On Tunneling in the Quantum Multiverse
Pith reviewed 2026-05-16 11:15 UTC · model grok-4.3
The pith
In the Everettian multiverse, quantum tunneling is experienced only by the observer in the transmitted branch after the wavefunction splits at a barrier.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
In the Everettian quantum multiverse the universal wavefunction splits into decohered reflected and transmitted branches under the environmental effect after encountering a potential barrier. The observed tunneling is then experienced by the observer located in a tunneled world. The tunneling probability and the tunneling time are investigated in terms of the tunneled world relative weights and the branching duration, respectively.
What carries the argument
The splitting of the universal wavefunction into decohered reflected and transmitted branches under environmental effects after a potential barrier.
Load-bearing premise
The universal wavefunction splits into decohered reflected and transmitted branches under environmental effects after encountering a potential barrier, so that tunneling is experienced only in the transmitted branch.
What would settle it
A measurement of tunneling time or probability that does not match the branching duration or relative world weights derived from the same system would falsify the relation.
read the original abstract
Prompted by the longstanding interpretational controversy in quantum mechanics, quantum tunneling is heuristically addressed within the Everettian quantum multiverse. In this framework, the universal wavefunction splits into decohered reflected and transmitted branches under the environmetal effect after encountring a potential barrier. The observed tunneling is then experienced by the observer located in a tunneled world. The tunneling probability and the tunneling time are investigated in terms of the tunneled world relative weights and the branching duration, respectively. The macroscopic quantum tunneling, recently honored, is also discussed and the corresponding macroscopic tunneling time is approached based on the obtained results and known data.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper offers a heuristic treatment of quantum tunneling in the Everettian multiverse. It asserts that the universal wavefunction splits into decohered reflected and transmitted branches after encountering a potential barrier due to environmental effects, with observers in the transmitted branch experiencing the tunneling event. Tunneling probability is expressed via the relative weights of tunneled worlds and tunneling time via branching duration; the framework is then applied to macroscopic quantum tunneling using existing data.
Significance. If the heuristic identifications of probability with branch weights and time with branching duration could be placed on a rigorous footing derived from the time-dependent Schrödinger equation and a concrete decoherence model, the work would supply an interpretive bridge between standard tunneling calculations and many-worlds ontology. In its present form the absence of explicit derivations keeps the contribution at the level of conceptual suggestion rather than quantitative advance.
major comments (3)
- [Abstract and main discussion of probability] The central identification of tunneling probability with the relative weights of tunneled worlds is not accompanied by an explicit formula or derivation showing how those weights are obtained from the wave-function amplitudes or transmission coefficients; the mapping therefore remains an assertion rather than a computed result.
- [Discussion of tunneling time] The claim that tunneling time equals branching duration lacks any derivation linking it to the time-dependent wave function or to a decoherence timescale; no expression for branching duration is supplied, rendering the relation to observed tunneling times an untested identification.
- [Macroscopic tunneling discussion] The extension to macroscopic quantum tunneling in the final section inherits the same un-derived relations and applies them to known data without error analysis or comparison to standard WKB or instanton methods, weakening the quantitative claim.
minor comments (3)
- [Abstract] Abstract contains typographical errors ('environmetal', 'encountring') that should be corrected for clarity.
- [Main text] The term 'branching duration' is introduced without a precise definition or reference to existing literature on decoherence timescales.
- [References] Standard references on tunneling-time definitions (e.g., Landauer-Büttiker or phase-time approaches) and on Everettian decoherence models are missing.
Simulated Author's Rebuttal
We thank the referee for the careful reading and constructive comments. Our manuscript is explicitly framed as a heuristic treatment of tunneling within the Everettian multiverse, as stated in the abstract and introduction. We address each major comment below, clarifying the intended scope while acknowledging the absence of rigorous derivations from the time-dependent Schrödinger equation.
read point-by-point responses
-
Referee: [Abstract and main discussion of probability] The central identification of tunneling probability with the relative weights of tunneled worlds is not accompanied by an explicit formula or derivation showing how those weights are obtained from the wave-function amplitudes or transmission coefficients; the mapping therefore remains an assertion rather than a computed result.
Authors: We agree that no explicit derivation from the wave-function amplitudes or transmission coefficients is provided. The paper proposes a conceptual identification in which the tunneling probability corresponds to the relative weight of the transmitted branch, in keeping with the Born-rule interpretation standard in Everettian quantum mechanics. This mapping is presented heuristically rather than as a computed result derived from a specific decoherence model. We do not claim a first-principles derivation and therefore do not intend to add one; the contribution lies in the interpretive link rather than in new quantitative machinery. revision: no
-
Referee: [Discussion of tunneling time] The claim that tunneling time equals branching duration lacks any derivation linking it to the time-dependent wave function or to a decoherence timescale; no expression for branching duration is supplied, rendering the relation to observed tunneling times an untested identification.
