M THEORY ACTION
S_{\text{M-Theory}} = \int d^{11}x \, \sqrt{-g} \left( -\frac{1}{2\kappa^2} R + \frac{1}{12} F_{\mu\nu\rho\sigma} F^{\mu\nu\rho\sigma} \right) - \frac{1}{6} \int d^{11}x \, \epsilon^{\mu_1 \dots \mu_{11}} C_{\mu_1 \mu_2 \mu_3} F_{\mu_4 \dots \mu_7} F_{\mu_8 \dots \mu_{11}} + \mathcal{L}_{\text{M2}} + \mathcal{L}_{\text{M5}}
11D SURGA ACTION
S_{\text{SUGRA}} = \frac{1}{2 \kappa^2} \int d^{11}x \, \sqrt{-g} \left( R - \frac{1}{48} F_{\mu\nu\rho\sigma} F^{\mu\nu\rho\sigma} \right) - \frac{1}{6} \int d^{11}x \, \epsilon^{\mu_1 \dots \mu_{11}} C_{\mu_1 \mu_2 \mu_3} F_{\mu_4 \dots \mu_7} F_{\mu_8 \dots \mu_{11}} + \text{fermionic terms}
SUPERSTRINGS ACTION
S_{\text{Superstrings}} = \int d^2 \sigma \left( -\frac{1}{2} \sqrt{-h} h^{ab} \partial_a X^\mu \partial_b X^\nu g_{\mu\nu} - i \bar{\psi} \gamma^a \partial_a \psi \right)
MSSM ACTION
S_{\text{MSSM}} = \int d^4x \left( \mathcal{L}_{\text{SM}} + \sum_{\text{superpartners}} \left( \bar{\psi} i \gamma^\mu D_\mu \psi - \frac{1}{4} F_{\mu\nu} F^{\mu\nu} \right) + \mathcal{L}_{\text{Yukawa}} + \mathcal{L}_{\text{Higgs}} \right)
SUSY ACTION
S_{\text{SUSY}} = \int d^4x \left( \bar{\psi} \gamma^\mu D_\mu \psi + \frac{1}{2} F_{\mu\nu} F^{\mu\nu} + \text{superpotential terms} \right)
CDT ACTION
S_{\text{CDT}} = \sum_{\Delta_2} \left( \frac{1}{2 \kappa^2} \text{Vol}(\Delta_2) R(\Delta_2) \right) - \sum_{\Delta_3} \text{Vol}(\Delta_3)
M + SURGA + MSSM + CDT
S_{\text{Total}} = \int d^{11}x \, \sqrt{-g} \left( -\frac{1}{2\kappa^2} R + \frac{1}{12} F_{\mu\nu\rho\sigma} F^{\mu\nu\rho\sigma} \right) - \frac{1}{6} \int d^{11}x \, \epsilon^{\mu_1 \dots \mu_{11}} C_{\mu_1 \mu_2 \mu_3} F_{\mu_4 \dots \mu_7} F_{\mu_8 \dots \mu_{11}}
+ \frac{1}{2 \kappa^2} \int d^{11}x \, \sqrt{-g} \left( R - \frac{1}{48} F_{\mu\nu\rho\sigma} F^{\mu\nu\rho\sigma} \right) + \text{fermionic terms}
+ \int d^2 \sigma \left( -\frac{1}{2} \sqrt{-h} h^{ab} \partial_a X^\mu \partial_b X^\nu g_{\mu\nu} - i \bar{\psi} \gamma^a \partial_a \psi \right)
+ \int d^4x \left( \mathcal{L}_{\text{SM}} + \sum_{\text{superpartners}} \left( \bar{\psi} i \gamma^\mu D_\mu \psi - \frac{1}{4} F_{\mu\nu} F^{\mu\nu} \right) + \mathcal{L}_{\text{Yukawa}} + \mathcal{L}_{\text{Higgs}} \right)
+ \int d^4x \left( \bar{\psi} \gamma^\mu D_\mu \psi + \frac{1}{2} F_{\mu\nu} F^{\mu\nu} + \text{superpotential terms} \right)
+ \sum_{\Delta_2} \left( \frac{1}{2 \kappa^2} \text{Vol}(\Delta_2) R(\Delta_2) \right) - \sum_{\Delta_3} \text{Vol}(\Delta_3)
FRACTON LAGRANGIAN
