Binary flow hypothesis
Dual Energy Universe: A Speculative Model with Falsifiable Predictions
Author's note: The mathematical formulation proposed in this hypothesis has not been duly reviewed by experts in the field. Any conclusion drawn from the reading of this work must be thoroughly contrasted.
1. Simple universe: electron + positron
Schrödinger's equation for two bodies
Reduced mass:
μ
=
m
e
2
μ
=
m
e
2
mu=(m_(e))/(2) \mu = \frac{m_e}{2} μ = m e 2
i
ℏ
∂
Ψ
(
r
,
t
)
∂
t
=
[
−
ℏ
2
2
μ
∇
2
−
e
2
4
π
ϵ
0
r
]
Ψ
(
r
,
t
)
i
ℏ
∂
Ψ
(
r
,
t
)
∂
t
=
−
ℏ
2
2
μ
∇
2
−
e
2
4
π
ϵ
0
r
Ψ
(
r
,
t
)
iℏ(del Psi(r,t))/(del t)=[-(ℏ^(2))/(2mu)grad^(2)-(e^(2))/(4piepsilon_(0)r)]Psi(r,t) i\hbar \frac{\partial \Psi(\mathbf{r}, t)}{\partial t} = \left[ -\frac{\hbar^2}{2\mu} \nabla^2 - \frac{e^2}{4\pi \epsilon_0 r} \right] \Psi(\mathbf{r}, t) i ℏ ∂ Ψ ( r , t ) ∂ t = [ − ℏ 2 2 μ ∇ 2 − e 2 4 π ϵ 0 r ] Ψ ( r , t )
Bound States: Positronium
E
n
=
−
μ
e
4
2
(
4
π
ϵ
0
)
2
ℏ
2
⋅
1
n
2
=
−
6.8
eV
n
2
E
n
=
−
μ
e
4
2
(
4
π
ϵ
0
)
2
ℏ
2
⋅
1
n
2
=
−
6.8
eV
n
2
E_(n)=-(mue^(4))/(2(4piepsilon_(0))^(2)ℏ^(2))*(1)/(n^(2))=-(6.8"eV")/(n^(2)) E_n = -\frac{\mu e^4}{2(4\pi\epsilon_0)^2 \hbar^2} \cdot \frac{1}{n^2} = -\frac{6.8 \, \text{eV}}{n^2} E n = − μ e 4 2 ( 4 π ϵ 0 ) 2 ℏ 2 ⋅ 1 n 2 = − 6.8 eV n 2
Duration
Para-positronium (singlet,
):
τ
≈
1.25
×
10
−
10
s
τ
≈
1.25
×
10
−
10
s
tau~~1.25 xx10^(-10)"s" \tau \approx 1.25 \times 10^{-10} \, \text{s} τ ≈ 1.25 × 10 − 10 s
Ortho-positronium (triplet,
):
τ
≈
1.42
×
10
−
7
s
τ
≈
1.42
×
10
−
7
s
tau~~1.42 xx10^(-7)"s" \tau \approx 1.42 \times 10^{-7} \, \text{s} τ ≈ 1.42 × 10 − 7 s
Annihilation Energy
E
annihilation
=
2
m
e
c
2
=
1.022
MeV
E
annihilation
=
2
m
e
c
2
=
1.022
MeV
E_("annihilation")=2m_(e)c^(2)=1.022"MeV" E_{\text{annihilation}} = 2 m_e c^2 = 1.022 \, \text{MeV} E annihilation = 2 m e c 2 = 1.022 MeV
2. Simple universe: photon + "antiphoton"
The photon is its own antiparticle → two identical photons.
They do not interact linearly (Maxwell is linear in vacuum).
In QED, weak interaction via Euler-Heisenberg:
L
EH
∼
α
2
90
m
e
4
[
(
F
μ
ν
F
μ
ν
)
2
+
7
4
(
F
μ
ν
F
~
μ
ν
)
2
]
L
EH
∼
α
2
90
m
e
4
(
F
μ
ν
F
μ
ν
)
2
+
7
4
(
F
μ
ν
F
~
μ
ν
)
2
L_("EH")∼(alpha^(2))/(90m_(e)^(4))[(F_(mu nu)F^(mu nu))^(2)+(7)/(4)(F_(mu nu) tilde(F)^(mu nu))^(2)] \mathcal{L}_{\text{EH}} \sim \frac{\alpha^2}{90 m_e^4} \left[ (F_{\mu\nu}F^{\mu\nu})^2 + \frac{7}{4} (F_{\mu\nu}\tilde{F}^{\mu\nu})^2 \right] L EH ∼ α 2 90 m e 4 [ ( F μ ν F μ ν ) 2 + 7 4 ( F μ ν F ~ μ ν ) 2 ]
Duration : infinite (photons do not decay).
