Quantum Decay Tail: How the Memory of Birth Depends on Color ✛

Original: "Quantum Late-Time Decay and Channel Dependence"
arXiv:2509.17163 · 2025-09-21 · CC BY 4.0 · 3 min
Fluorescence of two dyes showed that the late power-law decay in different spectral channels has different exponents, even though the lifetime is the same.

Context

Deviations from exponential decay are a long-standing prediction of quantum mechanics. At short times, decay slows down (the Zeno effect); at long times, it transitions into a power-law tail. Experimental confirmations are scarce: for short times, there are experiments with tunneling of sodium atoms; for long times, fluorescence of rhodamine and polyfluorene. Alongside this work, the archive contains studies on quantum memory, gravitational tails, and quantum decay in various systems. This article fills a gap: independent confirmation of the late power-law decay and the first case where two channels of the same decay show different exponents.

Methods

The experiment was performed on an inverted confocal microscope Nikon Eclipse Ti-E with a picosecond laser diode (438 nm) for excitation. Fluorescence was collected through two hybrid detectors PicoQuant PMA Hybrid 40, separated by a dichroic mirror and bandpass filters 520/35 nm and 600/50 nm. Photon counting was done using time-correlated single photon counting with a PicoHarp 300 module. Solutions of five dyes (fluorescein, acridine orange, rhodamine B, erythrosine B, eosin Y) in methanol or water at a concentration of 10⁻⁵ mol/dm³. Data were fitted with two models: a double exponential and an exponential plus power law. Fit quality was assessed by the chi-square criterion.

Results

For erythrosine B and eosin Y, the nonexponential model (exponential plus power-law tail) gave significantly better agreement with the data than the double exponential. The lifetime τ was the same for both channels: about 0.448 ns for erythrosine B and 1.054 ns for eosin Y. The power-law exponent β differed: for erythrosine B, 1.559±0.014 in channel 1 and 2.019±0.017 in channel 2; for eosin Y, 1.512±0.019 and 1.845±0.051, respectively. The power-law tail appeared after about 10 lifetimes. A theoretical model with a threshold spectral density of the form ρ(E) ∝ (E−Eth)^γ with γ<0 reproduces the observed β in the range 1<β<3. Multichannel analysis shows that the late channel intensities behave as $t^{-(2γ_{i+3})}$ for one channel and $t^{-(γ_1+γ_{2+3})}$ for the other, explaining the difference in exponents.

Implications

This work provides the first direct experimental confirmation of channel dependence in late nonexponential decay. It generalizes previous results that considered only a single channel. The theoretical conclusion is universal: for any quantum decay with multiple channels, the lifetime is the same, but the power-law tails depend on the channel. This changes our understanding of late-stage decay in molecular physics, nuclear physics, and particle physics.

Future development

Possible directions: testing the predicted oscillations in the spectral density at high temporal resolution, studying the influence of state preparation conditions on the shape of the tail, extending to quantum tunneling and nuclear decays. It is also interesting to investigate the transition to a continuous spectrum of channels and the effect of thresholds.

Impact

The results are important for quantum optics, molecular spectroscopy, and the physics of unstable states. They may affect the interpretation of fluorescence measurements in biology and chemistry.

Next steps

Check oscillations in survival at higher resolution, change excitation conditions to determine the origin of the anomalous spectral density, and extend measurements to other dyes.

Key open problems

In quantum mechanics, the question remains open about the physical mechanism that forms the spectral density diverging at the threshold. It is unclear whether it is related to the state preparation process or to internal interactions. Also, the connection between channel dependence and the system's memory of the moment of birth requires clarification.

The knowledge machine's view

This section is addressed to the author of the paper and their colleagues. Neighbouring works were found by meaning-based search across our archive, not by word overlap. We do not review: we show the field around the work.

What the work does

The study records a late power-law tail in the fluorescence of erythrosine B and eosin Y after about ten lifetimes. Two detectors tuned to different spectral windows yielded different power-law exponents (about 1.5 and 2.0), while the lifetime in both channels was the same. Theoretical analysis explains the difference in exponents through multichannel decay with a threshold spectral density.

Where its strength is

For the first time, the dependence of the late power-law decay exponent on the observation channel is directly demonstrated, confirming theoretical predictions about non-exponential tails in multichannel systems.

Where it could go next

Worth trying

  • Test whether the difference in exponents persists when the polarization of excitation or detection is varied.
  • Investigate the dependence of the exponent on dye concentration to reveal possible collective effects.
  • Try to describe the data with a model featuring a continuous spectrum of threshold states, varying the parameter γ for different channels.

The late power-law tail means that a quantum system remembers the moment of its birth even after dozens of lifetimes. In the experiment, photon counting continued up to 95 nanoseconds, which corresponds to about 200 lifetimes for erythrosine B.

In Stanislaw Lem's novel 'Solaris', the ocean manifests memory of the past in unexpected forms. Here, a quantum system also retains memory of the moment of birth, but manifests it in a channel-dependent power-law decay tail.

\beta = 2\gamma + 3
β determines the slope of the power-law tail of the decay intensity
I_1(t) \propto t^{-(2\gamma_1+3)}
Channel 1 decays by a power law with an exponent determined by its own γ
I_2(t) \propto t^{-(\gamma_1+\gamma_2+3)}
Channel 2 depends on both γ parameters, leading to different exponents

Key numbers

  • lifetime of erythrosine B: 0.448 ns
  • exponent β channel 1 erythrosine B: 1.559
  • exponent β channel 2 erythrosine B: 2.019
  • lifetime of eosin Y: 1.054 ns
  • onset of power-law tail: about 10 lifetimes
Scientists
Alan GuthAlexander FriedmannAndrei LindeGeorges LemaîtreJames Peebles
Concepts
lifetime qubit lifetime quantum law decay channel decay probability degeneracy half life uncertainty decadal variability power law distribution time uncertainty time reversal symmetry complementarity principle quasi biennial oscillation age of the universe trajectory second stochastic fluctuations de Broglie formula delay differential equation