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Elliptic flow from event-by-event hydrodynamics with fluctuating initial state
High Energy Physics - Phenomenology · Submitted 1 Dec 2010
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Our studies also show that the participant plane is quite a good approximation for the event plane.
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The abstract, sentence by sentence
We develop an event-by-event ideal hydrodynamical framework where initial state density fluctuations are present and where we use a similar flow-analysis method as in the experiments to make a one-to-one $v_2$ comparison with the measured data. Our studies also show that the participant plane is quite a good approximation for the event plane.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We develop an event-by-event ideal hydrodynamical framework where initial state density fluctuations are present and where we use a similar flow-analysis method as in the experiments to make a one-to-one $v_2$ comparison with the measured data. | method 0.64 | 0.95 | 0.16 | asserted 0.99 |
| s1 | Our studies also show that the participant plane is quite a good approximation for the event plane. | result 0.98 | 0.93 | 0.28 | asserted 1.00 |
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The paper
Original abstract
We develop an event-by-event ideal hydrodynamical framework where initial state density fluctuations are present and where we use a similar flow-analysis method as in the experiments to make a one-to-one $v_2$ comparison with the measured data. Our studies also show that the participant plane is quite a good approximation for the event plane.
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How the literature uses it
What this paper does with the arXiv papers it cites
What it cites · 2 sentences without a confident label
Uses the method or tool of 2 papers
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We apply the two-subevent method [ref] to estimate the event plane resolution $ℛ_2$, which corrects $v_2 { obs }$ for the event plane fluctuations.
Methods for analyzing anisotropic flow in relativistic nuclear collisions · Event-by-event hydrodynamics framework · 1.00
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For this, we let the unstable thermal hadrons decay one by one using PYTHIA 6.4 [ref] .
PYTHIA 6.4 Physics and Manual · Event-by-event hydrodynamics framework · 1.00
Uses data or values from 1 paper
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The overall normalization constant $K$ and the initial time $τ_0 = 0.17$ fm are taken from the EKRT pQCD+saturation model [ref] .
Scaling of transverse energies and multiplicities with atomic number and energy in ultrarelativistic nuclear collisions · Event-by-event hydrodynamics framework · 0.80
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