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Does time follow information? Indications from the zeptosecond birth-time data of H₂

Ram Kirpitch

Published Oct 14, 2026• 0 citations
Publisher

Abstract

We re-analyse the published molecular-frame data of the zeptosecond birth-delay experiment in one-photon double ionization of H₂ at 800 eV [Grundmann et al., Science 370, 339 (2020)]. Four estimators of the zeroth-order fringe phase that are insensitive to the emission envelope give a delay slope of 391 ± 39 (stat) ± 52 (method) ± 50 (zero point) zs, (1.59 ± 0.33) R/c, linear in cos β; the fringe maximum gives (2.06 ± 0.28) R/c. The fast-electron fringe visibility is V = 0.543 ± 0.013. A coherence-scaled transit law, τ_eff = τ_ref/α with α the measured visibility of the analysed wave and τ_ref = R/c, predicts these values without a free parameter. Against the light-phase model and the ab initio time-dependent Schrödinger predictions, the fast-electron data give χ² = 8.2 for 2 degrees of freedom (p = 0.017) for the standard description and χ² = 0.9 (p = 0.63) for the coherence law, a likelihood ratio of 38. The product of visibility and delay, the invariant of the law, is 1.03 ± 0.15 and 0.86 ± 0.18 in units of R/c for the two fast-electron observables, against 1 predicted; correlated ab initio dynamics gives 0.63. The data favour an addition to standard quantum dynamics at the level of 2.4–3.3 standard deviations, confined to the zeptosecond birth window. Two checks that use no fringe-position fit support the result: the smearing of the β-integrated fringe gives a total pattern shift of 511 ± 35 zs, and the visibility differs between forward and backward light directions (0.579 against 0.508, 4.2 standard deviations) while the product of visibility and delay is the same in both halves. The law follows from one principle: the birth completes at the energy spread of the minimal-energy split of the electron's state, which by a theorem of Tóth and Petz is its quantum Fisher information, αΔE, rather than at its variance; the split is realised by the record the event writes into the ion and the second electron, and the effect is confined to the birth window in which that record is written. The birth is an entanglement event: the delay obeys τ_eff √(1 − C²) = τ_ref with C the concurrence of the electron with its record, C = 0.84 for the fast electron. The thesis that accompanies the measurement shows the coherence lost by the fast electron conserved in the electron pair, the balance on which the law rests. We explain why energy measurements of the photoelectric effect could not see the effect, identify three tests in data already recorded (the delay slope across bond length and energy sharing, and Auger-gated K-shell ionization of N₂ at six photon energies), and specify a repetition of the experiment that decides at the five-standard-deviation level.

DOI
10.5281/zenodo.23370670

Related papers

A Proposed Coherence-Time Invariant from Information Conservation and Its Experimental Tests

Ram Kirpitch

Does the zeptosecond birth-time delay of molecular photoemission depend on the quantum coherence of the emitting two-centre superposition? Standard QED answers no: the delay is the geometric light-travel value τ_ref = ξ/c, 247 zs for H₂, independent of the Cohen–Fano fringe visibility α. A single information-geometric postulate (A1: a transition completes a fixed Anandan–Aharonov phase at the rate set by the quantum Fisher information of the state) predicts instead a universal lengthening, τ_eff = τ_ref/α, equivalently the invariant α τ_eff = ξ/c. The published zeptosecond experiment of Grundmann et al. already contains reduced coherence: the fast electron of one-photon double ionization of H₂ has visibility α = 0.543 ± 0.013, for which the law predicts τ_eff ≈ 455 zs, not 247. A re-analysis of the deposited data gives a fringe-phase slope of 391 ± 39 (stat) ± 52 (method) ± 50 (zero point) zs, (1.59 ± 0.33) ξ/c, and a fringe-maximum slope of (2.06 ± 0.28) ξ/c; the invariant is 0.86 ± 0.18 and 1.03 ± 0.15 in units of ξ/c, against 1 predicted and 0.63 from correlated ab initio dynamics. Against the standard description the data give χ² = 8.2 for 2 degrees of freedom (p = 0.017), against the law χ² = 0.9 (p = 0.63), a Bayes factor of 38; a smearing observable that uses no fringe-position fit departs from standard dynamics by 3.3 standard deviations, and the visibility and delay differ between forward and backward light directions with their product unchanged. Standard quantum mechanics gives τ/τ_ref = 1 at every coherence; the data do not, and independently of the explanation proposed here this difference requires examination and explanation. The evidence is at the level of 2.4–3.3 standard deviations, not decisive. The postulate is stated as one principle: the transit completes at the energy spread of the minimal-energy split of the electron's state, which by a theorem of Tóth and Petz is its quantum Fisher information. We identify three tests in data already recorded and keep the alternating differential COLTRIMS α-scan, in which the predicted shift is +48.1 zs at α = 0.837, detectable at 5.1σ, and at ≳9σ over a five-point scan. The completion target of A1 is single-valued, and its two candidate readings, separated by 24–47%, are resolved to ±2% on quantum hardware. On the entanglement route the same law fixes a second observable in the same event, I(e;ion) = 2h(½ + τ_ref/2τ_eff). A null result refutes A1; a positive one would show that physical timing tracks the quantum Fisher information. In addition to the content of the previous version, this version contains a re-analysis of the published experiment of Grundmann et al. and of the accompanying thesis, which strengthens the motivation for the additional experiments proposed here.