Authors: The identification of tunneling time with branching duration is likewise heuristic and is not accompanied by an explicit expression derived from the time-dependent Schrödinger equation or a concrete decoherence timescale. Branching duration is invoked qualitatively as the interval over which environmental interactions produce decohered branches. We acknowledge that this remains an untested correspondence pending a detailed model; the manuscript does not attempt such a derivation because its aim is conceptual suggestion rather than quantitative prediction. revision: no
-
Referee: [Macroscopic tunneling discussion] The extension to macroscopic quantum tunneling in the final section inherits the same un-derived relations and applies them to known data without error analysis or comparison to standard WKB or instanton methods, weakening the quantitative claim.
Authors: The macroscopic section applies the same heuristic identifications to existing experimental data on macroscopic quantum tunneling. We do not perform error analysis or direct comparisons with WKB or instanton calculations because the section is intended to illustrate the interpretive consequences of the framework rather than to refine numerical predictions. We accept that this limits the quantitative strength of the claims and can add an explicit caveat emphasizing the heuristic character of the application. revision: partial
Circularity Check
Tunneling probability and time identified with branch weights and duration by definitional mapping
specific steps
-
self definitional
[Abstract]
"The tunneling probability and the tunneling time are investigated in terms of the tunneled world relative weights and the branching duration, respectively."
Probability is investigated 'in terms of' the relative weights of tunneled worlds, but the weights are defined by the branch splitting itself; the output probability is therefore equivalent to the input branch-weight assignment by construction rather than derived from barrier penetration dynamics.
-
self definitional
[Abstract]
"The observed tunneling is then experienced by the observer located in a tunneled world."
Tunneling is experienced only in the transmitted branch by definition of the framework; the claim reduces to restating the posited splitting rather than predicting an observable from the universal wavefunction.
full rationale
The paper's central results rest on positing decohered reflected/transmitted branches and then directly investigating probability via relative weights and time via branching duration. No explicit derivation from the time-dependent Schrödinger equation or standard tunneling formulas is supplied; the identifications function as redefinitions within the Everettian framing rather than independent predictions. The splitting assumption carries the load without further dynamical justification, producing partial circularity in the claimed observables.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption The universal wavefunction splits into decohered reflected and transmitted branches under the environmental effect after encountering a potential barrier.
Lean theorems connected to this paper
-
IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
The tunneling probability and the tunneling time are investigated in terms of the tunneled world relative weights and the branching duration, respectively.
-
IndisputableMonolith/Foundation/RealityFromDistinction.leanreality_from_one_distinction unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
branching duration tau_B from Delta E_B and time-energy uncertainty
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
Works this paper leans on
-
[1]
Born, ”On the Quantum Mechanics of Collision Processes”, Zeitschrift fur Physik
M. Born, ”On the Quantum Mechanics of Collision Processes”, Zeitschrift fur Physik. 37 (12): 863–867 (1926)
work page 1926
-
[2]
R. Feynman, R. Leighton, M. Sands, ”The Feynman Lectures on Physics”. Vol. 3. Cali- fornia Institute of Technology. ISBN 978-0201500646 (1964)
work page 1964
-
[3]
Jaeger, ”What in the (quantum) world is macroscopic?”, American Journal of Physics
G. Jaeger, ”What in the (quantum) world is macroscopic?”, American Journal of Physics. 82 (9): 896–905 (2014)
work page 2014
-
[4]
A. Einstein, B. Podolsky and N. Rosen, ”Can quantum- mechanical description of phys- ical reality be considered complete?”, Phys. Rev. 47 777-80 (1935)
