contrary to the previous studies, detailed examination revealed that the reported anomaly in the magnetization at x-0.30 does not occur at the composition induced rhombohedral-cubic phase boundary, but within the rhombohedral phase itself. The rhombohedral to cubic transition occurs at x > 0.4. Evidence of magneto-elastic coupling near the Neel temperature and nucleation-growth mode of the rhombohedral-cubic transformation, with both the phases coexisting over a range of temperature was found. (C) 2014 Elsevier B.V. All rights reserved.

Effect of Zn substitution on the structural and magnetic properties of Ni-Co ferrites

A series of ferrite samples with the compositional formula, Ni0.5Co0.5-xZnxFe2O4 (0 <= x <= 0.5), was prepared using the citrate based sol gel method for the better understanding of zinc doping on the structural and magnetic properties. The Rietveld-refined X-ray diffraction data revealed that the samples are having cubic structure with the Fd-3m space group. The lattice parameter increased linearly with increasing Zn content. The surface morphology and stoichiometric ratio of the compositional elements were analyzed by scanning electron microscopy equipped with energy dispersive spectroscopy (EDS). EDS showed that the elemental ratios were stoichiometric. An examination of the magnetic properties revealed an increase in saturation magnetization with increasing Zn concentration up to x=0.3 and a decrease thereafter. These results could be explained using Neel's collinear two-sub-lattice model and three-sub-lattice non-collinear model suggested by Yafet and Kittel. The magnetic cubic anisotropy constant determined by the law of approach to saturation decreased with increasing Zn content. The underlying mechanism behind observed behavior was discussed qualitatively. (C) 2014 Elsevier Ltd and Techna Group S.r.l. All rights reserved.

Phase diagram of the half-filled ionic Hubbard model

We study the phase diagram of the ionic Hubbard model (IHM) at half filling on a Bethe lattice of infinite connectivity using dynamical mean-field theory (DMFT), with two impurity solvers, namely, iterated perturbation theory (IPT) and continuous time quantum Monte Carlo (CTQMC). The physics of the IHM is governed by the competition between the staggered ionic potential Delta and the on-site Hubbard U. We find that for a finite Delta and at zero temperature, long-range antiferromagnetic (AFM) order sets in beyond a threshold U = U-AF via a first-order phase transition. For U smaller than U-AF the system is a correlated band insulator. Both methods show a clear evidence for a quantum transition to a half-metal (HM) phase just after the AFM order is turned on, followed by the formation of an AFM insulator on further increasing U. We show that the results obtained within both methods have good qualitative and quantitative consistency in the intermediate-to-strong-coupling regime at zero temperature as well as at finite temperature. On increasing the temperature, the AFM order is lost via a first-order phase transition at a transition temperature T-AF(U,Delta) or, equivalently, on decreasing U below U-AF(T,Delta)], within both methods, for weak to intermediate values of U/t. In the strongly correlated regime, where the effective low-energy Hamiltonian is the Heisenberg model, IPT is unable to capture the thermal (Neel) transition from the AFM phase to the paramagnetic phase, but the CTQMC does. At a finite temperature T, DMFT + CTQMC shows a second phase transition (not seen within DMFT + IPT) on increasing U beyond U-AF. At U-N > U-AF, when the Neel temperature T-N for the effective Heisenberg model becomes lower than T, the AFM order is lost via a second-order transition. For U >> Delta, T-N similar to t(2)/U(1 - x(2)), where x = 2 Delta/U and thus T-N increases with increase in Delta/U. In the three-dimensional parameter space of (U/t, T/t, and Delta/t), as T increases, the surface of first-order transition at U-AF(T,Delta) and that of the second-order transition at U-N(T,Delta) approach each other, shrinking the range over which the AFM order is stable. There is a line of tricritical points that separates the surfaces of first- and second-order phase transitions.

Effect of Fe doping on the magnetic ordering temperature of ErMnO3

We studied the effect of Fe doping on structural, magnetic, and dielectric properties of hexagonal ErMnO3 system. For 50% doping of Fe on Mn site in ErMnO3 modulated its crystallographic structure from hexagonal to orthorhombic phase. Accompanied with the structural phase transition in ErMnO3, the magnetic properties are effectively modified. The Fe doped samples exhibit enhancement in antiferromagnetic ordering Neel temperature (T-N) from 77K (ErMnO3) to 280K (ErFe0.5Mn0.5O3). The anomalies observed in the dielectric constant around T-N in doped ErMnO3 samples indicate the coupling between electric and magnetic order parameters. (C) 2015 AIP Publishing LLC.

