We solve a nonequilibrium statistical-mechanics problem exactly, namely, the single-file dynamics of
N hard-core interacting particles (the particles cannot pass each other) of size

diffusing in a one-dimensional system of finite length
L with reflecting boundaries at the ends. We obtain an exact expression for the conditional probability density function

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(
y![[script T]](http://scitation.aip.org/servlet/GetImg?key=PLEEE8000080000005051103000001%3A0%3A0%3A28)
,
t|
y![[script T],0](http://scitation.aip.org/servlet/GetImg?key=PLEEE8000080000005051103000001%3A0%3A1%3A28)
) that a tagged particle
![[script T]](http://scitation.aip.org/servlet/GetImg?key=PLEEE8000080000005051103000001%3A0%3A2%3A28)
(
![[script T]](http://scitation.aip.org/servlet/GetImg?key=PLEEE8000080000005051103000001%3A0%3A2%3A28)
=1,…,
N) is at position
y![[script T]](http://scitation.aip.org/servlet/GetImg?key=PLEEE8000080000005051103000001%3A0%3A0%3A28)
at time
t given that it at time
t=0 was at position
y![[script T],0](http://scitation.aip.org/servlet/GetImg?key=PLEEE8000080000005051103000001%3A0%3A1%3A28)
. Using a Bethe ansatz we obtain the
N-particle probability density function and, by integrating out the coordinates (and averaging over initial positions) of all particles but particle
![[script T]](http://scitation.aip.org/servlet/GetImg?key=PLEEE8000080000005051103000001%3A0%3A2%3A28)
, we arrive at an exact expression for

![[script T]](http://scitation.aip.org/servlet/GetImg?key=PLEEE8000080000005051103000001%3A0%3A0%3A28)
(
y![[script T]](http://scitation.aip.org/servlet/GetImg?key=PLEEE8000080000005051103000001%3A0%3A0%3A28)
,
t|
y![[script T],0](http://scitation.aip.org/servlet/GetImg?key=PLEEE8000080000005051103000001%3A0%3A1%3A28)
) in terms of Jacobi polynomials or hypergeometric functions. Going beyond previous studies, we consider the asymptotic limit of large
N, maintaining
L finite, using a nonstandard asymptotic technique. We derive an exact expression for

![[script T]](http://scitation.aip.org/servlet/GetImg?key=PLEEE8000080000005051103000001%3A0%3A0%3A28)
(
y![[script T]](http://scitation.aip.org/servlet/GetImg?key=PLEEE8000080000005051103000001%3A0%3A0%3A28)
,
t|
y![[script T],0](http://scitation.aip.org/servlet/GetImg?key=PLEEE8000080000005051103000001%3A0%3A1%3A28)
) for a tagged particle located roughly in the middle of the system, from which we find that there are three time regimes of interest for finite-sized systems: (A) for times much smaller than the collision time
t

coll=1/(
2D), where

=
N/
L is the particle concentration and
D is the diffusion constant for each particle, the tagged particle undergoes a normal diffusion; (B) for times much larger than the collision time
t

coll but times smaller than the equilibrium time
t

eq=
L2/
D, we find a single-file regime where

![[script T]](http://scitation.aip.org/servlet/GetImg?key=PLEEE8000080000005051103000001%3A0%3A0%3A28)
(
y![[script T]](http://scitation.aip.org/servlet/GetImg?key=PLEEE8000080000005051103000001%3A0%3A0%3A28)
,
t|
y![[script T],0](http://scitation.aip.org/servlet/GetImg?key=PLEEE8000080000005051103000001%3A0%3A1%3A28)
) is a Gaussian with a mean-square displacement scaling as
t1/2; and (C) for times longer than the equilibrium time
t

eq,

![[script T]](http://scitation.aip.org/servlet/GetImg?key=PLEEE8000080000005051103000001%3A0%3A0%3A28)
(
y![[script T]](http://scitation.aip.org/servlet/GetImg?key=PLEEE8000080000005051103000001%3A0%3A0%3A28)
,
t|
y![[script T],0](http://scitation.aip.org/servlet/GetImg?key=PLEEE8000080000005051103000001%3A0%3A1%3A28)
) approaches a polynomial-type equilibrium probability density function. Notably, only regimes (A) and (B) are found in the previously considered infinite systems.