# How does saddlepoint approximation work?

How does saddlepoint approximation work? What sort of problem is it good for?
(Feel free to use a particular example or examples by way of illustration)

Are there any drawbacks, difficulties, things to watch out for, or traps for the unwary?

The saddlepoint approximation to a probability density function (it works likewise for mass functions, but I will only talk here in terms of densities) is a surprisingly well working approximation, that can be seen as a refinement on the central limit theorem. So, it will only work in settings where there is a central limit theorem, but it needs stronger assumptions.

We start with the assumption that the moment generating function exists and is twice differentiable. This implies in particular that all moments exist. Let $$X$$ be a random variable with moment generating function (mgf) $$\DeclareMathOperator{\E}{\mathbb{E}} M(t) = \E e^{t X}$$ and cgf (cumulant generating function) $$K(t)=\log M(t)$$ (where $$\log$$ denotes the natural logarithm). In the development I will follow closely Ronald W Butler: "Saddlepoint Approximations with Applications" (CUP). We will develop the saddlepoint approximation using the Laplace approximation to a certain integral. Write $$e^{K(t)} = \int_{-\infty}^\infty e^{t x} f(x) \; dx =\int_{-\infty}^\infty \exp(tx+\log f(x) ) \; dx \\ = \int_{-\infty}^\infty \exp(-h(t,x)) \; dx$$ where $$h(t,x) = -tx - \log f(x)$$. Now we will Taylor expand $$h(t,x)$$ in $$x$$ considering $$t$$ as a constant. This gives $$h(t,x)=h(t,x_0) + h'(t,x_0)(x-x_0) +\frac12 h''(t,x_0) (x-x_0)^2 +\dotsm$$ where $$'$$ denotes differentiation with respect to $$x$$. Note that $$h'(t,x)=-t-\frac{\partial}{\partial x}\log f(x) \\ h''(t,x)= -\frac{\partial^2}{\partial x^2} \log f(x) > 0$$ (the last inequality by assumption as it is needed for the approximation to work). Let $$x_t$$ be the solution to $$h'(t,x_t)=0$$. We will assume that this gives a minimum for $$h(t,x)$$ as a function of $$x$$. Using this expansion in the integral and forgetting about the $$\dotsm$$ part, gives $$e^{K(t)} \approx \int_{-\infty}^\infty \exp(-h(t,x_t)-\frac12 h''(t,x_t) (x-x_t)^2 ) \; dx \\ = e^{-h(t,x_t)} \int_{-\infty}^\infty e^{-\frac12 h''(t,x_t) (x-x_t)^2} \; dx$$ which is a Gaussian integral, giving $$e^{K(t)} \approx e^{-h(t,x_t)} \sqrt{\frac{2\pi}{h''(t,x_t)}}.$$ This gives (a first version) of the saddlepoint approximation as $$f(x_t) \approx \sqrt{\frac{h''(t,x_t)}{2\pi}} \exp(K(t) -t x_t) \\ \tag{*} \label{*}$$ Note that the approximation has the form of an exponential family.

Now we need to do some work to get this in a more useful form.

From $$h'(t,x_t)=0$$ we get $$t = -\frac{\partial}{\partial x_t} \log f(x_t).$$ Differentiating this with respect to $$x_t$$ gives $$\frac{\partial t}{\partial x_t} = -\frac{\partial^2}{\partial x_t^2} \log f(x_t) > 0$$ (by our assumptions), so the relationship between $$t$$ and $$x_t$$ is monotone, so $$x_t$$ is well defined. We need an approximation to $$\frac{\partial}{\partial x_t} \log f(x_t)$$. To that end, we get by solving from \eqref{*} $$\log f(x_t) = K(t) -t x_t -\frac12 \log \frac{2\pi}{-\frac{\partial^2}{\partial x_t^2} \log f(x_t)}. \tag{**} \label{**}$$ Assuming the last term above only depends weakly on $$x_t$$, so its derivative with respect to $$x_t$$ is approximately zero (we will come back to comment on this), we get $$\frac{\partial \log f(x_t)}{\partial x_t} \approx (K'(t)-x_t) \frac{\partial t}{\partial x_t} - t$$ Up to this approximation we then have that $$0 \approx t + \frac{\partial \log f(x_t)}{\partial x_t} = (K'(t)-x_t) \frac{\partial t}{\partial x_t}$$ so that $$t$$ and $$x_t$$ must be related through the equation $$K'(t) - x_t=0, \\ \tag{§} \label{§}$$ which is called the saddlepoint equation.

