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)

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Weak gravity conjecture

See also

References