•Jun 5, 2026•0 citations

Temporal behavior and quantum Zeno time of an excited state of the hydrogen atom

Paolo Facchi A, Saverio Pascazio

arXiv:quant-ph/9905017•Physics Letters A•Apr 1, 1998•103 citations

Power-Law Holographic Forces and Causal Transport in MERA Quantum Circuits

Jon Cackler

CORRECTION NOTICE (v5, 2026-09-06). The central result of v1-v4 is WITHDRAWN. This record has not been peer reviewed. Issued 2026-09-06 by the author (v5 of this record). This notice was added to the archived record; the manuscript itself is unaltered. This record has not been peer reviewed. What is wrong The force exponent reported here as alpha = 3.92 +/- 0.16 is an artifact of the fitting procedure, not a property of the data. The fit was unweighted least squares in linear space applied to a steeply falling profile, which places 95.8 percent of its objective on the single point at the shortest retained separation. Re-fitting the same data with nothing discarded, changing only the error model, gives 2.82 (relative-error weighting) or 2.89 (log-space regression). Across fifteen combinations of standard estimator and fit window the exponent spans 2.53 to 3.92, and the value published here is the largest of them. What the data show instead, and how firmly The retraction is certain. The replacement is not. On the open 24-site chain the same data give alpha = 2.6 +/- 0.2, where the interval is the spread of a plateau in the local logarithmic slope over six consecutive separations, not a statistical error (the bootstrap error on the published fit to the same data is 0.63); the plateau value was reproduced at 2.5921 by a separately written implementation run on the same recorded state (SIM-2026-073). This is a single geometry at a single size. On a 24-site periodic ring, analysed with chord distance as pre-registered, two probes that are both energy-density-like (Delta = 1) give 1.83 and 2.37 against a CFT two-point value of 2 (SIM-2026-074): one size, not converged, disagreeing with each other by 29 percent, and not attributable to a single operator channel. No corrected exponent is established. The exchange channel is an open question. Treat 2.6 +/- 0.2 as the provisional open-chain value, not as a result. Also withdrawn or voided alpha = 3.92 +/- 0.16 (24 sites) and alpha = 3.97 +/- 0.15 (16 sites, exact) from stress-tensor exchange. Was: headline result and its first corroboration. Now: withdrawn. Why: the same estimator artifact: both move in lockstep under it (3.92 to 2.56, 3.97 to 2.75 on dropping the contact point), because they share one observable, one fit window and one fitting routine. scalar exchange (alpha = 2) excluded. Was: stated as excluded at about 12 sigma. Now: withdrawn. Why: the 12 sigma used the covariance error 0.16; at the bootstrap error 0.63 computed before release the exclusion is about 2.2 sigma, and under any window starting at separation 3 the point estimate itself falls to about 2.56. alpha = 4 is universal; alpha = 4.00 at Ising, tricritical Ising and Potts. Was: confirmed at three classes. Now: withdrawn; the operator towers at all three classes stand. Why: the exponent was measured only at Ising and inherited by the other two; the towers are spectra, not forces. third independent evaluation alpha = 4.07 (chi = 3 MERA), and with it the statement that this was the first holographic force measurement from an optimized tensor network state. Was: supporting evidence and a priority claim. Now: both withdrawn. Why: the profile changes sign inside its own fit window and cannot be a fixed-sign power law; the priority claim rests on that evaluation alone and was never gated against prior work. the discriminating test: stress tensor (Z_j Z_j+1) versus spin primary (X_j). Was: registered killer test. Now: void. Why: at the critical point these are one operator, related by exact Kramers-Wannier self-duality. Measured on the periodic ring: identical expectation values to 1e-15 and identical force profiles to 1e-13 at 14 sites, 2.4e-9 at 24 sites (SIM-2026-074). Open boundaries break the duality, which is why the open-chain run of this test (SIM-2026-073) showed a spurious difference between the two arms. The test compared the energy density to itself. Neither label was correct: Z_j Z_j+1 is the energy density, not the stress tensor; X_j is its dual, not the spin primary. transport time T = (pi/2) l_AdS to 1.2 percent as a geometric prediction. Was: confirmed. Now: measurement stands (T = 2.239 at N = 16); geometric reading not established. Why: l_AdS cancels in the cited derivation, which also gives pi rather than the pi/2 the manuscript compares against; the chi = 3 estimate of l_AdS gives a 57 percent miss; the transport driver never applies a MERA. The true spin primary Z_j was never in the design, and the direct replacement test is blocked: Z_j is odd under the Z2 symmetry, so the energy-difference observable used throughout this work subtracts across symmetry sectors and