What we miss now in determining \eqref{*} is $$h''(t,x_t) = -\frac{\partial^2 \log f(x_t)}{\partial x_t^2} \\ = -\frac{\partial}{\partial x_t} (\frac{\partial log f(x_t)}{\partial x_t} ) \\ = -\frac{\partial}{\partial x_t}(-t)= (\frac{\partial x_t}{\partial t})^{-1}$$ and that we can find by implicit differentiation of the saddlepoint equation $$K'(t)=x_t$$: $$\frac{\partial x_t}{\partial t} = K''(t).$$ The result is that (up to our approximation) $$h''(t,x_t) = \frac1{K''(t)}$$ Putting everything together, we have the final saddlepoint approximation of the density $$f(x)$$ as $$f(x_t) \approx e^{K(t)- t x_t} \sqrt{\frac1{2\pi K''(t)}}.$$ Now, to use this practically, to approximate the density at a specific point $$x_t$$, we solve the saddlepoint equation for that $$x_t$$ to find $$t$$.

The saddlepoint approximation is often stated as an approximation to the density of the mean based on $$n$$ iid observations $$X_1, X_2, \dotsc, X_n$$. The cumulant generating function of the mean is simply $$n K(t)$$, so the saddlepoint approximation for the mean becomes $$f(\bar{x}_t) = e^{nK(t) - n t \bar{x}_t} \sqrt{\frac{n}{2\pi K''(t)}}$$

Let us look at a first example. What does we get if we try to approximate the standard normal density $$f(x)=\frac1{\sqrt{2\pi}} e^{-\frac12 x^2}$$ The mgf is $$M(t)=\exp(\frac12 t^2)$$ so $$K(t)=\frac12 t^2 \\ K'(t)=t \\ K''(t)=1$$ so the saddlepoint equation is $$t=x_t$$ and the saddlepoint approximation gives $$f(x_t) \approx e^{\frac12 t^2 -t x_t} \sqrt{\frac1{2\pi \cdot 1}} = \frac1{\sqrt{2\pi}} e^{-\frac12 x_t^2}$$ so in this case the approximation is exact.

Let us look at a very different application: Bootstrap in the transform domain, we can do bootstrapping analytically using the saddlepoint approximation to the bootstrap distribution of the mean!

Assume we have $$X_1, X_2, \dotsc, X_n$$ iid distributed from some density $$f$$ (in the simulated example we will use a unit exponential distribution). From the sample we calculate the empirical moment generating function $$\hat{M}(t)= \frac1{n} \sum_{i=1}^n e^{t x_i}$$ and then the empirical cgf $$\hat{K}(t) = \log \hat{M}(t)$$. We need the empirical mgf for the mean which is $$\log ( \hat{M}(t/n)^n )$$ and the empirical cgf for the mean $$\hat{K}_{\bar{X}}(t) = n \log \hat{M}(t/n)$$ which we use to construct a saddlepoint approximation. In the following some R code (R version 3.2.3):

set.seed(1234)
x  <-  rexp(10)

require(Deriv)   ### From CRAN
drule[["sexpmean"]]   <-  alist(t=sexpmean1(t))  # adding diff rules to
# Deriv
drule[["sexpmean1"]]  <-  alist(t=sexpmean2(t))

###

make_ecgf_mean  <-   function(x)   {
n  <-  length(x)
sexpmean  <-  function(t) mean(exp(t*x))
sexpmean1 <-  function(t) mean(x*exp(t*x))
sexpmean2 <-  function(t) mean(x*x*exp(t*x))
emgf  <-  function(t) sexpmean(t)
ecgf  <-   function(t)  n * log( emgf(t/n) )
ecgf1 <-   Deriv(ecgf)
ecgf2 <-   Deriv(ecgf1)
return( list(ecgf=Vectorize(ecgf),
ecgf1=Vectorize(ecgf1),
ecgf2 =Vectorize(ecgf2) )    )
}

