13 research outputs found

    Acceleration for Compressed Gradient Descent in Distributed and Federated Optimization

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    Due to the high communication cost in distributed and federated learning problems, methods relying on compression of communicated messages are becoming increasingly popular. While in other contexts the best performing gradient-type methods invariably rely on some form of acceleration/momentum to reduce the number of iterations, there are no methods which combine the benefits of both gradient compression and acceleration. In this paper, we remedy this situation and propose the first accelerated compressed gradient descent (ACGD) methods. In the single machine regime, we prove that ACGD enjoys the rate O((1+ω)Lμlog1ϵ)O\Big((1+\omega)\sqrt{\frac{L}{\mu}}\log \frac{1}{\epsilon}\Big) for μ\mu-strongly convex problems and O((1+ω)Lϵ)O\Big((1+\omega)\sqrt{\frac{L}{\epsilon}}\Big) for convex problems, respectively, where ω\omega is the compression parameter. Our results improve upon the existing non-accelerated rates O((1+ω)Lμlog1ϵ)O\Big((1+\omega)\frac{L}{\mu}\log \frac{1}{\epsilon}\Big) and O((1+ω)Lϵ)O\Big((1+\omega)\frac{L}{\epsilon}\Big), respectively, and recover the optimal rates of accelerated gradient descent as a special case when no compression (ω=0\omega=0) is applied. We further propose a distributed variant of ACGD (called ADIANA) and prove the convergence rate O~(ω+Lμ+(ωn+ωn)ωLμ)\widetilde{O}\Big(\omega+\sqrt{\frac{L}{\mu}}+\sqrt{\big(\frac{\omega}{n}+\sqrt{\frac{\omega}{n}}\big)\frac{\omega L}{\mu}}\Big), where nn is the number of devices/workers and O~\widetilde{O} hides the logarithmic factor log1ϵ\log \frac{1}{\epsilon}. This improves upon the previous best result O~(ω+Lμ+ωLnμ)\widetilde{O}\Big(\omega + \frac{L}{\mu}+\frac{\omega L}{n\mu} \Big) achieved by the DIANA method of Mishchenko et al. (2019). Finally, we conduct several experiments on real-world datasets which corroborate our theoretical results and confirm the practical superiority of our accelerated methods.Comment: ICML 202
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