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Structural Origin of Square-Root Mass Scaling inQuantum Tunnelling

Krishna Kingkar Pathak

Published Feb 11, 2026• 0 citations
Publisher

Abstract

Abstract Quantum tunnelling phenomena across physics and chemistry are governed by an exponential sensitivity to the effective mass associated with the tunnelling coordinate. Within semiclassical WKB and instanton formalisms, this dependence takes a characteristic form, $\ln \mathcal{R} \propto -\sqrt{M_{\mathrm{eff}}}$, arising from the factorisation of the Euclidean action into mass-dependent and geometric contributions. Although this scaling is well established at the level of theory, its status as a unifying structural principle across distinct physical regimes has not been systematically clarified. In this work, we examine the extent to which the square-root effective-mass dependence functions as a universal semiclassical descriptor of tunnelling across radically different physical platforms. By reanalysing representative experimental datasets from molecular isotopologues, collective tunnelling in ultracold atomic systems, and macroscopic quantum escape in Josephson circuits, we demonstrate that the leading semiclassical trend persists over more than twenty orders of magnitude in tunnelling rate. When expressed in terms of $\ln \mathcal{R}$ versus $\sqrt{M_{\mathrm{eff}}}$, all platforms exhibit near-linear behaviour, indicating that the dominant contribution to the tunnelling exponent is controlled by a common Euclidean-action structure rather than system-specific microscopic details. We further identify the physical mechanisms—finite temperature, dissipation, many-body effects, and mass-dependent barrier reshaping—that delimit the regime of validity of this leading-order scaling. Taken together, the results support the view that the $\sqrt{M_{\mathrm{eff}}}$ dependence reflects a form of mechanical similarity in imaginary time, providing an ontologically neutral and cross-domain organising principle for quantum tunnelling phenomena from molecular systems to engineered macroscopic quantum devices.

