Periodicity-dependence of the ferroelectric properties in BiFeO3/SrTiO3 multiferroic superlattices

Artificial superlattices of (BiFeO3)m(SrTiO3)m (m= 1 to 10 unit cells) consisting of multiferroic BiFeO3 and insulating SrTiO3 layers were fabricated on (100)-oriented SrTiO3 substrates by pulsed laser ablation. The remnant polarization and leakage current behavior were studied varying the periodicity (8-80A) of the superlattice. The leakage current was reduced by few orders of magnitude on increase of periodicity compared to single layer BiFeO3 thin films. Reduced leakage and intrinsic polarization hysteresis was observed and was confirmed by PUND analysis for periodicities in the range 20-60A. The leakage current was observed to be dominated by space charge limited conductionComment: Submitted to Applied Physics Letter

Revolutionary War and an Amsterdam Privy: The Remarkable Background of a Rhode Island Ship Token

In 2008 the City of Amsterdam Office for Monuments & Archaeology (BMA) excavated a remarkable find from a late 18th-century privy in Amsterdam’s city centre that can be directly linked to the American Revolutionary War, a 1779 Rhode Island Ship Token. Approximately twenty-five examples of this token are known worldwide, but none of them come from an archaeological context. From this Amsterdam find one can examine these tokens from an entirely new aspect, namely the socio-economic context of the owner as well as the period in which the token was used. The Rhode Island Ship Token was a British propaganda piece ridiculing the weakness of the Americans in 1778 and distributed in the Netherlands to create negative views of the American revolutionaries to discourage the Dutch from intervening in the Anglo-American conflict. Whether the artifact from the privy expressed its owner’s political preferences or was simply a curiosity will remain unknown. What we do know is that with the outbreak of the Fourth Anglo-Dutch War in 1780, the tokens had become worthless and that this particular piece ended in a cesspit after a final use as a clothing ornament, a counter for card games, or possibly even as a child’s toy

Interfacial contribution to the dielectric response in semiconducting LaBiMn4/3Co2/3O6

Impedance measurements have been performed on a sintered polycrystalline sample of the perovskite LaBiMn4/3Co2/3O6. Colossal dielectric permittivity often is measured in this class of semiconducting materials as a result of extrinsic factors. Our results show that a large offset in the capacitance, measured on a series of samples with different thickness, is due to the interfacial polarization. This contribution then can be removed from the data, creating a general procedure for dielectric measurements in semiconducting samples.Comment: 13 pages, 4 figure

Design and Implementation of a Secure Communication Protocol

The main object of this paper is to present a mutual authentication protocol that guarantees security, integrity and authenticity of messages, transferred over a network system. In this paper a symmetric key cryptosystem, that satisfies all the above requirements, is developed using theorems of J.R. Chen, I.M. Vinogradov and Fermat and the decimal expansion of an irrational number

Frustration of square cupola in Sr(TiO)Cu4_{4}(PO4_{4})4_{4}

The structural and magnetic properties of the square-cupola antiferromagnet Sr(TiO)Cu$_{4}$(PO$_{4}$)$_{4}$ are investigated via x-ray diffraction, magnetization, heat capacity, and $^{31}$P nuclear magnetic resonance experiments on polycrystalline samples, as well as density-functional band-structure calculations. The temperature-dependent unit cell volume could be described well using the Debye approximation with the Debye temperature of $\theta_{\rm D} \simeq$ 550~K. Magnetic response reveals a pronounced two-dimensionality with a magnetic long-range-order below $T_{\rm N} \simeq 6.2$~K. High-field magnetization exhibits a kink at $1/3$ of the saturation magnetization. Asymmetric $^{31}$P NMR spectra clearly suggest strong in-plane anisotropy in the magnetic susceptibility, as anticipated from the crystal structure. From the $^{31}$P NMR shift vs bulk susceptibility plot, the isotropic and axial parts of the hyperfine coupling between $^{31}$P nuclei and the Cu$^{2+}$ spins are calculated to be $A_{\rm hf}^{\rm iso} \simeq 6539$ and $A_{\rm hf}^{\rm ax} \simeq 952$~Oe/$\mu_{\rm B}$, respectively. The low-temperature and low-field $^{31}$P NMR spectra indicate a commensurate antiferromagnetic ordering. Frustrated nature of the compound is inferred from the temperature-dependent $^{31}$P NMR spin-lattice relaxation rate and confirmed by our microscopic analysis that reveals strong frustration of the square cupola by next-nearest-neighbor exchange couplings.Comment: 11 pages, 13 figures, 1 table, Phys. Rev. B (Accepted, 2018

Collinear order in a frustrated three-dimensional spin-12\frac12 antiferromagnet Li2_2CuW2_2O8_8

Magnetic frustration in three dimensions (3D) manifests itself in the spin-$\frac12$ insulator Li$_2$CuW$_2$O$_8$. Density-functional band-structure calculations reveal a peculiar spin lattice built of triangular planes with frustrated interplane couplings. The saturation field of 29 T contrasts with the susceptibility maximum at 8.5 K and a relatively low N\'eel temperature $T_N\simeq 3.9$ K. Magnetic order below $T_N$ is collinear with the propagation vector $(0,\frac12,0)$ and an ordered moment of 0.65(4) $\mu_B$ according to neutron diffraction data. This reduced ordered moment together with the low maximum of the magnetic specific heat ($C^{\max}/R\simeq 0.35$) pinpoint strong magnetic frustration in 3D. Collinear magnetic order suggests that quantum fluctuations play crucial role in this system, where a non-collinear spiral state would be stabilized classically.Comment: published version with supplemental material merged into the tex

Design and Stress Analysis for Spur Gears Using Solid Works Simulation

Spur gear is the most important component which is used to transfer the power and it also transmits the motion among the machine parts between two parallel axis. The reason for causing failures in Spur gear are compressive stress, friction, bending stress, wear and tear etc. In this study the compressive stress and bending stress of a spur gear are calculated mathematically with the help of PSG DDB, and the spur gear model is simulated by using solid works software. The PSG DDB values and formulae’s are used in the mathematical calculations and then compared with solid works analysis. The final out comes are checked by comparing those results and we choose a better material for our assumed data. (PSG DDB –PSG Design Data Book