cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.96029.v1/t2
title: "Table 2" of "Measurement of nuclear effects on $\psi\rm{(2S)}$ production in p-Pb collisions at $\sqrt{\textit{s}_{\rm NN}} = 8.16$ TeV"

description: Inclusive $\psi(2{\rm S})$ differential cross section times branching ratio as a function of $p_{\rm T}$, at forward rapidity at $\sqrt{s_{\rm NN}}$ = 8.16 TeV .The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a correlated systematic uncertainty.
description: Inclusive $\psi(2{\rm S})$ production is measured in \ppb collisions at the centre-of-mass energy per nucleon--nucleon pair $\sqrt{s_{_{\rm NN}}}=8.16$ TeV, using the ALICE detector at the CERN LHC. The production of $\psi(2{\rm S})$ is studied at forward ($2.03 &lt; y_{\rm cms} &lt; 3.53$) and backward ($-4.46 &lt; y_{\rm cms} &lt; -2.96$) centre-of-mass rapidity and for transverse momentum \pt $&lt;$ 12 \gevc via the decay to muon pairs. In this paper, we report the integrated as well as the $y_{\rm cms}$- and $p_{\rm T}$-differential inclusive production cross sections. Nuclear effects on $\psi(2{\rm S})$ production are studied via the determination of the nuclear modification factor that shows a strong suppression at both forward and backward centre-of-mass rapidities. Comparisons with corresponding results for inclusive J$/psi$ show a similar suppression for the two states at forward rapidity (p-going direction), but a stronger suppression for $\psi(2{\rm S})$ at backward rapidity (Pb-going direction). As a function of $p_{\rm T}$, no clear dependence of the nuclear modification factor is found. The relative size of nuclear effects on $\psi(2{\rm S})$ production compared to J$/psi$ is also studied via the double ratio of production cross sections $[\sigma_{\psi({\rm 2S})}/\sigma_{{\rm J/}\psi}]_{\rm pPb}/[\sigma_{\psi({\rm 2S})}/\sigma_{{\rm J/}\psi}]_{\rm pp}$ between \ppb and \pp collisions. The results are compared with theoretical models that include various effects related to the initial and final state of the collision system and also with previous measurements at $\sqrt{s_{_{\rm NN}}}=5.02$ TeV.
DOI: 10.17182/hepdata.96029.v1/t3
title: "Table 3" of "Measurement of nuclear effects on $\psi\rm{(2S)}$ production in p-Pb collisions at $\sqrt{\textit{s}_{\rm NN}} = 8.16$ TeV"

description: Inclusive $\psi(2{\rm S})$ differential cross section times branching ratio as a function of $p_{\rm T}$, at backward rapidity at $\sqrt{s_{\rm NN}}$ = 8.16 TeV .The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a correlated systematic uncertainty.
description: Inclusive $\psi(2{\rm S})$ production is measured in \ppb collisions at the centre-of-mass energy per nucleon--nucleon pair $\sqrt{s_{_{\rm NN}}}=8.16$ TeV, using the ALICE detector at the CERN LHC. The production of $\psi(2{\rm S})$ is studied at forward ($2.03 &lt; y_{\rm cms} &lt; 3.53$) and backward ($-4.46 &lt; y_{\rm cms} &lt; -2.96$) centre-of-mass rapidity and for transverse momentum \pt $&lt;$ 12 \gevc via the decay to muon pairs. In this paper, we report the integrated as well as the $y_{\rm cms}$- and $p_{\rm T}$-differential inclusive production cross sections. Nuclear effects on $\psi(2{\rm S})$ production are studied via the determination of the nuclear modification factor that shows a strong suppression at both forward and backward centre-of-mass rapidities. Comparisons with corresponding results for inclusive J$/psi$ show a similar suppression for the two states at forward rapidity (p-going direction), but a stronger suppression for $\psi(2{\rm S})$ at backward rapidity (Pb-going direction). As a function of $p_{\rm T}$, no clear dependence of the nuclear modification factor is found. The relative size of nuclear effects on $\psi(2{\rm S})$ production compared to J$/psi$ is also studied via the double ratio of production cross sections $[\sigma_{\psi({\rm 2S})}/\sigma_{{\rm J/}\psi}]_{\rm pPb}/[\sigma_{\psi({\rm 2S})}/\sigma_{{\rm J/}\psi}]_{\rm pp}$ between \ppb and \pp collisions. The results are compared with theoretical models that include various effects related to the initial and final state of the collision system and also with previous measurements at $\sqrt{s_{_{\rm NN}}}=5.02$ TeV.
DOI: 10.17182/hepdata.96029.v1/t4
title: "Table 4" of "Measurement of nuclear effects on $\psi\rm{(2S)}$ production in p-Pb collisions at $\sqrt{\textit{s}_{\rm NN}} = 8.16$ TeV"

