Chapter 2 |
Standard convention is to use the complex
conjugate of the polarisation vector in Eq.(2.12) and in the
discussion that follows, because the gluon is outgoing. |
Oleh Fedkevych |
Chapter 2 |
The notation used in Eqs. (2.12), (2.13),
(2.14), and (2.15)
for the colour matrices is
wrong as they cannot be freely moved across the Dirac spinor. |
one of us |
Chapter 2 |
Eq.(2.18) should have in the integral measure (2
π)4 rather than (2 π) d | .
Oleh Fedkevych |
Chapter 2 |
Eq.(2.20) should have the inverse of the right-hand side. |
Oleh Fedkevych |
Chapter 2 |
After the first equal sign in Eq.(2.24) there
should be no minus sign. |
one of us |
Chapter 4 |
Eq.(4.6) has two typos: the upper limit of the
ω integration should be Q/2 and there is a factor of 2
missing in the mass Θ-function. |
Oleh Fedkevych |
Chapter 4 |
The third Θ-function in Eq.(4.5) should be Θ(ρi<ρ). |
Oleh Fedkevych |
Chapter 4 |
The integration variables in the second line of Eq.(4.16) should be z and ρ'. |
Oleh Fedkevych |
Chapter 4 |
The last Θ-function in Eq.(4.38) should be Θ(θ24<1). |
Prasanna Dhani |
Chapter 4 |
Eq.(4.47) and (4.48) should have an overall minus sign. |
one of us |
Chapter 5 |
In Eq.(5.12), the azimuthal component of the distance should be φi-φjet. |
Oleh Fedkevych |
Chapter 5 |
The RHS of Eq.(5.19) and (5.20) should have a superscript (β). |
Oleh Fedkevych |
Chapter 6 |
The Θ-function in Eq.(6.4) should be
Θ(z> ...). |
Prasanna Dhani |
Chapter 7 |
The caption of Fig.7.5 should read: "ROC curves for quark/gluon separation using ECFs (solid lines) and angularities (dashed lines).". |
Oleh Fedkevych |
Chapter 9 |
The colour factor in Eq.(9.12) is already
included in the splitting function. |
one of us |