by Naresh Jain
Professor Kai Lai Chung’s contributions to probability theory have had a major influence on several areas of research in the subject. I will restrict my comments to some of his work in two areas, sums of independent random variables and the theory of Markov chains, which led to a significant amount of further work, including some of my own.
Sums of independent random variables
Kai Lai has made many outstanding contributions to this field, but
I would like to concentrate on his
1948
paper
[1].
If
In the i.i.d. case, two questions arose after Chung’s work. The
first one was raised by Chung himself: If
As to the first question, several papers appeared on the subject
getting close to the conditions stipulated by Chung. The question
was finally settled in the affirmative by
Jain and Pruitt
in 1975
[e12].
The probability distribution given in
Fristedt had already observed that an
analogue
of
Donsker and Varadhan
[e13]
approached these problems through their
large-deviations probability estimates for stable processes, and
obtained explicit expressions for the limit constants.
Jain
[e14]
was then able to show, through an invariance principle, that the
limit constant for the
The story by no means ends here. For a two-parameter Brownian
motion
Markov chains
It is difficult to imagine that anybody working in the area of Markov processes would not be familiar with Chung’s monograph, Markov Chains with Stationary Transition Probabilities [3]. This monograph deals with countable-state Markov chains in both discrete time (Part I) and continuous time (Part II). Much of Kai Lai’s fundamental work in the field is included in this monograph. My comments will be confined to Part I. Here, for the first time, Kai Lai gave a systematic exposition of the subject, which includes classification of states, ratio ergodic theorems, and limit theorems for functionals of the chain.
For a general state space, Doeblin had given a classification scheme
in a seminal paper
in 1937
[e1].
This and other work of Doeblin had
a major impact on the field, and led to further developments by
Chung
[2],
Doob
[e4],
Harris
[e5],
and Orey
[e6],
[e9].
In the early
1960s there were a number of basic ingredients of a general
state-space theory that would lead to an exact counterpart of Part I of
Chung
[3].
Much fundamental ground work, including positive
recurrence (the so-called Doeblin’s condition), was done by Doob
[e4].
Harris
[e5]
introduced his recurrence condition: There exists
a nonzero