description: Ratio of inclusive $\psi(2{\rm S})$ over J/$\psi$ yields times their branching ratios as a function of $y_{\rm cms}$ in p--Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV .The first uncertainty is statistical, while the second is the systematic.
description: Inclusive $\psi(2{\rm S})$ production is measured in \ppb collisions at the centre-of-mass energy per nucleon--nucleon pair $\sqrt{s_{_{\rm NN}}}=8.16$ TeV, using the ALICE detector at the CERN LHC. The production of $\psi(2{\rm S})$ is studied at forward ($2.03 &lt; y_{\rm cms} &lt; 3.53$) and backward ($-4.46 &lt; y_{\rm cms} &lt; -2.96$) centre-of-mass rapidity and for transverse momentum \pt $&lt;$ 12 \gevc via the decay to muon pairs. In this paper, we report the integrated as well as the $y_{\rm cms}$- and $p_{\rm T}$-differential inclusive production cross sections. Nuclear effects on $\psi(2{\rm S})$ production are studied via the determination of the nuclear modification factor that shows a strong suppression at both forward and backward centre-of-mass rapidities. Comparisons with corresponding results for inclusive J$/psi$ show a similar suppression for the two states at forward rapidity (p-going direction), but a stronger suppression for $\psi(2{\rm S})$ at backward rapidity (Pb-going direction). As a function of $p_{\rm T}$, no clear dependence of the nuclear modification factor is found. The relative size of nuclear effects on $\psi(2{\rm S})$ production compared to J$/psi$ is also studied via the double ratio of production cross sections $[\sigma_{\psi({\rm 2S})}/\sigma_{{\rm J/}\psi}]_{\rm pPb}/[\sigma_{\psi({\rm 2S})}/\sigma_{{\rm J/}\psi}]_{\rm pp}$ between \ppb and \pp collisions. The results are compared with theoretical models that include various effects related to the initial and final state of the collision system and also with previous measurements at $\sqrt{s_{_{\rm NN}}}=5.02$ TeV.
DOI: 10.17182/hepdata.96029.v1/t5
title: "Table 5" of "Measurement of nuclear effects on $\psi\rm{(2S)}$ production in p-Pb collisions at $\sqrt{\textit{s}_{\rm NN}} = 8.16$ TeV"

description: Ratio of inclusive $\psi(2{\rm S})$ over J/$\psi$ yields times their branching ratios as a function of $p_{\rm T}$ in p--Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV at forward rapidity.The first uncertainty is statistical, while the second is the systematic.
description: Inclusive $\psi(2{\rm S})$ production is measured in \ppb collisions at the centre-of-mass energy per nucleon--nucleon pair $\sqrt{s_{_{\rm NN}}}=8.16$ TeV, using the ALICE detector at the CERN LHC. The production of $\psi(2{\rm S})$ is studied at forward ($2.03 &lt; y_{\rm cms} &lt; 3.53$) and backward ($-4.46 &lt; y_{\rm cms} &lt; -2.96$) centre-of-mass rapidity and for transverse momentum \pt $&lt;$ 12 \gevc via the decay to muon pairs. In this paper, we report the integrated as well as the $y_{\rm cms}$- and $p_{\rm T}$-differential inclusive production cross sections. Nuclear effects on $\psi(2{\rm S})$ production are studied via the determination of the nuclear modification factor that shows a strong suppression at both forward and backward centre-of-mass rapidities. Comparisons with corresponding results for inclusive J$/psi$ show a similar suppression for the two states at forward rapidity (p-going direction), but a stronger suppression for $\psi(2{\rm S})$ at backward rapidity (Pb-going direction). As a function of $p_{\rm T}$, no clear dependence of the nuclear modification factor is found. The relative size of nuclear effects on $\psi(2{\rm S})$ production compared to J$/psi$ is also studied via the double ratio of production cross sections $[\sigma_{\psi({\rm 2S})}/\sigma_{{\rm J/}\psi}]_{\rm pPb}/[\sigma_{\psi({\rm 2S})}/\sigma_{{\rm J/}\psi}]_{\rm pp}$ between \ppb and \pp collisions. The results are compared with theoretical models that include various effects related to the initial and final state of the collision system and also with previous measurements at $\sqrt{s_{_{\rm NN}}}=5.02$ TeV.
DOI: 10.3535/td4-qv4-81t
title: Anthriscus cerefolium (L.) Hoffm.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.96029.v1/t10
title: "Table 10" of "Measurement of nuclear effects on $\psi\rm{(2S)}$ production in p-Pb collisions at $\sqrt{\textit{s}_{\rm NN}} = 8.16$ TeV"

