16,901 research outputs found

    Criteria for accurate determination of the magnon relaxation length from the nonlocal spin Seebeck effect

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    The nonlocal transport of thermally generated magnons not only unveils the underlying mechanism of the spin Seebeck effect, but also allows for the extraction of the magnon relaxation length (λm\lambda_m) in a magnetic material, the average distance over which thermal magnons can propagate. In this study, we experimentally explore in yttrium iron garnet (YIG)/platinum systems much further ranges compared with previous investigations. We observe that the nonlocal SSE signals at long distances (dd) clearly deviate from a typical exponential decay. Instead, they can be dominated by the nonlocal generation of magnon accumulation as a result of the temperature gradient present away from the heater, and decay geometrically as 1/d21/d^2. We emphasize the importance of looking only into the exponential regime (i.e., the intermediate distance regime) to extract λm\lambda_m. With this principle, we study λm\lambda_m as a function of temperature in two YIG films which are 2.7 and 50 μ\mum in thickness, respectively. We find λm\lambda_m to be around 15 μ\mum at room temperature and it increases to 40 μ\mum at T=T= 3.5 K. Finite element modeling results agree with experimental studies qualitatively, showing also a geometrical decay beyond the exponential regime. Based on both experimental and modeling results we put forward a general guideline for extracting λm\lambda_m from the nonlocal spin Seebeck effect.Comment: 9 pages, 7 figure

    Magnon Planar Hall Effect and Anisotropic Magnetoresistance in a Magnetic Insulator

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    Electrical resistivities can be different for charge currents travelling parallel or perpendicular to the magnetization in magnetically ordered conductors or semiconductors, resulting in the well-known planar Hall effect and anisotropic magnetoresistance. Here, we study the analogous anisotropic magnetotransport behavior for magnons in a magnetic insulator Y3_{3}Fe5_{5}O12_{12}. Electrical and thermal magnon injection, and electrical detection methods are used at room temperature with transverse and longitudinal geometries to measure the magnon planar Hall effect and anisotropic magnetoresistance, respectively. We observe that the relative difference between magnon current conductivities parallel and perpendicular to the magnetization, with respect to the average magnon conductivity, i.e. (σmσm)/σ0m|(\sigma_{\parallel}^{\textrm{m}}-\sigma_{\perp}^{\textrm{m}})/\sigma_{0}^{\textrm{m}}| , is approximately 5% with the majority of the measured devices showing σm>σm\sigma_{\perp}^{\textrm{m}}>\sigma_{\parallel}^{\textrm{m}}.Comment: 18 pages, 16 figure

    Trans-arterial embolisation therapies for unresectable intrahepatic cholangiocarcinoma: A systematic review

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    Background: Unresectable intrahepatic cholangiocarcinoma (ICC) portends a poor prognosis despite standard systemic treatments which confer minimal survival benefits and significant adverse effects. This study aimed to assess clinical outcomes, complications and prognostic factors of TAE therapies using chemotherapeutic agents or radiation. Methods: A literature search and article acquisition was conducted on PubMed (MEDLINE), OVID (MEDLINE) and EBSCOhost (EMBASE). Original articles published after January 2000 on trans-arterial therapies for unresectable ICC were selected using strict eligibility criteria. Radiological response, overall survival, progression-free survival, safety profile, and prognostic factors for overall survival were assessed. Quality appraisal and data tabulation were performed using pre-determined forms. Results were synthesized by narrative review and quantitative analysis. Results: Twenty articles were included (n=929 patients). Thirty three percent of patients presented with extrahepatic metastases. After treatment, the average rate of complete and partial radiological response was 10% and 22.2%, respectively. Overall median survival time was 12.4 months with a median 30-day mortality and 1-year survival rate of 0.6% and 53%, respectively. Acute treatment toxicity (within 30 days) was reported in 34.9% of patients, of which 64.3% were mild to moderate in severity. The most common clinical toxicities were abdominal pain, nausea and vomiting, and fatigue. Multiplicity, localization and vascularity of the tumor may predict worse overall survival. Conclusions: Trans-arterial therapies are safe and effective treatment options which should be considered routinely for unresectable ICC. Consistent and standardized methodology and data collection is required to facilitate a meta-analysis. Randomized controlled trials will be valuable in the future

    Effects of Residue Background Events in Direct Dark Matter Detection Experiments on the Determination of the WIMP Mass

