As of January 23, 2019, the following corrections have been found:

p.9. In the paragraph after (2.15) ε>0 and ε<0 are exchanged. The text should read "... we choose ε>0 in the low-energy region and ε<0 in the high-energy region" and "we only choose ε>0 to be ..." (thanks to Arash Yunesi)

p.23, (3.9) and p.24 (3.10). The factors of λ do not include the fields, whose scaling depends on the dimension (thanks to Samuel Favrod)

p.27, (3.22). The coefficient
*C*_{2}^{(1)} should be
multiplied by a factor g^{2} for the equality to hold (thanks to Arash Yunesi)

p.29, (3.34). The coefficient
*C*_{2}^{(1)} should be
multiplied by a factor g^{2} (thanks to Marcel Balsiger)

p.35, second paragraph in 1.): the quark field must be denoted by
*ψ(x)* rather than *q _{μ}(x)* (thanks to Arash Yunesi)

p.35, (4.3) the right hand side should be colored in blue (thanks to Arash Yunesi)

p.41, (4.29) ξ should be colored blue (thanks to Marcel Balsiger)

p.42, line after (4.34): Δ^{⊥} must read
Δ^{⊥}_{μ} (thanks to Monika Hager)

p.46, (4.49). To be careful, one should write W(x) = [ x, x − ∞ n ] , instead of W(x) = [ x, − ∞ n ]. As long as the fields vanish at infinity (as they do in dim. reg.) the difference is irrelevant (thanks to Monika Hager)

p.46, (4.50) Replace *P* with *P̅* in the third
line to make it explicit that *W ^{†}* is anti path ordered (thanks to Arash Yunesi)

p.46, footnote 6. x = x' + s n should read x = x' − s n (thanks to Monika Hager)

p.47, (4.57). The ξ on the l.h.s. should be colored blue and
ξ should read ξ^{(0)} on the r.h.s in the first line (thanks to Marcel Balsiger)

p.58, Figure
5.1. *C*_{2}^{bare}(*Q*^{2}) must
read *C*_{V}^{bare}(*Q*^{2}) (thanks to Monika Hager)

p.76, after (6.46). The approximate equality *M ≃ s* must read *M ^{2} ≃ s* (thanks to Yaroslav Balytskyi)

p.97, before (7.7) missing word: differential cross *section* (thanks to Monika Hager)

p.98, (7.7). *f _{i/N1}* on the rhs must
read

p.100, last line of (7.14): δ(1-z_{2}) must read
δ(1-z_{1}) (thanks to Monika Hager)

p.134, (8.76). One should specify that *s _{Ij} = 2 σ_{Ij} p _{I} · p_{j}* .

p.164, (A.5): p_{⊥}^{2} must
read p_{⊥}^{μ} (thanks to Monika Hager)

p.168, (B.6): χ^{3}(x,y,k)= ... should read
χ(x,y,k)= ... (thanks to Monika Hager)

p.168, (B.9) must read V(x,y) = p^{2}y^{2} +
l^{2}(1-x)^{2} +2ply(1-x) = ... (thanks to Monika Hager)

p.173 (B.39) (-ν)^{α} should change to
(-ν^{2})^{α} (thanks to Arash Yunesi)

p.181 paragraph 2: "however, it the following discussion" should read "however, in the following discussion". (thanks to Arash Yunesi)

p.182 Delete extra word: "Next we will ~~to~~ prove" (thanks to Marcel Balsiger)

p.183, (D.8). The integration measure *ds* is missing (thanks to Monika Hager)

p.184, (D.14). The upper limit of right-most integral should read
*s _{n-1}* instead of

p.190, (E.7) first line: add superscript (0) on the right-most φ (thanks to Marcel Balsiger)

p.193, first sentence: "relating it to the evaluating" must read "relating it to the evaluation of" (thanks to Monika Hager)

p.194, after (G.6) "color or the quark" must read "color of the quark" (thanks to Monika Hager)

p.196, "the α→0 is finite," must read "the α→0 limit is finite," (thanks to Monika Hager)