Boltzmann Machines : High-Order Interactions and Synchronous Learning

1992 ◽  
pp. 14-45 ◽  
Author(s):  
Robert Azencott
Keyword(s):  
High Order ◽  
Boltzmann Machines ◽  
Synchronous Learning

Boltzmann Machines Reduction by High-Order Decimation

2008 ◽  
Vol 19 (10) ◽  
pp. 1816-1821 ◽  
Author(s):  
E. Farguell ◽  
F. Mazzanti ◽  
E. Gomez-Ramirez
Keyword(s):  
High Order ◽  
Boltzmann Machines

Convergence Properties of High-order Boltzmann Machines

1996 ◽  
Vol 9 (9) ◽  
pp. 1561-1567 ◽  
Author(s):  
F.Xabier Albizuri ◽  
Alicia d'Anjou ◽  
Manuel Graña ◽  
J.Antonio Lozano
Keyword(s):  
High Order ◽  
Convergence Properties ◽  
Boltzmann Machines

scholarly journals High-Order Boltzmann Machines for MAX-SAT and SAT

ICANN ’93 ◽  
1993 ◽  
pp. 479-479
Author(s):  
M. C. Hernández ◽  
F. X. Albizuri ◽  
A. d’Anjou ◽  
M. Graña ◽  
F. J. Torrealdea
Keyword(s):  
High Order ◽  
Boltzmann Machines ◽  
Max Sat

Conditional High-Order Boltzmann Machines for Supervised Relation Learning

2017 ◽  
Vol 26 (9) ◽  
pp. 4297-4310 ◽  
Author(s):  
Yan Huang ◽  
Wei Wang ◽  
Liang Wang ◽  
Tieniu Tan
Keyword(s):  
High Order ◽  
Boltzmann Machines ◽  
Relation Learning

Determination of the Burgers vector of a dislocation in a Fe-Mn alloy by weak-beam image in HVEM

1978 ◽  
Vol 36 (1) ◽  
pp. 330-331
Author(s):  
Y. Ishida ◽  
H. Ishida ◽  
K. Kohra ◽  
H. Ichinose
Keyword(s):  
High Order ◽  
Simulation Technique ◽  
The Other ◽  
Image Simulation ◽  
Diffraction Vector ◽  
Burgers Vector ◽  
Weak Beam ◽  
Beam Image ◽  
Edge Component

IntroductionA simple and accurate technique to determine the Burgers vector of a dislocation has become feasible with the advent of HVEM. The conventional image vanishing technique(1) using Bragg conditions with the diffraction vector perpendicular to the Burgers vector suffers from various drawbacks; The dislocation image appears even when the g.b = 0 criterion is satisfied, if the edge component of the dislocation is large. On the other hand, the image disappears for certain high order diffractions even when g.b ≠ 0. Furthermore, the determination of the magnitude of the Burgers vector is not easy with the criterion. Recent image simulation technique is free from the ambiguities but require too many parameters for the computation. The weak-beam “fringe counting” technique investigated in the present study is immune from the problems. Even the magnitude of the Burgers vector is determined from the number of the terminating thickness fringes at the exit of the dislocation in wedge shaped foil surfaces.

The usefulness of high index low symmetry zone axes for holz line analysis

1987 ◽  
Vol 45 ◽  
pp. 384-385
Author(s):  
C. M. Sung ◽  
D. B. Williams
Keyword(s):  
Lattice Parameter ◽  
High Order ◽  
Zone Axis ◽  
High Index ◽  
High Symmetry ◽  
Second Phases ◽  
Line Patterns ◽  
Low Symmetry ◽  
Line Analysis

Researchers have tended to use high symmetry zone axes (e.g. <111> <114>) for High Order Laue Zone (HOLZ) line analysis since Jones et al reported the origin of HOLZ lines and described some of their applications. But it is not always easy to find HOLZ lines from a specific high symmetry zone axis during microscope operation, especially from second phases on a scale of tens of nanometers. Therefore it would be very convenient if we can use HOLZ lines from low symmetry zone axes and simulate these patterns in order to measure lattice parameter changes through HOLZ line shifts. HOLZ patterns of high index low symmetry zone axes are shown in Fig. 1, which were obtained from pure Al at -186°C using a double tilt cooling holder. Their corresponding simulated HOLZ line patterns are shown along with ten other low symmetry orientations in Fig. 2. The simulations were based upon kinematical diffraction conditions.

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