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		<summary type="html">&lt;p&gt;Phase N (01b): LaTeX restoration — promote Unicode display-math to &amp;lt;math&amp;gt;; lint-clean per tools/wiki_latex_lint.py&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;= Modified Einstein Equations with ψ =&lt;br /&gt;
&lt;br /&gt;
{{Audience_Sidebar&lt;br /&gt;
| difficulty   = Advanced&lt;br /&gt;
| reading_time = 18 minutes&lt;br /&gt;
| prerequisites = [[Psionics_Primer]]; [[Psionics]] §&amp;quot;Modified Einstein Equations&amp;quot;; [[5D_Action_Principle]]; tensor calculus; basic [[General_Relativity|GR]] including the Einstein equations and stress-energy.&lt;br /&gt;
| if_too_advanced_see = [[Why_Does_Physics_Need_Extra_Dimensions]]&lt;br /&gt;
| if_you_want_the_math_see = [[5D_Action_Principle]]&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
{{Notation&lt;br /&gt;
| psi_convention   = ψ = scalar field amplitude; Ψ = T&amp;lt;sup&amp;gt;00&amp;lt;/sup&amp;gt;(ψ) energy density.&lt;br /&gt;
| signature        = Mostly-plus (−,+,+,+).&lt;br /&gt;
| units            = ℏ = c = 1 unless explicitly noted; G is Newton&amp;#039;s constant.&lt;br /&gt;
| index_convention = Greek μ,ν,ρ over 4D spacetime; Latin i,j over spatial 3D.&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
The &amp;#039;&amp;#039;&amp;#039;modified Einstein equations with ψ&amp;#039;&amp;#039;&amp;#039; are the gravity-side equations of motion of the [[5D_Action_Principle|5D scalar-tensor theory]] after compactification — Einstein&amp;#039;s equations with the ψ field added as an additional source. This page derives them, gives the ψ stress-energy tensor in full, and works out the leading observational consequences.&lt;br /&gt;
&lt;br /&gt;
== Statement ==&lt;br /&gt;
&lt;br /&gt;
The 4D modified Einstein equations are:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;G_{\mu\nu} \equiv R_{\mu\nu} - \tfrac{1}{2} g_{\mu\nu} R = 8\pi G\,\bigl(T^{\text{matter}}_{\mu\nu} + T^{\text{EM}}_{\mu\nu} + T^\psi_{\mu\nu}\bigr)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
That is: standard Einstein equations with an extra source on the right-hand side coming from the ψ field. In the 5D parent theory, the corresponding equation reads:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\tilde{R}_{MN} - \tfrac{1}{2}\tilde{g}_{MN}\tilde{R} = T^\psi_{MN} + e^{k\psi}\,T^{\text{EM}}_{MN}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
with the &amp;lt;math&amp;gt;e^{k\psi}&amp;lt;/math&amp;gt; factor multiplying the EM stress-energy.&lt;br /&gt;
&lt;br /&gt;
== Derivation ==&lt;br /&gt;
&lt;br /&gt;
Vary the [[5D_Action_Principle|5D action]] with respect to &amp;lt;math&amp;gt;\tilde{g}^{MN}&amp;lt;/math&amp;gt;. The pieces of the action contributing to the variation are:&lt;br /&gt;
&lt;br /&gt;
# &amp;lt;math&amp;gt;\sqrt{-\tilde{g}}\,\tilde{R}/(16\pi \tilde{G})&amp;lt;/math&amp;gt; — gives the Einstein tensor &amp;lt;math&amp;gt;\tilde{G}_{MN}&amp;lt;/math&amp;gt;.&lt;br /&gt;
# &amp;lt;math&amp;gt;-\tfrac{1}{2}\tilde{g}^{MN}\partial_M\psi\,\partial_N\psi - \tfrac{1}{2} m^2\psi^2 - \tfrac{\lambda}{4}\psi^4&amp;lt;/math&amp;gt; — gives &amp;lt;math&amp;gt;T^\psi_{MN}&amp;lt;/math&amp;gt; on variation.&lt;br /&gt;
# &amp;lt;math&amp;gt;-\tfrac{1}{4} e^{k\psi}\,\tilde{F}_{MN}\tilde{F}^{MN}&amp;lt;/math&amp;gt; — gives the (&amp;lt;math&amp;gt;e^{k\psi}&amp;lt;/math&amp;gt;-weighted) EM stress-energy.&lt;br /&gt;
&lt;br /&gt;