description: Double ratio of $\psi$(2S) and J/$\psi$ cross sections in p--Pb and pp collisions as a function of rapidity, at $\sqrt{s_{\mathrm{NN}}} = 8.16$ TeV. The first uncertainty is statistical, while the second is the systematic.
description: Inclusive $\psi(2{\rm S})$ production is measured in \ppb collisions at the centre-of-mass energy per nucleon--nucleon pair $\sqrt{s_{_{\rm NN}}}=8.16$ TeV, using the ALICE detector at the CERN LHC. The production of $\psi(2{\rm S})$ is studied at forward ($2.03 &lt; y_{\rm cms} &lt; 3.53$) and backward ($-4.46 &lt; y_{\rm cms} &lt; -2.96$) centre-of-mass rapidity and for transverse momentum \pt $&lt;$ 12 \gevc via the decay to muon pairs. In this paper, we report the integrated as well as the $y_{\rm cms}$- and $p_{\rm T}$-differential inclusive production cross sections. Nuclear effects on $\psi(2{\rm S})$ production are studied via the determination of the nuclear modification factor that shows a strong suppression at both forward and backward centre-of-mass rapidities. Comparisons with corresponding results for inclusive J$/psi$ show a similar suppression for the two states at forward rapidity (p-going direction), but a stronger suppression for $\psi(2{\rm S})$ at backward rapidity (Pb-going direction). As a function of $p_{\rm T}$, no clear dependence of the nuclear modification factor is found. The relative size of nuclear effects on $\psi(2{\rm S})$ production compared to J$/psi$ is also studied via the double ratio of production cross sections $[\sigma_{\psi({\rm 2S})}/\sigma_{{\rm J/}\psi}]_{\rm pPb}/[\sigma_{\psi({\rm 2S})}/\sigma_{{\rm J/}\psi}]_{\rm pp}$ between \ppb and \pp collisions. The results are compared with theoretical models that include various effects related to the initial and final state of the collision system and also with previous measurements at $\sqrt{s_{_{\rm NN}}}=5.02$ TeV.
DOI: 10.17182/hepdata.96029.v1/t11
title: "Table 11" of "Measurement of nuclear effects on $\psi\rm{(2S)}$ production in p-Pb collisions at $\sqrt{\textit{s}_{\rm NN}} = 8.16$ TeV"

description: Double ratio of $\psi$(2S) and J/$\psi$ cross sections in p--Pb and pp collisions as a function of $p_{\rm T}$, at $\sqrt{s_{\mathrm{NN}}} = 8.16$ TeV at forward rapidity. The first uncertainty is statistical, while the second is the systematic.
description: Inclusive $\psi(2{\rm S})$ production is measured in \ppb collisions at the centre-of-mass energy per nucleon--nucleon pair $\sqrt{s_{_{\rm NN}}}=8.16$ TeV, using the ALICE detector at the CERN LHC. The production of $\psi(2{\rm S})$ is studied at forward ($2.03 &lt; y_{\rm cms} &lt; 3.53$) and backward ($-4.46 &lt; y_{\rm cms} &lt; -2.96$) centre-of-mass rapidity and for transverse momentum \pt $&lt;$ 12 \gevc via the decay to muon pairs. In this paper, we report the integrated as well as the $y_{\rm cms}$- and $p_{\rm T}$-differential inclusive production cross sections. Nuclear effects on $\psi(2{\rm S})$ production are studied via the determination of the nuclear modification factor that shows a strong suppression at both forward and backward centre-of-mass rapidities. Comparisons with corresponding results for inclusive J$/psi$ show a similar suppression for the two states at forward rapidity (p-going direction), but a stronger suppression for $\psi(2{\rm S})$ at backward rapidity (Pb-going direction). As a function of $p_{\rm T}$, no clear dependence of the nuclear modification factor is found. The relative size of nuclear effects on $\psi(2{\rm S})$ production compared to J$/psi$ is also studied via the double ratio of production cross sections $[\sigma_{\psi({\rm 2S})}/\sigma_{{\rm J/}\psi}]_{\rm pPb}/[\sigma_{\psi({\rm 2S})}/\sigma_{{\rm J/}\psi}]_{\rm pp}$ between \ppb and \pp collisions. The results are compared with theoretical models that include various effects related to the initial and final state of the collision system and also with previous measurements at $\sqrt{s_{_{\rm NN}}}=5.02$ TeV.
DOI: 10.17182/hepdata.96029.v1/t6
title: "Table 6" of "Measurement of nuclear effects on $\psi\rm{(2S)}$ production in p-Pb collisions at $\sqrt{\textit{s}_{\rm NN}} = 8.16$ TeV"

