7 research outputs found
Most likely paths to error when estimating the mean of a reflected random walk
It is known that simulation of the mean position of a Reflected Random Walk
(RRW) exhibits non-standard behavior, even for light-tailed increment
distributions with negative drift. The Large Deviation Principle (LDP) holds
for deviations below the mean, but for deviations at the usual speed above the
mean the rate function is null. This paper takes a deeper look at this
phenomenon. Conditional on a large sample mean, a complete sample path LDP
analysis is obtained. Let denote the rate function for the one dimensional
increment process. If is coercive, then given a large simulated mean
position, under general conditions our results imply that the most likely
asymptotic behavior, , of the paths is
to be zero apart from on an interval and to satisfy the
functional equation \begin{align*} \nabla
I\left(\ddt\psi^*(t)\right)=\lambda^*(T_1-t) \quad \text{whenever } \psi(t)\neq
0. \end{align*} If is non-coercive, a similar, but slightly more involved,
result holds.
These results prove, in broad generality, that Monte Carlo estimates of the
steady-state mean position of a RRW have a high likelihood of over-estimation.
This has serious implications for the performance evaluation of queueing
systems by simulation techniques where steady state expected queue-length and
waiting time are key performance metrics. The results show that na\"ive
estimates of these quantities from simulation are highly likely to be
conservative.Comment: 23 pages, 8 figure
On the tail asymptotics of the area swept under the Brownian storage graph
In this paper, the area swept under the workload graph is analyzed: with
denoting the stationary workload process, the asymptotic
behavior of is analyzed. Focusing on regulated Brownian
motion, first the exact asymptotics of are given for the case
that grows slower than , and then logarithmic asymptotics for
(i) (relying on sample-path large deviations), and (ii)
but . Finally, the Laplace
transform of the residual busy period are given in terms of the Airy function.Comment: Published in at http://dx.doi.org/10.3150/12-BEJ491 the Bernoulli
(http://isi.cbs.nl/bernoulli/) by the International Statistical
Institute/Bernoulli Society (http://isi.cbs.nl/BS/bshome.htm
Most likely paths to error when estimating the mean of a reflected random walk
It is known that simulation of the mean position of a Reflected Random Walk (RRW) {Wn}
exhibits non-standard behavior, even for light-tailed increment distributions with negative
drift. The Large Deviation Principle (LDP) holds for deviations below the mean, but for
deviations at the usual speed above the mean the rate function is null. This paper takes a
deeper look at this phenomenon. Conditional on a large sample mean, a complete sample path
LDP analysis is obtained. Let I denote the rate function for the one dimensional increment
process. If I is coercive, then given a large simulated mean position, under general conditions
our results imply that the most likely asymptotic behavior, ∗, of the paths n−1W⌊tn⌋ is to
be zero apart from on an interval [T0, T1] ⊂ [0, 1] and to satisfy the functional equation
∇
Most likely paths to error when estimating the mean of a reflected random walk
It is known that simulation of the mean position of a reflected random walk {Wn} exhibits non-standard behavior, even for light-tailed increment distributions with negative drift. The Large Deviation Principle (LDP) holds for deviations below the mean, but for deviations at the usual speed above the mean the rate function is null. This paper takes a deeper look at this phenomenon. Conditional on a large sample mean, a complete sample path LDP analysis is obtained. Let I denote the rate function for the one dimensional increment process. If I is coercive, then given a large simulated mean position, under general conditions our results imply that the most likely asymptotic behavior, ψ, of the paths n −1 W ⌊tn ⌋ is to be zero apart from on an interval [T0, T1] ⊂ [0, 1] and to satisfy the functional equation ∇I ( d dt ψ(t)) = λ ∗ (T1 − t) whenever ψ(t) ̸ = 0. If I is non-coercive, a similar, but slightly more involved, result holds
Tail asymptotics for busy periods
The busy period for a queue is cast as the area swept under the random walk
until it first returns to zero, . Encompassing non-i.i.d. increments, the
large-deviations asymptotics of is addressed, under the assumption that the
increments satisfy standard conditions, including a negative drift. The main
conclusions provide insight on the probability of a large busy period, and the
manner in which this occurs:
I) The scaled probability of a large busy period has the asymptote, for any
, \lim_{n\to\infty} \frac{1}{\sqrt{n}} \log P(B\geq bn) = -K\sqrt{b},
\hbox{where} \quad K = 2 \sqrt{-\int_0^{\lambda^*} \Lambda(\theta) d\theta},
\quad \hbox{with ,} and with
denoting the scaled cumulant generating function of the increments
process.
II) The most likely path to a large swept area is found to be a simple
rescaling of the path on given by, [\psi^*(t) =
-\Lambda(\lambda^*(1-t))/\lambda^*.] In contrast to the piecewise linear most
likely path leading the random walk to hit a high level, this is strictly
concave in general. While these two most likely paths have very different
forms, their derivatives coincide at the start of their trajectories, and at
their first return to zero.
These results partially answer an open problem of Kulick and Palmowski
regarding the tail of the work done during a busy period at a single server
queue. The paper concludes with applications of these results to the estimation
of the busy period statistics based on observations of the
increments, offering the possibility of estimating the likelihood of a large
busy period in advance of observing one.Comment: 15 pages, 5 figure
Anomalous scalings of fluctuations of the area swept by a Brownian particle trapped in a potential
We study the fluctuations of the area under a
one-dimensional Brownian motion in a trapping potential , at
long times . We find that typical fluctuations of follow a
Gaussian distribution with a variance that grows linearly in time (at large
), as do all higher cumulants of the distribution. However, large deviations
of are not described by the ``usual'' scaling (i.e., the large deviations
principle), and are instead described by two different anomalous scaling
behaviors: Moderatly-large deviations of , obey the anomalous scaling
while very large
deviations behave as . We
find the associated rate functions and exactly. Each of the two
functions contains a singularity, which we interpret as dynamical phase
transitions of the first and third order, respectively. We uncover the origin
of these striking behaviors by characterizing the most likely scenario(s) for
the system to reach a given atypical value of . We extend our analysis by
studying the absolute area and also by generalizing to
higher spatial dimension, focusing on the particular case of three dimensions.Comment: 18 pages, 4 figure
Explicit Mean-Square Error Bounds for Monte-Carlo and Linear Stochastic Approximation
This paper concerns error bounds for recursive equations subject to Markovian
disturbances. Motivating examples abound within the fields of Markov chain
Monte Carlo (MCMC) and Reinforcement Learning (RL), and many of these
algorithms can be interpreted as special cases of stochastic approximation
(SA). It is argued that it is not possible in general to obtain a Hoeffding
bound on the error sequence, even when the underlying Markov chain is
reversible and geometrically ergodic, such as the M/M/1 queue. This is
motivation for the focus on mean square error bounds for parameter estimates.
It is shown that mean square error achieves the optimal rate of ,
subject to conditions on the step-size sequence. Moreover, the exact constants
in the rate are obtained, which is of great value in algorithm design