80 research outputs found

    Restricted Max-Min Allocation: Approximation and Integrality Gap

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    Asadpour, Feige, and Saberi proved that the integrality gap of the configuration LP for the restricted max-min allocation problem is at most 4. However, their proof does not give a polynomial-time approximation algorithm. A lot of efforts have been devoted to designing an efficient algorithm whose approximation ratio can match this upper bound for the integrality gap. In ICALP 2018, we present a (6 + delta)-approximation algorithm where delta can be any positive constant, and there is still a gap of roughly 2. In this paper, we narrow the gap significantly by proposing a (4+delta)-approximation algorithm where delta can be any positive constant. The approximation ratio is with respect to the optimal value of the configuration LP, and the running time is poly(m,n)* n^{poly(1/(delta))} where n is the number of players and m is the number of resources. We also improve the upper bound for the integrality gap of the configuration LP to 3 + 21/26 =~ 3.808

    Restricted Max-Min Fair Allocation

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    The restricted max-min fair allocation problem seeks an allocation of resources to players that maximizes the minimum total value obtained by any player. It is NP-hard to approximate the problem to a ratio less than 2. Comparing the current best algorithm for estimating the optimal value with the current best for constructing an allocation, there is quite a gap between the ratios that can be achieved in polynomial time: 4+delta for estimation and 6 + 2 sqrt{10} + delta ~~ 12.325 + delta for construction, where delta is an arbitrarily small constant greater than 0. We propose an algorithm that constructs an allocation with value within a factor 6 + delta from the optimum for any constant delta > 0. The running time is polynomial in the input size for any constant delta chosen

    Initial data gluing in the asymptotically flat regime via solution operators with prescribed support properties

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    We give new proofs of general relativistic initial data gluing results on unit-scale annuli based on explicit solution operators for the linearized constraint equation around the flat case with prescribed support properties. These results retrieve and optimize - in terms of positivity, regularity, size and/or spatial decay requirements - a number of known theorems concerning asymptotically flat initial data, including Kerr exterior gluing by Corvino-Schoen and Chru\'sciel-Delay, interior gluing (or "fill-in") by Bieri-Chru\'sciel, and obstruction-free gluing by Czimek-Rodnianski. In particular, our proof of the strengthened obstruction-free gluing theorem relies on purely spacelike techniques, rather than null gluing as in the original approach.Comment: 30 pages, 1 figure. Comments are welcome

    Separating the memory of reionization from cosmology in the Lyα\alpha forest power spectrum at the post-reionization era

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    It has been recently shown that the astrophysics of reionization can be extracted from the Lyα\alpha forest power spectrum by marginalizing the memory of reionization over cosmological information. This impact of cosmic reionization on the Lyα\alpha forest power spectrum can survive cosmological time scales because cosmic reionization, which is inhomogeneous, and subsequent shocks from denser regions can heat the gas in low-density regions to 3×104\sim 3\times10^4 K and compress it to mean-density. Current approach of marginalization over the memory of reionization, however, is not only model-dependent, based on the assumption of a specific reionization model, but also computationally expensive. Here we propose a simple analytical template for the impact of cosmic reionization, thereby treating it as a broadband systematic to be marginalized over for Bayesian inference of cosmological information from the Lyα\alpha forest in a model-independent manner. This template performs remarkably well with an error of 6%\leq 6 \% at large scales k0.19k \approx 0.19 Mpc1^{-1} where the effect of the memory of reionization is important, and reproduces the broadband effect of the memory of reionization in the Lyα\alpha forest correlation function, as well as the expected bias of cosmological parameters due to this systematic. The template can successfully recover the morphology of forecast errors in cosmological parameter space as expected when assuming a specific reionization model for marginalization purposes, with a slight overestimation of tens of per cent for the forecast errors on the cosmological parameters. We further propose a similar template for this systematic on the Lyα\alpha forest 1D power spectrum.Comment: Comments welcome, 13 pages, 10 figure

    Faster Algorithms for Bounded Knapsack and Bounded Subset Sum Via Fine-Grained Proximity Results

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    We investigate pseudopolynomial-time algorithms for Bounded Knapsack and Bounded Subset Sum. Recent years have seen a growing interest in settling their fine-grained complexity with respect to various parameters. For Bounded Knapsack, the number of items nn and the maximum item weight wmaxw_{\max} are two of the most natural parameters that have been studied extensively in the literature. The previous best running time in terms of nn and wmaxw_{\max} is O(n+wmax3)O(n + w^3_{\max}) [Polak, Rohwedder, Wegrzycki '21]. There is a conditional lower bound of O((n+wmax)2o(1))O((n + w_{\max})^{2-o(1)}) based on (min,+)(\min,+)-convolution hypothesis [Cygan, Mucha, Wegrzycki, Wlodarczyk '17]. We narrow the gap significantly by proposing a O~(n+wmax12/5)\tilde{O}(n + w^{12/5}_{\max})-time algorithm. Note that in the regime where wmaxnw_{\max} \approx n, our algorithm runs in O~(n12/5)\tilde{O}(n^{12/5}) time, while all the previous algorithms require Ω(n3)\Omega(n^3) time in the worst case. For Bounded Subset Sum, we give two algorithms running in O~(nwmax)\tilde{O}(nw_{\max}) and O~(n+wmax3/2)\tilde{O}(n + w^{3/2}_{\max}) time, respectively. These results match the currently best running time for 0-1 Subset Sum. Prior to our work, the best running times (in terms of nn and wmaxw_{\max}) for Bounded Subset Sum is O~(n+wmax5/3)\tilde{O}(n + w^{5/3}_{\max}) [Polak, Rohwedder, Wegrzycki '21] and O~(n+μmax1/2wmax3/2)\tilde{O}(n + \mu_{\max}^{1/2}w_{\max}^{3/2}) [implied by Bringmann '19 and Bringmann, Wellnitz '21], where μmax\mu_{\max} refers to the maximum multiplicity of item weights

    A Nearly Quadratic-Time FPTAS for Knapsack

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    We investigate polynomial-time approximation schemes for the classic 0-1 knapsack problem. The previous algorithm by Deng, Jin, and Mao (SODA'23) has approximation factor 1 + \eps with running time \widetilde{O}(n + \frac{1}{\eps^{2.2}}). There is a lower Bound of (n + \frac{1}{\eps})^{2-o(1)} conditioned on the hypothesis that (min,+)(\min, +) has no truly subquadratic algorithm. We close the gap by proposing an approximation scheme that runs in \widetilde{O}(n + \frac{1}{\eps^2}) time

    THE HYDRAULICS OF NATURE-LIKE FISHWAYS

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    Nature-like fishway arrangements are commonly used because these structures imitate the characteristics of natural rivers and effectively allow fish to migrate past river sections blocked by hydraulic structures. In this paper, physical models were analyzed, and the velocity distributions of two different fishway structures (Types I and II) were compared. Results showed that the maximum mainstream velocity of the Type I structure was 5.3% lower than that of the Type II structure. However, the average mainstream velocity of the Type I structure was 21.1% greater than that of the Type II structure. The total per-cycle length of the mainstream path in the Type II structure was 2.1 times greater than that of the Type I structure, which indicated that the length of the mainstream path was somewhat proportional to the average velocity of the mainstream. When the flow rate was kept constant, increases in the velocity of the main flow associated with changes in the internal structure of the fishway decreased the average velocity of the main flow, while decreases in the total length of the flow path led to increases in the average velocity of the main flow. Due to frictional head loss along the fishway and local head loss, as well as the overlaps between these factors, the overall flow rate gradually decreased every cycle, despite periodic fluctuations
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