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Route to Chaos in the $^{15}NH_{3}$ far infrared ring laser

chao-dyn · Submitted 21 Aug 1997

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

The authors' main claim It is also shown that the experimental system has a small parameter regime where the route to chaos is the same as in the Lorenz Haken equations.

how it is stated · asserted 1.00 read the record →

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arXiv IDchao-dyn/9708012 (version 1)
Pith IDMHOUED3P, Pith's permanent record of this paper and its review
CitationM.Y. Li, N.R. Heckenberg, R. Dykstra. "Route to Chaos in the $^{15}NH_{3}$ far infrared ring laser." arXiv:chao-dyn/9708012 (1997). https://pith.science/paper/MHOUED3P
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The compiled record

The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.

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Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 2,979 input tokens, $0.0001 reported.

What the abstract itself states, as probabilities: claims first 0.03 · states limitation 0.45 · human participants 0.02 · controlled comparison 0.37 · randomized assignment 0.01 · states quantitative result 0.05 · compares with prior results 0.93 · mentions code or data availability 0.01.

The abstract, sentence by sentence

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

The route to chaos as the pump power is raised in the Lorenz-like ammonia laser is studied using transients and compared with the route which is expected in the Lorenz Haken equations. The differences between the routes to chaos, as normally displayed by the experimental system and the Lorenz Haken equations, is described in terms of the bifurcations experienced in each system. It is also shown that the experimental system has a small parameter regime where the route to chaos is the same as in the Lorenz Haken equations.

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 The route to chaos as the pump power is raised in the Lorenz-like ammonia laser is studied using transients and compared with the route which is expected in the Lorenz Haken equations. contribution 0.96 0.92 0.13 asserted 0.98
s1 The differences between the routes to chaos, as normally displayed by the experimental system and the Lorenz Haken equations, is described in terms of the bifurcations experienced in each system. interpretation 0.42 0.80 0.18 asserted 1.00
s2 It is also shown that the experimental system has a small parameter regime where the route to chaos is the same as in the Lorenz Haken equations. result 1.00 0.90 0.37 asserted 1.00

What kind of paper the classifier reports this is: empirical study 1.00 · evidence from observation or experiment 0.99.

What was examined, and what was not

sources read
  • arXiv listing abstract v1
not examined
  • full text
  • figures and tables
  • references and citing sentences
  • relations to other papers
levels run
  • P abstract
not run
  • S sections
  • T body sentences
  • C citations
  • R cross-paper relations

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

The route to chaos as the pump power is raised in the Lorenz-like ammonia laser is studied using transients and compared with the route which is expected in the Lorenz Haken equations. The differences between the routes to chaos, as normally displayed by the experimental system and the Lorenz Haken equations, is described in terms of the bifurcations experienced in each system. It is also shown that the experimental system has a small parameter regime where the route to chaos is the same as in the Lorenz Haken equations.

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