is undefined for it. A replacement test using two Z2-even probes has been pre-registered (PREREGISTRATION-T.md, committed before its driver) and run; its result is deliberately not part of this correction and will appear in a later version. Not previously reported The published fit has a reduced chi-squared of 6.008 on 9 degrees of freedom, and a bootstrap standard deviation of 0.63 rather than the quoted 0.16. Both were computed before release and omitted. What is unaffected Of the claims in this record: the two-phase optimization method, the chi = 3 criticality threshold, the exact-diagonalization gates, the measured OPE coefficient C_sigma-sigma-epsilon = 0.50 +/- 0.03 against the exact 1/2, and the conformal towers at all three classes. Not part of this record, mentioned only because they are sometimes read together with it: the later C_TTT stress-tensor self-coupling measurements (SIM-2026-067/068/069, dated after this record) and the matched off-critical ring control (SIM-2026-074) are unaffected by this correction and make no claim about the force exponent. How the error was found and what this record contains The error was found by the author's own internal adversarial audit, not by a reviewer; the journal submission it was found after is closed, and no review of this work has taken place. Files in this record: the full re-analysis (SIM-2026-072.json, driver, figure), the pre-registered chain test (SIM-2026-073.json) and ring test (SIM-2026-074.json) with both pre-registrations as committed before the runs, the runnable drivers with their shared module and the negative test suite for their validation gates, and the error register (ERRATA.md). Concept DOI 10.5281/zenodo.19660302 always resolves to the current version. The abstract of the original manuscript follows unchanged, for the record. Every claim in it about the force exponent should be read against the correction above. We report results from classical simulation of critical spin chains that establish quantitative physical content in the MERA-AdS correspondence. First, the interaction energy between boundary-primary excitations follows a power law F(dr) ~ dr^(-alpha) with three consistent evaluations yielding alpha = 3.92 +/- 0.16 (24q), 3.97 +/- 0.15 (16q), and 4.07 +/- 0.18 (16q chi=3 MERA), all consistent with stress-tensor exchange (alpha = 2*Delta_T = 4) and inconsistent with scalar exchange (alpha = 2); the exponent is explained by the Ising CFT fusion rule eps x eps = [1]. Because Delta_T = 2 is fixed by conformal symmetry in every unitary 2D CFT, alpha = 4 is universal: we confirm this at two further fixed points - the tricritical Ising model (c = 7/10), where a scale-invariant MERA recovers the full M(4,5) primary spectrum (Delta_sigma = 0.092, Delta_eps = 0.204, Delta_T = 1.999), and the three-state Potts model (c = 4/5), where a Z3-symmetric MERA at chi = 12 recovers Delta_sigma = 0.134, Delta_eps = 0.805, Delta_T = 2.001 - giving alpha = 4.00 at all three universality classes. Second, the holographic transport time matches the AdS_3 null geodesic prediction T = (pi/2) l_AdS to 1.2% at N = 16 sites on a time-grid-converged measurement, with the residual shrinking from 2.8% at N = 12. Third, we introduce a two-phase optimization method (ALM + Z2 projection) for Z2-symmetric MERA ground states at 24 qubits. Fourth, extending the MERA bond dimension from chi=2 to chi=3 overcomes the expressibility barrier, achieving 0.15% energy error at 16 qubits and enabling the first holographic force measurement from an optimized tensor network state. The OPE coefficient is also measured directly from the fixed-point tensors: C_sigma-sigma-eps = 0.50 +/- 0.03 against the exact Ising value 1/2. A hardware path is designed for Quantinuum Helios (57 CNOTs, 0.57% logical error). Version 4 changes (relative to v3): Transport: N=16 residual restated as the time-grid-converged value of -1.21% (dt = 1e-3), with -2.78% at N=12 showing the finite-size trend; the 0.72% figure in v3 was an artifact of the dt = 0.05 integration grid and is now labeled as such. The N=24 transport point carries a new reliability caveat (double-lobe trace structure). The l_AdS comparison table is recomputed against the converged transport time (best fit 1.425, deviation 1.21%). Effective-mass derivation rewritten in a consistent AdS3 convention m^2 l^2 = Delta(Delta-2); m_eff = 0.693 = 1/l_AdS follows from Delta = 1 exactly. NEW: universality section extended to a third fixed point - a Z3-symmetric MERA at chi = 12 recovers the three-state Potts (c = 4/5) tower, giving alpha = 4.00 at all three universality classes (c = 1/2, 7/10, 4/5). NEW: the OPE coefficient C_sigma-sigma-eps = 0.50 +/- 0.03 measured directly from the fixed-point tensors, with C_sigma-sigma-sigma = 0 at machine precision as the Z2 structural check. Supplemental table row SIM-007 annotated (record lost; script preserved); data availability expanded; Zenodo DOI added to the front matter.

