271 research outputs found

    Manifestation of geometric frustration on magnetic and thermodynamic properties of pyrochlores Sm2X2O7Sm_2X_2O_7 (X=Ti, Zr)

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    We present here magnetization, specific heat and Raman studies on single-crystalline specimens of the first pyrochlore member Sm2Ti2O7Sm_2Ti_2O_7 of the rare-earth titanate series. Its analogous compound Sm2Zr2O7Sm_2Zr_2O_7 in the rare-earth zirconate series is also investigated in the polycrystalline form. The Sm spins in Sm2Ti2O7Sm_2Ti_2O_7 remain unordered down to at least T = 0.5 K. The absence of magnetic ordering is attributed to very small values of exchange (θcw −0.26K\theta_{cw} ~ -0.26 K) and dipolar interaction (μeff 0.15μB\mu_{eff} ~ 0.15 \mu_B) between the Sm3+Sm^{3+} spins in this pyrochlore. In contrast, the pyrochlore Sm2Zr2O7Sm_2Zr_2O_7 is characterized by a relatively large value of Sm-Sm spin exchange (θcw −10K\theta_{cw} ~ - 10 K); however, long-range ordering of the Sm3+Sm^{3+} spins is not established at least down to T = 0.67 K, due to frustration of the Sm3+Sm^{3+} spins on the pyrochlore lattice. The ground state of Sm3+Sm^{3+} ions in both pyrochlores is a well-isolated Kramer's doublet. The higher-lying crystal field excitations are observed in the low-frequency region of the Raman spectra of the two compounds recorded at T = 10 K. At higher temperatures, the magnetic susceptibility of Sm2Ti2O7Sm_2Ti_2O_7 shows a broad maximum at T = 140 K while that of Sm2Zr2O7Sm_2Zr_2O_7 changes monotonically. Whereas Sm2Ti2O7Sm_2Ti_2O_7 is a promising candidate for investigating spin-fluctuations on a frustrated lattice as indicated by our data, the properties of Sm2Zr2O7Sm_2Zr_2O_7 seem to conform to a conventional scenario where geometrical frustration of the spin exclude their long-range ordering.Comment: 24 pages, 6 figures, Accepted for publication in Phys. Rev.

    Gender differences in perceived health related quality of life among persons living with HIV

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    In the era of HlV/AlDS and in the context of the developing world HIV/AIDS has led to a pandemic. HIV antiretroviral drugs are inaccessible and unaffordable and the only choice that health care providers have is to work towards improving the quality of life of individuals as long as they live with this dreaded disease. This study on 203 seropositive individuals, 102 women and 101 men, was undertaken to find out the differences in the quality of life perceived by women and men living with HIV/AIDS. The WHOQOL-BREF scale was used to assess the quality of life. The findings from this study reveal that men report a poor quality of life in the psychological domain (p<0.01) while women in the sociological domain (p=0.03). The stage of illness does not seem to influence quality of life among women and men. The findings emphasize the need for health providers to assess the QOL among people living with HIV/AIDS. This information would be helpful in planning effective intervention strategies for men and women living with HlV/AlDS in order to be ensured of a quality of life

    Magnetic order in double-layer manganites (La(1-z)Pr(z))1.2Sr1.8Mn2O7: intrinsic properties and role of the intergrowths

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    We report on an investigation of the double-layer manganite series (La(1-z)Pr(z))1.2Sr1.8Mn2O7 (0 <= z <= 1), carried out on single crystals by means of both macroscopic magnetometry and local probes of magnetism (muSR, 55Mn NMR). Muons and NMR demonstrate an antiferromagnetically ordered ground state at non-ferromagnetic compositions (z >= 0.6), while more moderate Pr substitutions (0.2 <= z <= 0.4) induce a spin reorientation transition within the ferromagnetic phase. A large magnetic susceptibility is detected at {Tc,TN} < T < 250K at all compositions. From 55Mn NMR spectroscopy, such a response is unambiguously assigned to the intergrowth of a ferromagnetic pseudocubic phase (La(1-z)Pr(z))(1-x)Sr(x)MnO3, with an overall volume fraction estimated as 0.5-0.7% from magnetometry. Evidence is provided for the coupling of the magnetic moments of these inclusions with the magnetic moments of the surrounding (La(1-z)Pr(z))1.2Sr1.8Mn2O7 phase, as in the case of finely dispersed impurities. We argue that the ubiquitous intergrowth phase may play a role in the marked first-order character of the magnetic transition and the metamagnetic properties above Tc reported for double-layer manganites.Comment: 11 pages, 9 figures. Submitted to Phys. Rev.

