# On the Link Between Optimization and Polynomials, Part 2

Momentum: when Chebyshev meets Chebyshev.

We can tighten the analysis of momentum methods through Chebyshev polynomials of the first and second kind. Following this connection, we'll derive one of the most iconic methods in optimization: Polyak momentum.

## Momentum

Gradient descent with momentum –momentum for short– are a class of optimization
methods
designed to solve unconstrained optimization problems of the form
\begin{equation}
\argmin_{\xx \in \RR^d} f(\xx)\,,
\end{equation}
where the objective function $f$ is differentiable and we have access to its gradient $\nabla
f$. In momentum
the udpate is a sum of two terms. The first term is the
difference between current and previous iterate $(\xx_{t} - \xx_{t-1})$, also known as *momentum
term*. The second term is the gradient $\nabla f(\xx_t)$ of the objective function.

**Gradient Descent with Momentum**

**Input**: starting guess $\xx_0$, step-size ${\color{colorstepsize} h} > 0$ and momentum
parameter ${\color{colormomentum} m} \in (0, 1)$.

$\xx_1 = \xx_0 - \dfrac{{\color{colorstepsize} h}}{1 + {\color{colormomentum} m}} \nabla f(\xx_0)$

**For** $t=1, 2, \ldots$ compute
\begin{equation}\label{eq:momentum_update}
\xx_{t+1} = \xx_t + {\color{colormomentum} m}(\xx_{t} - \xx_{t-1}) - {\color{colorstepsize}
h}\nabla
f(\xx_t)
\end{equation}

Momentum method have seen a renewed interest in recent years, as a stochastic variant that replaces the true gradient with a stochastic estimate has shown to be very effective for deep learning.

### Quadratic model

Although momentum can be applied to any problem with a twice differentiable objective, in this post we'll assume for simplicity the objective function $f$ quadratic.

**Example: Polyak Momentum**, also known as the HeavyBall method, is a widely used instance of momentum. Originally developed for the solution of linear equations and known as Frankel's method,

Boris Polyak (1935 —) is a Russian mathematician and pioneer of optimization. Currently, he leads the Laboratory at Institute of Control Science in Moscow.

Polyak momentum follows the update \eqref{eq:momentum_update} with momentum and step-size parameters \begin{equation}\label{eq:polyak_parameters} {\color{colormomentum}m = {\Big(\frac{\sqrt{L}-\sqrt{\ell}}{\sqrt{L}+\sqrt{\ell}}\Big)^2}} \text{ and } {\color{colorstepsize}h = \Big(\frac{ 2}{\sqrt{L}+\sqrt{\ell}}\Big)^2}\,. \end{equation}

### Residual Polynomials

In the last post we saw that to each gradient-based optimizer we can associate a sequence of
polynomials $P_1, P_2,
...$ that we named *residual polynomials* and that determines the converge of the method:

This is a special case of the Residual polynomial Lemma proved in the last post.

In the last post we also gave an expression for this residual polynomial. Although this expression is rather involved in the general case, it simplifies for momentum, where it follows the simple recurrence:

Given a momentum method with parameters ${\color{colormomentum} m}$, ${\color{colorstepsize} h}$, the associated residual polynomials $P_0, P_1, \ldots$ verify the following recursion \begin{equation} \begin{split} &P_{t+1}(\lambda) = (1 + {\color{colormomentum}m} - {\color{colorstepsize} h} \lambda ) P_{t}(\lambda) - {\color{colormomentum}m} P_{t-1}(\lambda)\\ &P_0(\lambda) = 1\,,~ P_1(\lambda) = 1 - \frac{{\color{colorstepsize} h}}{1 + {\color{colormomentum}m}} \lambda \,. \end{split}\label{eq:def_residual_polynomial2} \end{equation}

A consequence of this result is that not only the method, but also its residual polynomial, has a simple recurrence. We will soon leverage this to simplify the analysis.