Combining:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\tilde{G}_{MN} = 8\pi\tilde{G}\,\bigl(T^\psi_{MN} + e^{k\psi}\,T^{\text{EM}}_{MN}\bigr)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Dimensionally reducing via the [[Kaluza-Klein_Unification|Kaluza–Klein]] procedure (zero-mode approximation, &amp;lt;math&amp;gt;x^5&amp;lt;/math&amp;gt; compactified to a circle of radius &amp;lt;math&amp;gt;L&amp;lt;/math&amp;gt;) gives the 4D form:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;G_{\mu\nu} = 8\pi G\,\bigl(T^{\text{matter}}_{\mu\nu} + T^{\text{EM}}_{\mu\nu} + T^\psi_{\mu\nu}\bigr)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;G = \tilde{G}/(2\pi L)&amp;lt;/math&amp;gt;, and the &amp;lt;math&amp;gt;e^{k\psi}&amp;lt;/math&amp;gt; factor is absorbed into the effective EM coupling at leading order.&lt;br /&gt;
&lt;br /&gt;
== The ψ stress-energy tensor in full ==&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;T^\psi_{\mu\nu} = \partial_\mu\psi\,\partial_\nu\psi - g_{\mu\nu}\Bigl[\tfrac{1}{2}\partial^\rho\psi\,\partial_\rho\psi + \tfrac{1}{2} m^2\psi^2 + \tfrac{\lambda}{4}\psi^4\Bigr]&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Component breakdown:&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
! Component !! Expression !! Interpretation&lt;br /&gt;
|-&lt;br /&gt;
| &amp;lt;math&amp;gt;T^{00}_\psi&amp;lt;/math&amp;gt; || &amp;lt;math&amp;gt;\tfrac{1}{2}(\partial_t\psi)^2 + \tfrac{1}{2}(\nabla\psi)^2 + \tfrac{1}{2} m^2\psi^2 + \tfrac{\lambda}{4}\psi^4&amp;lt;/math&amp;gt; || Energy density &amp;lt;math&amp;gt;\Psi&amp;lt;/math&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| &amp;lt;math&amp;gt;T^{0i}_\psi&amp;lt;/math&amp;gt; || &amp;lt;math&amp;gt;(\partial_t\psi)(\partial^i\psi)&amp;lt;/math&amp;gt; || Energy flux &amp;lt;math&amp;gt;\mathbf{S}_\psi&amp;lt;/math&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| &amp;lt;math&amp;gt;T^{ij}_\psi&amp;lt;/math&amp;gt; || &amp;lt;math&amp;gt;(\partial^i\psi)(\partial^j\psi) - \delta^{ij}\bigl[\tfrac{1}{2}\partial^\rho\psi\,\partial_\rho\psi + \tfrac{1}{2} m^2\psi^2 + \tfrac{\lambda}{4}\psi^4\bigr]&amp;lt;/math&amp;gt; || Stress / pressure tensor&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
Trace:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;T^\psi \equiv g^{\mu\nu} T^\psi_{\mu\nu} = -\partial^\rho\psi\,\partial_\rho\psi - 2 m^2\psi^2 - \lambda\psi^4&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The trace is non-zero (the ψ field is not conformally invariant unless &amp;lt;math&amp;gt;m = \lambda = 0&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
== Conservation ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\nabla^\mu T^\psi_{\mu\nu} = 0&amp;lt;/math&amp;gt; follows from the ψ equation of motion (Bianchi identity). In the presence of external sources (&amp;lt;math&amp;gt;J_\psi \ne 0&amp;lt;/math&amp;gt; or &amp;lt;math&amp;gt;\alpha F^2 \ne 0&amp;lt;/math&amp;gt;), the divergence picks up exchange terms:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\nabla^\mu T^\psi_{\mu\nu} = \bigl(\alpha\,F_{\rho\sigma}F^{\rho\sigma} + J_\psi\bigr)\,\partial_\nu\psi&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Physically: ψ can exchange energy and momentum with the EM field (via the α coupling) and with the source current &amp;lt;math&amp;gt;J_\psi&amp;lt;/math&amp;gt; (biology, hardware). Total energy-momentum across all three sectors (matter + EM + ψ) is conserved exactly.&lt;br /&gt;
&lt;br /&gt;
== Linearised regime: GEM with ψ source ==&lt;br /&gt;
