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Possibility to disentangle anisotropic flow, flow fluctuation, and nonflow assuming Gaussian fluctuations
Nuclear Experiment · Submitted 24 Jan 2011
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We show that such disentanglement is possible when the flow fluctuations are large, comparable to the average flow magnitude.
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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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The abstract, sentence by sentence
We suggest the possibility to disentangle anisotropic flow, flow fluctuation, and nonflow using two-, four-, and six-particle azimuthal moments assuming Gaussian fluctuations. We show that such disentanglement is possible when the flow fluctuations are large, comparable to the average flow magnitude. When fluctuations are small, the disentanglement becomes difficult. We verify our results with a toy-model Monte Carlo simulation.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We suggest the possibility to disentangle anisotropic flow, flow fluctuation, and nonflow using two-, four-, and six-particle azimuthal moments assuming Gaussian fluctuations. | contribution 0.98 | 0.76 | 0.67 | hedged possibility 1.00 |
| s1 | We show that such disentanglement is possible when the flow fluctuations are large, comparable to the average flow magnitude. | result 0.96 | 0.91 | 0.44 | asserted 0.97 |
| s2 | When fluctuations are small, the disentanglement becomes difficult. | limitation 0.79 | 0.75 | 0.11 | asserted 0.98 |
| s3 | We verify our results with a toy-model Monte Carlo simulation. | method 0.94 | 0.95 | 0.04 | asserted 1.00 |
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The paper
Original abstract
We suggest the possibility to disentangle anisotropic flow, flow fluctuation, and nonflow using two-, four-, and six-particle azimuthal moments assuming Gaussian fluctuations. We show that such disentanglement is possible when the flow fluctuations are large, comparable to the average flow magnitude. When fluctuations are small, the disentanglement becomes difficult. We verify our results with a toy-model Monte Carlo simulation.
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References
How the literature uses it
10 arXiv papers cite this in 13 sentences
Papers citing it · 11 sentences without a confident label
Uses its method or tool 2 papers
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The Q-cumulant method [ref] is used with the acceptance correction in calculation.
Isolation of Flow and Nonflow by Two- and Multi-Particle Cumulant Measurements of $v_n$ in $\sqrt{s_{NN}} = 200$ GeV Au+Au Collisions by STAR · Data Analysis and Results · 1.00
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Two-particle correlation Fourier coefficients $$ are calculated using the direct Q-Cumulants method [ref] , which avoids nested loops in the analysis.
Nonflow "factorization" and a novel method to disentangle anisotropic flow and nonflow · Nonflow factorization · 1.00
What it cites · 7 sentences without a confident label
Uses the method or tool of 1 paper
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We use the Q-vector method [ref] to calculate the two-, four-, and six-particle azimuthal moments from the simulated events.
Flow analysis with cumulants: direct calculations · Toy-Model Simulations · 1.00
Cites as background 8 papers
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Triangular flow, $v_3$, can arise from the triangularity of the initial overlap geometry [ref] , and may be dominated by fluctuations.
Translation of collision geometry fluctuations into momentum anisotropies in relativistic heavy-ion collisions · Introduction · 0.91
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Triangular flow, $v_3$, can arise from the triangularity of the initial overlap geometry [ref] , and may be dominated by fluctuations.
Elliptic and triangular flow in event-by-event (3+1)D viscous hydrodynamics · Introduction · 0.91
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Triangular flow, $v_3$, can arise from the triangularity of the initial overlap geometry [ref] , and may be dominated by fluctuations.
Triangularity and Dipole Asymmetry in Heavy Ion Collisions · Introduction · 0.91
Discussion
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