cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.15468/dl.syksfz
title: Occurrence Download

description: A dataset containing 23462489 species occurrences available in GBIF matching the query:
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 "TaxonKey is one of (Pediobius multisetis Boucek, 1977, Emersonella palmae Boucek, 1977, Brachymeria mnestor (Walker, 1841), Trichospilus vorax Boucek, 1976, Brachymeria deesensis (Cameron, 1905), Pseudoligosita longiclavata (Viggiani, 1971), Erythmelus tingitiphagus (Soares, 1941), Brachymeria subconica Boucek, 1992, Horismenus carolinensis Burks, 1971, Pediobius vigintiquinque Kerrich, 1970, Pediobius setigerus Kerrich, 1970, Conura immaculata (Cresson, 1865), Pediobius anomalus (Gahan, 1920), Pleurotroppopsis podagrica (Waterston, 1925), Closterocerus africanus Waterston, 1925, Tineobius brachartonae (Gahan, 1927), Protoxerus stangeri eborivorus (Du Chaillu, 1860), Funisciurus lemniscatus lemniscatus, Heliosciurus rufobrachium aubryi (Milne-Edwards, 1867), Pteroteinon caenira (Hewitson, 1867), Elymnias bammakoo (Westwood), Lophoceros fasciatus (Shaw, 1812), Corythaeola cristata (Vieillot, 1816), Bycanistes albotibialis (Cabanis & Reichenow, 1877), Crinifer piscator (Boddaert, 1783), Ceratogymna atrata (Temminck, 1835), Tauraco persa (Linnaeus, 1758), Polyboroides typus A.Smith, 1829, Eulemur flavifrons (Gray, 1867), Gypohierax angolensis (Gmelin, 1788), Epixerus ebii wilsoni (Du Chaillu, 1860), Cathartes burrovianus Cassin, 1845, Bycanistes fistulator (Cassin, 1850), Colobus satanas Waterhouse, 1838, Poicephalus gulielmi (Jardine, 1849), Cercopithecus cephus (Linnaeus, 1758), Cercopithecus pogonias Bennett, 1833, Cercopithecus nictitans (Linnaeus, 1766), Gorilla gorilla (Savage, 1847), Strategus aloeus (Linnaeus, 1758), Coragyps atratus (Bechstein, 1793), Cercopithecus campbelli Waterhouse, 1838, Cathartes aura (Linnaeus, 1758), Psittacus erithacus Linnaeus, 1758, Mandrillus sphinx (Linnaeus, 1758), Milvus migrans (Boddaert, 1783), Grasidius hybridus O'Brien & Beserra, 2004, Piaractus brachypomus (Cuvier, 1818), Pseudotaenia ajax (Saunders, 1872), Bemisia gigantea Martin, 1999)",
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 The dataset includes 23462489 records from 4723 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0016535-250515123054153/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.89442.v1/t2
title: "Table 1b" of "Transverse momentum spectra in Au + Au and d + Au collisions at s(NN)**(1/2) = 200-GeV and the pseudorapidity dependence of high p(T) suppression."

description: $\frac{1}{2\pi p_{\mathrm{T}}}\frac{\mathrm{d}^2N}{\mathrm{d}p_{\mathrm{T}}\mathrm{d}\eta}$ versus $p_{\mathrm{T}}$ for $\frac{h^{+}+h^{-}}{2}$ in $\mathrm{d}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$ near $\eta=0$
description: BNL-RHIC-BRAHMS. We present spectra of charged hadrons from Au+Au and d+Au collisions at $\sqrt{s_{NN}}=200$ GeV measured with the BRAHMS experiment at RHIC. The spectra for different collision centralities are compared to spectra from ${\rm p}+\bar{{\rm p}}$ collisions at the same energy scaled by the number of binary collisions. The resulting ratios (nuclear modification factors) for central Au+Au collisions at $\eta=0$ and $\eta=2.2$ evidence a strong suppression in the high $p_{T}$ region ($&gt;$2 GeV/c). In contrast, the d+Au nuclear modification factor (at $\eta=0$) exhibits an enhancement of the high $p_T$ yields. These measurements indicate a high energy loss of the high $p_T$ particles in the medium created in the central Au+Au collisions. The lack of suppression in d+Au collisions makes it unlikely that initial state effects can explain the suppression in the central Au+Au collisions.
