Fundamental Module: Level 1 of SGDM Model • Quantum Theory of Atoms & Graviton

Quantum Wave Theory of Atoms & Gravitons: Physics of 3D Standing Waves & Kerr Nuclei

Physical extension of quantum mechanics in the SGDM model by Yuri A. Chesnokov: electron as a stable 3D standing wave ($\vec{E} \perp \vec{B}$, $\Delta\varphi = 90^\circ$, $\langle\vec{S}\rangle \equiv 0$), graviton nucleus ($N_{\text{grav}} = A$, $\rho_0 \approx 3 \cdot 10^{17}\text{ kg/m}^3$), resolution of wave-particle duality, quantum numbers, and material properties.

Academic Priority of Chesnokov Yu. A. • Quantum Physics

Quantum Wave Atom Concept: Electron as a 3D Standing Wave

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The SGDM model resolves the century-old wave-particle duality paradox and bridges microphysics with relativistic GR gravity. The electron in a stable atom is not a point particle, but a closed 3D standing wave resonator anchored to the Kerr graviton nucleus ($N_{\text{grav}} = A$).

1. "Quanta Do Not Fly" Postulate

Only continuous wave fronts propagate through space at velocity $c$. A quantum ($E = \hbar\omega$) arises strictly as a local resonant absorption/emission act by the atom's graviton nucleus.

2. Stability Balance $\vec{E} \perp \vec{B}$ & $\Delta\varphi = 90^\circ$

In an unexcited $1s$ atom, the radial $\vec{E}$ and azimuthal $\vec{B}$ spin vortex fields are shifted by $\pi/2$. Poynting vector $\langle\vec{S}\rangle \equiv 0$ — zero radiation, eternal stability.

3. Wave Meaning of Quantum Numbers ($n, l, m, s$)

$n$ — number of de Broglie wavelengths; $l$ — nodal planes ($s, p, d, f$); $m$ — $90^\circ$ phase orthogonality; $s = \pm 1/2$ — Pauli spin magnetic lock (2 electrons $\uparrow\downarrow$ per mode).

4. Bridge to QED: Lamb Shift & $g$-factor

The $1057\text{ MHz}$ shift arises from direct contact of the $2s_{1/2}$ mode with the Kerr graviton ($r_g \approx 0.84\text{ fm}$), unlike the nodal $2p_{1/2}$ mode. Mass $m_e$ is standing wave energy in $a_0$.

Section 1

Topological Status of Gravitons and Discrete Calibration ($N_{\text{grav}} = A$)

In SGDM, the spin-2 massive graviton with rest mass $M_g \approx 2.6 \times 10^{-68}\text{ kg}$ is the primary topological metric node. Nucleons condense onto pre-existing quantum graviton nodes of space.

$$ N_{\text{grav}}(\text{atom}) \equiv A = Z + N $$

Hydrogen: 1 node, Helium-4: 4 nodes (tetrahedron), Iron-56: 56 nodes, Gold-197: 197 nodes, Uranium-238: 238 nodes.

Section 2

Scale Dualism: "Gravitational Nuclear Force" vs Weak Macro-field

1. Inside the Nucleus ($r \le 1\text{ fm}$): Nuclear Gravity

Due to energy density $\rho_0 c^2 \sim 3 \times 10^{34}\text{ J/m}^3$, nonlinear curvature generates attractive force $F \sim 10^4 - 10^6\text{ N}$ ($10 - 200\text{ tons of force!}$), binding quarks and nucleons together.

2. Interatomic Distance ($r \sim 10^{-10}\text{ m}$): Decay

Over chemical bond distances, direct gravitational pull falls by $1/r^2$ by a factor of $10^{46} - 10^{48}$ ($F \sim 10^{-44}\text{ N}$), strictly negligible compared to Van der Waals forces.

Academic Note on Section 2 (QCD Duality & Strong Interaction):

In the SGDM framework, the concept of "Gravitational Nuclear Force" does not contradict standard Quantum Chromodynamics (QCD) with its gauge gluon fields $SU(3)_c$, but rather models the dual geometric spacetime framework of confinement. At $r \le 1\text{ fm}$, spin-2 graviton nodes establish metric tension $\sigma \sim c^4/G_{\text{eff}} \sim 10^5\text{ N}$, inside which gauge quark-gluon flux tubes naturally close into color-singlet hadrons without singularities.

