19 research outputs found

    Wire width and density dependence of the crossover in the peak of the static structure factor from 2kF2k_\text{F} \rightarrow 4kF4k_\text{F} in one-dimensional paramagnetic electron gases

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    We use the variational quantum Monte Carlo (VMC) method to study the wire width (bb) and electron density (rsr_\text{s}) dependences of the ground-state properties of quasi-one-dimensional paramagnetic electron fluids. The onset of a quasi-Wigner crystal phase is known to depend on electron density, and the crossover occurs in the low density regime. We study the effect of wire width on the crossover of the dominant peak in the static structure factor from k=2kFk=2k_\text{F} to k=4kFk=4k_\text{F}. It is found that for a fixed electron density, in the charge structure factor the crossover from the dominant peak occurring at 2kF2k_\text{F} to 4kF4k_\text{F} occurs as the wire width decreases. Our study suggests that the crossover is due to interplay of both rsr_\text{s} and b<rsb<r_\text{s}. The finite wire width correlation effect is reflected in the peak height of the charge and spin structure factors. We fit the dominant peaks of the charge and spin structure factors assuming fit functions based on our finite wire width theory and clues from bosonization, resulting in a good fit of the VMC data. The pronounced peaks in the charge and spin structure factors at 4kF4 k_\text{F} and 2kF2 k_\text{F}, respectively, indicate the complete decoupling of the charge and spin degrees of freedom. Furthermore, the wire width dependence of the electron correlation energy and the Tomonaga-Luttinger parameter KρK_{\rho} is found to be significant

    Ground-state properties of electron-electron biwire systems

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    The correlation between electrons in different quantum wires is expected to affect the electronic properties of quantum electron-electron biwire systems. Here, we use the variational Monte Carlo method to study the ground-state properties of parallel, infinitely thin electron-electron biwires for several electron densities ( r s ) and interwire separations ( d ). Specifically, the ground-state energy, the correlation energy, the interaction energy, the pair-correlation function (PCF), the static structure factor (SSF), and the momentum distribution (MD) function are calculated. We find that the interaction energy increases as ln ( d ) for d → 0 and it decreases as d − 2 when d → ∞ . The PCF shows oscillatory behavior at all densities considered here. As two parallel wires approach each other, interwire correlations increase while intrawire correlations decrease as evidenced by the behavior of the PCF, SSF, and MD. The system evolves from two monowires of density parameter r s to a single monowire of density parameter r s / 2 as d is reduced from infinity to zero. The MD reveals Tomonaga-Luttinger (TL) liquid behavior with a power-law nature near k F even in the presence of an extra interwire interaction between the electrons in biwire systems. It is observed that when d is reduced the MD decreases for k k F , similar to its behavior with increasing r s . The TL liquid exponent is extracted by fitting the MD data near k F , from which the TL liquid interaction parameter K ρ is calculated. The value of the TL parameter is found to be in agreement with that of a single wire for large separation between the two wires

    Year-wise snakebites and death summary.

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    <p>From the study population, the information about the year of snakebite was obtained from the household members. The information obtained is presented accordingly for each type of study village.</p

    Circumstances of snakebites and their socio-economic impacts.

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    <p>The circumstances of snakebite such as where and when the bite occurred, the activities of victims during bite and the place of bite on the body were obtained from the victims. In addition, the direct costs involved in the treatment of snakebites and their socio-economic impacts were also assessed. The information provided here was from 129 interviewed victims and percentages were calculated accordingly.</p

    Characteristics of the sample population.

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    <p>Types I, II and III villages have <100, 100–250 and >250 houses respectively. The percentages in each case were calculated relative to the total population in each type of village. For the snakebite prevalence the percentages indicate the % of the male, female and total population in each village type who suffered snakebites and who died due to snakebite. This data was obtained from the 30 sampling villages.</p
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