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Adam, named for adaptive moment estimation, is an adaptive gradient method that scales a running gradient estimate by a running squared-gradient estimate. Diederik P. Kingma and Jimmy Lei Ba presented it as a first-order method for stochastic optimization. Its state makes the next optimizer update depend on gradient history as well as the current parameters.^[ref]

Starting from $m_0=v_0=0$, the basic minimization rule isHere $g_t$ is the supplied gradient, ${\eta }_t>0$ is the learning rate, $0\le {\beta }_1,{\beta }_2<1$, and $ϵ>0$. The Hadamard product, square root and division act coordinatewise. Adam bias correction supplies the two normalization factors. The accumulator $v_t$ concerns a raw second moment, rather than a centered variance.^[ref]

For an original scalar calculation, choose ${\theta }_0=0$, ${\beta }_1={\beta }_2=1/2$, ${\eta }_t=0.1$ and $ϵ=0.1$, and supply $g_1=2$, $g_2=-2$. The first step hasThe second hasEqual and opposite supplied gradients have not undone one another: the running histories give the second step a different magnitude. Plain gradient descent with the same constant learning rate would return to zero for this sequence.

The calculation specifies the recurrence, rather than a convergence guarantee for an unspecified objective function. An optimization checkpoint needs these histories and the step count to reproduce subsequent steps. AdamW adds decoupled weight decay; feeding a penalty gradient into Adam instead implements coupled L2 regularization and changes the histories.

Durk Kingma is a computer scientist who publishes as Diederik P. Kingma. His personal profile describes research on machine learning and generative models, and records a 2017 doctorate at the University of Amsterdam.^[ref] The institutional thesis front matter gives his full formal name as Diederik Pieter Kingma.^[ref]

Kingma and Max Welling coauthored Auto-Encoding Variational Bayes by Diederik P. Kingma and Max Welling. A variational autoencoder couples a latent-variable model with an approximating posterior distribution that can be optimized through variational inference. Their reparameterization gradients represent a simulated random variable as a differentiable transformation of parameter-independent noise, allowing derivatives through the transformation.^[ref] Kingma also coauthored the Adam paper with Jimmy Lei Ba.^[ref]

An original scalar calculation makes the noise handling concrete. Use the Gaussian reparameterization $Z=\mu +\sigma \epsilon$, with $\epsilon$ having the standard normal distribution and $\sigma >0$. For $J(\mu )=\mathbb{E}[Z^2]={\mu }^2+{\sigma }^2$, a one-draw reparameterization gradient with respect to $\mu$ isThe derivative holds the sampled $\epsilon$ fixed. This pathwise gradient is justified here by direct calculation; a general interchange of derivative and expected value requires differentiation under the integral sign conditions.

Noise coupling matters even for a central finite difference. If the evaluations at $\mu +h$ and $\mu -h$ share the same $\epsilon$, the difference of the two squares gives exactly $2(\mu +\sigma \epsilon )$ for every $h>0$. This is a use of common random numbers. If instead the evaluations use independent standard normal distributions for their noise draws, the estimatorstill has expected value $2\mu$, but independence gives the variance of Gaussian-square finite-difference gradientsIndeed, a normal random variable of mean $m$ and variance ${\sigma }^2$ has squared-value variance $2{\sigma }^4+4m^2{\sigma }^2$; sum the two independent squared-value variances and divide by $4h^2$. Thus shrinking $h$ need not suppress simulation noise.

For chosen $\mu =1$, $\sigma =2$ and $h=0.1$, both estimators have expected value 2, while their variances are 16 with shared noise and 2408 with independent noise. The example is a separate exact quadratic model; its purpose is to explain the role of keeping base noise fixed, not to reproduce a published variational-autoencoder benchmark.

Jamie Ryan Kiros coauthored the 2016 layer normalization paper with Jimmy Lei Ba and Geoffrey E. Hinton. The original paper gives the full byline Jamie Ryan Kiros and a University of Toronto affiliation. Its normalization statistics are computed across the inputs within one case, rather than across different cases in a batch.^[ref]

A small original implementation experiment tests that distinction without measuring training speed. Fix one case's two inputs at $h=(2,6)$, unit gains, zero biases and a variance stabilizer of $1$. The within-case mean is $4$ and variance is $4$, so its normalized outputs areEvaluate this case first beside another case $(-100,100)$ and then beside $(1000,2000)$. The stated isolated normalization computation returns the same output for $h$ in both evaluations, because neither companion enters its statistics. This tests a concrete dependency of the computation, not a claim about every layer of a complete network.

The paper also studies recurrent neural networks, computing the statistics separately at each time step.^[ref] That application makes the choice of averaging axes consequential. The paper establishes a collaborative contribution; its byline does not assign a separate invention to each author.

Jimmy Lei Ba, also known as Jimmy Ba, is a computer scientist whose published work includes Adam and layer normalization. His personal research biography identifies Geoffrey Hinton as his doctoral supervisor and describes a focus on efficient algorithms for deep learning.^[ref] The 2016 layer-normalization manuscript prints his University of Toronto affiliation and the name Jimmy Lei Ba.^[ref]

Ba coauthored Adam: A Method for Stochastic Optimization by Diederik P. Kingma and Jimmy Lei Ba with Diederik P. Kingma. The algorithm maintains optimizer state based on gradients, so its update depends on the history of the optimization. Adam bias correction accounts for the early effect of initializing its exponential accumulators at zero.^[ref]

The layer normalization paper, coauthored with Jamie Ryan Kiros and Geoffrey E. Hinton, addresses a different part of a neural network: it computes a mean and variance across feature coordinates of an individual example, then applies learned gain and bias. It avoids making those statistics depend on the other examples in the mini-batch.^[ref]

An original numerical example illustrates one precise symmetry. In the stabilized formula of layer normalization, set all gains to 1, all biases to 0, and layer-normalization epsilon to $\epsilon =1/3$. For $z=(1,2,3)$, the coordinate arithmetic mean is 2 and the coordinate variance is $2/3$, so the normalized output is $(-1,0,1)$. Adding 10 to every coordinate gives $(11,12,13)$, whose output is again $(-1,0,1)$: layer normalization is invariant under a common input shift because the coordinate mean shifts by the same amount and the deviations remain unchanged.

The fixed layer-normalization epsilon affects scaling differently. With $2z=(2,4,6)$, the coordinate variance is $8/3$ and the output is $(-2/\sqrt{3},0,2/\sqrt{3})$, which differs from the original output. This calculation distinguishes the exact common-shift symmetry from idealized scale invariance when the stabilizer is omitted. It does not assign either numerical example to the paper's experiments.