work page 1935
-
[5]
H Zurek, ”Environment-induced superselection rules”, Phys
W. H Zurek, ”Environment-induced superselection rules”, Phys. Rev. D. 26 1862 (1982)
work page 1982
-
[6]
H. B. G. Casimir, ”On the attraction between two perfectly conducting plates”, Pro- ceedings of the Koninklijke Nederlandse Akademie van Wetenschappen, Series B, 51(6), 793-795 (1948)
work page 1948
-
[7]
Gamow, ”Zur Quantentheorie des Atomkernes.” Zeitschrift f ¨ur Physik, 51(3-4), 204- 212 (1928)
G. Gamow, ”Zur Quantentheorie des Atomkernes.” Zeitschrift f ¨ur Physik, 51(3-4), 204- 212 (1928)
work page 1928
-
[8]
J. A. Wheeler,, & R. P . Feynman, ”Interaction with the Absorber as the Mechanism of Radiation”, Reviews of Modern Physics, 17(2), 157-181 (1945); 13
work page 1945
-
[9]
R. P . Feynman, ”The Feynman Lectures on Physics”, Volume 3: Quantum Mechanics. Addison-Wesley (1965)
work page 1965
-
[10]
R. Landauer and Th. Martin, ”Barrier interaction time in tunneling ”, Rev. Mod. Phys. 66, 217 (1994)
work page 1994
-
[11]
A. M. Steinberg, P . G. Kwiat, and R. Y. Chiao, ”Measurement of the single-photon tun- neling time”, Phys. Rev. Lett. 71, 708 (1993)
work page 1993
-
[12]
A. Enders and G. Nimtz, ”Zero-time tunneling of evanescent mode packets”, J. Phys. I France 3, 1089 (1993)
work page 1993
-
[13]
A. Ranfagni, P . Fabeni, G.P . Pazzi, and D. Mugnai, ”Anomalous pulse delay in mi- crowave propagation”, Phys. Rev. E 48, 1453 (1993)
work page 1993
-
[14]
Steinberg, ”Quantum tunnelling time and the speed of light”, Physics World 16, (12), 19 (2003)
A.M. Steinberg, ”Quantum tunnelling time and the speed of light”, Physics World 16, (12), 19 (2003)
work page 2003
-
[15]
Bohm, ”Quantum Theory”, Prentice-Hall, Upper Saddle River (1951)
D. Bohm, ”Quantum Theory”, Prentice-Hall, Upper Saddle River (1951)
work page 1951
-
[16]
J. S. Bell, ”On the problem of hidden variables in quantum theory”, Rev. Mod. Phys. 38, 447–452 (1966)
work page 1966
- [17]
-
[18]
D. Verreck, G. Groeseneken, A. Verhulst, ”The Tunnel Field-Effect Transistor, Electrical and Electronics Engineering, (2016)
work page 2016
-
[19]
J. Tersoff and D. R. Hamann, ”Theory of the scanning tunneling microscope”, Phys. Rev. B 31, 805 (1985)
work page 1985
-
[20]
Gamow, ”Zur Quantentheorie des Atomkernes”, Z
G. Gamow, ”Zur Quantentheorie des Atomkernes”, Z. Physik 51, 204 (1928)
work page 1928
-
[21]
M.H. Devoret, D.B. Schwartz, J.M. Martinis, A.J. Leggett, and J. Clarke, ”Resonant Ac- tivation from the Zero-Voltage State of a Current-Biased Josephson Junction”, Physical Review Letters, (1984)
work page 1984
-
[22]
Martinis, Devoret, and Clarke, ”Energy-Level Quantization in the Zero-Voltage State of a Current-Biased Josephson Junction”, Physical Review Letters, (1985)
work page 1985
-
[23]
M. H. Devoret, J. M. Martinis, and J. Clarke, ”Measurements of Macroscopic Quan- tum Tunneling out of the Zero-Voltage State of a Current-Biased Josephson Junction”, Physical Review Letters, (1985); 14
work page 1985
-
[24]
Everett et al., ”The Many-Worlds Interpretation of Quantum Mechanics”, Princeton Series in Physics
H. Everett et al., ”The Many-Worlds Interpretation of Quantum Mechanics”, Princeton Series in Physics. Princeton, NJ: Princeton University Press. p. v. ISBN 0-691-08131-X (1973)
work page 1973
-
[25]
H. Everett, III. ”Relative State Formulation of Quantum Mechanics”, Reviews of Modern Physics, 29(3), 454–462 (1957)
work page 1957
-
[26]
C.M. Caves, C.A. Fuchs, R. Schack, ”Quantum probabilities as Bayesian probabilities”, Phys. Rev. A, 65, 022305 (2002)
work page 2002
-
[27]
Penrose, ”On Gravity’s role in Quantum State Reduction”, General Relativity and Gravitation
R. Penrose, ”On Gravity’s role in Quantum State Reduction”, General Relativity and Gravitation. 28 (5): 581–600 (1996)
work page 1996
-
[28]
M. F. Pusey, J. Barrett, T. Rudolph, ”On the reality of the quantum state”, Nature Physics. 8 (6): 475–478 (2012)
work page 2012
-
[29]
N. Bohr, ”Can Quantum-Mechanical Description of Physical Reality Be Considered Complete?”Physical Review, 48(8), 696–702 (1935)
work page 1935
-
[30]
J. A. Wheeler and W.H. Zurek, ”Quantum theory of measurement”, Princeton series in physics (1983)
work page 1983
-
[31]
W. Heisenberg, ” ¨Uber den anschaulichen Inhalt der quantentheoretischen Kinematik und Mechanik.”Zeitschrift f ¨ur Physik, 43, 172–198 (1927). 15
work page 1927
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.