If
E
C
M
>
2
m
e
c
2
=
1.022
MeV
E
C
M
>
2
m
e
c
2
=
1.022
MeV
E_(CM) > 2m_(e)c^(2)=1.022"MeV" E_{CM} > 2m_e c^2 = 1.022 \, \text{MeV} E C M > 2 m e c 2 = 1.022 MeV
, can create a pair
e
−
e
+
e
−
e
+
e^(-)e^(+) e^- e^+ e − e +
and then they are annihilated.
3. Dual matter-antimatter universe with black/white hole
3.1 Refined model: bidirectional black/white hole
A single object connects
and
:
Black hole on one side, white hole on the other.
Bidirectional.
Hawking radiation is the leftover from matter-antimatter annihilation in the center of the throat.
3.2 Net Flow
Φ
=
E
γ
τ
transit
=
h
ν
τ
Φ
=
E
γ
τ
transit
=
h
ν
τ
Phi=(E_( gamma))/(tau_("transit"))=(h nu)/(tau) \Phi = \frac{E_\gamma}{\tau_{\text{transit}}} = \frac{h \nu}{\tau} Φ = E γ τ transit = h ν τ
Φ
net
=
Φ
M
→
A
−
Φ
A
→
M
Φ
net
=
Φ
M
→
A
−
Φ
A
→
M
Phi_("net")=Phi_(M rarr A)-Phi_(A rarr M) \Phi_{\text{net}} = \Phi_{M \to A} - \Phi_{A \to M} Φ net = Φ M → A − Φ A → M
Φ
effective
=
(
1
−
η
)
⋅
|
Φ
net
|
Φ
effective
=
(
1
−
η
)
⋅
|
Φ
net
|
Phi_("effective")=(1-eta)*|Phi_("net")| \Phi_{\text{effective}} = (1 - \eta) \cdot |\Phi_{\text{net}}| Φ effective = ( 1 − η ) ⋅ | Φ net |
3.3 Differential equations
d
E
M
d
t
=
−
Φ
M
→
A
+
Φ
A
→
M
−
E
Hawking
2
d
E
M
d
t
=
−
Φ
M
→
A
+
Φ
A
→
M
−
E
Hawking
2
(dE_(M))/(dt)=-Phi_(M rarr A)+Phi_(A rarr M)-(E_("Hawking"))/(2) \frac{dE_M}{dt} = -\Phi_{M \to A} + \Phi_{A \to M} - \frac{E_{\text{Hawking}}}{2} d E M d t = − Φ M → A + Φ A → M − E Hawking 2
d
E
A
d
t
=
−
Φ
A
→
M
+
Φ
M
→
A
−
E
Hawking
2
d
E
A
d
t
=
−
Φ
A
→
M
+
Φ
M
→
A
−
E
Hawking
2
(dE_(A))/(dt)=-Phi_(A rarr M)+Phi_(M rarr A)-(E_("Hawking"))/(2) \frac{dE_A}{dt} = -\Phi_{A \to M} + \Phi_{M \to A} - \frac{E_{\text{Hawking}}}{2} d E A d t = − Φ A → M + Φ M → A − E Hawking 2
Where
E
Hawking
=
η
(
Φ
M
→
A
+
Φ
A
→
M
)
E
Hawking
=
η
(
Φ
M
→
A
+
Φ
A
→
M
)
E_("Hawking")=eta(Phi_(M rarr A)+Phi_(A rarr M)) E_{\text{Hawking}} = \eta (\Phi_{M \to A} + \Phi_{A \to M}) E Hawking = η ( Φ M → A + Φ A → M )
Total energy loss:
d
E
total
d
t
=
−
E
Hawking
=
−
η
(
Φ
M
→
A
+
Φ
A
→
M
)
d
E
total
d
t
=
−
E
Hawking
=
−
η
(
Φ
M
→
A
+
Φ
A
→
M
)
