1.3. The Equal-Mass Point-Particle Approximation
Bob: Let us first look at the history. I presume you know how star
cluster modeling got started. You have seen more of it than I have.
Alice: When it all got started, I had barely arrived on this planet, and
I wasn't reading the Astrophysical Journal yet, or anything else for
that matter. But yes, I know the rough history. It took some 25 to
35 years to understand the dynamical evolution of a star cluster,
modeled as a collection of equal-mass point particles, depending on
how you count, since the earliest N-body calculations were performed
on modern computers, around 1960. But you know the details better
than I do. I guess it is your turn to do some summarizing.
Bob: During the sixties, simulations by Aarseth, Wielen, and others
showed how three-body interactions form the dynamical engine at the
heart of an N-body system, the agents of change in their evolution.
Even if no binary stars were present initially, they would be formed
dynamically in simultaneous three-body encounters. And once there,
encounters between these binaries and single stars would complicate
the normally weak heat flow mediated by two-body relaxation: a single
scattering encounter can suddenly release a large amount of energy
when a binary increases its internal binding energy by a significant
amount.
During the seventies, Henon and Spitzer and co-workers used
approximate Monte Carlo Fokker-Planck simulations to model the
contraction of the core of a star cluster, on a time scale that is
only an order of magnitude larger than that of the half-mass
relaxation time scale. This so-called gravothermal catastrophe was
predicted in the sixties, and actually observed by Henon in
rudimentary form in the sixties as well. But it was seen much more
clearly in the seventies in statistical simulations. While more
difficult to observe in actual N-body calculations, because of the
still low number of particles, a few hundred at most, they were seen
there as well. In fact, one could even argue that in the late
sixties, some N-body simulations already showed hints of this effect.
In the eighties, finally the behavior of an equal-mass point particle
system after core collapse was elucidated, first by Sugimoto and
Bettwieser, who showed that a post-collapse cluster can undergo
so-called gravothermal oscillations, a series of local mini collapses
and expansions in the very center of a star cluster.
Alice: And then Goodman gave a detailed stability analysis in which he
predicted the minimal N value for which an equal-mass N-body system
would show such behavior. At that point, theoretically the equal-mass
evolution was well understood, wouldn't you say?
Bob: I only consider something understood if it comes out of my
simulations, in a repeatable and robust way. I have seen too many
semi-analytic predictions come and go in my young life to have too
much trust in those!
Alice: What Goodman did was finding roots in the complex plane of
relatively straightforward and certainly well defined equations; I
wouldn't call that semi-analytic, and I certainly would trust the
complex plane a lot more than the complexities of any complicated
simulation.
Bob: I guess we're talking about matters of taste here, though many
would think this an odd thing to say about `hard' science. But moving
right along, let me make my main point.
It would be another decade before the predictions would be tested in
simulations. In the late eighties, various simulations based on
Fokker-Planck approximations as well as gas models verified what
Sugimoto and Bettwieser had seen in the early eighties, and in the mid
nineties saw the first observation of gravothermal oscillations in a
real N-body simulation, by Makino. In a way, this was the end of a
chapter in stellar dynamics, and further progress had to come from
more realistic systems.
Alice: But surely people had used a mass spectrum long before that.
Bob: Yes, in fact the very first paper by Aarseth already described a
multi-mass simulation, in the early sixties. But it was only in the
seventies that more detailed studies elucidated the main physical
mechanisms of mass segregation.
By the way, the field of stellar dynamics owes a lot to the inspiration
provided by Sverre Aarseth. For the last several decades he has
shared his codes with anyone interested, operating in an `open source'
mode long before the term was invented. Not only that, with his
constant readiness to help anyone interested in using his code, he has
set the tone for collaboration for at least two generations of stellar
dynamicists. I believe that the attitude toward collaboration is more
prevalent in stellar dynamics than in most areas in astrophysics, and
as such this simple fact may be Sverre's single-handed accomplishment.