•Apr 20, 2026•1 citation

Electron Wave Trajectories Within Schrodinger’s Hydrogen Atom, and Relativistic Consequences

Leslie Smith

Foundations of Physics•Aug 26, 2023•0 citations

Coherence effects of diatomic homonuclear molecules and sequential two-photon processes of noble gases in the photoionization

Gregor Hartmann

Bei der atomaren und molekularen Photoionisation werden Elektronen und Ionen erzeugt, die mit Flugzeitspektroskopie hinsichtlich des Wirkungsquerschnitts und der Winkelverteilung untersucht werden können. Die Elektronenwinkelverteilungen von beiden Ionisationsstufen bei der sequentiellen Doppelionisation in Edelgasen werden in einem Photonenenergiebereich von 38 - 91 eV analysiert. Die Winkelabhängigkeit der emittierten Photoelektronen wird durch die Drehimpulsübertragung vom Photon an das Elektron verursacht. Bei der Doppelionisation durch zwei Photonen führt der totale Drehimpulstransfer zu einem Legendre Polynom vierter Ordnung. Dieser sogenannte \beta_4-Term hat einen Gewichtungsfaktor, der durch das Alignment des in der ersten Ionisationsstufe erzeugten Ions gegeben ist. Interessanterweise zeigt sich, dass dieser zusätzliche Term nicht nur die Winkelverteilung der zweiten Stufe beeinflusst, sondern ebenfalls die der ersten, die durch nur ein Photon erzeugt wird, was auf eine kohärente Koppelung beider Prozesse schließen lässt. Dieser Effekt wird für die Zwei-Photonen-Doppelionisation der Edelgase Neon, Argon und Krypton gezeigt, wobei die Messungen am FLASH in einer Kugelkammer mit 19 unabhängig voneinander arbeitenden Elektronenflugzeitspektrometern ausgeführt wurden. Die Winkelverteilung von 1s-Schalen-Photoionisation in Helium sollte kein \beta_4-Verhalten aufweisen, da sowohl das neutrale Atom wie auch das einfach geladene Ion eine isotrope Elektronenverteilung haben, was durch Messungen bei 79 eV und 91 eV bestätigt wird. Jedoch wird bei einer Photonenenergie von 61 eV in beiden Stufen ein starker \beta_4-Effekt beobachtet. Dieses unerwartete Ergebnis wird als induziert durch eine autoionisierende Doppelanregungsresonanz in Helium interpretiert. Da bei den FEL-Experimenten sehr große Datenmengen aufgenommen werden, wurde eine auf CUDA basierende Auswertungs- und Visualisierungssoftware entwickelt, die detailliert diskutiert wird. Die Analogie von homonuklearen zweiatomigen Molekülen zu dem Young'schen Doppelspaltexperiment war Gegenstand vieler wissenschaftlicher Photoionisationsuntersuchungen. Ein Beispiel sind Wirkungsquerschnittoszillationen in der Photoionisation von N2, die von Cohen und Fano als Interferenzerscheinung interpretiert wurde. Diese Zwei-Zentren-Interferenz wird durch Nichtlokalität der Elektronen in einem homonuklearen Molekül verursacht. Gegenstand dieser Arbeit ist die Untersuchung relativer Wirkungsquerschnittoszillationen im Wasserstoffmolekül H2 über einen weiten Photonenenergiebereich (29 - 1200 eV). Dabei wird zwischen dem zufällig im Raum verteilten Molekül und dem orientierten Target, bei dem die Orientierung der Molekülachse zu dem Polarisationsvektor des Lichts bestimmt wird, unterschieden. Ein Übergangseffekt von zufällig verteilten zu orientierten Targeteigenschaften wird beobachtet, wenn die de Broglie Wellenlänge des Photoelektrons die Molekülbindungslänge auflöst. Die durch den \beta_m Parameter beschriebene Winkelverteilung der Ionenfragmente wird analysiert und als Grund für den Übergangseffekt bestimmt. Bei hohen Photonenenergien konvergiert der \beta_m Parameter gegen -1, was eine bevorzugte Orientierung des Moleküls zur Polarisationsachse für den Ionisationsvorgang zur Folge hat. Es wurden mehrere Varianten von Ionenflugzeitdetektoren mit der Option auf Koinzidenzbetrieb mit einem Elektronenflugzeitspektrometer benutzt. Die Experimente wurden bei BESSY II und PETRA III ausgeführt. Ein gleichartiger Übergangseffekt wird in Innerschalenionisationdaten von N2 beobachtet.

•Apr 14, 2014•6 citations

A Trajectory Density Formula for the Double-Slit Interference Pattern: Source Temperature, Coherence, and a New Energy-Dependent Visibility Prediction

Apostolos Douzenis

We propose a trajectory density formulation of the double-slit interference pattern that reproduces observed fringe intensities without wave superposition. The intensity at screen position x is the weighted density of particle trajectories arriving there, suppressed exponentially by the deflection cost in energy space: I(x) = V_{Trit}(KE) \times \sum_n w_n \cdot \delta\!\left(x - \frac{n\lambda L}{d}\right) \cdot e^{-k|n|} where k = dθ_eff/λ_dB is the coherence parameter set by the effective illumination semiangle θ_eff, and V_Trit(KE) = 2γβ/(1+γ²β²) is a new energy-dependent visibility factor from the Trit framework [1–3]. The parameter k connects to the effective source temperature through the emission physics: higher source temperature → larger emission area → larger θ_eff → larger k → fewer visible fringes. We test the formula against five independent experiments across five orders of magnitude in particle energy and three particle types. For thermionic and Schottky electron sources the formula outperforms standard QM by a factor of 2–6× in R². For cold FEG sources and C60 molecules the formula correctly reduces to QM (k → 0). The C60 result leads to a clean new distinction: V_Trit(KE) applies to elementary particles, where the energy space geometry directly governs wave-particle balance; for composite particles V_Trit = 1 and interference is from the centre-of-mass de Broglie wave. This difference is falsifiable: varying electron energy should reveal a visibility peak at KE = 211.66 keV; varying C60 velocity should show no such peak.