(dE_("total"))/(dt)=-E_("Hawking")=-eta(Phi_(M rarr A)+Phi_(A rarr M)) \frac{dE_{\text{total}}}{dt} = -E_{\text{Hawking}} = -\eta (\Phi_{M \to A} + \Phi_{A \to M}) d E total d t = − E Hawking = − η ( Φ M → A + Φ A → M )
3.4 Characteristic times
Equilibrium Time:
t
balance
≈
E
0
⋅
τ
transit
2
h
ν
(
1
−
η
/
2
)
t
balance
≈
E
0
⋅
τ
transit
2
h
ν
(
1
−
η
/
2
)
t_("balance")~~(E_(0)*tau_("transit"))/(2h nu(1-eta//2)) t_{\text{balance}} \approx \frac{E_0 \cdot \tau_{\text{transit}}}{2 h \nu (1 - \eta/2)} t balance ≈ E 0 ⋅ τ transit 2 h ν ( 1 − η / 2 )
Evaporation Time:
t
death
≈
E
0
⋅
τ
transit
η
⋅
h
ν
t
death
≈
E
0
⋅
τ
transit
η
⋅
h
ν
t_("death")~~(E_(0)*tau_("transit"))/(eta*h nu) t_{\text{death}} \approx \frac{E_0 \cdot \tau_{\text{transit}}}{\eta \cdot h \nu} t death ≈ E 0 ⋅ τ transit η ⋅ h ν
Frequency of Transit:
f
transit
=
1
τ
transit
≈
c
3
4
G
M
BH
f
transit
=
1
τ
transit
≈
c
3
4
G
M
BH
f_("transit")=(1)/(tau_("transit"))~~(c^(3))/(4GM_("BH")) f_{\text{transit}} = \frac{1}{\tau_{\text{transit}}} \approx \frac{c^3}{4 G M_{\text{BH}}} f transit = 1 τ transit ≈ c 3 4 G M BH
Frequency of Hawking radiation (annihilation):
ν
Hawking
=
2
m
c
2
h
ν
Hawking
=
2
m
c
2
h
nu_("Hawking")=(2mc^(2))/(h) \nu_{\text{Hawking}} = \frac{2 m c^2}{h} ν Hawking = 2 m c 2 h
4. Exotic matter and photonic dark matter
4.1 Exotic matter to stabilize the throat
Condition: violate the Null Energy Condition (NEC) :
ρ
+
p
<
0
ρ
+
p
<
0
rho+p < 0 \rho + p < 0 ρ + p < 0
Options: Phantom Scalar Field, Casimir Energy, Negative Cosmic Strings.
4.2 Photons with collective mass
Invariant mass of a system of
Photons:
M
2
c
4
=
(
∑
i
E
i
)
2
−
|
∑
i
p
i
c
|
2
M
2
c
4
=
∑
i
E
i
2
−
∑
i
p
i
c
2
M^(2)c^(4)=(sum _(i)E_(i))^(2)-|sum _(i)p_(i)c|^(2) M^2 c^4 = \left( \sum_i E_i \right)^2 - \left| \sum_i \mathbf{p}_i c \right|^2 M 2 c 4 = ( ∑ i E i ) 2 − | ∑ i p i c | 2
If
∑
p
i
≈
0
∑
p
i
≈
0
sump_(i)~~0 \sum \mathbf{p}_i \approx 0 ∑ p i ≈ 0
(Isotropic directions):
M
system
≈
E
total
c
2
≠
0
M
system
≈
E
total
c
2
≠
0
M_("system")~~(E_("total"))/(c^(2))!=0 M_{\text{system}} \approx \frac{E_{\text{total}}}{c^2} \neq 0 M system ≈ E total c 2 ≠ 0
Proposal : Dark matter is clouds of photons confined in swirls with zero net momentum.
There is only energy
. Everything emerges from its flow.