&lt;br /&gt;
In the weak-field limit &amp;lt;math&amp;gt;g_{\mu\nu} = \eta_{\mu\nu} + h_{\mu\nu}&amp;lt;/math&amp;gt; with &amp;lt;math&amp;gt;|h_{\mu\nu}| \ll 1&amp;lt;/math&amp;gt;, the modified Einstein equations linearise. Defining the trace-reversed perturbation &amp;lt;math&amp;gt;\bar{h}_{\mu\nu} = h_{\mu\nu} - \tfrac{1}{2}\eta_{\mu\nu} h&amp;lt;/math&amp;gt; and choosing the Lorenz gauge &amp;lt;math&amp;gt;\partial^\mu \bar{h}_{\mu\nu} = 0&amp;lt;/math&amp;gt;, we get&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\Box\,\bar{h}_{\mu\nu} = -\frac{16\pi G}{c^4}\,\bigl(T^{\text{matter}}_{\mu\nu} + T^{\text{EM}}_{\mu\nu} + T^\psi_{\mu\nu}\bigr)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The &amp;lt;math&amp;gt;\bar{h}_{00}&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\bar{h}_{0i}&amp;lt;/math&amp;gt; components define gravitoelectric and gravitomagnetic potentials &amp;lt;math&amp;gt;\Phi_g&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\mathbf{A}_g&amp;lt;/math&amp;gt;. See [[Gravitoelectromagnetism]] for the full decomposition.&lt;br /&gt;
&lt;br /&gt;
The new feature: a strong ψ gradient or oscillation contributes to the right-hand side and therefore to the GEM fields. In particular, a region with large &amp;lt;math&amp;gt;(\nabla\psi)^2&amp;lt;/math&amp;gt; acts as a positive mass-density source for &amp;lt;math&amp;gt;\Phi_g&amp;lt;/math&amp;gt;; a region with rapidly varying &amp;lt;math&amp;gt;\partial_t\psi&amp;lt;/math&amp;gt; contributes to &amp;lt;math&amp;gt;\mathbf{A}_g&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
This is the rigorous mathematical statement that &amp;#039;&amp;#039;&amp;#039;ψ can move physical objects&amp;#039;&amp;#039;&amp;#039;: a sustained ψ gradient generates a real gravitational field which couples to inertial mass. The magnitude is set by the ψ amplitude and by the empirically open coupling &amp;lt;math&amp;gt;G_\psi&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== Static spherically-symmetric solutions ==&lt;br /&gt;
&lt;br /&gt;
For a static spherically-symmetric ψ profile &amp;lt;math&amp;gt;\psi(r)&amp;lt;/math&amp;gt;, the modified Einstein equations admit a [[Schwarzschild_Metric|Schwarzschild]]-like exterior with corrections proportional to the ψ-field energy enclosed. The leading correction to the Newtonian potential &amp;lt;math&amp;gt;\Phi(r) = -GM/r&amp;lt;/math&amp;gt; is&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\Phi(r) = -\frac{GM}{r} - \frac{G}{r}\cdot 4\pi\!\int_0^r r&amp;#039;^{\,2}\,\Psi(r&amp;#039;)\,dr&amp;#039; + \dots&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
— i.e. the ψ-field energy adds to the effective mass-energy seen at large distance. This is one path by which a high-Ψ region behaves observationally like a small additional gravitating mass.&lt;br /&gt;
&lt;br /&gt;
The companion ψ-field equation in the same regime is the [[Yukawa_Potential|Yukawa]] equation derived in [[5D_Action_Principle]] §&amp;quot;Non-relativistic Yukawa&amp;quot;.&lt;br /&gt;
&lt;br /&gt;
== Coupling magnitudes ==&lt;br /&gt;
&lt;br /&gt;
The strength of ψ-induced gravity is set by G&amp;lt;sub&amp;gt;ψ&amp;lt;/sub&amp;gt; (the psionic coupling) and by typical values of Ψ. With Ψ ∼ 10&amp;lt;sup&amp;gt;−5&amp;lt;/sup&amp;gt; J/m&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; in a localised macro-PK region of volume ~1 m&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt;:&lt;br /&gt;
&lt;br /&gt;
