Weak gravity conjecture

Modern physics
${\hat {H}}\|\psi _{n}(t)\rangle =i\hbar {\frac {\partial }{\partial t}}\|\psi _{n}(t)\rangle$ ${\frac {1}{{c}^{2}}}{\frac {{\partial }^{2}{\phi }_{n}}{{\partial t}^{2}}}-{{\nabla }^{2}{\phi }_{n}}+{\left({\frac {mc}{\hbar }}\right)}^{2}{\phi }_{n}=0$ Manifold dynamics: Schrödinger and Klein–Gordon equations
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The weak gravity conjecture (WGC) is a conjecture regarding the strength gravity can have in a theory of quantum gravity relative to the gauge forces in that theory. It roughly states that gravity should be the weakest force in any consistent theory of quantum gravity.^[1]

References

↑ "The string landscape, black holes and gravity as the weakest force", Nima Arkani-Hamed, Luboš Motl, Alberto Nicolis and Cumrun Vafa, published 15 June 2007, Journal of High Energy Physics, Volume 2007, JHEP06 (2007).

The fundamental interactions of physics
Physical forces	Strong interaction Fundamental Residual Electroweak interaction Weak interaction Electromagnetism Gravitation
Radiations	Electromagnetic radiation Gravitational radiation
Hypothetical forces	Quintessence Weak gravity conjecture
Glossary of physics Particle physics Philosophy of physics Universe Weakless Universe

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Weak gravity conjecture

See also

References