What are the Feynman rules for the spinor-helicity formalism?

Question

If we do not work with helicity amplitudes, there are Feynman rules for the external legs of a Feynman diagram, i.e. $u_s(k),overline{v}_s(k),epsilon_r(k)$ for an incoming fermion, antifermion and gauge boson, respectively, and $overline{u}_s(k),v_s(k),epsilon^ast_r(k)$ for their outgoing pendants.
Are these correct rules for external states in the spinor-helicity formalism?

Particle & helicity
rule for incoming
rule for outgoing

L-fermion
$u_L(k)=k]$
$overline{u}_L(k)=langle k$

R-fermion
$u_R(k)=krangle$
$overline{u}_R(k)=[k$

L-antifermion
$overline{v}_L(k)=langle k$
$v_L(k)=k]$

R-antifermion
$overline{v}_R(k)=[k$
$v_R(k)=krangle$

(+)-gauge boson
$epsilon^mu_+(k,r)=-frac{1}{sqrt{2}}frac{[rgamma^mu krangle}{[rk]}$
$epsilon^{muast}_+(k,r)=frac{1}{sqrt{2}}frac{[kgamma^mu rrangle}{langle rkrangle}$

(-)-gauge boson
$epsilon^mu_-(k,r)=frac{1}{sqrt{2}}frac{[kgamma^mu rrangle}{langle rkrangle}$
$epsilon^{muast}_-(k,r)=-frac{1}{sqrt{2}}frac{[rgamma^mu krangle}{[rk]}$

Here, $r$ shall be an arbitrary reference momentum with $r^2=0,rkneq0$, and of course all fermions shall be massless.

Thomas Wening · Accepted Answer

The table I have given turns out to be wrong for the antifermions. As I have explained in this answer, a left-chiral antifermion $overline{v}_L=(v_R)^daggergamma_0$ is described by the Dirac-conjugate of a right-chiral Dirac-spinor $v_R$. That means, $v_R(k)=k]leftrightarrowoverline{v}_L(k)=[k$ and conversely $v_L(k)=krangleleftrightarrowoverline{v}_R(k)=langle k$.
All this can now be put into a neat table.

Particle & helicity
rule for incoming
rule for outgoing

L-fermion
$u_L(k)=k]$
$overline{u}_L(k)=langle k$

R-fermion
$u_R(k)=krangle$
$overline{u}_R(k)=[k$

L-antifermion
$overline{v}_L(k)=[k$
$v_L(k)=krangle$

R-antifermion
$overline{v}_R(k)=langle k$
$v_R(k)=k]$

(+)-gauge boson
$epsilon^mu_+(k,r)=-frac{1}{sqrt{2}}frac{[rgamma^mu krangle}{[rk]}$
$epsilon^{muast}_+(k,r)=frac{1}{sqrt{2}}frac{[kgamma^mu rrangle}{langle rkrangle}$

(-)-gauge boson
$epsilon^mu_-(k,r)=frac{1}{sqrt{2}}frac{[kgamma^mu rrangle}{langle rkrangle}$
$epsilon^{muast}_-(k,r)=-frac{1}{sqrt{2}}frac{[rgamma^mu krangle}{[rk]}$

What are the Feynman rules for the spinor-helicity formalism?

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Particle & helicity	rule for incoming	rule for outgoing
L-fermion	$u_L(k)=k]$	$overline{u}_L(k)=langle k$
R-fermion	$u_R(k)=krangle$	$overline{u}_R(k)=[k$
L-antifermion	$overline{v}_L(k)=langle k$	$v_L(k)=k]$
R-antifermion	$overline{v}_R(k)=[k$	$v_R(k)=krangle$
(+)-gauge boson	$epsilon^mu_+(k,r)=-frac{1}{sqrt{2}}frac{[rgamma^mu krangle}{[rk]}$	$epsilon^{muast}_+(k,r)=frac{1}{sqrt{2}}frac{[kgamma^mu rrangle}{langle rkrangle}$
(-)-gauge boson	$epsilon^mu_-(k,r)=frac{1}{sqrt{2}}frac{[kgamma^mu rrangle}{langle rkrangle}$	$epsilon^{muast}_-(k,r)=-frac{1}{sqrt{2}}frac{[rgamma^mu krangle}{[rk]}$