\mathcal{L}_{\text{Fracton}} = \overline{\Psi}_f \left( i \gamma^\mu D_\mu - m_f - \frac{S_b}{2} \Phi_{\text{string}} \right) \Psi_f - \frac{1}{4} F_{\mu\nu} F^{\mu\nu} - \frac{\lambda}{2} \left( \nabla^2 \Phi_{\text{string}} \right)^2
BOREON LAGRANGIAN
\mathcal{L}_{\text{Boreon}} = \frac{1}{2} (\partial_\mu \Phi_B)(\partial^\mu \Phi_B) - \frac{1}{2} m_B^2 \Phi_B^2 - \frac{\lambda_B}{4} \Phi_B^4 + g_B \Phi_B \overline{\Psi} \gamma^\mu \Psi
Mashtakov Metric
A = \frac{1}{1 + \alpha_B \Phi_B^2} \left( 1 + \frac{g_B \Phi_B}{M} \right)
AURORA LAGRANGIAN
\mathcal{L}_{\text{Aurora}} = \frac{1}{2} (\partial_\mu \Phi_A)(\partial^\mu \Phi_A) - \frac{1}{2} m_A^2 \Phi_A^2 - \frac{\kappa}{4} \Phi_A^4 - \xi \Phi_A^2 \Phi_B^2 + \lambda_S S_A^2
AXION LAGRANGIAN
GRAVITON FULL LAGRANGIAN
\mathcal{L}_{\text{Graviton}} = -\frac{1}{2} h^{\mu\nu} \mathcal{E}_{\mu\nu}^{\alpha\beta} h_{\alpha\beta} + \frac{\lambda}{2} \left( \partial_\lambda h_{\mu\nu} \partial^\lambda h^{\mu\nu} - \partial_\lambda h \partial^\lambda h \right) + \frac{\xi}{2} \Phi_p^2 h_{\mu\nu} h^{\mu\nu} + \lambda_S S_G^2
DUAL GRAVITON
\mathcal{L}_{\text{Dual-Graviton}} = \lambda_D (h_{\mu\nu} h^{\mu\nu})^2
GRAVITINO LAGRANGIAN
\mathcal{L}_{\text{Gravitino}} = \bar{\psi}_\mu \left( i \gamma^{\mu\nu\lambda} \partial_\lambda - m \gamma^{\mu\nu} \right) \psi_\nu + \frac{1}{2} \kappa \, \bar{\psi}_\mu \gamma^{\mu\nu} \psi_\nu h_{\alpha\beta} + \frac{\lambda_S}{2} S_G^2 \, \bar{\psi}_\mu \gamma^\mu \psi^\mu + \mathcal{L}_{\text{int}}^{\text{dim}}
POTENTIAL INTERACTIONS
The potential interaction between the Fracton and Boreon fields, including the reduced interdimensional coupling constant \Phi_k:
\mathcal{L}_{\text{Fracton-Boreon}} = K_{\text{FB}} \cdot \bar{\psi}_{\mu\nu} \varphi \psi^{\mu\nu} + M \cdot \partial^\mu \varphi \partial_\mu \psi
DUAL GRAVITON INTERACTION WITH MATTER FIELDS
\mathcal{L}_{\text{Dual Graviton Interaction}} = \frac{1}{2} \left( h_{\mu \nu} h^{\mu \nu} \right) \left( \bar{\psi}_\mu h^{\mu \nu} \psi_\nu \right) + \Phi_{11}(h_{\mu \nu}, h_{\rho \sigma})
COMBINED LAGRANGIAN FOR TOPOLOGICAL ENTANGLEMENT
\mathcal{L}_{\text{entanglement}} = \mathcal{L}_{\text{Fracton}} + \mathcal{L}_{\text{Boreon}} + \frac{k}{4\pi} \epsilon^{\mu\nu\alpha} A_{\mu} \partial_\nu \varphi \partial_\alpha \bar{\psi} + g \cdot \bar{\psi} \gamma^\mu (\partial_\mu \varphi) \psi + \xi \cdot |\nabla \varphi|^2 + \lambda \cdot \varphi^4
TOPOLOGICAL ENTANGLEMENT WITHIN BRIDGES
V_{\text{total}} = \sum_{i=1}^{N_B} V_{\text{wormhole}, i} - \beta \sum_{i=1}^{N_B} \sum_{j > i}^{N_B} \left( E_B^{(i)} \cdot E_B^{(j)} \right) \cdot \Phi_{ij} - \gamma \sum_{i=1}^{N_B} \lambda_i \left( \frac{1}{r_{\text{throat}, i}} \right)^{2}