5.1 Maxwell-type equations
Electromagnetism
Dual energy model
Electric Charge
q
q
q q q
Power Charging
Υ
Υ
Υ \Upsilon Υ
Electric field
E
E
E \mathbf{E} E
Concentration flow
C
C
C \mathbf{C} C
Magnetic field
B
B
B \mathbf{B} B
Circulation flow
R
R
R \mathbf{R} R
Potential
A
μ
A
μ
A^( mu) A^\mu A μ
Flow potential
Ψ
μ
Ψ
μ
Psi ^(mu) \Psi^\mu Ψ μ
∇
⋅
C
=
Υ
ϵ
E
∇
⋅
C
=
Υ
ϵ
E
grad*C=(Υ)/(epsilon_(E)) \nabla \cdot \mathbf{C} = \frac{\Upsilon}{\epsilon_\mathcal{E}} ∇ ⋅ C = Υ ϵ E
∇
⋅
R
=
0
∇
⋅
R
=
0
grad*R=0 \nabla \cdot \mathbf{R} = 0 ∇ ⋅ R = 0
∇
×
C
=
−
1
c
E
∂
R
∂
t
∇
×
C
=
−
1
c
E
∂
R
∂
t
grad xxC=-(1)/(c_(E))(delR)/(del t) \nabla \times \mathbf{C} = -\frac{1}{c_\mathcal{E}} \frac{\partial \mathbf{R}}{\partial t} ∇ × C = − 1 c E ∂ R ∂ t
∇
×
R
=
1
c
E
∂
C
∂
t
+
μ
E
J
E
∇
×
R
=
1
c
E
∂
C
∂
t
+
μ
E
J
E
grad xxR=(1)/(c_(E))(delC)/(del t)+mu_(E)J_(E) \nabla \times \mathbf{R} = \frac{1}{c_\mathcal{E}} \frac{\partial \mathbf{C}}{\partial t} + \mu_\mathcal{E} \mathbf{J}_\mathcal{E} ∇ × R = 1 c E ∂ C ∂ t + μ E J E
Where
c
E
=
1
/
ϵ
E
μ
E
c
E
=
1
/
ϵ
E
μ
E
c_(E)=1//sqrt(epsilon_(E)mu_(E)) c_\mathcal{E} = 1/\sqrt{\epsilon_\mathcal{E} \mu_\mathcal{E}} c E = 1 / ϵ E μ E
is the speed of propagation of energy waves.
5.2 Dual pressure confinement
Energy Polarization Tensor:
Π
μ
ν
=
(
ρ
E
P
E
P
E
σ
E
)
Π
μ
ν
=
ρ
E
P
E
P
E
σ
E
Pi^(mu nu)=([rho_(E),P_(E)],[P_(E),sigma_(E)]) \Pi^{\mu\nu} = \begin{pmatrix}
\rho_\mathcal{E} & \mathbf{P}_\mathcal{E} \\
\mathbf{P}_\mathcal{E} & \sigma_\mathcal{E}
\end{pmatrix} Π μ ν = ( ρ E P E P E σ E )
Pressure Transfer Matrix:
d
d
t
(
P
M
P
A
)
=
(
−
α
β
β
−
α
)
(
P
M
P
A
)
d
d
t
P
M
P
A
=
−
α
β
β
−
α
P
M
P
A
(d)/(dt)([P_(M)],[P_(A)])=([-alpha,beta],[beta,-alpha])([P_(M)],[P_(A)]) \frac{d}{dt} \begin{pmatrix} P_M \\ P_A \end{pmatrix} =
\begin{pmatrix}
-\alpha & \beta \\
\beta & -\alpha
\end{pmatrix}
\begin{pmatrix} P_M \\ P_A \end{pmatrix} d d t ( P M P A ) = ( − α β β − α ) ( P M P A )
Self-values:
λ
±
=
−
α
±
β
λ
±
=
−
α
±
β
lambda_(+-)=-alpha+-beta \lambda_\pm = -\alpha \pm \beta λ ± = − α ± β
Stable confinement condition (Fixed Point):
α
≈
β
α
≈
β
alpha~~beta \alpha \approx \beta α ≈ β
The rate of dissipation equals the rate of exchange.
5.3 Compton-Schwarzschild confinement ratio
Compton Length of Swirl:
λ
C
=
ℏ
M
effective
c
λ
C
=
ℏ
M
effective
c
lambda _(C)=(ℏ)/(M_("effective")c) \lambda_C = \frac{\hbar}{M_{\text{effective}} c} λ C = ℏ M effective c
Schwarzschild Radio:
λ
R
=
G
M
effective
c
2
λ
R
=
G
M
effective
c
2
lambda _(R)=(GM_("effective"))/(c^(2)) \lambda_R = \frac{G M_{\text{effective}}}{c^2} λ R = G M effective c 2
Equalizing:
M
effective
=
ℏ
c
G
=
M
Planck
M
effective
=
ℏ
c
G
=
M
Planck
M_("effective")=sqrt((ℏc)/(G))=M_("Planck") M_{\text{effective}} = \sqrt{\frac{\hbar c}{G}} = M_{\text{Planck}} M effective = ℏ c G = M Planck
For arbitrary masses, we enter coupling parameter
:
λ
C
⋅
λ
R
=
ξ
⋅
ℓ
P
2
λ
C
⋅
λ
R
=
ξ
⋅
ℓ
P
2
lambda _(C)*lambda _(R)=xi*ℓ_(P)^(2) \lambda_C \cdot \lambda_R = \xi \cdot \ell_P^2 λ C ⋅ λ R = ξ ⋅ ℓ P 2
with
ξ
∼
N
photons in the vortex
ξ
∼
N
photons in the vortex
xi∼N_("photons in the vortex") \xi \sim N_{\text{photons in the vortex}} ξ ∼ N photons in the vortex
.