## Chebyshev meets Chebyshev

Chebyshev polynomials of the first kind appeared in the last post when deriving the optimal worst-case method. These are polynomials $T_0, T_1, \ldots$ defined by the recurrence relation \begin{align} &T_0(\lambda) = 1 \qquad T_1(\lambda) = \lambda\\ &T_{k+1}(\lambda) = 2 \lambda T_k(\lambda) - T_{k-1}(\lambda)~. \end{align} A fact that we didn't use in the last post is that Chebyshev polynomials are orthogonal with respect to the weight function \begin{equation} \dif\mu(\lambda) = \begin{cases} \frac{1}{\pi\sqrt{1 - \lambda^2}} &\text{ if $\lambda \in [-1, 1]$} \\ 0 &\text{ otherwise}\,. \end{cases} \end{equation} That is, they verify the orthogonality condition \begin{equation} \int T_i(\lambda) T_j(\lambda) \dif\mu(\lambda) \begin{cases} > 0 \text{ if $i = j$}\\ = 0 \text{ otherwise}\,.\end{cases} \end{equation}

I mentioned that these are the Chebyshev polynomials of the first kind because there are
also Chebyshev polynomials *of the second kind*, and although less used, also of the third
kind, fourth kind and so on.

Chebyshev polynomials of the second kind, denoted $U_1, U_2, \ldots$, are defined by the integral \begin{equation} U_t(\lambda) = \int \frac{T_{t+1}(\xi) - T_{t+1}(\lambda)}{\xi- \lambda}\dif\mu(\xi)\,. \end{equation}

Although we will only use this construction for Chebyshev polynomials, it extends beyond this
setup and is very natural because these polynomials are the numerators for the convergents of
certain continued fractions.

The polynomials of the second kind verify the same recurrence formula as the original sequence, but with different initial conditions. In particular, the Chebyshev polynomials of the second kind are determined by the recurrence \begin{align} &U_0(\lambda) = 1 \qquad U_1(\lambda) = 2 \lambda\\ &U_{k+1}(\lambda) = 2 \lambda U_k(\lambda) - U_{k-1}(\lambda)~. \end{align} Note how $U_1(\lambda)$ is different from $T_1$, but other than that, the coefficients in the recurrence are the same. Because of this, both sequences behave somewhat similarly, but also have important differences. For example, both kinds have extrema at the endpoints, but the value is different. For the first kind, the extrema is $\pm 1$, while for the second kind its $\pm (t+1)$.

## Momentum's residual polynomial

Time has finally come for the main result: the residual polynomial of momentum is nothing else than a combination of Chebyshev polynomials of the first and second kind. Since the properties of Chebyshev polynomials are well known, this will provide a way to derive convergence bounds for momentum.

The residual polynomial $P_t$ associated with a momentum method with parameters ${\color{colormomentum}m}, {\color{colorstepsize}h}$ can be written in terms of Chebyshev polynomials as \begin{equation}\label{eq:theorem} P_t(\lambda) = {\color{colormomentum}m}^{t/2} \left( {\small\frac{2 {\color{colormomentum}m}}{1 + {\color{colormomentum}m}}}\, T_t(\sigma(\lambda)) - {\small\frac{{\color{colormomentum}m} - 1}{1 + {\color{colormomentum}m}}}\, U_t(\sigma(\lambda))\right)\,, \end{equation} with $\sigma(\lambda) = {\small\dfrac{1}{2\sqrt{{\color{colormomentum}m}}}}(1 + {\color{colormomentum}m} - {\color{colorstepsize} h}\,\lambda)\,$.

Let's denote by $\widetilde{P}_t$ the right hand side of the above equation, that is, \begin{equation} \widetilde{P}_{t}(\lambda) \defas {\color{colormomentum}m}^{t/2} \left( {\small\frac{2 {\color{colormomentum}m}}{1 + {\color{colormomentum}m}}}\, T_t(\sigma(\lambda)) - {\small\frac{{\color{colormomentum}m}-1}{1 + {\color{colormomentum}m}}}\, U_t(\sigma(\lambda))\right)\,. \end{equation} Our goal is to show that $P_t = \widetilde{P}_t$ for all $t$.