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    In the earlier work on the development of a model-independent data analysis method for determining the mass of Weakly Interacting Massive Particles (WIMPs) by using measured recoil energies from direct Dark Matter detection experiments directly, it was assumed that the analyzed data sets are background-free, i.e., all events are WIMP signals. In this article, as a more realistic study, we take into account a fraction of possible residue background events, which pass all discrimination criteria and then mix with other real WIMP-induced events in our data sets. Our simulations show that, for the determination of the WIMP mass, the maximal acceptable fraction of residue background events in the analyzed data sets of O(50) total events is ~20%, for background windows of the entire experimental possible energy ranges, or in low energy ranges; while, for background windows in relatively higher energy ranges, this maximal acceptable fraction of residue background events can not be larger than ~10%. For a WIMP mass of 100 GeV with 20% background events in the windows of the entire experimental possible energy ranges, the reconstructed WIMP mass and the 1-sigma statistical uncertainty are ~97 GeV^{+61%}_{-35%} (~94 GeV^{+55%}_{-33%} for background-free data sets).Comment: 27 pages, 22 eps figures; v2: revised version for publication, references added and update

    Entanglement and quantum phase transition in alternating XY spin chain with next-nearest neighbour interactions

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    By using the method of density-matrix renormalization-group to solve the different spin-spin correlation functions, the nearest-neighbouring entanglement(NNE) and next-nearest-neighbouring entanglement(NNNE) of one-dimensional alternating Heisenberg XY spin chain is investigated in the presence of alternating nearest neighbour interactions of exchange couplings, external magnetic fields and next-nearest neighbouring interactions. For dimerized ferromagnetic spin chain, NNNE appears only above the critical dimerized interaction, meanwhile, the dimerized interaction effects quantum phase transition point and improves NNNE to a large value. We also study the effect of ferromagnetic or antiferromagnetic next-nearest neighboring (NNN) interactions on the dynamics of NNE and NNNE. The ferromagnetic NNN interaction increases and shrinks NNE below and above critical frustrated interaction respectively, while the antiferromagnetic NNN interaction always decreases NNE. The antiferromagnetic NNN interaction results to a larger value of NNNE in comparison to the case when the NNN interaction is ferromagnetic.Comment: 13 pages, 4 figures,. accepted by Chinese Physics B 2008 11 (in press

    Weak coupling d-wave BCS superconductivity and unpaired electrons in overdoped La_{2-x}Sr_{x}CuO_{4} single crystals

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    The low-temperature specific heat (SH) of overdoped La_{2-x}Sr_{x}CuO_{4} single crystals (0.178=<x=<0.290) has been measured. For the superconducting samples (0.178=<x=<0.238), the derived gap values (without any adjusting parameters) approach closely onto the theoretical prediction \Delta_{0}=2.14k_{B}T_{c} for the weak-coupling d-wave BCS superconductivity. In addition, the residual term \gamma(0) of SH at H=0 increases with x dramatically when beyond x~0.22, and finally evolves into the value of a complete normal metallic state at higher doping levels, indicating growing amount of unpaired electrons. We argue that this large \gamma(0) cannot be simply attributed to the pair breaking induced by the impurity scattering, instead the phase separation is possible.Comment: 6 pages, 6 figures; Contents added; Accepted for publication in Phys. Rev.

    Unconventional Spin Density Waves in Dipolar Fermi Gases

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    The conventional spin density wave (SDW) phase (Overhauser, 1962), as found in antiferromagnetic metal for example (Fawcett 1988), can be described as a condensate of particle-hole pairs with zero angular momentum, =0\ell=0, analogous to a condensate of particle-particle pairs in conventional superconductors. While many unconventional superconductors with Cooper pairs of finite \ell have been discovered, their counterparts, density waves with non-zero angular momenta, have only been hypothesized in two-dimensional electron systems (Nayak, 2000). Using an unbiased functional renormalization group analysis, we here show that spin-triplet particle-hole condensates with =1\ell=1 emerge generically in dipolar Fermi gases of atoms (Lu, Burdick, and Lev, 2012) or molecules (Ospelkaus et al., 2008; Wu et al.) on optical lattice. The order parameter of these exotic SDWs is a vector quantity in spin space, and, moreover, is defined on lattice bonds rather than on lattice sites. We determine the rich quantum phase diagram of dipolar fermions at half-filling as a function of the dipolar orientation, and discuss how these SDWs arise amidst competition with superfluid and charge density wave phases.Comment: 5 pages, 3 figure

    Determining the Mass of Dark Matter Particles with Direct Detection Experiments

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    In this article I review two data analysis methods for determining the mass (and eventually the spin-independent cross section on nucleons) of Weakly Interacting Massive Particles with positive signals from direct Dark Matter detection experiments: a maximum likelihood analysis with only one experiment and a model-independent method requiring at least two experiments. Uncertainties and caveats of these methods will also be discussed.Comment: 24 pages, 10 figures, 1 reference added, typos fixed, published version, to appear in the NJP Focus Issue on "Dark Matter and Particle Physics
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