description: Ratio of inclusive $\psi(2{\rm S})$ over J/$\psi$ yields times their branching ratios as a function of $p_{\rm T}$ in p--Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV at backward rapidity.The first uncertainty is statistical, while the second is the systematic.
description: Inclusive $\psi(2{\rm S})$ production is measured in \ppb collisions at the centre-of-mass energy per nucleon--nucleon pair $\sqrt{s_{_{\rm NN}}}=8.16$ TeV, using the ALICE detector at the CERN LHC. The production of $\psi(2{\rm S})$ is studied at forward ($2.03 &lt; y_{\rm cms} &lt; 3.53$) and backward ($-4.46 &lt; y_{\rm cms} &lt; -2.96$) centre-of-mass rapidity and for transverse momentum \pt $&lt;$ 12 \gevc via the decay to muon pairs. In this paper, we report the integrated as well as the $y_{\rm cms}$- and $p_{\rm T}$-differential inclusive production cross sections. Nuclear effects on $\psi(2{\rm S})$ production are studied via the determination of the nuclear modification factor that shows a strong suppression at both forward and backward centre-of-mass rapidities. Comparisons with corresponding results for inclusive J$/psi$ show a similar suppression for the two states at forward rapidity (p-going direction), but a stronger suppression for $\psi(2{\rm S})$ at backward rapidity (Pb-going direction). As a function of $p_{\rm T}$, no clear dependence of the nuclear modification factor is found. The relative size of nuclear effects on $\psi(2{\rm S})$ production compared to J$/psi$ is also studied via the double ratio of production cross sections $[\sigma_{\psi({\rm 2S})}/\sigma_{{\rm J/}\psi}]_{\rm pPb}/[\sigma_{\psi({\rm 2S})}/\sigma_{{\rm J/}\psi}]_{\rm pp}$ between \ppb and \pp collisions. The results are compared with theoretical models that include various effects related to the initial and final state of the collision system and also with previous measurements at $\sqrt{s_{_{\rm NN}}}=5.02$ TeV.
DOI: 10.17182/hepdata.96029.v1/t7
title: "Table 7" of "Measurement of nuclear effects on $\psi\rm{(2S)}$ production in p-Pb collisions at $\sqrt{\textit{s}_{\rm NN}} = 8.16$ TeV"

description: Inclusive $\psi(2{\rm S})$ $R_{\rm pPb}$ values as a function of $y_{\rm {cms}}$ at $\sqrt{s_{\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a correlated systematic uncertainty.
description: Inclusive $\psi(2{\rm S})$ production is measured in \ppb collisions at the centre-of-mass energy per nucleon--nucleon pair $\sqrt{s_{_{\rm NN}}}=8.16$ TeV, using the ALICE detector at the CERN LHC. The production of $\psi(2{\rm S})$ is studied at forward ($2.03 &lt; y_{\rm cms} &lt; 3.53$) and backward ($-4.46 &lt; y_{\rm cms} &lt; -2.96$) centre-of-mass rapidity and for transverse momentum \pt $&lt;$ 12 \gevc via the decay to muon pairs. In this paper, we report the integrated as well as the $y_{\rm cms}$- and $p_{\rm T}$-differential inclusive production cross sections. Nuclear effects on $\psi(2{\rm S})$ production are studied via the determination of the nuclear modification factor that shows a strong suppression at both forward and backward centre-of-mass rapidities. Comparisons with corresponding results for inclusive J$/psi$ show a similar suppression for the two states at forward rapidity (p-going direction), but a stronger suppression for $\psi(2{\rm S})$ at backward rapidity (Pb-going direction). As a function of $p_{\rm T}$, no clear dependence of the nuclear modification factor is found. The relative size of nuclear effects on $\psi(2{\rm S})$ production compared to J$/psi$ is also studied via the double ratio of production cross sections $[\sigma_{\psi({\rm 2S})}/\sigma_{{\rm J/}\psi}]_{\rm pPb}/[\sigma_{\psi({\rm 2S})}/\sigma_{{\rm J/}\psi}]_{\rm pp}$ between \ppb and \pp collisions. The results are compared with theoretical models that include various effects related to the initial and final state of the collision system and also with previous measurements at $\sqrt{s_{_{\rm NN}}}=5.02$ TeV.
DOI: 10.17182/hepdata.96029.v1/t8
title: "Table 8" of "Measurement of nuclear effects on $\psi\rm{(2S)}$ production in p-Pb collisions at $\sqrt{\textit{s}_{\rm NN}} = 8.16$ TeV"

