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Rapidity and centrality dependence of azimuthal correlations in Deuteron-Gold collisions at RHIC
High Energy Physics - Phenomenology · Submitted 30 Dec 2009
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We calculate azimuthal correlations in dAu collisions at different rapidities and centralities and argue that experimentally observed depletion of the back-to-back pick can be quantitatively explained by gluon saturation in the Color Glass Condensate of the Gold nucleus.
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We calculate azimuthal correlations in dAu collisions at different rapidities and centralities and argue that experimentally observed depletion of the back-to-back pick can be quantitatively explained by gluon saturation in the Color Glass Condensate of the Gold nucleus.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We calculate azimuthal correlations in dAu collisions at different rapidities and centralities and argue that experimentally observed depletion of the back-to-back pick can be quantitatively explained by gluon saturation in the Color Glass Condensate of the Gold nucleus. | contribution 0.43 | 0.88 | 0.93 | asserted 0.91 |
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The paper
Original abstract
We calculate azimuthal correlations in dAu collisions at different rapidities and centralities and argue that experimentally observed depletion of the back-to-back pick can be quantitatively explained by gluon saturation in the Color Glass Condensate of the Gold nucleus.
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References
How the literature uses it
18 arXiv papers cite this in 25 sentences
Papers whose main result relates to this one's
States the same result 3 papers
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We discuss azimuthal correlations in $dAu$ collisions at different rapidities and centralities and argue that experimentally observed depletion of the back-to-back peak can be quantitatively explained by gluon saturation in the Color Glass Condensate of the Gold nucleus.
Rapidity and centrality dependence of azimuthal correlations in high energy d+Au collisions · 1.00
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Indeed, we argue that this effect, absent at mid-rapidity, is a consequence of the small-x evolution into the saturation regime of the Gold nucleus wave function.
Azimuthal correlations of forward di-hadrons in d+Au collisions suppressed by saturation · 0.84
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It is demonstrated that the suppression and broadening of the away side peak provide a unique signal for the onset of the saturation mechanism at small-$x$ in a large nucleus.
Back-to-Back Correlations of Di-hadrons in dAu Collisions at RHIC · 0.83
Papers citing it · 18 sentences without a confident label
Compares with it 1 paper
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Comparison between same data and CGC calculations using a different approach can be found in this reference [ref] .
Suppression of Forward Pion Correlations in d+Au Interactions at STAR · Results and Systematics · 0.90
Cites it as support 1 paper
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There are also numerous indications that $k_T$-factorization is phenomenologically reliable (see [ref] for examples).
Rapidity and centrality dependence of azimuthal correlations in high energy d+Au collisions · Introduction · 0.97
Cites it as background 5 papers
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A special role in the phenomenology of the CGC is played by correlations of particles in p+A collisions probed in the region of fragmentation of the protons [ref] , where the rapidities of the correlated particles are large and positive (forward rapidity region).
Forward di-hadron back-to-back correlations in $\boldsymbol{pA}$ collisions from rcBK evolution · Introduction · 0.91
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Particularly, our understanding of the so-called gluon saturation [ref] , predicted by QCD to emerge in high energy collisions, remains incomplete.
Investigating the broadening phenomenon in two-particle correlations induced by gluon saturation · Introduction · 0.99
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BFKL graphs were also discussed in the context of deuteron-gold collisions at RHIC in [ref] .] and compare these to forthcoming LHC data on the same.
Evidence for BFKL and saturation dynamics from di-hadron spectra at the LHC · Introduction · 0.90
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