8,465 research outputs found

    Tame kernels for biquadratic number fields

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    Transceiver Optimization for Two-Hop AF MIMO Relay Systems With DFE Receiver and Direct Link

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    In this paper, we consider precoding and receiving matrices optimization for a two-hop amplify-and-forward (AF) multiple-input multiple-output (MIMO) relay system with a decision feedback equalizer (DFE) at the destination node in the presence of the direct source-destination link. By adopting the minimum mean-squared error (MMSE) criterion, we develop two new transceiver design algorithms for such a system. The first one employs an iterative procedure to design the source, relay, feed-forward, and feedback matrices. The second algorithm is a non-iterative suboptimal approach which decomposes the optimization problem into two tractable subproblems and obtains the source and relay precoding matrices by solving the two subproblems sequentially. Simulation results validate the better MSE and bit-error-rate (BER) performance of the proposed algorithms and show that the non-iterative suboptimal method has a negligible performance loss when the ratio of the source node transmission power to the relay node transmission power is small. In addition, the computational complexity analysis suggests that the second algorithm and one iteration of the first algorithm have the same order of complexity. As the first algorithm typically converges within a few iterations, both proposed algorithms exhibit a low complexity order

    The linear complexity of whiteman's generalized cyclotomic sequences of period p {m+1}q n+1

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    In this paper, we mainly get three results. First, let p, q be distinct primes with \gcd ((p-1)p,(q-1)q)=\gcd (p-1,q-1)=e ; we give a method to compute the linear complexity of Whiteman's generalized cyclotomic sequences of period p^{m+1}q n+1. Second, if e=4, we compute the exact linear complexity of Whiteman's generalized cyclotomic sequences. Third, if p \equiv q \equiv 5∼({\rm mod}∼8), \gcd (p-1, q-1)=4, and we fix a common primitive root g of both p and q, then 2\in H-{0}=(g), which is a subgroup of the multiplicative group Z-{pq} \ast, if and only if Whiteman's generalized cyclotomic numbers of order 4 depend on the decomposition pq=a^{2}+4b 2 with 4\vert b. © 1963-2012 IEEE.published_or_final_versio

    Modelling Time-varying Dark Energy with Constraints from Latest Observations

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    We introduce a set of two-parameter models for the dark energy equation of state (EOS) w(z)w(z) to investigate time-varying dark energy. The models are classified into two types according to their boundary behaviors at the redshift z=(0,)z=(0,\infty) and their local extremum properties. A joint analysis based on four observations (SNe + BAO + CMB + H0H_0) is carried out to constrain all the models. It is shown that all models get almost the same χmin2469\chi^2_{min}\simeq 469 and the cosmological parameters (ΩM,h,Ωbh2)(\Omega_M, h, \Omega_bh^2) with the best-fit results (0.28,0.70,2.24)(0.28, 0.70, 2.24), although the constraint results on two parameters (w0,w1)(w_0, w_1) and the allowed regions for the EOS w(z)w(z) are sensitive to different models and a given extra model parameter. For three of Type I models which have similar functional behaviors with the so-called CPL model, the constrained two parameters w0w_0 and w1w_1 have negative correlation and are compatible with the ones in CPL model, and the allowed regions of w(z)w(z) get a narrow node at z0.2z\sim 0.2. The best-fit results from the most stringent constraints in Model Ia give (w0,w1)=(0.960.21+0.26,0.120.89+0.61)(w_0,w_1) = (-0.96^{+0.26}_{-0.21}, -0.12^{+0.61}_{-0.89}) which may compare with the best-fit results (w0,w1)=(0.970.18+0.22,0.151.33+0.85)(w_0,w_1) = (-0.97^{+0.22}_{-0.18}, -0.15^{+0.85}_{-1.33}) in the CPL model. For four of Type II models which have logarithmic function forms and an extremum point, the allowed regions of w(z)w(z) are found to be sensitive to different models and a given extra parameter. It is interesting to obtain two models in which two parameters w0w_0 and w1w_1 are strongly correlative and appropriately reduced to one parameter by a linear relation w1(1+w0)w_1 \propto (1+w_0).Comment: 30 pages, 7 figure

    Research Program towards Observation of Neutrino-Nucleus Coherent Scattering

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    The article describes the research program pursued by the TEXONO Collaboration towards an experiment to observe coherent scattering between neutrinos and the nucleus at the power reactor. The motivations of studying this process are surveyed. In particular, a threshold of 100-200 eV has been achieved with an ultra-low-energy germanium detector prototype. This detection capability at low energy can also be adapted to conduct searches of Cold Dark Matter in the low-mass region as well as to enhance the sensitivities in the study of neutrino magnetic moments.Comment: 5 pages, 8 figures ; Proceedings of TAUP-2005 Workshop, Spain, 2005. Updated on 2006/9/15 for Proceedings of Neutrino-2006 Conference, Santa Fe, 200

    Recent progress on weight distributions of cyclic codes over finite fields

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    Cyclic codes are an interesting type of linear codes and have wide applications in communication and storage systems due to their efficient encoding and decoding algorithms. In coding theory it is often desirable to know the weight distribution of a cyclic code to estimate the error correcting capability and error probability. In this paper, we present the recent progress on the weight distributions of cyclic codes over finite fields, which had been determined by exponential sums. The cyclic codes with few weights which are very useful are discussed and their existence conditions are listed. Furthermore, we discuss the more general case of constacyclic codes and give some equivalences to characterize their weight distributions

    Topological quantum phase transition in an extended Kitaev spin model

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    We study the quantum phase transition between Abelian and non-Abelian phases in an extended Kitaev spin model on the honeycomb lattice, where the periodic boundary condition is applied by placing the lattice on a torus. Our analytical results show that this spin model exhibits a continuous quantum phase transition. Also, we reveal the relationship between bipartite entanglement and the ground-state energy. Our approach directly shows that both the entanglement and the ground-state energy can be used to characterize the topological quantum phase transition in the extended Kitaev spin model.Comment: 9 Pages, 4 figure
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