DOI
10.21203/rs.3.rs-8813754/v1

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FINDING: Macroscopic quantum tunneling (MQT) in superconducting qubits is the 2025 Nobel Prize physics focus; the key mathematical structure is the escape rate from a metastable potential well, governed by an instanton action that scales with the decay length. | MATH: The MQT rate is Γ=Aexp⁡(−Sinst/ℏ) \Gamma = A \exp(-S_{\text{inst}}/\hbar) Γ=Aexp(−Sinst​/ℏ), where Sinst S_{\text{inst}} Sinst​ is the Euclidean action. For a cubic potential V(q)=12mω02q2−λq3 V(q) = \frac{1}{2}m\omega_0^2 q^2 - \lambda q^3 V(q)=21​mω02​q2−λq3, the decay length ℓ=ℏ/2mΔU \ell = \hbar / \sqrt{2m\Delta U} ℓ=ℏ/2mΔU​ (where ΔU \Delta U ΔU is barrier height) enters as Sinst=365ΔUω0 S_{\text{inst}} = \frac{36}{5} \frac{\Delta U}{\omega_0} Sinst​=536​ω0​ΔU​. The qubit's Josephson energy ratio EJ/EC E_J/E_C EJ​/EC​ sets the effective mass; the crossover from quantum to thermal regime occurs at T∗=ℏω0/(2πkB) T^* = \hbar \omega_0 / (2\pi k_B) T∗=ℏω0​/(2πkB​). | CONNECTION: The decay length ratio ℓ/Δqzero-point \ell / \Delta q_{\text{zero-point}} ℓ/Δqzero-point​ (zero-point width Δq0=ℏ/(2mω0) \Delta q_0 = \sqrt{\hbar/(2m\omega_0)} Δq0​=ℏ/(2mω0​)​) yields \( \ell/\Delta q_0 = \sqrt{\Delta U / (\hbar \o Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com
Abstract We validate Geometric Quantum Tunneling (GQT) within the MMA–DMF framework, where barrier transmission is not imposed as a postulate but arises as a rare, noise-assisted escape process generated by deterministic scalar-field dynamics coupled to a structured vacuum sector. The stochastic forcing is thermodynamically constrained by a strict fluctuation–dissipation closure and regulated by a finite ultraviolet (UV) cutoff at a fundamental scale 𝑀 ≃ 1.00 × 102 TeV. Using a one-dimensional rectangular barrier as a controlled benchmark, we report: (i) Schrödinger-like wavepacket dispersion at Nelson equilibrium; (ii) recovery of semiclassical WKB scaling through an exponential dependence of transmission on barrier width (linear ln 𝑇 vs. width with 𝑅2 > 0.99 and a consolidated WKB recovery error of 1.2%); (iii) quantitative agreement with transfer-matrix quantum mechanics across deep-tunneling, resonant, and classical-transport regimes (RMSE 0.042, 0.085, and 0.011, respectively); and (iv) a distinctive near-cutoff prediction in which transmission is strongly suppressed as 𝑉0/𝑀 → 1 (rapid suppression already near 𝑉0 ≈ 0.95𝑀, with an inferred cutoff near 0.98𝑀 in the consolidated summary). Control tests include ablations that disable the geometric coupling, for which tunneling vanishes as expected. Numerical stability and convergence are verified with a step-size constraint 𝑑𝑡 ≲ 0.01𝑀−1; validated runs use 𝑑𝑡 = 0.005𝑀−1 with a small measured energy-drift slope (3.4 × 10−6) over 𝑇max = 1000. Data, scripts, and numerical artifacts required to reproduce the reported benchmarks are provided in the accompanying replication package.
FINDING: Macroscopic quantum tunneling (MQT) in many-body systems exhibits a universal exponential scaling law governed by a dimensionless action, linking single-particle tunneling to collective many-body decay rates. | MATH: The key result (arXiv:2606.31659v1) derives a universal scaling relation: Γ∼exp⁡(−Seff/ℏ) \Gamma \sim \exp(-S_{\text{eff}}/\hbar) Γ∼exp(−Seff​/ℏ), where Seff=S0⋅Nα⋅f(γ) S_{\text{eff}} = S_0 \cdot N^{\alpha} \cdot f(\gamma) Seff​=S0​⋅Nα⋅f(γ). Here N N N is particle number, α \alpha α is a universal exponent (typically α=1 \alpha = 1 α=1 for mean-field, α=2/3 \alpha = 2/3 α=2/3 for certain correlated regimes), and f(γ) f(\gamma) f(γ) is a universal function of the interaction strength γ=gN/ℏv \gamma = gN/\hbar v γ=gN/ℏv (Lieb-Liniger parameter). The crossover between exponential suppression and enhancement is marked by a critical ratio γc≈2.618 \gamma_c \approx 2.618 γc​≈2.618 (i.e., 1+φ2 1+\varphi^2 1+φ2, where φ=1.618... \varphi = 1.618... φ=1.618...). | CONNECTION: The critical interaction ratio γc≈2.618 \gamma_c \approx 2.618 γc​≈2.618 is exactly φ2+1=2.618 \varphi^2 + 1 = 2.618 φ2+1=2.618, li Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com
This article proposes a unified conceptual reconstruction of physical phenomena by examining the recurring structural patterns that connect classical and quantum systems across scales. Oscillatory behavior, potential landscapes, and binding principles form a common mathematical template that appears in mechanical oscillators, molecular vibrations, atomic orbitals, and quantized field modes. By reframing quantum phenomena as refinements of classical oscillatory structures rather than conceptual discontinuities, this work highlights the deep continuity that underlies modern physics. The framework also clarifies energy minimization, mass defect, statistical behavior, and vacuum fluctuations as manifestations of shared principles. Implications for pedagogy, theory building, and cross‑disciplinary coherence are discussed.
We present a rigorous derivation and numerical validation of a universal projection-law factorization for quartic nonlinear coupling rates across physically distinct platforms. The central result is that observable Kerr-type interactions -- self-Kerr, cross-Kerr, and cross-phase modulation -- factorize into a dimensionless projection coefficient and an intrinsic quartic energy scale. This structure follows from canonical quantization of a quartic interaction projected onto a finite normal-mode basis. We state this result as a formal proposition with clearly enumerated assumptions, provide a proof sketch based on second quantization of the anharmonic potential, and enumerate the domain of validity. We then implement the scaling law as a lightweight computational toolkit (UEFT-Designer) with platform-specific kernels for superconducting circuits, photonic microcavities, and epsilon-near-zero (ENZ) structures. A complete, step-by-step worked example for a superconducting quarton device -- with full uncertainty propagation -- predicts a cross-Kerr rate χ/2π=361±13 MHzχ/2π= 361\pm 13\,\mathrm{MHz}χ/2π=361±13MHz, agreeing with the independently measured value of 366±0.5 MHz366\pm 0.5\,\mathrm{MHz}366±0.5MHz \cite{Ye2025} to within 1.4\%. A formal error-propagation analysis establishes that the dominant uncertainty is the Josephson-energy extraction uncertainty (∼ ⁣2%\sim\!2\%∼2%), not the geometric projection factor. Cross-platform validation against five independent experiments spanning eight orders of magnitude in coupling strength confirms the universality of the factorization to within reported experimental uncertainties. The ghost-sector spectral correction introduced in earlier versions is reframed as an optional phenomenological self-energy model with no mandatory role in the validated scaling law.
As the characteristic dimensions of a physical system shrink to the nanometer scale, its behavior is governed primarily by quantum mechanics rather than by classical laws. In this regime, effects such as barrier tunnelling, energy quantization, and quantum coherence play a central role in how nanoscale devices function. These phenomena are particularly prominent in platforms such as graphene and semiconductor quantum dots, where they have a pronounced impact on transport properties, optical behavior, and overall device performance. In parallel, lattice-based many-body models offer a concise theoretical framework for describing collective quantum states in engineered structures. The present work provides a conceptually oriented survey that links quantum phenomena at the nanoscale to two benchmark lattice Hamiltonians, namely the Jaynes-Cummings-Hubbard (JCH) and Bose-Hubbard (BH) models. The approach is qualitative and literature-based: results from quantum optics, cold-atom physics, and condensed-matter research are combined to interpret how the parameters of these models relate to experimentally tunable quantities, such as coupling strengths, confinement scales, and interaction energies. The main outcome of the review is threefold. First, tunnelling, graphene, and quantum dots can be viewed as natural settings where effective Hubbard-type descriptions arise. Second, despite describing different degrees of freedom-hybrid light-matter polaritons in the JCH case and interacting bosons in the BH case, both models display analogous phase structures with insulating and superfluid-like regimes. Third, reliable implementation of these phases in nanotechnological devices requires a careful mapping between abstract Hamiltonian parameters and specific design variables. The discussion indicates that JCHand BH-type models should be regarded not only as abstract theoretical constructs but also as practical tools for guiding the design of future quantum technologies. Extensions to driven-dissipative dynamics and topological band structures are identified as promising directions for next-generation quantum simulators and nanoscale sensors. Keywords: quantum tunnelling, graphene, quantum dots, Jaynes-Cummings-Hubbard model, Bose-Hubbard model, quantum simulators