LAGRANGIAN FOR AXION-GRAVITON-GRAVITINO AKA "GRAVIOLI" INTERACTION WITH WORMHOLE POTENTIAL
\mathcal{L}_{\text{Gravioli}} = \frac{1}{2} (\partial_\mu \varphi)(\partial^\mu \varphi) - \frac{1}{2} m_\varphi^2 \varphi^2 - g_{\varphi h} \varphi \, h^{\mu\nu} R_{\mu\nu} - g_{\varphi \psi} \varphi \, \bar{\psi_\mu} \gamma^\mu \psi_\nu - \left( \alpha_1 \varphi^2 R + \alpha_2 (\bar{\psi_\mu} \gamma^\mu \psi_\nu) h^{\mu\nu} + \alpha_3 \varphi^4 - \alpha_4 \frac{1}{M_{\text{Pl}}^2} (\bar{\psi_\mu} \gamma^\mu \psi_\nu)^2 \right)
WORMHOLE POTENTIAL
V_{\text{wormhole}}(\varphi, h_{\mu\nu}, \psi_\mu, g_{AB}) = \alpha_1 \varphi^2 R_4 + \alpha_2 (\bar{\psi}_A \Gamma^A \psi_B) h^{AB} + \alpha_3 \varphi^4 + \alpha_5 \, \frac{1}{M_{\text{Pl}}^2} (\bar{\psi}_A \Gamma^A \psi_B)^2 + \alpha_6 \, R_5
5D CYLINDRICAL WORMHOLE METRIC
ds^2 = - c^2 dt^2 + d\rho^2 + r^2(\rho) \, d\Omega_3^2 + \lambda^2(\rho) \, d\psi^2
TRAVERSABILITY OF WORMHOLE
The equation for throat radius stability is: \frac{d^2r(\rho)}{d\rho^2} + 4 \frac{r(\rho)}{\lambda(\rho)} \frac{d\lambda(\rho)}{d\rho} = 0
The effective gravitational force on a 3D object passing through the wormhole is: F_{\text{effective}} = - \frac{d}{d\rho} \left( r(\rho) \right) + \frac{\lambda(\rho)}{r(\rho)^2}
BRIDGE STABILITY LAGRANGIAN
\mathcal{L} = \int d^5x \left( -\frac{1}{2} \left( \partial_\mu h_{\nu \rho} \partial^\mu h^{\nu \rho} - \frac{1}{2} \partial_\mu h \partial^\mu h \right) + \frac{i}{2} \left( \bar{\psi}_\mu \gamma^\mu D_\nu \psi^\nu - \bar{\psi}_\nu \gamma^\mu D^\nu \psi_\mu \right) + \frac{1}{2} \left( \partial_\mu \phi_F \partial^\mu \phi_F - m_F^2 \phi_F^2 \right) + \frac{1}{2} \left( \partial_\mu \phi_A \partial^\mu \phi_A - m_A^2 \phi_A^2 \right) + g_{\text{FA}} \phi_F \phi_A + g_{\text{GrF}} h_{\mu \nu} \partial^\mu \phi_F \partial^\nu \phi_F + \frac{1}{2} \epsilon^{\mu \nu \rho \sigma \tau} \partial_\mu A_\nu \partial_\rho B_{\sigma \tau} \right)
BRIDGE EVAPORATION
\frac{dM_{\text{Bridge}}}{dt} = -\alpha \frac{\hbar c^2}{G} \frac{\Delta D}{r_{\text{Horizon}}^2} \exp\left(-\frac{\Phi_k}{k_B T}\right)
BRIDGE CONFIGURATION
\mathcal{S}_{\text{Bridge}} = \int d^5x \sqrt{-g} \left[ \frac{1}{2} R - \Lambda - \frac{1}{2} \left(\alpha_F |\nabla \phi_F|^2 + \alpha_B |\nabla \phi_B|^2 \right) + \beta \sum_{n} \frac{|\phi_{F,n}|^2}{\left(1 + r^2 \right)^{n}} + \gamma \epsilon^{\mu \nu \rho \sigma \tau} \partial_\mu A_\nu \partial_\rho B_{\sigma \tau} + \delta_{FB} \phi_F \phi_B + \eta_{GG} h_{\mu \nu} h^{\mu \nu} + \zeta \mathcal{A}_{\text{Boreon}} \right]
