# Kinematics of Scattering Amplitudes in $\left(2, 2\right)$ Signature within the Amplituhedron

I am just working my way through the concepts of Amplituhedron and often stumble across the phrase

[...] in $$\left(2,2\right)$$ signature $$\lambda$$, $$\tilde{\lambda}$$ are real and independent [...]

in various references (Jaroslav Trnka, 2014; page 7, Nima Arkani-Hamed, 2014; page 24 or Livia Ferro, 2020; page 3). What I don't quite understand is the following: If we take the following momentum four-vector: $$$$p_\mu = \begin{pmatrix} -1, 0, 1, 0 \\ \end{pmatrix} ,$$$$ and contract this with the Pauli Matrices in $$\left(2, 2\right)$$ signature (I am very sorry that I may not use the right terminology here), we obtain the following matrix: $$$$P_{\alpha\dot{\alpha}} =\frac{1}{2} \begin{pmatrix} p_0 + p_3, p_1 - p_2 \\ p_1 + p_2, p_0 - p_3 \\ \end{pmatrix} = \begin{pmatrix} -\frac{1}{2}, -\frac{1}{2} \\ \frac{1}{2}, -\frac{1}{2} \\ \end{pmatrix} .$$$$

However, unlike in $$\left(3, 1\right)$$ signature, the determinant of the matrix is not $$0$$, but $$\frac{1}{2}$$.

In all the YouTube videos and references I found, this $$\left(2, 2\right)$$ signature is never properly explained or referenced. Do you have any sources about the signature that can help me identify my mistakes or that can help me understand this concept better?

• Minor comment to the post (v2): In the future please link to abstract pages rather than pdf files. Aug 3, 2021 at 12:50

1. There is bijective isometry from the split-signature space $$(\mathbb{R}^{2,2},||⋅||^2)$$ to the space of $$2\times 2$$ real matrices $$({\rm Mat}_{2\times 2}(\mathbb{R}),\det(⋅))$$, where \begin{align} ||p||^2~=~&(p^0)^2-(p^1)^2+(p^2)^2-(p^3)^2~=~\det(P), \cr p~=~&(p^0,p^1,p^2,p^3)~\in~\mathbb{R}^{2,2},\cr P~=~&\sum_{\mu=0}^3p^{\mu}\sigma_{\mu}~\in~ {\rm span}_{\mathbb{R}}\{ \sigma_0,\sigma_1,i\sigma_2,\sigma_3\} ~=~{\rm Mat}_{2\times 2}(\mathbb{R}).\end{align}
2. There is a bilinear map $$\mathbb{R}^2\times \mathbb{R}^2~\ni~(\lambda,\tilde{\lambda})\quad\mapsto\quad P~:=~\lambda\tilde{\lambda}^T~\in~ {\rm Mat}_{2\times 2} (\mathbb{R}),$$ from 2 Weyl spinors $$\lambda,\tilde{\lambda}$$ to a rank-1 operator $$P$$, which necessarily has vanishing determinant, i.e. the corresponding momentum is light-like/null.