6. Wave and mass spectrum solutions
6.1 Free waves
In the void (
J
E
=
0
J
E
=
0
J_(E)=0 \mathbf{J}_\mathcal{E}=0 J E = 0
):
∇
2
C
−
1
c
E
2
∂
2
C
∂
t
2
=
0
∇
2
C
−
1
c
E
2
∂
2
C
∂
t
2
=
0
grad^(2)C-(1)/(c_(E)^(2))(del^(2)C)/(delt^(2))=0 \nabla^2 \mathbf{C} - \frac{1}{c_\mathcal{E}^2} \frac{\partial^2 \mathbf{C}}{\partial t^2} = 0 ∇ 2 C − 1 c E 2 ∂ 2 C ∂ t 2 = 0
∇
2
R
−
1
c
E
2
∂
2
R
∂
t
2
=
0
∇
2
R
−
1
c
E
2
∂
2
R
∂
t
2
=
0
grad^(2)R-(1)/(c_(E)^(2))(del^(2)R)/(delt^(2))=0 \nabla^2 \mathbf{R} - \frac{1}{c_\mathcal{E}^2} \frac{\partial^2 \mathbf{R}}{\partial t^2} = 0 ∇ 2 R − 1 c E 2 ∂ 2 R ∂ t 2 = 0
→ Photons free.
6.2 Swirl solutions (vortex)
Cylindrical symmetry,
R
=
R
ϕ
(
r
)
ϕ
^
R
=
R
ϕ
(
r
)
ϕ
^
R=R_( phi)(r) hat(phi) \mathbf{R} = R_\phi(r) \hat{\boldsymbol{\phi}} R = R ϕ ( r ) ϕ ^
,
C
=
C
r
(
r
)
r
^
C
=
C
r
(
r
)
r
^
C=C_(r)(r) hat(r) \mathbf{C} = C_r(r) \hat{\mathbf{r}} C = C r ( r ) r ^
:
R
ϕ
(
r
)
=
μ
E
ω
3
ρ
0
r
2
(
r
<
r
0
)
R
ϕ
(
r
)
=
μ
E
ω
3
ρ
0
r
2
(
r
<
r
0
)
R_( phi)(r)=(mu_(E)omega)/(3)rho_(0)r^(2)quad(r < r_(0)) R_\phi(r) = \frac{\mu_\mathcal{E} \omega}{3} \rho_0 r^2 \quad (r < r_0) R ϕ ( r ) = μ E ω 3 ρ 0 r 2 ( r < r 0 )
R
ϕ
(
r
)
=
μ
E
ω
ρ
0
r
0
3
3
r
(
r
>
r
0
)
R
ϕ
(
r
)
=
μ
E
ω
ρ
0
r
0
3
3
r
(
r
>
r
0
)
R_( phi)(r)=(mu_(E)omegarho_(0)r_(0)^(3))/(3r)quad(r > r_(0)) R_\phi(r) = \frac{\mu_\mathcal{E} \omega \rho_0 r_0^3}{3r} \quad (r > r_0) R ϕ ( r ) = μ E ω ρ 0 r 0 3 3 r ( r > r 0 )
6.3 Effective mass of the eddy
Total Energy:
E
vortex
=
1
2
μ
E
∫
(
|
C
|
2
+
|
R
|
2
)
d
V
E
vortex
=
1
2
μ
E
∫
(
|
C
|
2
+
|
R
|
2
)
d
V
E_("vortex")=(1)/(2mu_(E))int(|C|^(2)+|R|^(2))dV E_{\text{vortex}} = \frac{1}{2\mu_\mathcal{E}} \int (|\mathbf{C}|^2 + |\mathbf{R}|^2) dV E vortex = 1 2 μ E ∫ ( | C | 2 + | R | 2 ) d V
Effective mass:
M
vortex
=
E
vortex
c
E
2
=
2
π
ρ
0
2
r
0
3
3
μ
E
c
E
2
(
1
+
3
μ
E
2
ω
2
r
0
2
10
)
M
vortex
=
E
vortex
c
E
2
=
2
π
ρ
0
2
r
0
3
3
μ
E
c
E
2
1
+
3
μ
E
2
ω
2
r
0
2
10
M_("vortex")=(E_("vortex"))/(c_(E)^(2))=(2pirho_(0)^(2)r_(0)^(3))/(3mu_(E)c_(E)^(2))(1+(3mu_(E)^(2)omega^(2)r_(0)^(2))/(10)) M_{\text{vortex}} = \frac{E_{\text{vortex}}}{c_\mathcal{E}^2} = \frac{2\pi \rho_0^2 r_0^3}{3\mu_\mathcal{E} c_\mathcal{E}^2} \left(1 + \frac{3\mu_\mathcal{E}^2 \omega^2 r_0^2}{10} \right) M vortex = E vortex c E 2 = 2 π ρ 0 2 r 0 3 3 μ E c E 2 ( 1 + 3 μ E 2 ω 2 r 0 2 10 )