BRIDGE STABILITY SAFEGUARD
\mathcal{L}_{\text{Stability}} = \lambda_{\text{GF}} \bar{\psi}_\mu \gamma^\mu \Psi
AURORA-BOREALIS ASYMPTOTIC SAFETY
\mathcal{L}_{\text{Aurora-Boreon}} = g_{\text{AB}} \phi_B \partial_\mu \phi_A + \lambda_{\text{AB}} \phi_A \phi_B^2
V_{\text{total}}(d) = \frac{1}{d^\beta} - \frac{1}{d^\gamma}, \quad \gamma > \beta
GENERAL ACTION OF ADS DRIVE DYNAMICS
S = \int d\tau \, \mathcal{L}_{\text{AdS}}(x^\mu, \dot{x}^\mu, \phi, g_{\mu\nu}, \epsilon, E)
LAGRANGIAN FOR ADS DRIVE DYNAMICS
\mathcal{L}_{\text{AdS}} = \frac{1}{2} m \left( g_{\mu\nu} \dot{x}^\mu \dot{x}^\nu - 1 \right) - \epsilon \, g_{\mu\nu} \, \phi \, F(\dot{x}^\mu, \partial_\mu \phi) + \frac{\alpha}{2} \dot{x}^\mu \frac{d}{d\tau} \dot{x}_\mu - \frac{\beta}{r^2 + \gamma} + \mathcal{L}_{\text{AdS Transition}}
EQUATION OF MOTION (ADS)
\frac{d}{d\tau} \left( \frac{\partial \mathcal{L}_{\text{AdS}}}{\partial \dot{x}^\mu} \right) - \frac{\partial \mathcal{L}_{\text{AdS}}}{\partial x^\mu} = 0
EQUATION OF TRANSITION (ADS)
t_{\text{transition}} = \frac{2d}{\sqrt{\frac{2P}{m}} + \sqrt{\frac{2Q}{m}}}
ADS STRESS BUILD-UP
\tau = S_0 + \kappa_1 \,\epsilon\,\tau + \kappa_2 \,\epsilon^2\,\tau^2 - \delta\,e^{-\lambda\,\tau}
ENERGY CONSUMPTION
E(\tau) = E_0 + \eta\,\epsilon\,\tau + \zeta\,\epsilon^2\,\tau^2
SUBSPACE PROJECTION FROM 4D TO 3D
V_{3D} = P_{4 \to 3} \cdot V_{4D}
V_{4D} = \begin{bmatrix} x \\ y \\ z \\ w \end{bmatrix}, \quad V_{3D} = \begin{bmatrix} x' \\ y' \\ z' \end{bmatrix}
P_{4 \to 3} = \begin{bmatrix} 1 & 0 & 0 & a \\ 0 & 1 & 0 & b \\ 0 & 0 & 1 & c \end{bmatrix}
SUBSPACE SET OF VECTORS
M = [v_1 \quad v_2 \quad \dots \quad v_k] \in \mathbb{R}^{n \times k}
Conditions:
\forall \alpha, \beta \in \mathbb{R}, \quad \alpha v_1 + \beta v_2 \in V
ANTI DE SITTER
g_{\mu\nu}^{(AdS)} = \eta_{\mu\nu} + h_{\mu\nu}
DE SITTER
g_{\mu\nu}^{(dS)} = \eta_{\mu\nu} - h_{\mu\nu}
CHRISTOFFEL SYMBOLS
\Gamma^\rho_{\mu\nu} = \frac{1}{2} g^{\rho\sigma} \left( \partial_\mu g_{\nu\sigma} + \partial_\nu g_{\mu\sigma} - \partial_\sigma g_{\mu\nu} \right)
NON-ZERO CHRISTOFFEL SYMBOL DERIVATION (KERR)
ds^2 = -\Bigl(1 - \frac{2 G M r}{\Sigma c^2}\Bigr) c^2 dt^2 - \frac{4 G M a r \sin^2\theta}{\Sigma c}\,dt\,d\phi + \frac{\Sigma}{\Delta}\,dr^2 + \Sigma\, d\theta^2 + \Bigl(r^2 + \frac{a^2 G^2}{c^4} + \frac{2 G M a^2 r \sin^2\theta}{\Sigma c^2}\Bigr)\sin^2\theta\,d\phi^2
\Sigma = r^2 + \frac{a^2 G^2}{c^4}\cos^2\theta, \quad \Delta = r^2 - \frac{2 G M r}{c^2} + \frac{a^2 G^2}{c^4}.