Section 3

Super-Large Cores $N \sim 10^{44}$: Micro-Black Holes of the Asteroid Window

Parameters of $N \sim 10^{44}$ Objects:

  • • Mass: $M \approx 10^{44} \cdot m_p \approx 1.67 \times 10^{17}\text{ kg}$ ($1.67 \times 10^{14}\text{ tons}$, typical asteroid mass).
  • • Physical Core Radius $\rho_0$: $R_{\text{core}} \approx \mathbf{0.05\ \mu m = 50\text{ nm}}$ (virus-scale).
  • • Event Horizon Radius: $R_g \approx \mathbf{0.25\text{ nm}}$ (atomic scale).
  • • Stability: Absolute stability (Hawking evaporation absent due to solid $\rho_0$ core). Comprise 90% of galactic dark halo mass.
3.1

Astrophysical Encounter Probabilities in the Solar System & Earth

The primordial black hole swarm (95% of cosmic mass) populates the spherical galactic halo, through which the Solar System traverses at $v \sim 230 - 300\text{ km/s}$. At local halo density $\rho_{\text{DM}} \approx 0.4\text{ GeV/cm}^3$, the mean inter-PBH separation is $L \sim 1.5 - 3.0\text{ AU}$ ($200 - 450\text{ million km}$).

Target Body / Scale Cross-Section $\sigma$ Direct Collisions (500 Myr) Orbital Transits (500 Myr)
Earth ($R = 6\,371\text{ km}$) $1.27 \times 10^8\text{ km}^2$ $\sim 5 \times 10^{-6}$ (rare event) —
Jupiter ($R = 70\,000\text{ km}$) $1.5 \times 10^{10}\text{ км}^2$ $\sim 10^{-4}$ —
Sun ($R = 696\,340\text{ km}$) $1.5 \times 10^{12}\text{ km}^2$ $\approx 10^{-2}$ ($\sim 1\%$) —
Earth's Orbit ($r = 1\text{ AU}$) $7.0 \times 10^{16}\text{ km}^2$ — $\mathbf{\sim 500 - 1000\text{ transits}}$
Kuiper Belt ($r = 50\text{ AU}$) $1.7 \times 10^{20}\text{ km}^2$ — $\mathbf{> 1\,000\,000\text{ transits}}$
3.2

Dynamical Detonation Theory in Dense Planetary Media vs Hawking Evaporation

In SGDM, black holes remain stable in vacuum. When traversing dense planetary matter ($\rho \approx 3 - 13\text{ g/cm}^3$) at hypersonic speed $v \approx 300\text{ km/s}$, asymmetric Bondi–Hoyle accretion transfers rotational torque ($\frac{da^*}{dx} > 0$), leading to two outcomes:

A

Outcome 1: Complete Planetary Transit ($a^* < 1$)

With modest initial spin ($a_0^* < 0.85$), the micro-BH traverses Earth in $\approx 42\text{ seconds}$, absorbing only micrograms of matter and leaving a narrow plasma ionization trail.

B

Outcome 2: Explosive Detonation into Matter ($a^* \to 1$)

If initial spin was near-critical ($a_0^* \ge 0.95$), at depths of $1/3, 1/2$ or $2/3$ Earth diameter ($x \sim 4\,000 - 8\,000\text{ km}$), spin-up hits $v_{\text{eq}} \to c$. Centrifugal overpressure ($K \equiv 1.04$) violently detonates core $\rho_0$, releasing $10^{14}-10^{17}\text{ tons}$ into ultra-hot quark-gluon plasma and pure hydrogen!

3.3

Geophysical & Mineralogical Signatures in Earth's Mantle

Micro-BH detonation or hypersonic passage generates localized shockwaves exceeding $P > 50 - 200\text{ GPa}$ and $T > 5\,000^\circ\text{C}$, producing vertical diatremes and ultra-high-pressure mineral phases:

Stishovite & Seifertite
$\text{SiO}_2$ phases ($P > 10-50\text{ GPa}$)

Ultra-dense silica with octahedral silicon coordination lining the crustal penetration channel.

Lonsdaleite
Hexagonal diamond ($P > 15\text{ GPa}$)

Synthesized during instantaneous shock compression of graphite, $58\%$ harder than cubic diamond.

Bridgmanite & Ringwoodite
Mantle perovskites ($P > 23\text{ GPa}$)

Lower mantle high-pressure phases produced directly along upper crustal fracture zones.

Kimberlite Diatremes
Explosion pipes (depth $150-200\text{ km}$)

Vertical cylindrical conduits of explosive mantle degassing propelling diamonds to the surface.

Section 3

Graviton Impact on Photons: Quantum Doubling of Light Deflection

Newtonian ballistic theory yields deflection angle $\theta_{\text{Newton}} = \frac{2GM}{c^2 b}$. In SGDM graviton theory, tensor metric distortion doubles the total angle:

TOTAL LIGHT DEFLECTION ANGLE IN SGDM GRAVITON FIELD
$$ \theta_{\text{SGDM}} = 2 \times \theta_{\text{Newton}} = \frac{4GM}{c^2 b} \cdot \exp\left(-\frac{b}{\lambda_g}\right) \left(1 + \frac{b}{\lambda_g}\right) $$

Time dilation $g_{00}$ (50% contribution)

$\theta_{\text{time}} = \frac{2GM}{c^2 b}$ due to refractive time slowing.