    Temperature dependent Raman and x-ray studies of spin-ice pyrochlore Dy2Ti2O7Dy_2Ti_2O_7 and non-magnetic pyrochlore Lu2Ti2O7Lu_2Ti_2O_7

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    We present here temperature-dependent Raman, x-ray diffraction and specific heat studies between room temperature and 12 K on single crystals of spin-ice pyrochlore compound Dy2Ti2O7Dy_2Ti_2O_7 and its non-magnetic analogue Lu2Ti2O7Lu_2Ti_2O_7. Raman data show a "new" band not predicted by factor group analysis of Raman-active modes for the pyrochlore structure in Dy2Ti2O7Dy_2Ti_2O_7, appearing below a temperature of Tc=T_c=110 K with a concomitant contraction of the cubic unit cell volume as determined from the powder x-ray diffraction analysis. Low temperature Raman experiments on O18^{18}-isotope substituted Dy2Ti2O7Dy_2Ti_2O_7 confirm the phonon origin of the "new" mode. These findings, absent in Lu2Ti2O7Lu_2Ti_2O_7, suggest that the room temperature cubic lattice of the pyrochlore Dy2Ti2O7Dy_2Ti_2O_7 undergoes a "subtle" structural transformation near TcT_c. We find anomalous \textit{red-shift} of some of the phonon modes in both the Dy2Ti2O7Dy_2Ti_2O_7 and the Lu2Ti2O7Lu_2Ti_2O_7 as the temperature decreases, which is attributed to strong phonon-phonon anharmonic interactions.Comment: 28 pages, 9 figures (Accepted for publication in Physical Review B

    Use of cetylpyridinium chloride for the storage of sputum samples and isolation of M. tuberculosis

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    Of 220 sputum specimens collected from pulmonary tuberculosis patients, 85 were culture positive when the sputum aliquots were stored with cetypyridinium chloride (CPC) and processed on 7th day (CPC method), whereas only 70 were culture positive when the aliquots of the same specimens were stored without CPC and processed by sodium hydroxide (NaOH) method. The difference in the culture positivity was statistically significant. The number of positive, cultures obtained by the CPC method (85) was comparable to that obtained by the NaOH method before storage (95) and the difference was not statistically significant

    Structural, magnetic, electrical and supraconducting properties of the high temperature superconductor Nd(SrBa)Cu3O6+z Effect of argon annealing

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    We have studied the structural and superconducting properties of two samples superconductors Nd(SrBa)Cu3O6+z. One was a conventionally annealed sample at 450°C in oxygen (0) and the other was heated in argon at 850°C followed by oxygen annealing (A0). The Tc of the sample (O) was 68 K and that of (AO) sample was 78 K. This was confirmed by our AC susceptibility, resistivity and Seebeck effect measurements. Further, there was an enhancement in the shielding and the intergranular critical current. The X-ray and neutron data showed a tetragonal structure, and that the (O) sample had a higher impurity level arising from Nd entering the Sr/Ba sites that may result in a decrease in the carrier density (p) which also was confirmed by our thermopower measurements. A combination of several factors such as changes in the Cu (1) apical oxygen distance, chain oxygen ordering, increase in p and in-phase purity for the (AO) sample may qualitatively account for the observed data.We have studied the structural and superconducting properties of two samples superconductors Nd(SrBa)Cu3O6+z. One was a conventionally annealed sample at 450°C in oxygen (0) and the other was heated in argon at 850°C followed by oxygen annealing (A0). The Tc of the sample (O) was 68 K and that of (AO) sample was 78 K. This was confirmed by our AC susceptibility, resistivity and Seebeck effect measurements. Further, there was an enhancement in the shielding and the intergranular critical current. The X-ray and neutron data showed a tetragonal structure, and that the (O) sample had a higher impurity level arising from Nd entering the Sr/Ba sites that may result in a decrease in the carrier density (p) which also was confirmed by our thermopower measurements. A combination of several factors such as changes in the Cu (1) apical oxygen distance, chain oxygen ordering, increase in p and in-phase purity for the (AO) sample may qualitatively account for the observed data

    Magneto-optical investigation of the field-induced spin-glass insulator to ferromagnetic metallic transition of the bilayer manganite (La0.4_{0.4}Pr0.6_{0.6})1.2_{1.2}Sr1.8_{1.8}Mn2_2O7_7

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    We measured the magneto-optical response of (La0.4_{0.4}Pr0.6_{0.6})1.2_{1.2}Sr1.8_{1.8}Mn2_2O7_7 in order to investigate the microscopic aspects of the magnetic field driven spin-glass insulator to ferromagnetic metal transition. Application of a magnetic field recovers the ferromagnetic state with an overall redshift of the electronic structure, growth of the bound carrier localization associated with ferromagnetic domains, development of a pseudogap, and softening of the Mn-O stretching and bending modes that indicate a structural change. We discuss field- and temperature-induced trends within the framework of the Tomioka-Tokura global electronic phase diagram picture and suggest that controlled disorder near a phase boundary can be used to tune the magnetodielectric response. Remnants of the spin-glass insulator to ferromagnetic metallic transition can also drive 300 K color changes in (La0.4_{0.4}Pr0.6_{0.6})1.2_{1.2}Sr1.8_{1.8}Mn2_2O7_7.Comment: 9 pages, 8 figure
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