6.4 Quantization of angular momentum
L
=
∫
ρ
E
ω
r
2
d
V
=
n
ℏ
L
=
∫
ρ
E
ω
r
2
d
V
=
n
ℏ
L=intrho_(E)omegar^(2)dV=nℏ L = \int \rho_\mathcal{E} \omega r^2 dV = n\hbar L = ∫ ρ E ω r 2 d V = n ℏ
L
=
4
π
5
ρ
0
ω
r
0
5
=
n
ℏ
L
=
4
π
5
ρ
0
ω
r
0
5
=
n
ℏ
L=(4pi)/(5)rho_(0)omegar_(0)^(5)=nℏ L = \frac{4\pi}{5} \rho_0 \omega r_0^5 = n\hbar L = 4 π 5 ρ 0 ω r 0 5 = n ℏ
Quantized Angular Frequency:
ω
=
5
n
ℏ
4
π
ρ
0
r
0
5
ω
=
5
n
ℏ
4
π
ρ
0
r
0
5
omega=(5nℏ)/(4pirho_(0)r_(0)^(5)) \omega = \frac{5 n \hbar}{4\pi \rho_0 r_0^5} ω = 5 n ℏ 4 π ρ 0 r 0 5
6.5 Mass spectrum
M
n
(
r
0
)
=
2
π
ρ
0
2
r
0
3
3
μ
E
c
E
2
[
1
+
3
μ
E
2
10
(
5
n
ℏ
4
π
ρ
0
r
0
4
)
2
]
M
n
(
r
0
)
=
2
π
ρ
0
2
r
0
3
3
μ
E
c
E
2
1
+
3
μ
E
2
10
5
n
ℏ
4
π
ρ
0
r
0
4
2
M_(n)(r_(0))=(2pirho_(0)^(2)r_(0)^(3))/(3mu_(E)c_(E)^(2))[1+(3mu_(E)^(2))/(10)((5nℏ)/(4pirho_(0)r_(0)^(4)))^(2)] M_n(r_0) = \frac{2\pi \rho_0^2 r_0^3}{3\mu_\mathcal{E} c_\mathcal{E}^2} \left[1 + \frac{3\mu_\mathcal{E}^2}{10} \left(\frac{5 n \hbar}{4\pi \rho_0 r_0^4}\right)^2 \right] M n ( r 0 ) = 2 π ρ 0 2 r 0 3 3 μ E c E 2 [ 1 + 3 μ E 2 10 ( 5 n ℏ 4 π ρ 0 r 0 4 ) 2 ]
For
:
M
0
∝
r
0
3
M
0
∝
r
0
3
M_(0)propr_(0)^(3) M_0 \propto r_0^3 M 0 ∝ r 0 3
For
n
≥
1
n
≥
1
n >= 1 n \geq 1 n ≥ 1
and
small:
M
n
≈
15
16
π
μ
E
n
2
ℏ
2
ρ
0
c
E
2
r
0
5
∝
1
r
0
5
M
n
≈
15
16
π
μ
E
n
2
ℏ
2
ρ
0
c
E
2
r
0
5
∝
1
r
0
5
M_(n)~~(15)/(16 pi)(mu_(E)n^(2)ℏ^(2))/(rho_(0)c_(E)^(2)r_(0)^(5))prop(1)/(r_(0)^(5)) M_n \approx \frac{15}{16\pi} \frac{\mu_\mathcal{E} n^2 \hbar^2}{\rho_0 c_\mathcal{E}^2 r_0^5} \propto \frac{1}{r_0^5} M n ≈ 15 16 π μ E n 2 ℏ 2 ρ 0 c E 2 r 0 5 ∝ 1 r 0 5
Critical radius minimizing mass:
r
0
∗
=
(
5
n
2
ℏ
2
μ
E
16
π
2
ρ
0
2
)
1
/
8
r
0
∗
=
5
n
2
ℏ
2
μ
E
16
π
2
ρ
0
2
1
/
8
r_(0)^(**)=((5n^(2)ℏ^(2)mu_(E))/(16pi^(2)rho_(0)^(2)))^(1//8) r_0^* = \left( \frac{5 n^2 \hbar^2 \mu_\mathcal{E}}{16 \pi^2 \rho_0^2} \right)^{1/8} r 0 ∗ = ( 5 n 2 ℏ 2 μ E 16 π 2 ρ 0 2 ) 1 / 8
Discrete spectrum:
M
n
mín
∝
n
3
/
4
M
n
mín
∝
n
3
/
4
