Addressing Gravity (G) as Coupling with (Electro-)(Magno-) Coupling Planck's Constant (hc) via Boltzmann's Constant Squared (kB^2)
ORAL
Abstract
Theoretical and computational physics have struggled where Gravity (G) does not so far flow from the quantum theory equations using Planck's constant (hc).
In this presentation, that linkage is mapped as classical coupling (before quantitization). Specifically, (G) and (hc) are linked as the square of (kB) when properly scaled via either a) the fine structure as (re/a0)^1/2)^(3/2) or DFT Local Density Adjustment (r)^(4/3). Using inverse, interactive logic of ((3/2G)(3/2hc)=(kB)^2 as (ab=k^2), then SI constant become linked and useful in equations.
So, the coupling path is electric (epsilon0) versus magno- (mu0) leads to (c) in (hc) by 1/distance-square versus 1/distance-cubed base equations.
Second, two fourth quantum number (electron duopoles transpositioning as causation for QED) states for phyiscs-spin generate the chain events leads to hyperbolic (e^x+(1/e^x)) and (e^x-(1/e^x)) two paths which as a separate coupling to create the experimental observation of (e^x). This leads to fine structure coupling for (electro-) as (hc*alpha) and (magno-) as (hc/alpha), so coupled (hc).
Importantly here and finally, as the shells and subshell equilibrium, the secondary coupling of potential (acceleration) versus momentum (velocity) where acceleration balance for static equations, but maximums at derivatives fields (dx=0, x=?) have need a third coupling. That is (hc) is . . . after the (G) base level of derivative, so we need equations accounting for that base level.
All current quantum equations currently present as (hc), but that should have the existing (G) coupling for any action beyond zero Kelvin static equilibrium. This leads to a new understand of the non-equilibrium states in the path of de Broglie-Bohm as a history wave.
So, the result is quantum point-equations segments understood as three layers of coupling to create an integration of (G) and (hc) as Boltzmann's squared. Note taht must get scaled to (re/a0)^(V/W) where fine is V=1, W=2, and LDA is (V=3, W=4) and so on. This does not cover the dimensioned adjustment to equation segments covered in separate lectures.
In this presentation, that linkage is mapped as classical coupling (before quantitization). Specifically, (G) and (hc) are linked as the square of (kB) when properly scaled via either a) the fine structure as (re/a0)^1/2)^(3/2) or DFT Local Density Adjustment (r)^(4/3). Using inverse, interactive logic of ((3/2G)(3/2hc)=(kB)^2 as (ab=k^2), then SI constant become linked and useful in equations.
So, the coupling path is electric (epsilon0) versus magno- (mu0) leads to (c) in (hc) by 1/distance-square versus 1/distance-cubed base equations.
Second, two fourth quantum number (electron duopoles transpositioning as causation for QED) states for phyiscs-spin generate the chain events leads to hyperbolic (e^x+(1/e^x)) and (e^x-(1/e^x)) two paths which as a separate coupling to create the experimental observation of (e^x). This leads to fine structure coupling for (electro-) as (hc*alpha) and (magno-) as (hc/alpha), so coupled (hc).
Importantly here and finally, as the shells and subshell equilibrium, the secondary coupling of potential (acceleration) versus momentum (velocity) where acceleration balance for static equations, but maximums at derivatives fields (dx=0, x=?) have need a third coupling. That is (hc) is . . . after the (G) base level of derivative, so we need equations accounting for that base level.
All current quantum equations currently present as (hc), but that should have the existing (G) coupling for any action beyond zero Kelvin static equilibrium. This leads to a new understand of the non-equilibrium states in the path of de Broglie-Bohm as a history wave.
So, the result is quantum point-equations segments understood as three layers of coupling to create an integration of (G) and (hc) as Boltzmann's squared. Note taht must get scaled to (re/a0)^(V/W) where fine is V=1, W=2, and LDA is (V=3, W=4) and so on. This does not cover the dimensioned adjustment to equation segments covered in separate lectures.
*No funding was used for this research.
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Publication: Preprint: Teaching HemiChem Coupling Constants
Presenters
-
Arno Vigen
- Independent Researcher