Expanding Man

that shape is my shade, there where I used to stand

Z=∫Dg Dψ DA DΦ exp⁡{i∫d4x−g[mp22R−14FμνaFaμν+iψˉi∇ψi+(ψˉiLVijΦψjR+h.c.)−∣∇Φ∣2−V(Φ)]} \mathcal{Z}= \int \mathcal{D}g~\mathcal{D}\psi~\mathcal{D}A~\mathcal{D}\Phi~\exp\left\{ i\int d^{4}x\sqrt{-g}\left[ \frac{m_{p}^{2}}{2}R - \frac{1}{4}F^{a}_{\mu\nu}F^{\mu\nu}_{a} + i\bar{\psi}_{i}\cancel{\nabla}\psi_{i} + \left(\bar{\psi}_{i}^{L}V_{ij}\Phi\psi_{j}^{R} + \textrm{h.c.}\right) - |\nabla\Phi|^{2} - V(\Phi) \right]\right\}

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by ExpandingMan. Last modified: May 01, 2024. Website built with Franklin.jl and the Julia programming language.