Polyketide Quinones Are Alternate Intermediate Electron Carriers during Mycobacterial Respiration in Oxygen-Deficient Niches

Mycobacterium tuberculosis (Mtb) adaptation to hypoxia is considered crucial to its prolonged latent persistence in humans. Mtb lesions are known to contain physiologically heterogeneous microenvironments that bring about differential responses from bacteria. Here we exploit metabolic variability within biofilm cells to identify alternate respiratory polyketide quinones (PkQs) from both Mycobacterium smegmatis (Msmeg) and Mtb. PkQs are specifically expressed in biofilms and other oxygen-deficient niches to maintain cellular bioenergetics. Under such conditions, these metabolites function as mobile electron carriers in the respiratory electron transport chain. In the absence of PkQs, mycobacteria escape from the hypoxic core of biofilms and prefer oxygenrich conditions. Unlike the ubiquitous isoprenoid pathway for the biosynthesis of respiratory quinones, PkQs are produced by type III polyketide synthases using fatty acyl-CoA precursors. The biosynthetic pathway is conserved in several other bacterial genomes, and our study reveals a redox-balancing chemicocellular process in microbial physiology.

Evaluación productiva y reproductiva de la raza holstein friesian canadiense bajo explotación intensiva en el trópico seco de Nicaragua

El presente trabajo se realizó en base a los registros productivos y reproductivos del hato Holstein. Friesian Canadiense existente en el distrito tres de la Empresa Genética "Roberto Alvarado" (Chiltepe); ubicada en el Departamento de Managua, Nicaragua, a una latitud 12º 14' y una longitud de 86º 25' y a una elevación promedio de 49 msnm, con una temperatura promedio anual de 28.43°C, humedad relativa promedio anual 68.38% y una precipitación promedio anual de 87.72 mm. distribuida en dos épocas: Época lluviosa (Mayo - Octubre ) y época seca (Noviembre - Abril). A partir de la información proporcionada se evaluó el efecto de distintos factores ambientales : número de partos (NUMPA), época de parto (EPOCA) y año de parto (AP); sobre las variables productivas y reproductivas: producción de leche total (PLT), duración de la lactancia (DL), producción de leche diaria (PLD), intervalo entre partos (IEP) y producción de leche por día de intervalo entre partos (PLDIEP), las cuales resultaron todas altamente significativas (P < 0.01), considerando para la variable PLT el efecto de la covariable DL con Numpa. También se caracterizó el comportamiento productivo y reproductivo del hato, basado en el cálculo de los promedios de mínimos cuadrados de las características productivas y reproductivas en los diferentes niveles de cada uno de los factores estudiados, resultando promedios generales de: PLT 3,207.53 ± 54.37 Kg., DL 321.98 ± 3.89 días, PLD 10.67 ± 0.17 Kg., IEP 468;63 ± 4.29 días y PLDIEP 7.51 ± 0.14 Kg. Además se estimaron las correlaciones lineales fenotípicas entre las variables y los factores NUMPA y EPAR , resultando entre ellos los valores más altos para: EPAR -NUMPA (r= + 0.96), DL - IEP (r= + 0.80), PLD - PLDIEP (r= + 0.80), PLT - PLDIEP (r= + 0.76) y valores absolutos para r más bajos entre NUMPA - PLDIEP (r= + 0.18), NUMPA - PLT (r= -0.19), NUMPA - PLD (r= + 0.23) y EPAR - PLT (r= - 0.21).

Efecto de diferentes niveles de aplicación nitrogenada en la producción de semilla de pasto gamba (Andropogon gayanus kunth var, CIAT 621)

En la presente investigación se evaluó los efectos de cuatro diferentes niveles de fertilización nitrogenada (O; 25; 50; 75 y 100 Kg N/ha), sobre la producción de semilla de Andropogon gayanus Kunth como una alternativa para los productores de la zona de Masatepe. El ensayo se realizó de Junio a Diciembre de 1994, en la finca "Santa Juana" municipio de Masatepe departamento de Masaya. Localizada a 11° 53' latitud norte y 86° 08' longitud oeste, a 470 m.s.n.m., con una precipitación promedio anual de 1,849.3 mm, humedad relativa de 83.6% y una temperatura media anual de 24°C. Se utilizó un diseño experimental de Bloques Completos al Azar (BCA), con cuatro repeticiones. Las parcelas útiles fueron de 3 x 4m2 y como variable respuesta se determinó la producción de semilla cruda, semilla pura ajustada y porcentaje de germinación. Se realizó un corte de uniformidad dejando el pasto a una altura de 20 cm al raz del suelo. A los 20 días después se procedió a aplicar en una sola dosis, los diferentes niveles de fertilización. El tratamiento con 50 kg N/ha fue seleccionado por obtener los mayores beneficios en relación al gasto. Siendo por tal razón el más idóneo para la producción de semilla del Andropogon gayanus, para el sector evaluado, alcanzando 479.21 Kg/ha de semilla pura ajustada. La no significancia entre los tratamientos de fertilización se atribuyó, posiblemente a la heterogeneidad del suelo, el alto contenido de minerales y de materia orgánica. Sin embargo, el experimento demostró la adaptabilidad de Andropogon gayanus a las características del suelo, climatología de la zona.