DOI: 10.17182/hepdata.89442.v1/t3
title: "Table 1c" of "Transverse momentum spectra in Au + Au and d + Au collisions at s(NN)**(1/2) = 200-GeV and the pseudorapidity dependence of high p(T) suppression."

description: $\frac{1}{2\pi p_{\mathrm{T}}}\frac{\mathrm{d}^2N}{\mathrm{d}p_{\mathrm{T}}\mathrm{d}\eta}$ versus $p_{\mathrm{T}}$ for $\mathrm{h}^{-}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$ near $\eta=2.2$, per centrality
description: BNL-RHIC-BRAHMS. We present spectra of charged hadrons from Au+Au and d+Au collisions at $\sqrt{s_{NN}}=200$ GeV measured with the BRAHMS experiment at RHIC. The spectra for different collision centralities are compared to spectra from ${\rm p}+\bar{{\rm p}}$ collisions at the same energy scaled by the number of binary collisions. The resulting ratios (nuclear modification factors) for central Au+Au collisions at $\eta=0$ and $\eta=2.2$ evidence a strong suppression in the high $p_{T}$ region ($&gt;$2 GeV/c). In contrast, the d+Au nuclear modification factor (at $\eta=0$) exhibits an enhancement of the high $p_T$ yields. These measurements indicate a high energy loss of the high $p_T$ particles in the medium created in the central Au+Au collisions. The lack of suppression in d+Au collisions makes it unlikely that initial state effects can explain the suppression in the central Au+Au collisions.
DOI: 10.17182/hepdata.89442.v1/t4
title: "Table 2a" of "Transverse momentum spectra in Au + Au and d + Au collisions at s(NN)**(1/2) = 200-GeV and the pseudorapidity dependence of high p(T) suppression."

description: $R_{\mathrm{AA}}$,$R_{\mathrm{CP}}$ versus $p_{\mathrm{T}}$ for $\frac{h^{+}+h^{-}}{2}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$ near $\eta=0$
description: BNL-RHIC-BRAHMS. We present spectra of charged hadrons from Au+Au and d+Au collisions at $\sqrt{s_{NN}}=200$ GeV measured with the BRAHMS experiment at RHIC. The spectra for different collision centralities are compared to spectra from ${\rm p}+\bar{{\rm p}}$ collisions at the same energy scaled by the number of binary collisions. The resulting ratios (nuclear modification factors) for central Au+Au collisions at $\eta=0$ and $\eta=2.2$ evidence a strong suppression in the high $p_{T}$ region ($&gt;$2 GeV/c). In contrast, the d+Au nuclear modification factor (at $\eta=0$) exhibits an enhancement of the high $p_T$ yields. These measurements indicate a high energy loss of the high $p_T$ particles in the medium created in the central Au+Au collisions. The lack of suppression in d+Au collisions makes it unlikely that initial state effects can explain the suppression in the central Au+Au collisions.
DOI: 10.17182/hepdata.89442.v1/t5
title: "Table 2b" of "Transverse momentum spectra in Au + Au and d + Au collisions at s(NN)**(1/2) = 200-GeV and the pseudorapidity dependence of high p(T) suppression."

description: $R_{\mathrm{AA}}$,$R_{\mathrm{CP}}$ versus $p_{\mathrm{T}}$ for $\mathrm{h}^{-}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$ near $\eta=2.2$
description: BNL-RHIC-BRAHMS. We present spectra of charged hadrons from Au+Au and d+Au collisions at $\sqrt{s_{NN}}=200$ GeV measured with the BRAHMS experiment at RHIC. The spectra for different collision centralities are compared to spectra from ${\rm p}+\bar{{\rm p}}$ collisions at the same energy scaled by the number of binary collisions. The resulting ratios (nuclear modification factors) for central Au+Au collisions at $\eta=0$ and $\eta=2.2$ evidence a strong suppression in the high $p_{T}$ region ($&gt;$2 GeV/c). In contrast, the d+Au nuclear modification factor (at $\eta=0$) exhibits an enhancement of the high $p_T$ yields. These measurements indicate a high energy loss of the high $p_T$ particles in the medium created in the central Au+Au collisions. The lack of suppression in d+Au collisions makes it unlikely that initial state effects can explain the suppression in the central Au+Au collisions.