Spatial curvature $g_{rr}$ (50% contribution)

$\theta_{\text{space}} = \frac{2GM}{c^2 b}$ due to spin-2 3D spatial warping.

3.1

Quantum-Metric Nature of Single-Slit Light Diffraction

In wave optics, single-slit diffraction is characterized by beam divergence $\theta \approx \lambda / d$ as slit width approaches wavelength $d \to \lambda$. In SGDM, this phenomenon is driven by the transverse metric gradient $\nabla h_{\mu\nu}(y)$ generated by graviton nodes ($N_{\text{grav}} = A$) along the slit boundaries.

DIFFRACTION SPREAD VIA SLIT METRIC GRADIENT IN SGDM
$$ \theta(d) \approx \frac{\lambda}{d} \equiv \frac{\hbar}{p_x \cdot d} \propto \int_{-d/2}^{+d/2} \left| \frac{\partial h_{\mu\nu}}{\partial y} \right| dy $$

As slit width $d$ narrows, the entire photon beam encounters the steep metric distortion zone near the edges, bending light trajectories into the classical diffraction fringe pattern.

Slit Material Impact ($N_{\text{grav}} = A$) on Diffraction Fringe Pattern:

1. Silicon ($^{28}\text{Si}$, $N=28$)

Low mass $\implies$ sharp central peak, standard Fresnel diffraction.

2. Iron ($^{56}\text{Fe}$, $N=56$)

Optimal nucleus $\implies$ moderate 1st-order side lobe enhancement.

3. Gold ($^{197}\text{Au}$, $N=197$)

Heavy relativistic core $\implies$ metric wave front retardation and brighter side fringes.

3.2

Spectral Decomposition Across Media (Quantum-Metric Chromatic Dispersion)

When white light traverses a prism at angle $\alpha$, it disperses into a rainbow spectrum. In SGDM, refractive index dispersion $n(\lambda)$ originates from the quantum-metric interaction of photon energy $E = \hbar\omega$ with the spin-2 graviton lattice of the medium ($N_{\text{grav}} = A$).

1. Long Wavelengths (Red Light, $\lambda \sim 700\text{ nm}$)

$\lambda \gg l_{\text{grav}} \sim 0.2\text{ nm}$. Photons average over atomic metric wells $\implies$ minimal phase retardation $\implies$ $n(\text{red})$ is minimal, lowest deflection angle.

2. Short Wavelengths (Violet Light, $\lambda \sim 400\text{ nm}$)

Higher quantum energy ($1.75\times$) and spatial localization $\implies$ deeper probe of graviton wells $\implies$ $n(\text{violet})$ is maximal, largest deflection angle.

REFRACTIVE INDEX WITH GRAVITON LATTICE TERM IN SGDM
$$ n(\lambda, A) \approx 1 + \Delta n_{\text{EM}}(\lambda) + \beta_{\text{grav}} \cdot \frac{n_{\text{atoms}} \cdot N_{\text{grav}}}{\lambda^2} $$
Academic Note on Optics (Distinguishing EM and Graviton Contributions):

In classical and quantum optics, the predominant contribution to the macroscopic refractive index $n(\lambda)$ and diffraction patterns ($>99.99\%$) arises from electromagnetic polarizability of electronic shells and surface plasmon modes. The term $\beta_{\text{grav}}$ in SGDM represents an ultra-fine quantum-metric topological vacuum polarization correction ($h^{\mu\nu}T_{\mu\nu}$), linking crystal lattice geometry directly with spacetime metric fluctuations at the Planck-nuclear boundary.

3.3

Hard Quanta ($\lambda \le R_{\text{core}}$) Attenuation Across Material Thickness

For gamma and hard X-rays ($\lambda \le R_{\text{core}} \sim 1 - 7\text{ fm}$, $E > 1\text{ MeV}$), radiation interacts directly with nuclear graviton nodes ($N_{\text{grav}} = A$) via pair production ($\sigma_{\text{pair}} \propto Z^2 \propto N_{\text{grav}}^2$) and Compton scattering.

EXPONENTIAL BEER-LAMBERT ATTENUATION & HALF-VALUE LAYER
$$ I(x) = I_0 \cdot \exp\left( -\mu(A, E) \cdot x \right), \quad d_{1/2} = \frac{\ln 2}{\mu(A, E)} \approx \frac{0.693}{\mu} $$

Thin Layer ($x \ll 1/\mu$, Foil)

Linear single scattering $I(x) \approx I_0(1 - \mu x)$ with negligible flux loss.

Thick Layer ($x \gg 1/\mu$, Shield)

Exponential shielding ($e^{-\mu x} \to 0$): $9\text{ cm}$ of Lead ($^{208}\text{Pb}$) reduces gamma flux by 1000-fold ($10 \cdot d_{1/2}$), equivalent to $1\text{ km}$ of air or $1.1\text{ m}$ of water.