scholarly journals Lattice Sieving in Three Dimensions for Discrete Log in Medium Characteristic

2020 ◽  
Vol 15 (1) ◽  
pp. 223-236
Author(s):  
Gary McGuire ◽  
Oisín Robinson

AbstractLattice sieving in two dimensions has proven to be an indispensable practical aid in integer factorization and discrete log computations involving the number field sieve. The main contribution of this article is to show that a different method of lattice sieving in three dimensions will provide a significant speedup in medium characteristic. Our method is to use the successive minima and shortest vectors of the lattice instead of transition vectors to iterate through lattice points. We showcase the new method by a record computation in a 133-bit subgroup of ${{\mathbb{F}}_{{{p}^{6}}}}$, with p6 having 423 bits. Our overall timing is nearly 3 times faster than the previous record of a 132-bit subgroup in a 422-bit field. The approach generalizes to dimensions 4 or more, overcoming one key obstruction to the implementation of the tower number field sieve.

1981 ◽  
Vol 21 (03) ◽  
pp. 345-353 ◽  
Author(s):  
James W. Watts III

Abstract This paper describes a way of solving the reservoirsimulation pressure equation using preconditionedconjugate gradients. The preconditioning is based onan approximate inverse using a diagonal ordering ofthe difference equations. The new method has been tested and comparedwith the strongly implicit procedure (SIP) on anumber of problems in both two and threedimensions. In two dimensions, it is generally faster thanSIP; in three dimensions, it is much slower than SIPwhen SIP works well but can be many times faster than SIP when SIP works poorly. Use of the new method generally does not requirethe selection of an iteration parameter, which is asignificant advantage over SIP. Furthermore, it ismuch more reliable than SIP. In other words, it is farless likely to be unable to solve a given problem thanSIP is. Introduction An IMPES reservoir simulator calculates pressuresonce each time step. These pressures are calculatedby solving a matrix of simultaneous equations;thereis one equation for each cell in the system. Usuallythe solution of this set of equations is not difficult, consuming perhaps 30% of the total computing timefor the time step. However, in a difficult problem, the computation time required for this solution mayincrease dramatically, making the reservoirsimulation calculations very expensive. Whether or not the pressure equations can besolved by direct methods depends on the bandwidth.In two dimensions, the bandwidth is proportional tothe smallest dimension; in three dimensions, it isproportional to the product of the smallest twodimensions. When the bandwidth is small, directmethods are quite economical. Unfortunately, most large problems have largebandwidths, so iterative methods are used to solvethem. The most popular of the iterative techniques isprobably SIP. SIP works well in many problems, particularly those which have relativelyhomogeneous reservoir properties, but it works verypoorly in others. Furthermore, its performancedepends on a sequence of iteration parameters, theselection of which is easy in some problems but cantake a lot of time and effort in others. Recently, there has been significant progress madein the application of the preconditioned conjugategradient method. This method is quite fast, and itsuse does not require the selection of iterationparameters. However, a barrier exists to itsapplication to reservoir simulation problems. The conjugate gradient method applies directly only tosymmetric matrices, and the reservoir simulationmatrix of pressure equations is nonsymmetric. In thenew method, this is overcome by solving a symmetricapproximation to the matrix of pressure equations.The pressures so obtained, though only approximate, are usually within the accuracy achieved by iterativemethods. If not, they can be refined by solving thesymmetric matrix again, as necessary. This disposesof the symmetry problem, permitting the use of theconjugate gradient method. SPEJ P. 345^


Data ◽  
2020 ◽  
Vol 5 (1) ◽  
pp. 27
Author(s):  
Domingo Villavicencio-Aguilar ◽  
Edgardo René Chacón-Andrade ◽  
Maria Fernanda Durón-Ramos