M_(n)^("mín")propn^(3//4) M_n^{\text{mín}} \propto n^{3/4} í M n mín ∝ n 3 / 4
7. Falsifiable observational predictions
Prediction 1: Discrete mass spectrum for dark matter halos
Spacing:
M
n
+
1
M
n
≈
(
1
+
1
n
)
3
/
4
M
n
+
1
M
n
≈
1
+
1
n
3
/
4
(M_(n+1))/(M_(n))~~(1+(1)/(n))^(3//4) \frac{M_{n+1}}{M_n} \approx \left(1 + \frac{1}{n}\right)^{3/4} M n + 1 M n ≈ ( 1 + 1 n ) 3 / 4
Test : Mass function of satellite galaxies with "steps". → LSST, Euclid.
Prediction 2: Gamma line series with logarithmic spacing
A whirlpool that loses a quantum of angular momentum (
Δ
n
=
1
Δ
n
=
1
Delta n=1 \Delta n = 1 Δ n = 1
) Broadcasts:
E
γ
(
n
→
n
−
1
)
≈
3
4
ℏ
2
ρ
0
r
0
5
∝
n
−
5
/
4
E
γ
(
n
→
n
−
1
)
≈
3
4
ℏ
2
ρ
0
r
0
5
∝
n
−
5
/
4
E_( gamma)(n rarr n-1)~~(3)/(4)(ℏ^(2))/(rho_(0)r_(0)^(5))propn^(-5//4) E_\gamma(n \to n-1) \approx \frac{3}{4} \frac{\hbar^2}{\rho_0 r_0^5} \propto n^{-5/4} E γ ( n → n − 1 ) ≈ 3 4 ℏ 2 ρ 0 r 0 5 ∝ n − 5 / 4
Logarithmic relationship:
log
E
γ
(
n
)
≈
cte
−
5
4
log
n
log
E
γ
(
n
)
≈
cte
−
5
4
log
n
log E_( gamma)^((n))~~"cte"-(5)/(4)log n \log E_\gamma^{(n)} \approx \text{cte} - \frac{5}{4} \log n log E γ ( n ) ≈ cte − 5 4 log n
Test : Find gamma line series with this pattern in the galactic center. → Fermi-LAT, CTA .
Prediction 3: Excess in the cosmic infrared background (CIB)
Non-Planckian Hawking radiation with excess in 10-100
m:
ν
F
ν
∝
ν
1.3
ν
F
ν
∝
ν
1.3
nuF_( nu)propnu^(1.3) \nu F_\nu \propto \nu^{1.3} ν F ν ∝ ν 1.3
Test : Compare with Galactic Dust Spectrum. → Planck, Herschel, SPHEREx .
Prediction 4: Deviation from the Tully-Fisher ratio
Modified centripetal force:
v
rot
2
r
=
G
M
(
<
r
)
r
2
+
1
μ
E
|
C
|
v
rot
2
r
=
G
M
(
<
r
)
r
2
+
1
μ
E
|
C
|
(v_("rot")^(2))/(r)=(GM( < r))/(r^(2))+(1)/(mu_(E))|C| \frac{v_{\text{rot}}^2}{r} = \frac{GM(<r)}{r^2} + \frac{1}{\mu_\mathcal{E}} |\mathbf{C}| v rot 2 r = G M ( < r ) r 2 + 1 μ E | C |
Prediction:
v
rot
4
=
a
M
b
+
b
v
rot
4
=
a
M
b
+
b
v_("rot")^(4)=aM_(b)+b v_{\text{rot}}^4 = a M_b + b v rot 4 = a M b + b
with
b
>
0
b
>
0
b > 0 b > 0 b > 0
for galaxies with low surface mass.
Test : Rotation curves of dwarf and ultra-diffuse galaxies. → WEAVE, DESI .