DOI: 10.17182/hepdata.89442.v1/t6
title: "Table 3" of "Transverse momentum spectra in Au + Au and d + Au collisions at s(NN)**(1/2) = 200-GeV and the pseudorapidity dependence of high p(T) suppression."

description: $R_{\mathrm{CP}}|_{\eta=2.2} / R_{\mathrm{CP}}|_{\eta=0}$ versus $p_{\mathrm{T}}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$
description: BNL-RHIC-BRAHMS. We present spectra of charged hadrons from Au+Au and d+Au collisions at $\sqrt{s_{NN}}=200$ GeV measured with the BRAHMS experiment at RHIC. The spectra for different collision centralities are compared to spectra from ${\rm p}+\bar{{\rm p}}$ collisions at the same energy scaled by the number of binary collisions. The resulting ratios (nuclear modification factors) for central Au+Au collisions at $\eta=0$ and $\eta=2.2$ evidence a strong suppression in the high $p_{T}$ region ($&gt;$2 GeV/c). In contrast, the d+Au nuclear modification factor (at $\eta=0$) exhibits an enhancement of the high $p_T$ yields. These measurements indicate a high energy loss of the high $p_T$ particles in the medium created in the central Au+Au collisions. The lack of suppression in d+Au collisions makes it unlikely that initial state effects can explain the suppression in the central Au+Au collisions.
DOI: 10.17182/hepdata.89442.v1/t7
title: "Table 4a" of "Transverse momentum spectra in Au + Au and d + Au collisions at s(NN)**(1/2) = 200-GeV and the pseudorapidity dependence of high p(T) suppression."

description: $R_{\mathrm{AA}}$ versus $p_{\mathrm{T}}$ in $\mathrm{d}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$
description: BNL-RHIC-BRAHMS. We present spectra of charged hadrons from Au+Au and d+Au collisions at $\sqrt{s_{NN}}=200$ GeV measured with the BRAHMS experiment at RHIC. The spectra for different collision centralities are compared to spectra from ${\rm p}+\bar{{\rm p}}$ collisions at the same energy scaled by the number of binary collisions. The resulting ratios (nuclear modification factors) for central Au+Au collisions at $\eta=0$ and $\eta=2.2$ evidence a strong suppression in the high $p_{T}$ region ($&gt;$2 GeV/c). In contrast, the d+Au nuclear modification factor (at $\eta=0$) exhibits an enhancement of the high $p_T$ yields. These measurements indicate a high energy loss of the high $p_T$ particles in the medium created in the central Au+Au collisions. The lack of suppression in d+Au collisions makes it unlikely that initial state effects can explain the suppression in the central Au+Au collisions.
DOI: 10.17182/hepdata.89442.v1/t8
title: "Table 4b" of "Transverse momentum spectra in Au + Au and d + Au collisions at s(NN)**(1/2) = 200-GeV and the pseudorapidity dependence of high p(T) suppression."

description: $R_{\mathrm{AA}}$ versus $p_{\mathrm{T}}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$
description: BNL-RHIC-BRAHMS. We present spectra of charged hadrons from Au+Au and d+Au collisions at $\sqrt{s_{NN}}=200$ GeV measured with the BRAHMS experiment at RHIC. The spectra for different collision centralities are compared to spectra from ${\rm p}+\bar{{\rm p}}$ collisions at the same energy scaled by the number of binary collisions. The resulting ratios (nuclear modification factors) for central Au+Au collisions at $\eta=0$ and $\eta=2.2$ evidence a strong suppression in the high $p_{T}$ region ($&gt;$2 GeV/c). In contrast, the d+Au nuclear modification factor (at $\eta=0$) exhibits an enhancement of the high $p_T$ yields. These measurements indicate a high energy loss of the high $p_T$ particles in the medium created in the central Au+Au collisions. The lack of suppression in d+Au collisions makes it unlikely that initial state effects can explain the suppression in the central Au+Au collisions.
