arXiv:0706.3639v1 [cs.AI] 25 Jun 2007

arXiv:0706.3639v1 [cs.AI] 25 Jun 2007 Technical Report IDSIA-07-07 A Collection of Definitions of Intelligence Shane Legg IDSIA, Galleria …

  Intelligence, Collection

Deep Residual Learning for Image Recognition - …

Deep Residual Learning for Image Recognition Kaiming He Xiangyu Zhang Shaoqing Ren Jian Sun Microsoft Research fkahe, v-xiangz, v-shren, jiansung@microsoft.com

  Image, Learning, Residual, Recognition, Residual learning for image recognition

arXiv:1301.3781v3 [cs.CL] 7 Sep 2013

For all the following models, the training complexity is proportional to O = E T Q; (1) where E is number of the training epochs, T is the number of …

@google.com arXiv:1609.03499v2 [cs.SD] 19 Sep 2016

where 1 <x t <1 and = 255. This non-linear quantization produces a significantly better reconstruction than a simple linear quantization scheme. …

A Tutorial on UAVs for Wireless Networks: …

A Tutorial on UAVs for Wireless Networks: Applications, Challenges, and Open Problems Mohammad Mozaffari 1, ... to UAVs in wireless communications is the work in …

  Network, Communication, Wireless, Wireless communications, Wireless networks

Adversarial Generative Nets: Neural Network …

Adversarial Generative Nets: Neural Network Attacks on State-of-the-Art Face Recognition Mahmood Sharif, Sruti Bhagavatula, Lujo Bauer Carnegie Mellon University

  Network, Attacks, Nets, Adversarial generative nets, Adversarial, Generative, Neural network, Neural, Neural network attacks

Massive Exploration of Neural Machine Translation ...

Massive Exploration of Neural Machine Translation Architectures Denny Britzy, Anna Goldie, Minh-Thang Luong, Quoc Le fdennybritz,agoldie,thangluong,qvlg@google.com Google Brain

  Architecture, Machine, Exploration, Translation, Neural, Exploration of neural machine translation, Exploration of neural machine translation architectures

Mastering Chess and Shogi by Self-Play with a …

Mastering Chess and Shogi by Self-Play with a General Reinforcement Learning Algorithm David Silver, 1Thomas Hubert, Julian Schrittwieser, Ioannis Antonoglou, 1Matthew Lai, Arthur Guez, Marc Lanctot,1

Going deeper with convolutions - arXiv

Going deeper with convolutions Christian Szegedy Google Inc. Wei Liu University of North Carolina, Chapel Hill Yangqing Jia Google Inc. Pierre Sermanet

  With, Going, Going deeper with convolutions, Deeper, Convolutions

Andrew G. Howard Menglong Zhu Bo Chen Dmitry ...

MobileNets: Efficient Convolutional Neural Networks for Mobile Vision Applications Andrew G. Howard Menglong Zhu Bo Chen Dmitry Kalenichenko Weijun Wang Tobias Weyand Marco Andreetto Hartwig Adam

  Applications

Generative Adversarial Nets - NIPS

specification of a probability distribution function. The model can then be trained by maximiz-ing the log likelihood. In this family of model, perhaps the most succesful is the deep Boltzmann machine [25]. Such models generally have intractable likelihood functions and therefore require numerous approximations to the likelihood gradient.

  Distribution, Boltzmann

Maximum Entropy Inverse Reinforcement Learning

sition distribution, T. Paths in these MDPs (Figure 1d) are now determined by the action choices of the agent and the random outcomes of the MDP. Our distribution over paths must take this randomness into account. We use the maximum entropy distribution of paths con-ditioned on the transition distribution, T, and constrained to

  Distribution, Learning, Maximum, Reinforcement, Inverse, Entropy, Maximum entropy inverse reinforcement learning

Boltzmann Transport - Physics Courses

The equilibrium Fermi distribution, f0(k) = ˆ exp "(k) k B T + 1 ˙ 1 (1.20) is a space-independent and time-independent solution to the Boltzmann equation. Since collisions act locally in space, they act on short time scales to establish a local equilibrium described by a distribution function f0(r;k;t) = ˆ exp "(k) (r;t) k B T(r;t) + 1 ˙ 1 ...

  Distribution, Boltzmann

Phys 446 Solid State Physics Lecture 7 (Ch. 4.1 – 4.3, 4.6.)

called Maxwell – Boltzmann distribution f (E) =e(µ−E) kBT. Effect of temperature on Fermi-Dirac distribution Free electron gas in three dimensions The Schrödinger equation in the three dimensions: If the electrons are confined to a cube of edge L, the solution is

  Distribution, Boltzmann, Boltzmann distribution

Part 5: The Bose-Einstein Distribution

Boltzmann distribution, or the chemical potential in the Fermi-Dirac distribution. Bis determined by the constraint: X i ni= N, (25) where N is the total number of particles. Let us find how B depends on temperature. Statistical Physics 15 Part 5: The Bose-Einstein Distribution.

  Distribution, Boltzmann, Boltzmann distribution

Boltzmann Machines

Conditional Boltzmann machines Boltzmann machines model the distribution of the data vectors, but there is a simple extension for modelling conditional distributions (Ackley et al., 1985). The only di erence between the visible and the hidden units is that, when sampling hsisjidata, the visible units are clamped and the hidden units are not.

  Distribution, Boltzmann

Poisson-Boltzmann - Florida State University

count the geometry of the charge distribution. 1.3.2. Charged plane. Suppose the plane is x= 0, The potential depends only on the distance rfrom the plane and the linearized Poisson-Boltzmann be-comes (26) d2ψ dr2 = κ2ψ with solution (27) ψ= ψ 0e−κr and the potential decays exponentially. In this case the Poisson-Boltzmann equation can

  Distribution, Boltzmann