scholarly journals A Uniform Lower Error Bound for Half-Space Learning

Author(s):  
Andreas Maurer ◽  
Massimiliano Pontil
Automatica ◽  
2014 ◽  
Vol 50 (8) ◽  
pp. 2196-2198 ◽  
Author(s):  
Ha Binh Minh ◽  
Carles Batlle ◽  
Enric Fossas

1998 ◽  
Vol 34 (16) ◽  
pp. 1555 ◽  
Author(s):  
S. Weiß ◽  
A. Stenger ◽  
R. Rabenstein ◽  
R.W. Stewart

2004 ◽  
Vol 14 (09) ◽  
pp. 1297-1341 ◽  
Author(s):  
E. CREUSÉ ◽  
S. NICAISE ◽  
G. KUNERT

The paper presents a posteriori error estimators for the stationary Stokes problem. We consider anisotropic finite element discretizations (i.e. elements with very large aspect ratio) where conventional, isotropic error estimators fail. Our analysis covers two- and three-dimensional domains, conforming and non-conforming discretizations as well as different elements. This large variety of settings requires different approaches and results in different estimators. Furthermore many examples of finite element pairs that are covered by the analysis are presented. Lower and upper error bounds form the main result with minimal assumptions on the elements. The lower error bound is uniform with respect to the mesh anisotropy with the exception of nonconforming 3D discretizations made of pentahedra or hexahedra. The upper error bound depends on a proper alignment of the anisotropy of the mesh which is a common feature of anisotropic error estimation. In the special case of isotropic meshes, the results simplify, and upper and lower error bounds hold unconditionally. Some of the corresponding results seem to be novel (in particular for 3D domains), and cover element pairs of practical importance. The numerical experiments confirm the theoretical predictions and show the usefulness of the anisotropic error estimators.


2015 ◽  
Vol 37 (4) ◽  
pp. 303-315 ◽  
Author(s):  
Pham Chi Vinh ◽  
Nguyen Thi Khanh Linh ◽  
Vu Thi Ngoc Anh

This paper presents  a technique by which the transfer matrix in explicit form of an orthotropic layer can be easily obtained. This transfer matrix is applicable for both the wave propagation problem and the reflection/transmission problem. The obtained transfer matrix is then employed to derive the explicit secular equation of Rayleigh waves propagating in an orthotropic half-space coated by an orthotropic layer of arbitrary thickness.


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