Two-lifetime model for the cuprates revisited
Pith reviewed 2026-05-25 07:35 UTC · model grok-4.3
The pith
A two-lifetime phenomenological model explains low-energy ARPES spectra in cuprates, distinguishes forward from large-angle scattering, and extracts the gap magnitude away from the Fermi surface.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The two-lifetime phenomenological model of the superconducting state accounts for salient low-energy features of ARPES spectra in cuprates. It enables discrimination between forward- and large-angle scattering and gives access to the magnitude of the gap function away from the Fermi surface.
What carries the argument
The two-lifetime phenomenological model, which parametrizes the electron self-energy using two distinct quasiparticle lifetimes to capture different scattering processes.
If this is right
- The model reproduces multiple observed low-energy ARPES features that single-lifetime models miss.
- ARPES data can be used to identify whether forward scattering dominates over large-angle scattering.
- The magnitude of the superconducting gap function becomes accessible at momenta away from the Fermi surface.
- Models of the strange-metal state that invoke strong inelastic forward scattering gain direct experimental support from ARPES.
Where Pith is reading between the lines
- If validated, the method could be extended to map scattering angles in other families of unconventional superconductors.
- The distinction between forward and large-angle scattering extracted here could constrain microscopic theories of pairing.
- Independent checks using other momentum-resolved probes would test whether the two-lifetime form captures real scattering physics.
Load-bearing premise
That a two-lifetime parametrization is physically meaningful rather than a convenient fitting form, and that ARPES line shapes directly encode the distinction between forward and large-angle scattering without additional assumptions about matrix elements or background.
What would settle it
An ARPES dataset from a cuprate that cannot be reproduced by any choice of two lifetimes, or an independent measurement of the gap function at momenta away from the Fermi surface that contradicts the model's extracted values.
Figures
read the original abstract
Several models of the strange-metal state of the cuprate superconductors postulate the existence of strong inelastic forward scattering of the electrons, but direct evidence of such scattering is missing. Here, we show that angle-resolved photoemission spectroscopy (ARPES) provides a unique tool which can address this issue. We propose a two-lifetime phenomenological model of the superconducting state of the cuprates, and we show that it explains several salient low-energy features of the measured ARPES spectra. The model enables discrimination between forward- and large-angle scattering and, in addition, gives access to the magnitude of the gap function away from the Fermi surface.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript proposes a two-lifetime phenomenological model for the superconducting state of the cuprates. It claims that this model accounts for several salient low-energy features in measured ARPES spectra, enables discrimination between forward- and large-angle scattering, and provides access to the magnitude of the gap function away from the Fermi surface.
Significance. If the two-lifetime form can be shown to be required by the data rather than merely accommodating it, and if the extracted lifetimes map uniquely to scattering angle without confounding matrix-element or background effects, the work would supply a useful phenomenological tool for interpreting ARPES line shapes in the cuprates and could strengthen the case for strong inelastic forward scattering in the strange-metal phase.
major comments (2)
- [Abstract / model definition] The central claim that the model 'enables discrimination between forward- and large-angle scattering' (abstract) rests on the assumption that ARPES line shapes encode a physically meaningful distinction via two distinct lifetimes. No uniqueness test against alternative self-energy parametrizations (e.g., a single lifetime with momentum-dependent scattering rate) is indicated, leaving open the possibility that the form simply fits the spectra without uniquely identifying the scattering mechanism.
- [Abstract / gap extraction claim] The assertion that the model 'gives access to the magnitude of the gap function away from the Fermi surface' requires explicit demonstration that the extracted gap values are robust to variations in the two lifetime parameters and to background subtraction choices; otherwise the off-FS gap extraction reduces to an additional fitting degree of freedom.
minor comments (1)
- Clarify the precise functional form of the two-lifetime self-energy (e.g., whether the lifetimes enter the imaginary part of the Green's function additively or via separate spectral functions) early in the text.
Simulated Author's Rebuttal
We thank the referee for their careful reading of the manuscript and for the constructive comments. We address each major comment below and have revised the manuscript to incorporate additional analysis that strengthens the claims.
read point-by-point responses
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Referee: The central claim that the model 'enables discrimination between forward- and large-angle scattering' (abstract) rests on the assumption that ARPES line shapes encode a physically meaningful distinction via two distinct lifetimes. No uniqueness test against alternative self-energy parametrizations (e.g., a single lifetime with momentum-dependent scattering rate) is indicated, leaving open the possibility that the form simply fits the spectra without uniquely identifying the scattering mechanism.
Authors: We agree that an explicit comparison to alternative parametrizations would strengthen the argument for the two-lifetime form. The model is physically motivated by the expectation of distinct forward and large-angle scattering channels in the cuprates, which produce qualitatively different effects on the ARPES line shape. In the revised manuscript we have added a direct comparison to a single-lifetime model with momentum-dependent scattering rate, showing that the latter fails to simultaneously reproduce the observed quasiparticle peak width and the incoherent background intensity across the measured momentum range. This supports the utility of the two-lifetime parametrization for discriminating scattering angles. revision: yes
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Referee: The assertion that the model 'gives access to the magnitude of the gap function away from the Fermi surface' requires explicit demonstration that the extracted gap values are robust to variations in the two lifetime parameters and to background subtraction choices; otherwise the off-FS gap extraction reduces to an additional fitting degree of freedom.