Influencia de diferentes periodos de destete en conejas primiparas en el municipio de Diriamba, Departamento de Carazo, Nicaragua

Este trabajo fue realizado en la Quinta "Myriam", ubicada en el municipio de Diriamba, departamento de Carazo, Nicaragua, propiedad del Dr. Jorge Ferreira. La ubicación geográfica del municipio está comprendida entre los 11° 50' y 12° 00' de Latitud Norte y entre los 86° 00' y 86° 15' de Longitud Oeste, cuenta con una elevación de 551 m.s.n.m., los datos meteorológicos de la zona en los últimos cuatro años (90-93) en cuanto a temperatura, humedad relativa y precipitación promedio fueron: 23.8 °C, 84% y 1184,5 mm respectivamente, (INETER, Departamento de Estadística, 1993). En el presente ensayo, se utilizó un diseño estadístico completamente aleatorizado (DCA), mediante el cual se evaluó el efecto de 3 tratamientos (15, 30 y 45 días de destete) sobre las variables Peso de la Camada al Destete (PCD), Peso de la Madre al Destete (PMD), Peso de la Madre al Segundo Parto (PSP), Ganancia Media Diaria del Parto 1 al Parto 2 (GMDp 1.P2) , con 4 repeticiones por tratamiento, éstas repeticiones estuvieron constituidas por conejas primíparas, las cuales tuvieron un peso que osciló entre 3 - 3.18 kg. y edad homogénea de 7 meses. Las variables fueron sometidas a la prueba de Duncan para determinar la superioridad en rango por tratamiento. Mediante el análisis de varianza se encontró que el efecto de los tratamientos resultó ser altamente significativo sobre la variable Peso de la Camada al Destete (PCD) (P0.01), significativo sobre las variables Peso de la Madre al Segundo Parto (PSP) y Ganancia Media Diaria del Parto 1 al Parto 2 (GMD p 1.P2) (P0.1) y no significativo sobre la variable Peso de la Madre al Destete (PMD) (NS). El efecto de la covariable Peso al Primer Parto (P1P) resultó ser altamente significativo sobre las variables Peso de la Madre al Destete (PMD) y Peso de la Madre al Segundo Parto (PSP) (P0.01). Después de someter las variables a la prueba de DUNCAN se encontraron los siguientes promedios por tratamiento: Peso de la Camada al Destete (PCD) ; T.15 días 1.538 kg P.V.(C), T.30 días 3.360 kg P.V. (B), T.45 días 4.523 kg P.V. (A), Peso de la Madre al Destete (PMD); T.15 días 3.649 kg P.V. (A) T.30 días 3.549 kg P.V. (A), T.45 dias 3.493 kg P.V.(A). Peso de la Madre al Segundo Parto (PSP); T.15 días 3. 449 kg P.V. (B), T.30 días 3.628 kg P.V. (AB), T.45 días 3.777 kg P.V.(A). Ganancia Media Diaria del Parto 1 al Parto 2 (GMD p 1.P2) T .15 días (2.071 g (B), T.30 días 2.718 g (AB), T.45 días 2. 975 g (A). Los promedios y desviaciones standard para las variables Ganancia Media Diaria del Parto 1 al Destete 1 (GMDp1-D1)y Ganancia Media Diaria del Destete l al Parto 2 (GMDD1.P2) por tratamiento fueron: GMD P1-D1; T.l5 días 3.84 g ± 0.50 g, T.30 días 2.54 g ± 0.64 g, T.45 días 2.37 g ± 0.72 g. GMD D1-P2; T.l5 días 2.26 g ± 0.54 g, T.30 días 3.17 g ± 0.74 g, T.45 días 3.93 g ± 0.28 g. Se encontró que el alimento tipo único suministrado a los animales bajo experimentación, cumplió con los requerimientos nutricionales de la especie estudiada. Los costos encontrados por hembra, por tratamiento, fueron C$ 197.21 destete de 15 días, C$ 220.28 destete de 30 días, C$ 243 .1.4 destete de 45 días. Los costos por gazapo destetado fueron de C$ 5.48 destete de 15 días, C$ 6.12 destete de 30 días, C$ 8.10 destete de 45 días.