DOI: 10.17182/hepdata.89443.v1/t1
title: "Table 1" of "Nuclear stopping in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: $\frac{1}{2\pi p_{\mathrm{T}}}\frac{\mathrm{d}^2N}{\mathrm{d}p_{\mathrm{T}}\mathrm{d}y}$ versus $p_{\mathrm{T}}$ for $\mathrm{p}$,$\overline{\mathrm{p}}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$ . NaN values means no observation.
description: BNL-RHIC-BRAHMS. Transverse momentum spectra and rapidity densities, dN/dy, of protons, anti-protons, and net--protons (p-pbar) from central (0-5%) Au+Au collisions at sqrt(sNN) = 200 GeV were measured with the BRAHMS experiment within the rapidity range 0 &lt; y &lt; 3. The proton and anti-proton dN/dy decrease from mid-rapidity to y=3. The net-proton yield is roughly constant for y&lt;1 at dN/dy~7, and increases to dN/dy~12 at y~3. The data show that collisions at this energy exhibit a high degree of transparency and that the linear scaling of rapidity loss with rapidity observed at lower energies is broken. The energy loss per participant nucleon is estimated to be 73 +- 6 GeV.
DOI: 10.17182/hepdata.89443.v1/t2
title: "Table 2" of "Nuclear stopping in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: $\frac{\mathrm{d}N}{\mathrm{d}y}$ versus $y$ for $\mathrm{p}$,$\overline{\mathrm{p}}$,$\mathrm{p}-\overline{\mathrm{p}}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$ . The correction for the $\Lambda$ contribution is not straight forward since BRAHMS does not measure the $\Lambda$s and PHENIX and STAR only measures the $\Lambda$s at mid-rapidity! If one assumes that the mid-rapidity estimated in the paper of $$R=\frac{\Lambda-\bar{\Lambda}}{\mathrm{p}-\bar{\mathrm{p}}} = \frac{\Lambda}{\mathrm{p}} = \frac{\bar{\Lambda}}{\bar{\mathrm{p}}} = 0.93\pm 0.11(\mathrm{stat})\pm 0.25(\mathrm{syst}) $$ and the BRAHMS "acceptance factor" of $A=0.53\pm 0.05$ which includes both that only 64% decays to protons and that some are rejected by the requirement of the track to point back to the IP. The corrected $\mathrm{p}$ ($\bar{\mathrm{p}}$ or net-$\mathrm{p}$) is then : $$\left.\frac{\mathrm{d}N}{\mathrm{d}y}\right|_{\mathrm{corrected}} = \frac{\mathrm{d}N}{\mathrm{d}y}(1/(1+RA))= \frac{\mathrm{d}N}{\mathrm{d}y}\left(0.67\pm 0.05(\mathrm{stat})\pm 0.11(\mathrm{syst})\right)$$ Which can be used at all rapidities if one believes that R is constant. The fact that net-$\mathrm{K}=\mathrm{K}^{+}-\mathrm{K}^{-}$ follows net-$\mathrm{p}$ (see fx. talk by Djamel Ouerdane at QM04), seems to indicate that the net-$\Lambda$ follow the net-$\mathrm{p}$ trend and the correction is reasonable.
description: BNL-RHIC-BRAHMS. Transverse momentum spectra and rapidity densities, dN/dy, of protons, anti-protons, and net--protons (p-pbar) from central (0-5%) Au+Au collisions at sqrt(sNN) = 200 GeV were measured with the BRAHMS experiment within the rapidity range 0 &lt; y &lt; 3. The proton and anti-proton dN/dy decrease from mid-rapidity to y=3. The net-proton yield is roughly constant for y&lt;1 at dN/dy~7, and increases to dN/dy~12 at y~3. The data show that collisions at this energy exhibit a high degree of transparency and that the linear scaling of rapidity loss with rapidity observed at lower energies is broken. The energy loss per participant nucleon is estimated to be 73 +- 6 GeV.
DOI: 10.17182/hepdata.89444.v1/t1
title: "Table 1a" of "On the evolution of the nuclear modification factors with rapidity and centrality in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: $\frac{1}{2\pi p_{\mathrm{T}}}\frac{\mathrm{d}^2N}{\mathrm{d}p_{\mathrm{T}}\mathrm{d}y}$ versus $p_{\mathrm{T}}$ for $\frac{h^{+}+h^{-}}{2}$,$\frac{h^{+}+h^{-}}{2}$ in $\mathrm{p}\mathrm{p}$,$\mathrm{d}-\mathrm{Au}$ at $\sqrt{s}=200\,\mathrm{Ge\!V}$ near $\eta=0$
description: BNL-RHIC-BRAHMS. We report on a study of the transverse momentum dependence of nuclear modification factors $R_{dAu}$ for charged hadrons produced in deuteron + gold collisions at $\sqrt{s_{NN}=\unit[200]{GeV}$, as a function of collision centrality and of the pseudorapidity ($\eta = 0,1,2.2,3.2 $) of the produced hadrons. We find significant and systematic decrease of $R_{dAu}$ with increasing rapidity. The midrapidity enhancement and the forward rapidity suppression are more pronounced in central collisions relative to peripheral collisions. These results are relevant to the study of the possible onset of gluon saturation at RHIC energies.
