58,468 research outputs found

    On the least common multiple of qq-binomial coefficients

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    In this paper, we prove the following identity \lcm({n\brack 0}_q,{n\brack 1}_q,...,{n\brack n}_q) =\frac{\lcm([1]_q,[2]_q,...,[n+1]_q)}{[n+1]_q}, where [nk]q{n\brack k}_q denotes the qq-binomial coefficient and [n]q=1qn1q[n]_q=\frac{1-q^n}{1-q}. This result is a qq-analogue of an identity of Farhi [Amer. Math. Monthly, November (2009)].Comment: 5 page

    Hemodynamic evaluation using four-dimensional flow magnetic resonance imaging for a patient with multichanneled aortic dissection

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    The hemodynamic function of multichanneled aortic dissection (MCAD) requires close monitoring and effective management to avoid potentially catastrophic sequelae. This report describes a 47-year-old man who underwent endovascular repair based on findings from four-dimensional (4D) flow magnetic resonance imaging of an MCAD. The acquired 4D flow data revealed complex, bidirectional flow patterns in the false lumens and accelerated blood flow in the compressed true lumen. The collapsed abdominal true lumen expanded unsatisfactorily after primary tear repair, which required further remodeling with bare stents. This case study demonstrates that hemodynamic analysis using 4D flow magnetic resonance imaging can help understand the complex pathologic changes of MCAD

    Optimal transfer of an unknown state via a bipartite operation

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    A fundamental task in quantum information science is to transfer an unknown state from particle AA to particle BB (often in remote space locations) by using a bipartite quantum operation EAB\mathcal{E}^{AB}. We suggest the power of EAB\mathcal{E}^{AB} for quantum state transfer (QST) to be the maximal average probability of QST over the initial states of particle BB and the identifications of the state vectors between AA and BB. We find the QST power of a bipartite quantum operations satisfies four desired properties between two dd-dimensional Hilbert spaces. When AA and BB are qubits, the analytical expressions of the QST power is given. In particular, we obtain the exact results of the QST power for a general two-qubit unitary transformation.Comment: 6 pages, 1 figur

    Anomalous quantum glass of bosons in a random potential in two dimensions

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    We present a quantum Monte Carlo study of the "quantum glass" phase of the 2D Bose-Hubbard model with random potentials at filling ρ=1\rho=1. In the narrow region between the Mott and superfluid phases the compressibility has the form κexp(b/Tα)+c\kappa \sim {\rm exp}(-b/T^\alpha)+c with α<1\alpha <1 and cc vanishing or very small. Thus, at T=0T=0 the system is either incompressible (a Mott glass) or nearly incompressible (a Mott-glass-like anomalous Bose glass). At stronger disorder, where a glass reappears from the superfluid, we find a conventional highly compressible Bose glass. On a path connecting these states, away from the superfluid at larger Hubbard repulsion, a change of the disorder strength by only 10%10\% changes the low-temperature compressibility by more than four orders of magnitude, lending support to two types of glass states separated by a phase transition or a sharp cross-over.Comment: Published version including supplementary material, 11 pages total, 15 figure

    Factors of sums and alternating sums involving binomial coefficients and powers of integers

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    We study divisibility properties of certain sums and alternating sums involving binomial coefficients and powers of integers. For example, we prove that for all positive integers n1,...,nmn_1,..., n_m, nm+1=n1n_{m+1}=n_1, and any nonnegative integer rr, there holds {align*} \sum_{k=0}^{n_1}\epsilon^k (2k+1)^{2r+1}\prod_{i=1}^{m} {n_i+n_{i+1}+1\choose n_i-k} \equiv 0 \mod (n_1+n_m+1){n_1+n_m\choose n_1}, {align*} and conjecture that for any nonnegative integer rr and positive integer ss such that r+sr+s is odd, k=0nϵk(2k+1)r((2nnk)(2nnk1))s0mod(2nn), \sum_{k=0}^{n}\epsilon ^k (2k+1)^{r}({2n\choose n-k}-{2n\choose n-k-1})^{s} \equiv 0 \mod{{2n\choose n}}, where ϵ=±1\epsilon=\pm 1.Comment: 14 pages, to appear in Int. J. Number Theor

    Metastable helium molecules as tracers in superfluid liquid 4^{4}He

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    Metastable helium molecules generated in a discharge near a sharp tungsten tip operated in either pulsed mode or continuous field-emission mode in superfluid liquid 4^{4}He are imaged using a laser-induced-fluorescence technique. By pulsing the tip, a small cloud of He2_{2}^{*} molecules is produced. At 2.0 K, the molecules in the liquid follow the motion of the normal fluid. We can determine the normal-fluid velocity in a heat-induced counterflow by tracing the position of a single molecule cloud. As we run the tip in continuous field-emission mode, a normal-fluid jet from the tip is generated and molecules are entrained in the jet. A focused 910 nm pump laser pulse is used to drive a small group of molecules to the vibrational a(1)a(1) state. Subsequent imaging of the tagged a(1)a(1) molecules with an expanded 925 nm probe laser pulse allows us to measure the velocity of the normal fluid. The techniques we developed demonstrate for the first time the ability to trace the normal-fluid component in superfluid helium using angstrom-sized particles.Comment: 4 pages, 7 figures. Submitted to Phys. Rev. Let
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