•Jun 12, 2026•0 citations
We re-analyse the published molecular-frame data of the zeptosecond birth-delay experiment in one-photon double ionization of H₂ at 800 eV [Grundmann et al., Science 370, 339 (2020)]. Four estimators of the zeroth-order fringe phase that are insensitive to the emission envelope give a delay slope of 391 ± 39 (stat) ± 52 (method) ± 50 (zero point) zs, (1.59 ± 0.33) R/c, linear in cos β; the fringe maximum gives (2.06 ± 0.28) R/c. The fast-electron fringe visibility is V = 0.543 ± 0.013. A coherence-scaled transit law, τ_eff = τ_ref/α with α the measured visibility of the analysed wave and τ_ref = R/c, predicts these values without a free parameter. Against the light-phase model and the ab initio time-dependent Schrödinger predictions, the fast-electron data give χ² = 8.2 for 2 degrees of freedom (p = 0.017) for the standard description and χ² = 0.9 (p = 0.63) for the coherence law, a likelihood ratio of 38. The product of visibility and delay, the invariant of the law, is 1.03 ± 0.15 and 0.86 ± 0.18 in units of R/c for the two fast-electron observables, against 1 predicted; correlated ab initio dynamics gives 0.63. The data favour an addition to standard quantum dynamics at the level of 2.4–3.3 standard deviations, confined to the zeptosecond birth window. Two checks that use no fringe-position fit support the result: the smearing of the β-integrated fringe gives a total pattern shift of 511 ± 35 zs, and the visibility differs between forward and backward light directions (0.579 against 0.508, 4.2 standard deviations) while the product of visibility and delay is the same in both halves. The law follows from one principle: the birth completes at the energy spread of the minimal-energy split of the electron's state, which by a theorem of Tóth and Petz is its quantum Fisher information, αΔE, rather than at its variance; the split is realised by the record the event writes into the ion and the second electron, and the effect is confined to the birth window in which that record is written. The birth is an entanglement event: the delay obeys τ_eff √(1 − C²) = τ_ref with C the concurrence of the electron with its record, C = 0.84 for the fast electron. The thesis that accompanies the measurement shows the coherence lost by the fast electron conserved in the electron pair, the balance on which the law rests. We explain why energy measurements of the photoelectric effect could not see the effect, identify three tests in data already recorded (the delay slope across bond length and energy sharing, and Auger-gated K-shell ionization of N₂ at six photon energies), and specify a repetition of the experiment that decides at the five-standard-deviation level.
Does the zeptosecond birth-time delay of molecular photoemission depend on the quantum coherence of the emitting two-centre superposition? Standard QED answers no: the delay is the geometric light-travel value τ_ref = ξ/c, 247 zs for H₂, independent of the Cohen–Fano fringe visibility α. A single information-geometric postulate (A1: a transition completes a fixed Anandan–Aharonov phase at the rate set by the quantum Fisher information of the state) predicts instead a universal lengthening, τ_eff = τ_ref/α, equivalently the invariant α τ_eff = ξ/c. The published zeptosecond experiment of Grundmann et al. already contains reduced coherence: the fast electron of one-photon double ionization of H₂ has visibility α = 0.543 ± 0.013, for which the law predicts τ_eff ≈ 455 zs, not 247. A re-analysis of the deposited data gives a fringe-phase slope of 391 ± 39 (stat) ± 52 (method) ± 50 (zero point) zs, (1.59 ± 0.33) ξ/c, and a fringe-maximum slope of (2.06 ± 0.28) ξ/c; the invariant is 0.86 ± 0.18 and 1.03 ± 0.15 in units of ξ/c, against 1 predicted and 0.63 from correlated ab initio dynamics. Against the standard description the data give χ² = 8.2 for 2 degrees of freedom (p = 0.017), against the law χ² = 0.9 (p = 0.63), a Bayes factor of 38; a smearing observable that uses no fringe-position fit departs from standard dynamics by 3.3 standard deviations, and the visibility and delay differ between forward and backward light directions with their product unchanged. Standard quantum mechanics gives τ/τ_ref = 1 at every coherence; the data do not, and independently of the explanation proposed here this difference requires examination and explanation. The evidence is at the level of 2.4–3.3 standard deviations, not decisive. The postulate is stated as one principle: the transit completes at the energy spread of the minimal-energy split of the electron's state, which by a theorem of Tóth and Petz is its quantum Fisher information. We identify three tests in data already recorded and keep the alternating differential COLTRIMS α-scan, in which the predicted shift is +48.1 zs at α = 0.837, detectable at 5.1σ, and at ≳9σ over a five-point scan. The completion target of A1 is single-valued, and its two candidate readings, separated by 24–47%, are resolved to ±2% on quantum hardware. On the entanglement route the same law fixes a second observable in the same event, I(e;ion) = 2h(½ + τ_ref/2τ_eff). A null result refutes A1; a positive one would show that physical timing tracks the quantum Fisher information. In addition to the content of the previous version, this version contains a re-analysis of the published experiment of Grundmann et al. and of the accompanying thesis, which strengthens the motivation for the additional experiments proposed here.