DOI: 10.17182/hepdata.89444.v1/t2
title: "Table 1b" of "On the evolution of the nuclear modification factors with rapidity and centrality in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: $\frac{1}{2\pi p_{\mathrm{T}}}\frac{\mathrm{d}^2N}{\mathrm{d}p_{\mathrm{T}}\mathrm{d}y}$ versus $p_{\mathrm{T}}$ for $\frac{h^{+}+h^{-}}{2}$,$\frac{h^{+}+h^{-}}{2}$ in $\mathrm{p}\mathrm{p}$,$\mathrm{d}-\mathrm{Au}$ at $\sqrt{s}=200\,\mathrm{Ge\!V}$ near $\eta=1$
description: BNL-RHIC-BRAHMS. We report on a study of the transverse momentum dependence of nuclear modification factors $R_{dAu}$ for charged hadrons produced in deuteron + gold collisions at $\sqrt{s_{NN}=\unit[200]{GeV}$, as a function of collision centrality and of the pseudorapidity ($\eta = 0,1,2.2,3.2 $) of the produced hadrons. We find significant and systematic decrease of $R_{dAu}$ with increasing rapidity. The midrapidity enhancement and the forward rapidity suppression are more pronounced in central collisions relative to peripheral collisions. These results are relevant to the study of the possible onset of gluon saturation at RHIC energies.
DOI: 10.17182/hepdata.89444.v1/t3
title: "Table 1c" of "On the evolution of the nuclear modification factors with rapidity and centrality in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: $\frac{1}{2\pi p_{\mathrm{T}}}\frac{\mathrm{d}^2N}{\mathrm{d}p_{\mathrm{T}}\mathrm{d}y}$ versus $p_{\mathrm{T}}$ for $\mathrm{h}^{-}$,$\mathrm{h}^{-}$ in $\mathrm{p}\mathrm{p}$,$\mathrm{d}-\mathrm{Au}$ at $\sqrt{s}=200\,\mathrm{Ge\!V}$ near $\eta=2.2$
description: BNL-RHIC-BRAHMS. We report on a study of the transverse momentum dependence of nuclear modification factors $R_{dAu}$ for charged hadrons produced in deuteron + gold collisions at $\sqrt{s_{NN}=\unit[200]{GeV}$, as a function of collision centrality and of the pseudorapidity ($\eta = 0,1,2.2,3.2 $) of the produced hadrons. We find significant and systematic decrease of $R_{dAu}$ with increasing rapidity. The midrapidity enhancement and the forward rapidity suppression are more pronounced in central collisions relative to peripheral collisions. These results are relevant to the study of the possible onset of gluon saturation at RHIC energies.
DOI: 10.17182/hepdata.89444.v1/t4
title: "Table 1d" of "On the evolution of the nuclear modification factors with rapidity and centrality in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: $\frac{1}{2\pi p_{\mathrm{T}}}\frac{\mathrm{d}^2N}{\mathrm{d}p_{\mathrm{T}}\mathrm{d}y}$ versus $p_{\mathrm{T}}$ for $\mathrm{h}^{-}$,$\mathrm{h}^{-}$ in $\mathrm{p}\mathrm{p}$,$\mathrm{d}-\mathrm{Au}$ at $\sqrt{s}=200\,\mathrm{Ge\!V}$ near $\eta=3.2$
description: BNL-RHIC-BRAHMS. We report on a study of the transverse momentum dependence of nuclear modification factors $R_{dAu}$ for charged hadrons produced in deuteron + gold collisions at $\sqrt{s_{NN}=\unit[200]{GeV}$, as a function of collision centrality and of the pseudorapidity ($\eta = 0,1,2.2,3.2 $) of the produced hadrons. We find significant and systematic decrease of $R_{dAu}$ with increasing rapidity. The midrapidity enhancement and the forward rapidity suppression are more pronounced in central collisions relative to peripheral collisions. These results are relevant to the study of the possible onset of gluon saturation at RHIC energies.