### Now we need a function solving the saddlepoint equation and constructing
### the approximation:
###

make_spa <-  function(cumgenfun_list) {
K  <- cumgenfun_list[[1]]
K1 <- cumgenfun_list[[2]]
K2 <- cumgenfun_list[[3]]
# local function for solving the speq:
solve_speq  <-  function(x) {
uniroot(function(s) K1(s)-x,lower=-100,
upper = 100,
extendInt = "yes")$root } # Function finding fhat for one specific x: fhat0 <- function(x) { # Solve saddlepoint equation: s <- solve_speq(x) # Calculating saddlepoint density value: (1/sqrt(2*pi*K2(s)))*exp(K(s)-s*x) } # Returning a vectorized version: return(Vectorize(fhat0)) } #end make_fhat  ( I have tried to write this as general code which can be modified easily for other cgfs, but the code is still not very robust ...) Then we use this for a sample of ten independent observations from a unit exponential distribution. We do the usual nonparametric bootstrapping "by hand", plot the resulting bootstrap histogram for the mean, and overplot the saddlepoint approximation: > ECGF <- make_ecgf_mean(x) > fhat <- make_spa(ECGF) > fhat function (x) { args <- lapply(as.list(match.call())[-1L], eval, parent.frame()) names <- if (is.null(names(args))) character(length(args)) else names(args) dovec <- names %in% vectorize.args do.call("mapply", c(FUN = FUN, args[dovec], MoreArgs = list(args[!dovec]), SIMPLIFY = SIMPLIFY, USE.NAMES = USE.NAMES)) } <environment: 0x4e5a598> > boots <- replicate(10000, mean(sample(x, length(x), replace=TRUE)), simplify=TRUE) > boots <- replicate(10000, mean(sample(x, length(x), replace=TRUE)), simplify=TRUE) > hist(boots, prob=TRUE) > plot(fhat, from=0.001, to=2, col="red", add=TRUE)  Giving the resulting plot: The approximation seems to be rather good! We could get an even better approximation by integrating the saddlepoint approximation and rescaling: > integrate(fhat, lower=0.1, upper=2) 1.026476 with absolute error < 9.7e-07  Now the cumulative distribution function based on this approximation could be found by numerical integration, but it is also possible to make a direct saddlepoint approximation for that. But that is for another post, this is long enough. Finally, some comments left out of the development above. In \eqref{**} we did an approximation essentially ignoring the third term. Why can we do that? One observation is that for the normal density function, the left-out term contributes nothing, so that approximation is exact. So, since the saddlepoint-approximation is a refinement on the central limit theorem, so we are somewhat close to the normal, so this should work well. One can also look at specific examples. Looking at the saddlepoint approximation to the Poisson distribution, looking at that left-out third term, in this case that becomes a trigamma function, which indeed is rather flat when the argument is not to close to zero. Finally, why the name? The name come from an alternative derivation, using complex-analysis techniques. Later we can look into that, but in another post! • What you have so far is great. The development there is very clear. Jan 22, 2016 at 0:28 • kjetil I attempted to fix four small typos 1. "In the development I wil follow" 2. "needed for the approximatrion to work" 3. "What we misses now" 4. "implicit differentiation of the sadlepoint" but in doing so it looks like I broke one of your equations - I have no idea how, since I changed nothing but those text items (as you can see from the edit history). I'd roll it back but since I can't explain how fixing those errors caused a problem I don't want to cause still further problems. My apologies. (It actually looked like it broke as soon as I opened the edit session) Jan 22, 2016 at 0:45 • It's possible there's a mathJax bug or a bug in the edit code that leads to this issue. Jan 22, 2016 at 0:48 • @Christoph Hanck: To get an approximation at some specifix$x_t$, you solve the saddlepoint equation \eqref{§} to find$t$. Jan 22, 2016 at 10:21 • Maybe it is worth pointing out that, when the empirical cgf is used, the resulting saddlepoint approximation is undefined outside the convex hull of the data. See Feuerverger (‎1989) "On the Empirical Saddlepoint Approximation". This should be the case also in the bootstrap example above. Jan 25, 2016 at 13:58 Here I expand upon kjetil's answer, and I focus on those situations where the Cumulant Generating Function (CGF) is unknown, but it can be estimated from the data$x_1,\dots,x_n$, where$x\in R^d$. The simplest CGF estimator is probably that of Davison and Hinkley (1988) $$\hat{K}(\lambda) = \frac{1}{n}\sum_{i=1}^{n}e^{\lambda^Tx_i},$$ which is the one used in kjetil's bootstrap example. This estimator has the drawback that the resulting saddlepoint equation $$\hat{K}'(\lambda) = y,$$ can be solved only if$y$, the point at which we want to evaluate the saddlepoint density, falls within the convex hull of$x_1,\dots,x_n$. Wong (1992) and Fasiolo et al. (2016) addressed this problem by proposing two alternative CGF estimators, designed in such a way that the saddlepoint equation can be solved for any$y$. The solution of Fasiolo et al. (2016), called the extended Empirical Saddlepoint Approximation ESA, is implemented in the esaddle R package and here I give a couple of examples. As a simple univariate example, consider using ESA to approximate a$\text{Gamma}(2, 1)$density. library("devtools") install_github("mfasiolo/esaddle") library("esaddle") ########## Simulating data x <- rgamma(1000, 2, 1) # Fixing tuning parameter of ESA decay <- 0.05 # Evaluating ESA at several point xSeq <- seq(-2, 8, length.out = 200) tmp <- dsaddle(y = xSeq, X = x, decay = decay, log = TRUE) # Plotting true density, ESA and normal approximation plot(xSeq, exp(tmp$llk), type = 'l', ylab = "Density", xlab = "x")
lines(xSeq, dgamma(xSeq, 2, 1), col = 3)
lines(xSeq, dnorm(xSeq, mean(x), sd(x)), col = 2)
suppressWarnings( rug(x) )
legend("topright", c("ESA", "Truth", "Gaussian"), col = c(1, 3, 2), lty = 1)