CORRECTION NOTICE (v5, 2026-09-06). The central result of v1-v4 is WITHDRAWN. This record has not been peer reviewed. Issued 2026-09-06 by the author (v5 of this record). This notice was added to the archived record; the manuscript itself is unaltered. This record has not been peer reviewed. What is wrong The force exponent reported here as alpha = 3.92 +/- 0.16 is an artifact of the fitting procedure, not a property of the data. The fit was unweighted least squares in linear space applied to a steeply falling profile, which places 95.8 percent of its objective on the single point at the shortest retained separation. Re-fitting the same data with nothing discarded, changing only the error model, gives 2.82 (relative-error weighting) or 2.89 (log-space regression). Across fifteen combinations of standard estimator and fit window the exponent spans 2.53 to 3.92, and the value published here is the largest of them. What the data show instead, and how firmly The retraction is certain. The replacement is not. On the open 24-site chain the same data give alpha = 2.6 +/- 0.2, where the interval is the spread of a plateau in the local logarithmic slope over six consecutive separations, not a statistical error (the bootstrap error on the published fit to the same data is 0.63); the plateau value was reproduced at 2.5921 by a separately written implementation run on the same recorded state (SIM-2026-073). This is a single geometry at a single size. On a 24-site periodic ring, analysed with chord distance as pre-registered, two probes that are both energy-density-like (Delta = 1) give 1.83 and 2.37 against a CFT two-point value of 2 (SIM-2026-074): one size, not converged, disagreeing with each other by 29 percent, and not attributable to a single operator channel. No corrected exponent is established. The exchange channel is an open question. Treat 2.6 +/- 0.2 as the provisional open-chain value, not as a result. Also withdrawn or voided alpha = 3.92 +/- 0.16 (24 sites) and alpha = 3.97 +/- 0.15 (16 sites, exact) from stress-tensor exchange. Was: headline result and its first corroboration. Now: withdrawn. Why: the same estimator artifact: both move in lockstep under it (3.92 to 2.56, 3.97 to 2.75 on dropping the contact point), because they share one observable, one fit window and one fitting routine. scalar exchange (alpha = 2) excluded. Was: stated as excluded at about 12 sigma. Now: withdrawn. Why: the 12 sigma used the covariance error 0.16; at the bootstrap error 0.63 computed before release the exclusion is about 2.2 sigma, and under any window starting at separation 3 the point estimate itself falls to about 2.56. alpha = 4 is universal; alpha = 4.00 at Ising, tricritical Ising and Potts. Was: confirmed at three classes. Now: withdrawn; the operator towers at all three classes stand. Why: the exponent was measured only at Ising and inherited by the other two; the towers are spectra, not forces. third independent evaluation alpha = 4.07 (chi = 3 MERA), and with it the statement that this was the first holographic force measurement from an optimized tensor network state. Was: supporting evidence and a priority claim. Now: both withdrawn. Why: the profile changes sign inside its own fit window and cannot be a fixed-sign power law; the priority claim rests on that evaluation alone and was never gated against prior work. the discriminating test: stress tensor (Z_j Z_j+1) versus spin primary (X_j). Was: registered killer test. Now: void. Why: at the critical point these are one operator, related by exact Kramers-Wannier self-duality. Measured on the periodic ring: identical expectation values to 1e-15 and identical force profiles to 1e-13 at 14 sites, 2.4e-9 at 24 sites (SIM-2026-074). Open boundaries break the duality, which is why the open-chain run of this test (SIM-2026-073) showed a spurious difference between the two arms. The test compared the energy density to itself. Neither label was correct: Z_j Z_j+1 is the energy density, not the stress tensor; X_j is its dual, not the spin primary. transport time T = (pi/2) l_AdS to 1.2 percent as a geometric prediction. Was: confirmed. Now: measurement stands (T = 2.239 at N = 16); geometric reading not established. Why: l_AdS cancels in the cited derivation, which also gives pi rather than the pi/2 the manuscript compares against; the chi = 3 estimate of l_AdS gives a 57 percent miss; the transport driver never applies a MERA. The true spin primary Z_j was never in the design, and the direct replacement test is blocked: Z_j is odd under the Z2 symmetry, so the energy-difference observable used throughout this work subtracts