DOI: 10.17182/hepdata.89444.v1/t5
title: "Table 2a" of "On the evolution of the nuclear modification factors with rapidity and centrality in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: $R_{\mathrm{dA}}$ versus $p_{\mathrm{T}}$ for $\frac{h^{+}+h^{-}}{2}$ in $\mathrm{d}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$ near $\eta=0$
description: BNL-RHIC-BRAHMS. We report on a study of the transverse momentum dependence of nuclear modification factors $R_{dAu}$ for charged hadrons produced in deuteron + gold collisions at $\sqrt{s_{NN}=\unit[200]{GeV}$, as a function of collision centrality and of the pseudorapidity ($\eta = 0,1,2.2,3.2 $) of the produced hadrons. We find significant and systematic decrease of $R_{dAu}$ with increasing rapidity. The midrapidity enhancement and the forward rapidity suppression are more pronounced in central collisions relative to peripheral collisions. These results are relevant to the study of the possible onset of gluon saturation at RHIC energies.
DOI: 10.17182/hepdata.89444.v1/t6
title: "Table 2b" of "On the evolution of the nuclear modification factors with rapidity and centrality in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: $R_{\mathrm{dA}}$ versus $p_{\mathrm{T}}$ for $\frac{h^{+}+h^{-}}{2}$ in $\mathrm{d}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$ near $\eta=1$
description: BNL-RHIC-BRAHMS. We report on a study of the transverse momentum dependence of nuclear modification factors $R_{dAu}$ for charged hadrons produced in deuteron + gold collisions at $\sqrt{s_{NN}=\unit[200]{GeV}$, as a function of collision centrality and of the pseudorapidity ($\eta = 0,1,2.2,3.2 $) of the produced hadrons. We find significant and systematic decrease of $R_{dAu}$ with increasing rapidity. The midrapidity enhancement and the forward rapidity suppression are more pronounced in central collisions relative to peripheral collisions. These results are relevant to the study of the possible onset of gluon saturation at RHIC energies.
DOI: 10.17182/hepdata.89444.v1/t7
title: "Table 2c" of "On the evolution of the nuclear modification factors with rapidity and centrality in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: $R_{\mathrm{dA}}$ versus $p_{\mathrm{T}}$ for $\mathrm{h}^{-}$ in $\mathrm{d}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$ near $\eta=2.2$
description: BNL-RHIC-BRAHMS. We report on a study of the transverse momentum dependence of nuclear modification factors $R_{dAu}$ for charged hadrons produced in deuteron + gold collisions at $\sqrt{s_{NN}=\unit[200]{GeV}$, as a function of collision centrality and of the pseudorapidity ($\eta = 0,1,2.2,3.2 $) of the produced hadrons. We find significant and systematic decrease of $R_{dAu}$ with increasing rapidity. The midrapidity enhancement and the forward rapidity suppression are more pronounced in central collisions relative to peripheral collisions. These results are relevant to the study of the possible onset of gluon saturation at RHIC energies.
DOI: 10.17182/hepdata.89444.v1/t8
title: "Table 2d" of "On the evolution of the nuclear modification factors with rapidity and centrality in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: $R_{\mathrm{dA}}$ versus $p_{\mathrm{T}}$ for $\mathrm{h}^{-}$ in $\mathrm{d}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$ near $\eta=3.2$
description: BNL-RHIC-BRAHMS. We report on a study of the transverse momentum dependence of nuclear modification factors $R_{dAu}$ for charged hadrons produced in deuteron + gold collisions at $\sqrt{s_{NN}=\unit[200]{GeV}$, as a function of collision centrality and of the pseudorapidity ($\eta = 0,1,2.2,3.2 $) of the produced hadrons. We find significant and systematic decrease of $R_{dAu}$ with increasing rapidity. The midrapidity enhancement and the forward rapidity suppression are more pronounced in central collisions relative to peripheral collisions. These results are relevant to the study of the possible onset of gluon saturation at RHIC energies.