For $t=1$, $T_1(\lambda) = \lambda$ and $U_1(\lambda) = 2\lambda$, so we have \begin{align} \widetilde{P}_1(\lambda) &= \sqrt{{\color{colormomentum}m}} \left(\tfrac{2 {\color{colormomentum}m}}{1 + {\color{colormomentum}m}} \sigma(\lambda) - \tfrac{{\color{colormomentum}m}-1}{1 + {\color{colormomentum}m}} 2 \sigma(\lambda)\right)\\ &= \frac{2 \sqrt{{\color{colormomentum}m}}}{1 + {\color{colormomentum}m}} \sigma(\lambda) = 1 - \frac{{\color{colorstepsize}h}}{1 + {\color{colormomentum}m}} \lambda\,, \end{align} which corresponds to the definition of $P_1$ in \eqref{eq:def_residual_polynomial2}.

Assume it's true for any iteration up to $t$, we will show it's true for $t+1$. Using the three-term recurrence of Chebyshev polynomials we have \begin{align} &\widetilde{P}_{t+1}(\lambda) = {\color{colormomentum}m}^{(t+1)/2} \left( {\small\frac{2 {\color{colormomentum}m}}{1 + {\color{colormomentum}m}}}\, T_{t+1}(\sigma(\lambda)) - {\small\frac{{\color{colormomentum}m}-1}{1 + {\color{colormomentum}m}}}\, U_{t+1}(\sigma(\lambda))\right) \\ &= {\color{colormomentum}m}^{(t+1)/2} \Big( {\small\frac{2 {\color{colormomentum}m}}{1 + {\color{colormomentum}m}}}\, (2 \sigma(\lambda) T_{t}(\sigma(\lambda)) - T_{t-1}(\sigma(\lambda))) \nonumber\\ &\qquad\qquad - {\small\frac{{\color{colormomentum}m}-1}{1 + {\color{colormomentum}m}}}\, (2 \sigma(\lambda) U_{t}(\sigma(\lambda)) - U_{t-1}(\sigma(\lambda)))\Big)\\ &= 2 \sigma(\lambda) \sqrt{{\color{colormomentum}m}} P_t(\lambda) - {\color{colormomentum}m} P_{t-1}(\lambda)\\ &= (1 + {\color{colormomentum}m} - {\color{colorstepsize}h} \lambda) P_t(\lambda) - {\color{colormomentum}m} P_{t-1}(\lambda) \end{align} where the third identity follows from grouping polynomials of same degree and the induction hypothesis. The last expression is the recursive definition of $P_{t+1}$ in \eqref{eq:def_residual_polynomial2}, which proves the desired $\widetilde{P}_{t+1} = {P}_{t+1}$.

**History bits.** The theorem above is a generalization

More recently, in a collaboration with Courtney, Bart and Elliot we used Ruthishauser's expression to derive an *average-case* analysis of Polyak momentum.

## Convergence Rates and Robust Region

In the last post se introduced the worst-case convergence rate as a tool to compare speed of convergence of optimization algorithms. These are an upper bound on the per-iteration progress of an optimization algorithm. In other words, a small convergence rate guarantees a fast convergence. Convergence rates can be expressed in term of the residual polynomial as \begin{equation} r_t \defas \max_{\lambda \in [\ell, L]} |P_t(\lambda)|\,, \end{equation} where $\ell, L$ are the smallest and largest eigenvalues of $\HH$ respectively. Using Hestenes and Stiefel's lemma, we can see that $r_t$ is an upper bound on the norm of the error in the sense that it verifies \begin{equation} \|\xx_t - \xx^\star\| \leq r_t\,\|\xx_0 - \xx^\star\|\,. \end{equation}

Deriving convergence rates is hard, but the previous Theorem allows us to convert this problem into the one of bounding Chebyshev polynomials. Hopefully, this problem is easier as we know a lot about Chebyshev polynomials. In particular, replacing $P_t$ with \eqref{eq:theorem} in the definition of convergence rate and upper bounding the joint maximum with a separate one on $T_t$ and $U_t$ we have \begin{equation} r_t \leq {\color{colormomentum}m}^{t/2} \left( {\small\frac{2 {\color{colormomentum}m}}{1 + {\color{colormomentum}m}}}\, \max_{\lambda \in [\ell, L]}|T_t(\sigma(\lambda))| + {\small\frac{1 - {\color{colormomentum}m}}{1 + {\color{colormomentum}m}}}\, \max_{\lambda \in [\ell, L]}|U_t(\sigma(\lambda))|\right)\,. \end{equation} In this equation we know everything except $\max_{\lambda \in [\ell, L]}|T_t(\sigma(\lambda))|$ and $\max_{\lambda \in [\ell, L]}|U_t(\sigma(\lambda))|$.

