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 timedependent by
timeindependent
 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 nonperiodic orbits were excluded by setting
x=x_{0} ,
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 phasespace 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 FrobeniusPerron operator, however, the Q propagator may be
an N_{q}^{2}
×N_{q}^{2}
matrix, where N_{q}^{2}
=Ω/h^{f}
is the number of Planck cells contained
in the classical accessible phasespace volume;
note that Weyl's law fixes N_{q} as the
effective number of components of the wave function.

page 320: Replace
N<<N_{q}
by N<<N_{q}2
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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