Prediction 5: Asymmetry in gravitational lensing due to frame dragging
Additional spin displacement of the swirl (
J
=
n
ℏ
J
=
n
ℏ
J=nℏ J = n\hbar J = n ℏ
):
Δ
ϕ
lens
=
4
G
M
c
2
b
+
4
G
J
c
3
b
2
Δ
ϕ
lens
=
4
G
M
c
2
b
+
4
G
J
c
3
b
2
Deltaphi_("lens")=(4GM)/(c^(2)b)+(4GJ)/(c^(3)b^(2)) \Delta \phi_{\text{lens}} = \frac{4GM}{c^2 b} + \frac{4G J}{c^3 b^2} Δ ϕ lens = 4 G M c 2 b + 4 G J c 3 b 2
Position difference between images:
δ
θ
≈
10
−
6
(
n
10
60
)
(
b
1
kpc
)
−
2
arcsec
δ
θ
≈
10
−
6
n
10
60
b
1
kpc
−
2
arcsec
delta theta~~10^(-6)((n)/(10^(60)))((b)/(1" kpc"))^(-2)"arcsec" \delta \theta \approx 10^{-6} \left( \frac{n}{10^{60}} \right) \left( \frac{b}{1 \text{ kpc}} \right)^{-2} \text{arcsec} δ θ ≈ 10 − 6 ( n 10 60 ) ( b 1 kpc ) − 2 arcsec
Test : VLBI in galactic lenses. → EHT, VLBI .
8. Prediction Summary
#
Prediction
Instrument
¿Differentiable from
Λ
Λ
Lambda \Lambda Λ CDM?
1
Discrete mass spectrum for DM halos
LSST, Euclid
Yes
2
Gamma line series
E
γ
∝
n
−
5
/
4
E
γ
∝
n
−
5
/
4
E_( gamma)propn^(-5//4) E_\gamma \propto n^{-5/4} E γ ∝ n − 5 / 4
Fermi-LAT, CTA
Yes (Only)
3
CIB Excess with
ν
F
ν
∝
ν
1.3
ν
F
ν
∝
ν
1.3
nuF_( nu)propnu^(1.3) \nu F_\nu \propto \nu^{1.3} ν F ν ∝ ν 1.3
SPHEREx, Planck
Yes
4
Tully-Fisher deviation for dwarfs
WEAVE, DESI
Yes
5
Asymmetry in lenses due to frame dragging
VLBI, EHT
Yes
9. Conclusion
A self-consistent framework has been constructed where:
Energy is the only fundamental quantity .
Two dual fields
(concentration) and
(circulation) describe all phenomena analogous to
and
.
3. The lockdown emerges from a fixed point
α
≈
β
α
≈
β
alpha~~beta \alpha \approx \beta α ≈ β
.
4. The masses of the eddies follow a discrete spectrum
M
n
∝
n
3
/
4
M
n
∝
n
3
/
4
M_(n)propn^(3//4) M_n \propto n^{3/4} M n ∝ n 3 / 4
.
5. Dark matter is naturally clouds of confined photons with collective mass.
5 falsifiable predictions are proposed with current and future missions.
The cleanest and most unique prediction is number 2 : a series of gamma lines with logarithmic spacing. Its detection would be an irrefutable signature of this model.
"Energy is the only currency of the universe. Everything else is exchange."
10. Explanation for laypeople
If you're left with the impression that you haven't understood anything,
don't worry. Mathematics is powerful, but
not very appealing. Despite appearances, what it
expresses is very simple, and I can summarize it in
a few lines.
The creation of the universe is currently explained by the inflationary Big Bang model, but certain elements have appeared that we do not understand: dark energy and dark matter, of which we were unaware and which, without knowing exactly what they are, become essential to explain how the universe moves.
In this hypothesis, I propose an alternative creation of the Universe
to the Big Bang, based on a dual equilibrium
between matter and antimatter, which could resolve the
observed mysteries and provide a more effective
and cleaner solution to many of the processes we observe
in the Universe.
As key points of novelty, what I explicitly suggest is that energy is balanced in a way that creates a cyclical process without a defined beginning or end. In this model, gravity is not determined by matter, as we currently think, but by an energy drag flow originating from black holes. Think of the Earth and the Moon as "pebbles" carried by the current of a river (light) flowing toward a waterfall (black hole).
Matter itself is made up of light, or, to continue the analogy, of a "calcareous residue" that it leaves behind as it swirls along its path.
I'm aware of how strange it seems, but if I'm not
terribly mistaken, both mathematics
and observations seem to predict it this way.
What do you think?...
Could this be how
our Universe works?
Yes
No
I don't know
Contact