Corrections to QSoC
Dear reader,
please email typos and other errors you find,
for inclusion here
and future reprinting.
Thanks!
PS file
(for those who want to copy and paste)
- page 29: Replace time-dependent by
time-independent
- page 30: First line of equation (2.11.9)

- page 84: Third line above (4.13.6) should read
|k|, n ≥ 1. Thus ...
-
page 85: Extend (4.13.13) by fourth member

-
page 99: Delete ship in second line below (4.14.25).
Extend (4.14.24) by third member

-
page 118: Replace (-1) n
by (-1) n +1
on rhs of last equation in exercise 4.13
-
page 149: In second line below (6.5.2), the vector should read

-
page 200: Insert 0 in (6.15.6),
... 0 for λ → 0
-
page 228: Replace reserved
by reversed in fifth line
of figure caption
-
page 233: Replace int by ∫
in first line of (7.4.19)
-
page 293: Insert sentence after
... window Δn. in first
line after (8.6.2)
Note that non-periodic orbits were excluded by setting
x=x0 ,
with appeal to the asymptotic independence of x in both members
of (8.6.1).
-
page 299: The sentence after equation (8.7.15) must read
That trace may obviously be interpreted as an
integrated return probability.
-
page 306: In second line after (8.9.11) replace
only for maps
by for maps, only
(note that only after that permutation of words the sentence begins to make sense)
-
page 315: In first line insert
not quite in front of the same
-
page 316: Replace (-1)n
by (-1)n+1
in both instances in (8.11.2)
as well as in the formula two lines below (8.11.2)
-
page 317: The last two lines must be replaced with
and
as phase-space fractions is approximated by
superimposing two
independent ladders of levels, one Poissonian and the other
Wignerian,
in the way explained in Sect. 5.6. The resulting
spacing distribution reads, for
,
-
page 318: The first line must be cancelled and equation (8.12.1) replaced with

-
page 320: The second sentence must read
In contrast to the Frobenius-Perron operator, however, the Q propagator may be
an Nq2
×Nq2
matrix, where Nq2
=Ω/hf
is the number of Planck cells contained
in the classical accessible phase-space volume;
note that Weyl's law fixes Nq as the
effective number of components of the wave function.
-
page 320: Replace
N<<Nq
by N<<Nq2
in ninth line
-
page 330: equation (9.3.6)

-
page 365: Replace tridiagonalizing by
triangularizing in first line and similarly
in the fourth line below (9.10.19)
-
page 417: In first line below (10.6.1) write
instead of 
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