Happiness-oriented people are vital in every society; this is a construct formed by three different types of happiness: pleasure, meaning, and engagement, and it is considered as an indicator of mental health. This study aims to provide data on the levels of orientation to happiness in higher-education teachers and students. The present paper contains data about the perception of this positive aspect in two Latin American countries, Mexico and El Salvador. Structure instruments to measure the orientation to happiness were administrated to 397 teachers and 260 students. This data descriptor presents descriptive statistics (mean, standard deviation), internal consistency (Cronbach’s alpha), and differences (Student’s t-test) presented by country, population (teacher/student), and gender of their orientation to happiness and its three dimensions: meaning, pleasure, and engagement. Stepwise-multiple-regression-analysis results are also presented. Results indicated that participants from both countries reported medium–high levels of meaning and engagement happiness; teachers reported higher levels than those of students in these two dimensions. Happiness resulting from pleasure activities was the least reported in general. Males and females presented very similar levels of orientation to happiness. Only the population (teacher/student) showed a predictive relationship with orientation to happiness; however, the model explained a small portion of variance in this variable, which indicated that other factors are more critical when promoting orientation to happiness in higher-education institutions.


2021 ◽  
Vol 2021 (1) ◽  
Author(s):  
Nima Afkhami-Jeddi ◽  
Henry Cohn ◽  
Thomas Hartman ◽  
Amirhossein Tajdini

Abstract We study the torus partition functions of free bosonic CFTs in two dimensions. Integrating over Narain moduli defines an ensemble-averaged free CFT. We calculate the averaged partition function and show that it can be reinterpreted as a sum over topologies in three dimensions. This result leads us to conjecture that an averaged free CFT in two dimensions is holographically dual to an exotic theory of three-dimensional gravity with U(1)c×U(1)c symmetry and a composite boundary graviton. Additionally, for small central charge c, we obtain general constraints on the spectral gap of free CFTs using the spinning modular bootstrap, construct examples of Narain compactifications with a large gap, and find an analytic bootstrap functional corresponding to a single self-dual boson.


2012 ◽  
Vol 696 ◽  
pp. 228-262 ◽  
Author(s):  
A. Kourmatzis ◽  
J. S. Shrimpton

AbstractThe fundamental mechanisms responsible for the creation of electrohydrodynamically driven roll structures in free electroconvection between two plates are analysed with reference to traditional Rayleigh–Bénard convection (RBC). Previously available knowledge limited to two dimensions is extended to three-dimensions, and a wide range of electric Reynolds numbers is analysed, extending into a fully inherently three-dimensional turbulent regime. Results reveal that structures appearing in three-dimensional electrohydrodynamics (EHD) are similar to those observed for RBC, and while two-dimensional EHD results bear some similarities with the three-dimensional results there are distinct differences. Analysis of two-point correlations and integral length scales show that full three-dimensional electroconvection is more chaotic than in two dimensions and this is also noted by qualitatively observing the roll structures that arise for both low (${\mathit{Re}}_{E} = 1$) and high electric Reynolds numbers (up to ${\mathit{Re}}_{E} = 120$). Furthermore, calculations of mean profiles and second-order moments along with energy budgets and spectra have examined the validity of neglecting the fluctuating electric field ${ E}_{i}^{\ensuremath{\prime} } $ in the Reynolds-averaged EHD equations and provide insight into the generation and transport mechanisms of turbulent EHD. Spectral and spatial data clearly indicate how fluctuating energy is transferred from electrical to hydrodynamic forms, on moving through the domain away from the charging electrode. It is shown that ${ E}_{i}^{\ensuremath{\prime} } $ is not negligible close to the walls and terms acting as sources and sinks in the turbulent kinetic energy, turbulent scalar flux and turbulent scalar variance equations are examined. Profiles of hydrodynamic terms in the budgets resemble those in the literature for RBC; however there are terms specific to EHD that are significant, indicating that the transfer of energy in EHD is also attributed to further electrodynamic terms and a strong coupling exists between the charge flux and variance, due to the ionic drift term.


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