Authors: We concur that robustness to parameter variations and background choices must be demonstrated. In the revised manuscript we have added a supplementary analysis in which the two lifetime parameters are varied independently by up to 25 % around their best-fit values and two different background subtraction procedures are applied. The extracted gap magnitude away from the Fermi surface changes by less than the reported uncertainty in all cases, confirming that the off-FS gap values are not an artifact of the fitting procedure. These checks are now described in the main text and shown in a new supplementary figure. revision: yes
Circularity Check
No circularity identified; model proposal is self-contained.
full rationale
The provided abstract and description present a phenomenological two-lifetime model proposed to explain ARPES features, with no quoted equations, sections, or self-citations showing a load-bearing reduction (such as parameters fitted to the target spectra then renamed as predictions, or a uniqueness theorem imported from the authors' prior work). The central claim is that the model explains observed spectra and enables discrimination, which is the standard purpose of a fitting form rather than a circular derivation. Without specific text exhibiting self-definition or fitted-input-called-prediction, the analysis finds the derivation self-contained against external benchmarks.
Axiom & Free-Parameter Ledger
free parameters (1)
- two lifetimes
axioms (1)
- domain assumption ARPES spectra encode scattering angle information through line-shape differences
Reference graph
Works this paper leans on
-
[1]
B. Keimer, S.A. Kivelson, M.R. Norman, S. Uchida, and J. Zaanen, Nature518, 179 (2015)
work page 2015
- [2]
-
[3]
Anderson,The theory of high temperature super- conductivity(Princeton University Press, NY, 1996)
P.W. Anderson,The theory of high temperature super- conductivity(Princeton University Press, NY, 1996)
work page 1996
- [4]
- [5]
- [6]
- [7]
-
[8]
Classification of non-Fermi liquids and universal superconducting fluctuations
S. Kukreja, D.M. Willerton, and Sung-Sik Lee, arXiv:2601.21047
work page internal anchor Pith review Pith/arXiv arXiv
- [9]
- [10]
- [11]
- [12]
- [13]
- [14]
-
[15]
T. J. Reber, N. C. Plumb, Z. Sun, Y. Cao, Q. Wang, K. McElroy, H. Iwasawa, M. Arita, J. S. Wen, Z. J. Xu, G. Gu, Y. Yoshida, H. Eisaki, Y. Aiura, and D. S. Dessau, Nature Physics8, 606-610 (2012)
work page 2012
- [16]
- [17]
-
[18]
See Supplemental Material at http://link.aps.org/... for the definition of Ω 1,2(ω), results for the spectral func- tions in various limiting cases, technical details on the fits to the experimental data atk=k F , and prediction of MRDP for the Eliashberg self-energies and joint den- sity of states, which include Ref. [30]
-
[19]
S.-D. Chen, M. Hashimoto, Y. He, D. Song, J.-F. He, Y.-F. Li, S. Ishida, H. Eisaki, J. Zaanen, T. P. Dev- ereaux, D.-H. Lee, D.-H. Lu, and Z.-X. Shen, Nature 601, 562–567 (2022)
work page 2022
-
[20]
T. J. Reber, S. Parham, N. C. Plumb, Y. Cao, H. Li, Z. Sun, Q. Wang, H. Iwasawa, M. Arita, J. S. Wen, Z. J. Xu, G.D. Gu, Y. Yoshida, H. Eisaki, G.B. Arnold, and D. S. Dessau, arXiv: 1508.06252 (2015)
work page internal anchor Pith review Pith/arXiv arXiv 2015
-
[21]
S. Ye, M. Xu, H. Yan, Z.-X. Li, C. Zou, X. Li, Y. Chen, X. Zhou, D.-H. Lee and Y. Wang, Nat. Commun.15, 4939 (2024)
work page 2024
- [23]
-
[24]
H. Li, X. Zhou, S. Parham, T.J. Reber, H. Berger, G.B. Arnold, and D.S. Dessau, Nat. Commun.9, 26 (2018)
work page 2018
- [25]
- [26]
-
[27]
G. Grissonnanche, Y. Fang, A. Legros, S. Verret, F. Lal- ibert´ e, C. Collignon, J. Zhou, D. Graf, P.A. Goddard, L. Taillefer, and B.J. Ramshaw, Nature595, 667 (2021)
work page 2021
-
[28]
A. Kaminski, H. M. Fretwell, M. R. Norman, M. Rande- ria, S. Rosenkranz, U. Chatterjee, J. C. Campuzano, J. Mesot, T. Sato, T. Takahashi, T. Terashima, M. Takano, K. Kadowaki, Z.Z. Li, and H. Raffy, Phys. Rev. B71, 014517 (2005)
work page 2005
-
[29]
More precisely speaking, the inelastic part of Γ s(T) in a singlet superconductor is a measure of the sum of forward and 2kF scattering
-
[30]
The octet model was introduced to interpret the quasi- particle interference observed by scanning tunneling spectroscopy of the cuprates, see K. McElroy, R. W. Simmonds, J. E. Hoffmann, D.-H. Lee, J. Orenstein, H. Eisaki, S. Uchida, and J. C. Davis, Nature422, 592 (2003). 1 Supplemental Material: Two-lifetime model for the cuprates revisited Lucia Gelenek...
work page 2003
-
[31]
The functionA(k F , ω) is even and it exhibits two peaks atω≈ ±ω ∗
[Ω2 1 + (Ω2 + Γs)2] ,(S2) whereω ∗ = √ ∆2 + Γ2. The functionA(k F , ω) is even and it exhibits two peaks atω≈ ±ω ∗. Figure S1 shows that the pair-breaking rate Γ symmetrically broadens the peaks, while the forward-scattering rate Γ s generates a finite asymmetry of the peaks, increasing their width predominantly for|ω|> ω ∗. Note that the shape ofA(k F , ...
discussion (0)
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