GEODESIC EQUATION
\frac{d^2 x^\rho}{d\tau^2} + \Gamma^\rho_{\mu\nu} \frac{dx^\mu}{d\tau} \frac{dx^\nu}{d\tau} = 0
EXAMPLE OF SIX DIMENSIONAL DE SITTER MATRICE EMBEDDING CURVATURE
g_{\mu\nu}^{(6D)} = \begin{bmatrix} -1 & 0 & 0 & 0 & 0 & \epsilon \\ 0 & 1 & 0 & 0 & \epsilon & 0 \\ 0 & 0 & 1 & \delta & 0 & 0 \\ 0 & 0 & \delta & 1 & 0 & 0 \\ 0 & \epsilon & 0 & 0 & 1 & 0 \\ \epsilon & 0 & 0 & 0 & 0 & 1 \end{bmatrix}
Tensorial Pressure & Anti-de Sitter Tensors
T^{\mu\nu}_{AdS} = \frac{\partial \mathcal{L}}{\partial (\partial_\mu \phi)} \partial^\nu \phi - g^{\mu\nu} \mathcal{L}
Electroweak Leakage Representation
\Psi_{Bino}(x,t) = A \cdot e^{-(\gamma + i\omega)t} \cdot \psi(x)
(AdS) Energy Requirement per Dimension:
E_d = E_3 \cdot k^{(d - 3)} \quad \text{with } k \in [2, 5]
(AdS) Estimated Travel Time Scaling:
T_d = \frac{T_3}{(d - 2)^{1.5}}
(AdS) Symmetry Preservation Function:
S_d = \begin{cases} 1 & \text{if } d \leq 4 \\\\ e^{-(d - 4)} & \text{if } d > 4 \end{cases}
GALACTIC NUMERICAL SYSTEM
\text{S}_r = \text{hex}\left( \left\lfloor \frac{r}{R_{\text{max}}} \times 0xFFFF \right\rfloor \right), \quad
\text{S}_\theta = \text{hex}\left( \left\lfloor \frac{\theta}{360^\circ} \times 0xFFFF \right\rfloor \right), \quad
\text{S}_\phi = \text{hex}\left( \left\lfloor \frac{\phi + \phi_{\text{offset}}}{\Phi_{\text{max}}} \times 0xFFFF \right\rfloor \right)
LIBRARY'S BERKENSTEIN BOUND
I_{\text{max}} \leq \frac{D R^\prime E^\prime}{\hbar c \ln 2},
GRAVITATIONAL WELL
G ⅁(r) = 1 - \frac{2G}{c^2 r} \left( M_c + \int_0^r 4\pi r'^2 \left( \rho_{g0} e^{-\beta r'} + \rho_{q}(r') \right) \, dr' \right) - \int_0^r \frac{G \left( \rho_{g0} e^{-\beta r'} + \rho_{q}(r') \right)}{r'^2} e^{-\alpha r'} \, dr' - \frac{k_B Φ_k}{\lambda_s^2} \int_0^r ρ_s(r') 4\pi r'^2 \, dr'.
ANGELIC METAL RESONANCE
\mathcal{R}_{\text{AM}} = \lambda_\text{res} \int d^4 x \left( \bar{\psi}_\mu h^{\mu \nu} \right))
\mathcal{L}_{\text{res}}^{(5D)} = \alpha \left( \bar{\psi}_{\mu} \gamma^{\nu} \psi^{\mu} \right) \left( h_{\mu\nu}^{(5D)} h^{\mu\nu(5D)} \right)
\ce{^{{314}}_{{126}}{AM}\ }
\ce{^{{318}}_{{126}}\text{AM}\ }
\ce{^{{325}}_{{140}}\text{AM}^{+}\ }
\ce{^{{314}}_{{126}}\text{AM}^{+}\ }
\ce{^{{314}}_{{126}}\text{AM}^{-}\ }
\ce{^{{318}}_{{126}}\text{AM} + \tilde{\gamma} -> \text{AM}^* + \phi_b + E_{\text{burst}} + \tilde{\gamma}_{\text{secondary}}}
\ce{\text{AM}^* \rightarrow \text{AM} + \phi_b + E_{\text{burst}} + \tilde{\gamma}_{\text{secondary}} + \tilde{e}^-}
\ce{ \tilde{e}^- \xrightarrow{\text{Absorption}} E_{\text{usable}} }
\ce{E_{\text{reaction}} = \phi_b + E_{\text{burst}}}
\ce{E_{\text{SSR}} = 500 \, \text{MeV/reaction}}