Gerenuk on Nostr: **How spinors square to 1** Spinors can be mapped to their bilinear covariants ...
**How spinors square to 1**
Spinors can be mapped to their bilinear covariants
\[\begin{aligned}
\Omega_1&=\psi^\dagger\gamma_0\psi\\J^\mu&=\psi^\dagger\gamma_0\gamma^\mu\psi\\
S^{\mu\nu}&=\psi^\dagger \gamma_0 i \gamma^{\mu\nu}\psi\\
K^\mu&=\psi^\dagger \gamma_0 u \gamma^{0123}\gamma_\mu\psi\\
\Omega_2&=\psi^\dagger \gamma_0 \gamma^{0123}\psi
\end{aligned}\]
These covariants can be collected into multivectors of the Clifford algebra Cl(1,3) (Lounesto Ch 10.5)
The spinor can be recovered from the covariants uniquely up to a complex phase (Lounesto Ch 11.2)
Since the spinor had only 8 parameters, but the covariants have 16 all together, the covariants satisfy some identities known as Fierz identities (in Clifford algebra)
\[\begin{aligned}
J^2&=\Omega_1^2+\Omega_2^2\\
&=-K^2\\
J\cdot K&=0\\
J\wedge K&=-(\Omega_2+\Omega_1\gamma_{0123})S
\end{aligned}\]
But what is surprising now and what I haven't seen in any other source is, that these identities are (almost) exactly what you need for a general element from the Clifford algebra to square to a real number:\[\begin{aligned}
A&=\Omega_1+J+S+I K+I\Omega_2\\
A^2&\in\mathbb{R}
\end{aligned}
\]
Therefore there is a 1-to-1 correspondence between spinors and multivectors (or equally real 4x4 matrices) squaring to a real number.
Has anyone seen that discussed somewhere?
There is a small difference in one sign and the Fierz identities with this choice covers only one type of element squaring to 1, but elements squaring to 1 thus describe the Fierz identities more generally.
Published at
2025-02-01 08:13:37 UTCEvent JSON
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"content": "**How spinors square to 1**\n\nSpinors can be mapped to their bilinear covariants\n\\[\\begin{aligned}\n\\Omega_1\u0026=\\psi^\\dagger\\gamma_0\\psi\\\\J^\\mu\u0026=\\psi^\\dagger\\gamma_0\\gamma^\\mu\\psi\\\\\nS^{\\mu\\nu}\u0026=\\psi^\\dagger \\gamma_0 i \\gamma^{\\mu\\nu}\\psi\\\\\nK^\\mu\u0026=\\psi^\\dagger \\gamma_0 u \\gamma^{0123}\\gamma_\\mu\\psi\\\\\n\\Omega_2\u0026=\\psi^\\dagger \\gamma_0 \\gamma^{0123}\\psi\n\\end{aligned}\\]\nThese covariants can be collected into multivectors of the Clifford algebra Cl(1,3) (Lounesto Ch 10.5)\n\nThe spinor can be recovered from the covariants uniquely up to a complex phase (Lounesto Ch 11.2)\n\nSince the spinor had only 8 parameters, but the covariants have 16 all together, the covariants satisfy some identities known as Fierz identities (in Clifford algebra)\n\\[\\begin{aligned}\nJ^2\u0026=\\Omega_1^2+\\Omega_2^2\\\\\n\u0026=-K^2\\\\\nJ\\cdot K\u0026=0\\\\\nJ\\wedge K\u0026=-(\\Omega_2+\\Omega_1\\gamma_{0123})S\n\\end{aligned}\\] \n\nBut what is surprising now and what I haven't seen in any other source is, that these identities are (almost) exactly what you need for a general element from the Clifford algebra to square to a real number:\\[\\begin{aligned}\nA\u0026=\\Omega_1+J+S+I K+I\\Omega_2\\\\\nA^2\u0026\\in\\mathbb{R}\n\\end{aligned}\n\\]\n\nTherefore there is a 1-to-1 correspondence between spinors and multivectors (or equally real 4x4 matrices) squaring to a real number.\nHas anyone seen that discussed somewhere?\n\nThere is a small difference in one sign and the Fierz identities with this choice covers only one type of element squaring to 1, but elements squaring to 1 thus describe the Fierz identities more generally.",
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