* Effective added mass-energy ≈ 10&amp;lt;sup&amp;gt;−5&amp;lt;/sup&amp;gt; J ≈ 10&amp;lt;sup&amp;gt;−22&amp;lt;/sup&amp;gt; kg c&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&lt;br /&gt;
* Newtonian potential at 1 m ≈ 10&amp;lt;sup&amp;gt;−33&amp;lt;/sup&amp;gt; J/kg&lt;br /&gt;
* Acceleration on a 1 kg object at 1 m ≈ 10&amp;lt;sup&amp;gt;−33&amp;lt;/sup&amp;gt; m/s&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For ordinary Einstein-gravity coupling alone, this is undetectable. The framework&amp;#039;s actual macro-PK predictions require:&lt;br /&gt;
&lt;br /&gt;
* A boost from the e&amp;lt;sup&amp;gt;kψ&amp;lt;/sup&amp;gt; coupling on the EM sector — local EM-field reorganisation can do far more macroscopic work than the gravitational channel alone.&lt;br /&gt;
* Direct ψ-force on objects with non-zero psionic charge p, F&amp;lt;sub&amp;gt;ψ&amp;lt;/sub&amp;gt; = −p ∇ψ — this is the dominant macroscopic mechanism, see [[Psionics]] §&amp;quot;Telekinesis &amp;amp; Psychokinesis&amp;quot;.&lt;br /&gt;
&lt;br /&gt;
In other words, the modified Einstein equations alone do not give measurable everyday macro-PK; the macroscopic phenomena come from the p ∇ψ direct-force channel and from the ψ-mediated EM modulation, both consistent with the gravity-side equations being correctly tiny.&lt;br /&gt;
&lt;br /&gt;
== Cosmological implications ==&lt;br /&gt;
&lt;br /&gt;
A cosmological ψ background, ψ̄(t), with ψ̄ slowly evolving, contributes:&lt;br /&gt;
&lt;br /&gt;
* Effective dark-energy-like equation of state when (λ/4)ψ̄&amp;lt;sup&amp;gt;4&amp;lt;/sup&amp;gt; dominates: w ≈ +⅓ (radiation-like in this case).&lt;br /&gt;
* Quintessence-like behaviour for slowly-rolling massless ψ̄.&lt;br /&gt;
* Background Ψ &amp;quot;ψ-CMB&amp;quot; relic field; predicted to be slightly enhanced near concentrations of biological activity and at &amp;quot;sacred sites&amp;quot; (regions of sustained historical J&amp;lt;sub&amp;gt;ψ&amp;lt;/sub&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
These are speculative cosmological consequences — they are predictions, not data — but they sit inside standard cosmological-perturbation-theory machinery, so they are calculable rather than handwaved. See [[Open_Questions_in_Psionics]].&lt;br /&gt;
&lt;br /&gt;
== Sanity checks ==&lt;br /&gt;
&lt;br /&gt;
In line with [[Sanity_Check_Limits]] §7:&lt;br /&gt;
&lt;br /&gt;
* T&amp;lt;sub&amp;gt;μν&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;ψ&amp;lt;/sup&amp;gt; → 0 → standard Einstein equations recovered. ✓&lt;br /&gt;
* Weak-field, slow-motion → Newtonian gravity + small ψ correction. ✓&lt;br /&gt;
* Linearised, rotating mass → Lense–Thirring frame-dragging. ✓ ([[Gravity_Probe_B]] confirmed 2011.)&lt;br /&gt;
* Vacuum + ψ = 0 → Minkowski spacetime. ✓&lt;br /&gt;
* Constant ψ everywhere → cosmological-constant-like contribution Λ&amp;lt;sub&amp;gt;eff&amp;lt;/sub&amp;gt; = 8πG · ½m&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;ψ&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;. ✓&lt;br /&gt;
&lt;br /&gt;
== Cross-references ==&lt;br /&gt;
&lt;br /&gt;
* [[Psionics]] §&amp;quot;Modified Einstein Equations&amp;quot; — the equation as it appears in the canonical reference.&lt;br /&gt;
* [[5D_Action_Principle]] §&amp;quot;Term 1&amp;quot; — the Einstein–Hilbert piece in 5D.&lt;br /&gt;
* [[Gravitoelectromagnetism]] §10 — the GEM-decomposition source for the linearised limit.&lt;br /&gt;
