1,816 research outputs found

    Cu-NMR study on the disordered quantum spin magnet with the Bose-glass ground state

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    Cu-NMR study has been performed on the disordered spin-gap system Tl1-xKxCuCl3 In the high-field H > HC=\Delta/\mu_B, where \Delta is the spin-gap, the hyperfine field becomes extremely inhomogeneous at low temperatures due to the field-induced magnetic order, indicating that the ordered spin state must be different from the pure TlCuCl3. In the low field H < HC, a saturating behavior in the longitudinal nuclear spin relaxation rate 1/T1 was observed at low temperatures, indicating existence of the magnetic ground state proposed to be Bose-glass phase by Fisher.Comment: RHMF200

    Rapid zygosity determination in mice by SYBR Green real-time genomic PCR of a crude DNA solution

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    The original publication is available at www.springerlink.com.ArticleTRANSGENIC RESEARCH. 17(1): 149-155 (2008)journal articl

    A computerized Langmuir probe system

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    For low pressure plasmas it is important to record entire single or double Langmuir probe characteristics accurately. For plasmas with a depleted high energy tail, the accuracy of the recorded ion current plays a critical role in determining the electron temperature. Even for high density Maxwellian distributions, it is necessary to accurately model the ion current to obtain the correct electron density. Since the electron and ion current saturation values are, at best, orders of magnitude apart, a single current sensing resistor cannot provide the required resolution to accurately record these values. We present an automated, personal computer based data acquisition system for the determination of fundamental plasma properties in low pressure plasmas. The system is designed for single and double Langmuir probes, whose characteristics can be recorded over a bias voltage range of ±70 V with 12 bit resolution. The current flowing through the probes can be recorded within the range of 5 nA–100 mA. The use of a transimpedance amplifier for current sensing eliminates the requirement for traditional current sensing resistors and hence the need to correct the raw data. The large current recording range is realized through the use of a real time gain switching system in the negative feedback loop of the transimpedance amplifier

    1^1H-NMR Study of the Random Bond Effect in the Quantum Spin System (CH3_3)2_2CHNH3_3Cu(Clx_xBr1x_{1-x})3_3

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    Spin-lattice relaxation rate T11T_1^{-1} of 1^1H-NMR has been measured in (CH3_3)2_2CHNH3_3Cu(Clx_xBr1x_{1-x})3_3 with x=0.88x=0.88, which has been reported to be gapped system with singlet ground state from the previous macroscopic magnetization and specific heat measurements, in order to investigate the bond randomness effect microscopically in the gapped composite Haldane system (CH3_3)2_2CHNH3_3CuCl3_3. It was found that the spin-lattice relaxation rate T11T_1^{-1} in the present system includes both fast and slow relaxation parts indicative of the gapless magnetic ground state and the gapped singlet ground state, respectively. We discuss the obtained results with the previous macroscopic magnetization and specific heat measurements together with the microscopic μ\muSR experiments.Comment: 4 pages, 2 figures, to be published in J. Phys. Soc. Jpn. vol.76 (2007) No.

    Precision spectroscopy of pionic 1s states of Sn nuclei and evidence for partial restoration of chiral symmetry in the nuclear medium

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    Deeply bound 1s states of π\pi^- in 115,119,123^{115,119,123}Sn were preferentially observed using the Sn(dd,3^3He) pion-transfer reaction under the recoil-free condition. The 1s binding energies and widths were precisely determined, and were used to deduce the isovector parameter of the s-wave pion-nucleus potential to be b1=0.115±0.007 mπ1b_1 =-0.115\pm 0.007 ~m_{\pi}^{-1}. The observed enhancement of b1|b_1| over the free πN\pi N value (b1free/b1=0.78±0.05b_1^{\rm free}/b_1 = 0.78 \pm 0.05) indicates a reduction of the chiral order parameter, fπ(ρ)2/fπ20.64f^{*}_{\pi} (\rho)^2/f_{\pi}^2 \approx 0.64, at the normal nuclear density, ρ=ρ0\rho = \rho_0.Comment: 4 pages including 3 postscript figures, RevTeX 4 with multirow.sty, submitted to Physical Review Letter
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