across symmetry sectors and is undefined for it. A replacement test using two Z2-even probes has been pre-registered (PREREGISTRATION-T.md, committed before its driver) and run; its result is deliberately not part of this correction and will appear in a later version. Not previously reported The published fit has a reduced chi-squared of 6.008 on 9 degrees of freedom, and a bootstrap standard deviation of 0.63 rather than the quoted 0.16. Both were computed before release and omitted. What is unaffected Of the claims in this record: the two-phase optimization method, the chi = 3 criticality threshold, the exact-diagonalization gates, the measured OPE coefficient C_sigma-sigma-epsilon = 0.50 +/- 0.03 against the exact 1/2, and the conformal towers at all three classes. Not part of this record, mentioned only because they are sometimes read together with it: the later C_TTT stress-tensor self-coupling measurements (SIM-2026-067/068/069, dated after this record) and the matched off-critical ring control (SIM-2026-074) are unaffected by this correction and make no claim about the force exponent. How the error was found and what this record contains The error was found by the author's own internal adversarial audit, not by a reviewer; the journal submission it was found after is closed, and no review of this work has taken place. Files in this record: the full re-analysis (SIM-2026-072.json, driver, figure), the pre-registered chain test (SIM-2026-073.json) and ring test (SIM-2026-074.json) with both pre-registrations as committed before the runs, the runnable drivers with their shared module and the negative test suite for their validation gates, and the error register (ERRATA.md). Concept DOI 10.5281/zenodo.19660302 always resolves to the current version. The abstract of the original manuscript follows unchanged, for the record. Every claim in it about the force exponent should be read against the correction above. We report results from classical simulation of critical spin chains that establish quantitative physical content in the MERA-AdS correspondence. First, the interaction energy between boundary-primary excitations follows a power law F(dr) ~ dr^(-alpha) with three consistent evaluations yielding alpha = 3.92 +/- 0.16 (24q), 3.97 +/- 0.15 (16q), and 4.07 +/- 0.18 (16q chi=3 MERA), all consistent with stress-tensor exchange (alpha = 2*Delta_T = 4) and inconsistent with scalar exchange (alpha = 2); the exponent is explained by the Ising CFT fusion rule eps x eps = [1]. Because Delta_T = 2 is fixed by conformal symmetry in every unitary 2D CFT, alpha = 4 is universal: we confirm this at two further fixed points - the tricritical Ising model (c = 7/10), where a scale-invariant MERA recovers the full M(4,5) primary spectrum (Delta_sigma = 0.092, Delta_eps = 0.204, Delta_T = 1.999), and the three-state Potts model (c = 4/5), where a Z3-symmetric MERA at chi = 12 recovers Delta_sigma = 0.134, Delta_eps = 0.805, Delta_T = 2.001 - giving alpha = 4.00 at all three universality classes. Second, the holographic transport time matches the AdS_3 null geodesic prediction T = (pi/2) l_AdS to 1.2% at N = 16 sites on a time-grid-converged measurement, with the residual shrinking from 2.8% at N = 12. Third, we introduce a two-phase optimization method (ALM + Z2 projection) for Z2-symmetric MERA ground states at 24 qubits. Fourth, extending the MERA bond dimension from chi=2 to chi=3 overcomes the expressibility barrier, achieving 0.15% energy error at 16 qubits and enabling the first holographic force measurement from an optimized tensor network state. The OPE coefficient is also measured directly from the fixed-point tensors: C_sigma-sigma-eps = 0.50 +/- 0.03 against the exact Ising value 1/2. A hardware path is designed for Quantinuum Helios (57 CNOTs, 0.57% logical error). Version 4 changes (relative to v3): Transport: N=16 residual restated as the time-grid-converged value of -1.21% (dt = 1e-3), with -2.78% at N=12 showing the finite-size trend; the 0.72% figure in v3 was an artifact of the dt = 0.05 integration grid and is now labeled as such. The N=24 transport point carries a new reliability caveat (double-lobe trace structure). The l_AdS comparison table is recomputed against the converged transport time (best fit 1.425, deviation 1.21%). Effective-mass derivation rewritten in a consistent AdS3 convention m^2 l^2 = Delta(Delta-2); m_eff = 0.693 = 1/l_AdS follows from Delta = 1 exactly. NEW: universality section extended to a third fixed point - a Z3-symmetric MERA at chi = 12 recovers the three-state Potts (c = 4/5) tower, giving alpha = 4.00 at all three universality classes (c = 1/2, 7/10, 4/5). NEW: the OPE coefficient C_sigma-sigma-eps = 0.50 +/- 0.03 measured directly from the fixed-point tensors, with C_sigma-sigma-sigma = 0 at machine precision as the Z2 structural check. Supplemental table row SIM-007 annotated (record lost; script preserved); data availability expanded; Zenodo DOI added to the front matter.
