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Resonant neutron scattering on the high Tc cuprates and pi and eta excitation of the t-J and Hubbard models

Strongly Correlated Electrons · Submitted 11 Mar 1999

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim We review the explanation for resonant neutron scattering experiments in $YBa_2Cu_3O_{6+\delta}$ and $Bi_2 Sr_2 Ca_2 O_{8+\delta}$ materials from the point of view of triplet excitation in the particle-particle channel, the pi excitation.

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arXiv IDcond-mat/9903195 (version 1)
Pith IDUO5LQTRN, Pith's permanent record of this paper and its review
CitationEugene Demler, Shou-Cheng Zhang. "Resonant neutron scattering on the high Tc cuprates and pi and eta excitation of the t-J and Hubbard models." arXiv:cond-mat/9903195 (1999). https://pith.science/paper/UO5LQTRN
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Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 3,755 input tokens, $0.0002 reported.

What the abstract itself states, as probabilities: claims first 0.03 · states limitation 0.11 · human participants 0.02 · controlled comparison 0.03 · randomized assignment 0.01 · states quantitative result 0.04 · compares with prior results 0.16 · mentions code or data availability 0.02.

The abstract, sentence by sentence

arXiv listing abstract v1. Results and the main claim are underlined; .

We review the explanation for resonant neutron scattering experiments in $YBa_2Cu_3O_{6+\delta}$ and $Bi_2 Sr_2 Ca_2 O_{8+\delta}$ materials from the point of view of triplet excitation in the particle-particle channel, the pi excitation. Relation of these resonances to the superconducting condensation energy and their role in stabilizing the superconducting state is discussed. Due to the superconducting fluctuations, the pi resonance may appear as a broad peak above Tc. Analogue problem to the pi excitation for the case of s-wave pairing, the eta excitation, is considered in the strong coupling limit with an emphasis on the resonance precursors in a state with no long range order.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 We review the explanation for resonant neutron scattering experiments in $YBa_2Cu_3O_{6+\delta}$ and $Bi_2 Sr_2 Ca_2 O_{8+\delta}$ materials from the point of view of triplet excitation in the particle-particle channel, the pi excitation. contribution 0.87 0.18 0.18 asserted 0.72
s1 Relation of these resonances to the superconducting condensation energy and their role in stabilizing the superconducting state is discussed. contribution 0.67 0.31 0.11 unclear 0.62
s2 Due to the superconducting fluctuations, the pi resonance may appear as a broad peak above Tc. result 0.59 0.23 0.11 hedged possibility 1.00
s3 Analogue problem to the pi excitation for the case of s-wave pairing, the eta excitation, is considered in the strong coupling limit with an emphasis on the resonance precursors in a state with no long range order. contribution 0.98 0.59 0.08 asserted 0.75

What kind of paper the classifier reports this is: review 1.00 · evidence from literature 0.67.

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

The paper
Original abstract

We review the explanation for resonant neutron scattering experiments in $YBa_2Cu_3O_{6+\delta}$ and $Bi_2 Sr_2 Ca_2 O_{8+\delta}$ materials from the point of view of triplet excitation in the particle-particle channel, the pi excitation. Relation of these resonances to the superconducting condensation energy and their role in stabilizing the superconducting state is discussed. Due to the superconducting fluctuations, the pi resonance may appear as a broad peak above Tc. Analogue problem to the pi excitation for the case of s-wave pairing, the eta excitation, is considered in the strong coupling limit with an emphasis on the resonance precursors in a state with no long range order.

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