319 research outputs found

    Challenges and Responsibilities in Successful Management of Municipal Solid Wastes in India

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    Management of Municipal Solid wastes (MSW) is a genuine problem to all Municipal Corporations irrespective to their size, population or financial condition in India. Scientific technologies are available for pollution free hygienic disposal of all biodegradable solid wastes by converting them to good quality compost and also for systematic recycling of non-biodegradable wastes for their beneficial utilization. Machineries are also available for converting Municipal solid wastes to energy for partial fulfillment of highly demanded electricity. But still all Municipal Corporation in India mainly depend on old open dumping of solid wastes in some low lying dump-yards creating known environmental pollution hazards. The Municipal authority, the district administration and the common citizens have to play a constructive role for overcoming this problem. Important challenges faced by Municipal authorities all over India are non-preparedness to handle huge quantity of MSW generated daily, lacking of awareness by common people on benefits of segregation of MSW at source, non-availability of infrastructure as well as expert / skilled manpower for scientific disposal of MSW, accurate forecasting about city wise MSW generation and proper encouragement to Public – private partnership (PPP) model for efficient management of MSW. Everyone is essential part of this management system. Citizens have to take the responsibility for segregating solid wastes at home before handing over to Municipal workers and for refraining themselves from throwing out any solid wastes. Municipal corporations have to consider MSW as important resource material, use it for beneficial purposes through vermicomposting and recycling, and to stop dumping of MSW at outskirt by unnecessary spending money on its transportation. It is mainly found that installation of costly machinery for mechanical composting and electricity generation have sometimes become not 2 much fruitful to Municipal authorities due to lack of their expertise as well as maintenance and repairing problem of machineries. Scientific disposal with the help of NGOs and Entrepreneurs are found more effective, employment generative and cheaper than adopting costly mechanical system. Paradigm shift in thought process of every citizen can change the situation of management of municipal solid waste successfully

    Magnetic frustration and spontaneous rotational symmetry breaking in PdCrO2

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    In the triangular layered magnet PdCrO2 the intralayer magnetic interactions are strong, however the lattice structure frustrates interlayer interactions. In spite of this, long-range, 120∘^\circ antiferromagnetic order condenses at TN=38T_N = 38~K. We show here through neutron scattering measurements under in-plane uniaxial stress and in-plane magnetic field that this occurs through a spontaneous lifting of the three-fold rotational symmetry of the nonmagnetic lattice, which relieves the interlayer frustration. We also show through resistivity measurements that uniaxial stress can suppress thermal magnetic disorder within the antiferromagnetic phase.Comment: 9 pages, 9 figure

    Role of crystal field ground state in the classical spin-liquid behavior of a quasi-one dimensional spin-chain system Sr3NiPtO6

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    The spin-chain compound Sr3NiPtO6 is known to have a nonmagnetic ground state. We have investigated the nature of ground state of Sr3NiPtO6 using magnetic susceptibility χ(T)\chi(T), heat capacity Cp(T)C_{\rm p}(T), muon spin relaxation (μ\muSR) and inelastic neutron scattering (INS) measurements. The χ(T)\chi(T) and Cp(T)C_{\rm p}(T) do not exhibit any pronounced anomaly that can be associated with a phase transition to a magnetically ordered state. Our μ\muSR data confirm the absence of long-range magnetic ordering down to 0.04 K. Furthermore, the muon spin relaxation rate increases below 20 K and exhibits temperature independent behavior at low temperature, very similar to that observed in a quantum spin-liquid system. The INS data show a large excitation near 8~meV, and the analysis of the INS data reveals a singlet CEF ground state with a first excited CEF doublet state at ΔCEF\Delta_{\rm CEF} = 7.7 meV. The estimated CEF parameters reveal a strong planar anisotropy in the calculated χ(T)\chi(T), consistent with the reported behavior of the χ(T)\chi(T) of single crystal Sr3NiPtO6. We propose that the nonmagnetic singlet ground state and a large ΔCEF\Delta_{\rm CEF} (much larger than the exchange interaction Jex\mathcal{J}_{\rm ex}) are responsible for the absence of long-range magnetic ordering and can mimic a classical spin-liquid behavior in this quasi-1D spin chain system Sr3NiPtO6. The classical spin-liquid ground state observed in Sr3NiPtO6 is due to the single-ion property, which is different from the quantum spin-liquid ground state observed in geometrically frustrated systems, where two-ion exchanges play an important role.Comment: 11 pages, 10 figures, 1 tabl

    A crossover from Kondo semiconductor to metallic antiferromagnet with 5d5d-electron doping in CeFe2_2Al10_{10}

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    We report a systematic study of the 5d5d-electron-doped system Ce(Fe1−x_{1-x}Irx_x)2_2Al10_{10} (0≤x≤0.150 \leq x \leq 0.15). With increasing xx, the orthorhombic bb~axis decreases slightly while accompanying changes in aa and cc leave the unit cell volume almost unchanged. Inelastic neutron scattering, along with thermal and transport measurements, reveal that for the Kondo semiconductor CeFe2_2Al10_{10}, the low-temperature energy gap which is proposed to be a consequence of strong c \mhyphen f hybridization, is suppressed by a small amount of Ir substitution for Fe, and that the system adopts a metallic ground state with an increase in the density of states at the Fermi level. The charge or transport gap collapses (at x=x=~0.04) faster than the spin gap with Ir substitution. Magnetic susceptibility, heat capacity, and muon spin relaxation measurements demonstrate that the system undergoes long-range antiferromagnetic order below a N\'eel temperature, TNT_{\mathrm{N}}, of 3.1(2)~K for x=0.15x = 0.15. The ordered moment is estimated to be smaller than 0.07(1)~μB\mu_\mathrm{B}/Ce although the trivalent state of Ce is confirmed by Ce L3_3-edge x-ray absorption near edge spectroscopy. It is suggested that the c \mhyphen f hybridization gap, which plays an important role in the unusually high ordering temperatures observed in CeT2T_2Al10_{10} (TT = Ru and Os), may not be necessary for the onset of magnetic order with a low TNT_{\mathrm{N}} seen here in Ce(Fe1−x_{1-x}Irx_x)2_2Al10_{10}.Comment: 12 pages, 11 figure

    Ab initio prediction of Boron compounds arising from Borozene: Structural and electronic properties

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    Structure and electronic properties of two unusual boron clusters obtained by fusion of borozene rings has been studied by means of first principles calculations, based on the generalized-gradient approximation of the density functional theory, and the semiempirical tight-binding method was used for the transport calculations. The role of disorder has also been considered with single vacancies and substitutional atoms. Results show that the pure boron clusters are topologically planar and characterized by (3c-2e) bonds, which can explain, together with the aromaticity (estimated by means of NICS), the remarkable cohesive energy values obtained. Such feature makes these systems competitive with the most stable boron clusters to date. On the contrary, the introduction of impurities compromises stability and planarity in both cases. The energy gap values indicate that these clusters possess a semiconducting character, while when the larger system is considered, zero-values of the density of states are found exclusively within the HOMO-LUMO gap. Electron transport calculations within the Landauer formalism confirm these indications, showing semiconductor-like low bias differential conductance for these stuctures. Differences and similarities with Carbon clusters are highlighted in the discussion.Comment: 10 pages, 2 tables, 5 figure
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