John A. Venables

*Cambridge University Press (2000)*

I had in mind that supervisors might not thank me for increasing their bill for copying and interlibrary loan, and students might also find that having got the papers they couldn't understand them. However, for completeness these references are given here for those who want to follow them up. They are Volmer & Weber (1926), Stranski & Krastanov (1938) and Frank & van der Merwe (1949). The first two of these papers are in German; the spelling of Dr K varies, since there is no unique transliteration of the cyrillic alphabet.

My own view is that quoting such papers just to show erudition is rather annoying, especially if one hasn't actually read them, which remains as a suspicion in the mind on reading some papers...

In this same section a point of confusion, primarily in the original (2000) printing,
has been noted by some students about the relation between a) the statement on page 146
starting "When we deposit material A on B, we get layer growth if
γ_{A} < γ_{B} + γ*, where γ* is the interface energy,
and vice versa for island growth", and b) the illustrations of figure 5.3(a) and (b) on page 147.
This confusion has been removed in the text of the 2006 printing; but the confusion was, and to a
certain extent still is, sufficiently messy for me to wish to hide it on a
separate page.

New references for section 5.1

In section 5.2.4 on page 154, a pre-exponential is referred to as
η(Z,i), and this quantity is illustrated for certain cases in figure
5.6 on page 155. Perhaps because the text is rather compressed, there may be some confusion
as to how this quantity should be used, though it is explicit in the review paper
of Venables *et al.* (1984, equation 2.15, page 411). This compression is a
consequence of the section * not* being a review paper; you may need the
relevant information from reviews and original papers in order to do full justice to
problems 5.1 and 5.2 on pages 181-2.

If you go back to page 153, you will see the statement: n_{x} ~ R^{p} multiplied
by an Arrhenius (exponential) term. However, this equation is not fully written out, and the term
in R doesn't have the same dimensions as n_{x}. The full equation, with n_{x}
in ML units and R in (ML/s), is

n_{x}=η(Z,i).(R/ν)^{p}.exp(E/kT),

where ν is a frequency factor, most obviously at low temperature the
diffusion frequency ν_{d} given in chapter 1, equation 1.16
on page 16. However, one can see on that same page that at higher temperatures, when
re-evaporation is involved in the equations, the pre-exponential may well contain
ν_{a}, in addition or instead, as might be deduced from table 5.1 on page 154.

My conclusion is given at the end of section 5.2.4 on page 155, namely that it is relatively
straightforward to check the energies E and power laws p in table 5.1, but that keeping track of
the pre-exponential terms requires patience and cross checks with the original literature. Even
that statement really underestimates the level of "scientific noise" in the system; there are
many papers which I *haven't* quoted in the book, simply because I didn't want to carry
on an ongoing, and possibly contentious, discussion of work in progress, minor differences of
interpretation, etc. Although resolution of such issues is important in principle, it can
rapidly send all but the most committed either to sleep or off to the nearest available bar.

In section 5.2.5 on page 156, figure 5.7(b) has the dotted and full lines reversed- the dotted lines correspond to the rate equation and the full lines to the KMC simulations.

New references for section 5.2

New references for section 5.3

New references for section 5.4

New references for section 5.5

In problem 5.2 on page 182, part c) is incorrectly stated. It should read:

By considering the boundary condition at the edge of the cluster, show that the concentration
*n*_{1}(*r*) = *R*τ(1-K_{0}(*X*)/K_{0}(*X _{k}*)),
where the argument of the Bessel function

*Note*: in part d) which follows, the case *r* = *r _{k}* results
in equation (5.12a) for σ

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