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        <identifier>oai:drops-oai.dagstuhl.de:18619</identifier>
        <datestamp>2024-03-06T11:02:17Z</datestamp>
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          <dc:title>Exponential Lower Bounds for Threshold Circuits of Sub-Linear Depth and Energy</dc:title>
          <dc:creator>Uchizawa, Kei</dc:creator>
          <dc:creator>Abe, Haruki</dc:creator>
          <dc:subject>Circuit complexity</dc:subject>
          <dc:subject>disjointness function</dc:subject>
          <dc:subject>equality function</dc:subject>
          <dc:subject>neural networks</dc:subject>
          <dc:subject>threshold circuits</dc:subject>
          <dc:subject>ReLU cicuits</dc:subject>
          <dc:subject>sigmoid circuits</dc:subject>
          <dc:subject>sparse activity</dc:subject>
          <dc:description>In this paper, we investigate computational power of threshold circuits and other theoretical models of neural networks in terms of the following four complexity measures: size (the number of gates), depth, weight and energy. Here, the energy of a circuit measures sparsity of their computation, and is defined as the maximum number of gates outputting non-zero values taken over all the input assignments.&#13;
As our main result, we prove that any threshold circuit C of size s, depth d, energy e and weight w satisfies log(rk(M_C)) ≤ ed (log s + log w + log n), where rk(M_C) is the rank of the communication matrix M_C of a 2n-variable Boolean function that C computes. Thus, such a threshold circuit C is able to compute only a Boolean function of which communication matrix has rank bounded by a product of logarithmic factors of s, w and linear factors of d, e. This implies an exponential lower bound on the size of even sublinear-depth and sublinear-energy threshold circuit. For example, we can obtain an exponential lower bound s = 2^Ω(n^{1/3}) for threshold circuits of depth n^{1/3}, energy n^{1/3} and weight 2^o(n^{1/3}). We also show that the inequality is tight up to a constant factor when the depth d and energy e satisfies ed = o(n/log n).&#13;
For other models of neural networks such as a discretized ReLU circuits and descretized sigmoid circuits, we define energy as the maximum number of gates outputting non-zero values. We then prove that a similar inequality also holds for a discretized circuit C: rk(M_C) = O(ed(log s + log w + log n)³). Thus, if we consider the number gates outputting non-zero values as a measure for sparse activity of a neural network, our results suggest that larger depth linearly helps neural networks to acquire sparse activity.</dc:description>
          <dc:publisher>Schloss Dagstuhl – Leibniz-Zentrum für Informatik</dc:publisher>
          <dc:contributor>Kei Uchizawa and Haruki Abe</dc:contributor>
          <dc:date>2023</dc:date>
          <dc:relation>Is Part Of LIPIcs, Volume 272, 48th International Symposium on Mathematical Foundations of Computer Science (MFCS 2023)</dc:relation>
          <dc:type>InProceedings</dc:type>
          <dc:type>Text</dc:type>
          <dc:type>doc-type:ResearchArticle</dc:type>
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          <dc:identifier>doi:10.4230/LIPIcs.MFCS.2023.85</dc:identifier>
          <dc:identifier>urn:nbn:de:0030-drops-186192</dc:identifier>
          <dc:identifier>https://drops.dagstuhl.de/entities/document/10.4230/LIPIcs.MFCS.2023.85</dc:identifier>
          <dc:language>eng</dc:language>
          <dc:rights>https://creativecommons.org/licenses/by/4.0/legalcode</dc:rights>
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