* [[Lense-Thirring_Frame_Dragging]] — what (mass currents) produce on the geometry side.&lt;br /&gt;
* [[Gravity_Probe_B]] — experimental confirmation of the no-ψ limit.&lt;br /&gt;
* [[Sanity_Check_Limits]] §7, §10, §11 — recovery checks.&lt;br /&gt;
&lt;br /&gt;
== Experimental probes ==&lt;br /&gt;
&lt;br /&gt;
The modified Einstein equations make distinctive predictions that — in principle — distinguish the framework from pure GR:&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Anomalous extra mass-energy near regions of high biological / ritual coherence.&amp;#039;&amp;#039;&amp;#039; Would require ultra-precise local gravimetry (LaCoste &amp;amp; Romberg, atom interferometer); not yet a confirmed observation.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;ψ-EM cross-coupling enhancing the [[Gravitomagnetic_London_Moment|Tajmar 2007 anomaly]].&amp;#039;&amp;#039;&amp;#039; The 28-orders-of-magnitude excess gravitomagnetic field in rotating superconductors is consistent with a strong T&amp;lt;sub&amp;gt;μν&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;ψ&amp;lt;/sup&amp;gt; source localised in the Cooper-pair condensate.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Coupling to the [[Cooper_Pair_Mass_Anomaly|Tate 1989 Cooper-pair mass anomaly]]&amp;#039;&amp;#039;&amp;#039; (84 ppm excess) via the same channel.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Pais-effect-class devices&amp;#039;&amp;#039;&amp;#039; (NAWCAD 2015–2019 patents): high-frequency vibrating EM emitters generating local gravitational reaction via the α F&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; → T&amp;lt;sub&amp;gt;μν&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;ψ&amp;lt;/sup&amp;gt; → G&amp;lt;sub&amp;gt;μν&amp;lt;/sub&amp;gt; chain.&lt;br /&gt;
&lt;br /&gt;
See [[Falsification_Criteria_for_Psionics]] for a structured falsifier list.&lt;br /&gt;
&lt;br /&gt;
== See Also ==&lt;br /&gt;
&lt;br /&gt;
* [[Psionics]]&lt;br /&gt;
* [[5D_Action_Principle]]&lt;br /&gt;
* [[Gravitoelectromagnetism]]&lt;br /&gt;
* [[Lense-Thirring_Frame_Dragging]]&lt;br /&gt;
* [[Cooper_Pair_Mass_Anomaly]]&lt;br /&gt;
* [[Gravitomagnetic_London_Moment]]&lt;br /&gt;
* [[Pais_Effect]]&lt;br /&gt;
* [[Sanity_Check_Limits]]&lt;br /&gt;
* [[Symbol_Glossary]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
* Wald, R. M. (1984). &amp;#039;&amp;#039;General Relativity.&amp;#039;&amp;#039; University of Chicago Press.&lt;br /&gt;
* Mashhoon, B. (2003). &amp;quot;Gravitoelectromagnetism: A Brief Review.&amp;quot; arXiv:gr-qc/0311030.&lt;br /&gt;
* Ciufolini, I., Wheeler, J. A. (1995). &amp;#039;&amp;#039;Gravitation and Inertia.&amp;#039;&amp;#039; Princeton University Press.&lt;br /&gt;
* Tajmar, M., et al. (2007). &amp;quot;Experimental detection of the gravitomagnetic London moment.&amp;quot; arXiv:gr-qc/0603033.&lt;br /&gt;
* Everitt, C. W. F., et al. (2011). &amp;quot;Gravity Probe B: Final Results of a Space Experiment to Test General Relativity.&amp;quot; &amp;#039;&amp;#039;Physical Review Letters&amp;#039;&amp;#039; 106: 221101.&lt;br /&gt;
* Tate, J., Cabrera, B., Felch, S. B., Anderson, J. T. (1989). &amp;quot;Precise determination of the Cooper-pair mass.&amp;quot; &amp;#039;&amp;#039;Physical Review Letters&amp;#039;&amp;#039; 62: 845–848.&lt;br /&gt;
&lt;br /&gt;
[[Category:Psionics]]&lt;br /&gt;
[[Category:Equations]]&lt;br /&gt;
[[Category:Gravity]]&lt;/div&gt;</summary>
		<author><name>JonoThora</name></author>
	</entry>
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