This is the fit

Looking at the rug it is clear that we evaluated the ESA density outside the range of the data. A more challenging example is the following warped bivariate Gaussian.

# Function that evaluates the true density
dwarp <- function(x, alpha) {
d <- length(alpha) + 1
lik <- dnorm(x[ , 1], log = TRUE)
tmp <- x[ , 1]^2
for(ii in 2:d)
lik <- lik + dnorm(x[ , ii] - alpha[ii-1]*tmp, log = TRUE)
lik
}

# Function that simulates from true distribution
rwarp <- function(n = 1, alpha) {
d <- length(alpha) + 1
z <- matrix(rnorm(n*d), n, d)
tmp <- z[ , 1]^2
for(ii in 2:d) z[ , ii] <- z[ , ii] + alpha[ii-1]*tmp
z
}

set.seed(64141)
# Creating 2d grid
m <- 50
expansion <- 1
x1 <- seq(-2, 3, length=m)* expansion;
x2 <- seq(-3, 3, length=m) * expansion
x <- expand.grid(x1, x2)

# Evaluating true density on grid
alpha <- 1
dw <- dwarp(x, alpha = alpha)

# Simulate random variables
X <- rwarp(1000, alpha = alpha)

# Evaluating ESA density
dwa <- dsaddle(as.matrix(x), X, decay = 0.1, log = FALSE)$llk # Plotting true density par(mfrow = c(1, 2)) plot(X, pch=".", col=1, ylim = c(min(x2), max(x2)), xlim = c(min(x1), max(x1)), main = "True density", xlab = expression(X[1]), ylab = expression(X[2])) contour(x1, x2, matrix(dw, m, m), levels = quantile(as.vector(dw), seq(0.8, 0.995, length.out = 10)), col=2, add=T) # Plotting ESA density plot(X, pch=".",col=2, ylim = c(min(x2), max(x2)), xlim = c(min(x1), max(x1)), main = "ESA density", xlab = expression(X[1]), ylab = expression(X[2])) contour(x1, x2, matrix(dwa, m, m), levels = quantile(as.vector(dwa), seq(0.8, 0.995, length.out = 10)), col=2, add=T)  The fit is pretty good. Thanks to Kjetil's great answer I am trying to come up with a little example myself, which I would like to discuss because it seems to raise a relevant point: Consider the$\chi^2(m)$distribution.$K(t)$and its derivatives may be found here and are reproduced in the functions in the code below. x <- seq(0.01,20,by=.1) m <- 5 K <- function(t,m) -1/2*m*log(1-2*t) K1 <- function(t,m) m/(1-2*t) K2 <- function(t,m) 2*m/(1-2*t)^2 saddlepointapproximation <- function(x) { t <- .5-m/(2*x) exp( K(t,m)-t*x )*sqrt( 1/(2*pi*K2(t,m)) ) } plot( x, saddlepointapproximation(x), type="l", col="salmon", lwd=2) lines(x, dchisq(x,df=m), col="lightgreen", lwd=2)  This produces This obviously produces an approximation that gets the qualitative features of the density right, but, as confirmed in Kjetil's comment, is not a proper density, as it is above the exact density everywhere. Rescaling the approximation as follows gives the almost negligible approximation error plotted below. scalingconstant <- integrate(saddlepointapproximation, x[1], x[length(x)])$value


• approximationerror_unscaled/approximationerror_scaled turns out to hover around 25.90798 Jan 22, 2016 at 12:07