Luckily, we have all sorts of bounds on Chebyshev polynomials. One of the simplest and most useful one bounds these polynomials in the $[-1, 1]$ interval.

Inside the interval $\xi \in [-1, 1]$, we have the
bounds
\begin{equation}\label{eq:bound_chebyshev}
|T_t(\xi)| \leq 1 \quad \text{ and } \quad |U_{t}(\xi)| \leq t+1\,.
\end{equation}
In our case, the Chebyshev polynomials are evaluated at $\sigma(\lambda)$, so these bounds are
valid whenever $\max_{\lambda \in [\ell, L]}|\sigma(\lambda)| \leq 1$,
which by a distinction of cases can be shown to be equivalent to the conditions
\begin{equation}\label{eq:condition_stable_region}
\frac{(1 - \sqrt{{\color{colormomentum}m}})^2 }{{\color{colorstepsize}h}} \leq \ell \leq L
\leq~\frac{(1 + \sqrt{{\color{colormomentum}m}})^2 }{{\color{colorstepsize}h}}
\end{equation}
We will refer to the set of parameters that
verify the above as the *robust region*. This is a subset of the set of admissible parameters –those for which the method converges– which is known to be

In the robust region, can use the bounds above and we have the rate
\begin{equation}\label{eq:convergence_rate_stable}
r_t \leq {\color{colormomentum}m}^{t/2} \left( 1
+ {\small\frac{1 - {\color{colormomentum}m}}{1 + {\color{colormomentum}m}}}\, t\right)
\end{equation}
This convergence rate is somewhat surprising, as one might expect
that the convergence depends on both the step-size and momentum. Instead, in the robust region the convergence rate
does not depend on the step-size. This
insensitivity to step-size can be leveraged for example to develop a momentum tuner.

Given that we would like the convergence rate to be as small as possible, it's natural to choose the momentum term as small as possible while staying in the robust region. But just how small can we make this momentum term?

## Polyak strikes back

This post ends as it starts: with Polyak momentum. We will see that minimizing the convergence rate while staying in the robust region will lead us naturally to this method.

Inside the robust region, the smallest momentum parameter is achieved when the inequalities \eqref{eq:condition_stable_region} becomes equalities, as otherwise one could find a smaller momentum term that still verifies the conditions. The problem then consists in solving \begin{equation} \frac{(1 - \sqrt{{\color{colormomentum}m}})^2 }{{\color{colorstepsize}h}} = \ell ~\text{ and }~\frac{(1 + \sqrt{{\color{colormomentum}m}})^2 }{{\color{colorstepsize}h}} = L \end{equation} for ${\color{colorstepsize}h}$, ${\color{colormomentum}m}$. This has two solutions, of which only one has a momentum parameter ${\color{colormomentum}m} < 1$: \begin{equation} {\color{colormomentum}m = {\Big(\frac{\sqrt{L}-\sqrt{\ell}}{\sqrt{L}+\sqrt{\ell}}\Big)^2}} \text{ and } {\color{colorstepsize}h = \Big(\frac{ 2}{\sqrt{L}+\sqrt{\ell}}\Big)^2}\,. \end{equation} These are the step-size and momentum parameter of Polyak momentum of \eqref{eq:polyak_parameters}.

This provides an alternative derivation of Polyak momentum from Chebyshev polynomials.

### Stay Tuned

In this post we've only scratched the surface of the rich dynamics of momentum. In the next post we will explore dig deeper into the robust region and explore the other regions too.

**Acknowledgements.** Thanks to Nicolas Le Roux for catching some mistakes in an initial version of this post and providing thoughtful feedback.