Using physical energy as the loss function lets a deep neural network solve a range of computational mechanics PDEs, from linear elasticity to fourth-order plate bending, without meshes or data.
Topological properties of the set of functions generated by neural networks of fixed size
1 Pith paper cite this work. Polarity classification is still indexing.
abstract
We analyze the topological properties of the set of functions that can be implemented by neural networks of a fixed size. Surprisingly, this set has many undesirable properties. It is highly non-convex, except possibly for a few exotic activation functions. Moreover, the set is not closed with respect to $L^p$-norms, $0 < p < \infty$, for all practically-used activation functions, and also not closed with respect to the $L^\infty$-norm for all practically-used activation functions except for the ReLU and the parametric ReLU. Finally, the function that maps a family of weights to the function computed by the associated network is not inverse stable for every practically used activation function. In other words, if $f_1, f_2$ are two functions realized by neural networks and if $f_1, f_2$ are close in the sense that $\|f_1 - f_2\|_{L^\infty} \leq \varepsilon$ for $\varepsilon > 0$, it is, regardless of the size of $\varepsilon$, usually not possible to find weights $w_1, w_2$ close together such that each $f_i$ is realized by a neural network with weights $w_i$. Overall, our findings identify potential causes for issues in the training procedure of deep learning such as no guaranteed convergence, explosion of parameters, and slow convergence.
citation-role summary
citation-polarity summary
fields
stat.ML 1years
2019 1verdicts
CONDITIONAL 1roles
background 1polarities
unclear 1representative citing papers
citing papers explorer
-
An Energy Approach to the Solution of Partial Differential Equations in Computational Mechanics via Machine Learning: Concepts, Implementation and Applications
Using physical energy as the loss function lets a deep neural network solve a range of computational mechanics PDEs, from linear elasticity to fourth-order plate bending, without meshes or data.