Bei der atomaren und molekularen Photoionisation werden Elektronen und Ionen erzeugt, die mit Flugzeitspektroskopie hinsichtlich des Wirkungsquerschnitts und der Winkelverteilung untersucht werden können. Die Elektronenwinkelverteilungen von beiden Ionisationsstufen bei der sequentiellen Doppelionisation in Edelgasen werden in einem Photonenenergiebereich von 38 - 91 eV analysiert. Die Winkelabhängigkeit der emittierten Photoelektronen wird durch die Drehimpulsübertragung vom Photon an das Elektron verursacht. Bei der Doppelionisation durch zwei Photonen führt der totale Drehimpulstransfer zu einem Legendre Polynom vierter Ordnung. Dieser sogenannte \beta_4-Term hat einen Gewichtungsfaktor, der durch das Alignment des in der ersten Ionisationsstufe erzeugten Ions gegeben ist. Interessanterweise zeigt sich, dass dieser zusätzliche Term nicht nur die Winkelverteilung der zweiten Stufe beeinflusst, sondern ebenfalls die der ersten, die durch nur ein Photon erzeugt wird, was auf eine kohärente Koppelung beider Prozesse schließen lässt. Dieser Effekt wird für die Zwei-Photonen-Doppelionisation der Edelgase Neon, Argon und Krypton gezeigt, wobei die Messungen am FLASH in einer Kugelkammer mit 19 unabhängig voneinander arbeitenden Elektronenflugzeitspektrometern ausgeführt wurden. Die Winkelverteilung von 1s-Schalen-Photoionisation in Helium sollte kein \beta_4-Verhalten aufweisen, da sowohl das neutrale Atom wie auch das einfach geladene Ion eine isotrope Elektronenverteilung haben, was durch Messungen bei 79 eV und 91 eV bestätigt wird. Jedoch wird bei einer Photonenenergie von 61 eV in beiden Stufen ein starker \beta_4-Effekt beobachtet. Dieses unerwartete Ergebnis wird als induziert durch eine autoionisierende Doppelanregungsresonanz in Helium interpretiert. Da bei den FEL-Experimenten sehr große Datenmengen aufgenommen werden, wurde eine auf CUDA basierende Auswertungs- und Visualisierungssoftware entwickelt, die detailliert diskutiert wird. Die Analogie von homonuklearen zweiatomigen Molekülen zu dem Young'schen Doppelspaltexperiment war Gegenstand vieler wissenschaftlicher Photoionisationsuntersuchungen. Ein Beispiel sind Wirkungsquerschnittoszillationen in der Photoionisation von N2, die von Cohen und Fano als Interferenzerscheinung interpretiert wurde. Diese Zwei-Zentren-Interferenz wird durch Nichtlokalität der Elektronen in einem homonuklearen Molekül verursacht. Gegenstand dieser Arbeit ist die Untersuchung relativer Wirkungsquerschnittoszillationen im Wasserstoffmolekül H2 über einen weiten Photonenenergiebereich (29 - 1200 eV). Dabei wird zwischen dem zufällig im Raum verteilten Molekül und dem orientierten Target, bei dem die Orientierung der Molekülachse zu dem Polarisationsvektor des Lichts bestimmt wird, unterschieden. Ein Übergangseffekt von zufällig verteilten zu orientierten Targeteigenschaften wird beobachtet, wenn die de Broglie Wellenlänge des Photoelektrons die Molekülbindungslänge auflöst. Die durch den \beta_m Parameter beschriebene Winkelverteilung der Ionenfragmente wird analysiert und als Grund für den Übergangseffekt bestimmt. Bei hohen Photonenenergien konvergiert der \beta_m Parameter gegen -1, was eine bevorzugte Orientierung des Moleküls zur Polarisationsachse für den Ionisationsvorgang zur Folge hat. Es wurden mehrere Varianten von Ionenflugzeitdetektoren mit der Option auf Koinzidenzbetrieb mit einem Elektronenflugzeitspektrometer benutzt. Die Experimente wurden bei BESSY II und PETRA III ausgeführt. Ein gleichartiger Übergangseffekt wird in Innerschalenionisationdaten von N2 beobachtet.
We propose a trajectory density formulation of the double-slit interference pattern that reproduces observed fringe intensities without wave superposition. The intensity at screen position x is the weighted density of particle trajectories arriving there, suppressed exponentially by the deflection cost in energy space: I(x) = V_{Trit}(KE) \times \sum_n w_n \cdot \delta\!\left(x - \frac{n\lambda L}{d}\right) \cdot e^{-k|n|} where k = dθ_eff/λ_dB is the coherence parameter set by the effective illumination semiangle θ_eff, and V_Trit(KE) = 2γβ/(1+γ²β²) is a new energy-dependent visibility factor from the Trit framework [1–3]. The parameter k connects to the effective source temperature through the emission physics: higher source temperature → larger emission area → larger θ_eff → larger k → fewer visible fringes. We test the formula against five independent experiments across five orders of magnitude in particle energy and three particle types. For thermionic and Schottky electron sources the formula outperforms standard QM by a factor of 2–6× in R². For cold FEG sources and C60 molecules the formula correctly reduces to QM (k → 0). The C60 result leads to a clean new distinction: V_Trit(KE) applies to elementary particles, where the energy space geometry directly governs wave-particle balance; for composite particles V_Trit = 1 and interference is from the centre-of-mass de Broglie wave. This difference is falsifiable: varying electron energy should reveal a visibility peak at KE = 211.66 keV; varying C60 velocity should show no such peak.