description: Inclusive $\psi(2{\rm S})$ $R_{\rm pPb}$ values as a function of $p_{\rm T}$ at $\sqrt{s_{\rm NN}}$ = 8.16 TeV at forward rapidity. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a correlated systematic uncertainty.
description: Inclusive $\psi(2{\rm S})$ production is measured in \ppb collisions at the centre-of-mass energy per nucleon--nucleon pair $\sqrt{s_{_{\rm NN}}}=8.16$ TeV, using the ALICE detector at the CERN LHC. The production of $\psi(2{\rm S})$ is studied at forward ($2.03 &lt; y_{\rm cms} &lt; 3.53$) and backward ($-4.46 &lt; y_{\rm cms} &lt; -2.96$) centre-of-mass rapidity and for transverse momentum \pt $&lt;$ 12 \gevc via the decay to muon pairs. In this paper, we report the integrated as well as the $y_{\rm cms}$- and $p_{\rm T}$-differential inclusive production cross sections. Nuclear effects on $\psi(2{\rm S})$ production are studied via the determination of the nuclear modification factor that shows a strong suppression at both forward and backward centre-of-mass rapidities. Comparisons with corresponding results for inclusive J$/psi$ show a similar suppression for the two states at forward rapidity (p-going direction), but a stronger suppression for $\psi(2{\rm S})$ at backward rapidity (Pb-going direction). As a function of $p_{\rm T}$, no clear dependence of the nuclear modification factor is found. The relative size of nuclear effects on $\psi(2{\rm S})$ production compared to J$/psi$ is also studied via the double ratio of production cross sections $[\sigma_{\psi({\rm 2S})}/\sigma_{{\rm J/}\psi}]_{\rm pPb}/[\sigma_{\psi({\rm 2S})}/\sigma_{{\rm J/}\psi}]_{\rm pp}$ between \ppb and \pp collisions. The results are compared with theoretical models that include various effects related to the initial and final state of the collision system and also with previous measurements at $\sqrt{s_{_{\rm NN}}}=5.02$ TeV.
DOI: 10.17182/hepdata.96029.v1/t9
title: "Table 9" of "Measurement of nuclear effects on $\psi\rm{(2S)}$ production in p-Pb collisions at $\sqrt{\textit{s}_{\rm NN}} = 8.16$ TeV"

description: Inclusive $\psi(2{\rm S})$ $R_{\rm pPb}$ values as a function of $p_{\rm T}$ at $\sqrt{s_{\rm NN}}$ = 8.16 TeV at backward rapidity. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a correlated systematic uncertainty.
description: Inclusive $\psi(2{\rm S})$ production is measured in \ppb collisions at the centre-of-mass energy per nucleon--nucleon pair $\sqrt{s_{_{\rm NN}}}=8.16$ TeV, using the ALICE detector at the CERN LHC. The production of $\psi(2{\rm S})$ is studied at forward ($2.03 &lt; y_{\rm cms} &lt; 3.53$) and backward ($-4.46 &lt; y_{\rm cms} &lt; -2.96$) centre-of-mass rapidity and for transverse momentum \pt $&lt;$ 12 \gevc via the decay to muon pairs. In this paper, we report the integrated as well as the $y_{\rm cms}$- and $p_{\rm T}$-differential inclusive production cross sections. Nuclear effects on $\psi(2{\rm S})$ production are studied via the determination of the nuclear modification factor that shows a strong suppression at both forward and backward centre-of-mass rapidities. Comparisons with corresponding results for inclusive J$/psi$ show a similar suppression for the two states at forward rapidity (p-going direction), but a stronger suppression for $\psi(2{\rm S})$ at backward rapidity (Pb-going direction). As a function of $p_{\rm T}$, no clear dependence of the nuclear modification factor is found. The relative size of nuclear effects on $\psi(2{\rm S})$ production compared to J$/psi$ is also studied via the double ratio of production cross sections $[\sigma_{\psi({\rm 2S})}/\sigma_{{\rm J/}\psi}]_{\rm pPb}/[\sigma_{\psi({\rm 2S})}/\sigma_{{\rm J/}\psi}]_{\rm pp}$ between \ppb and \pp collisions. The results are compared with theoretical models that include various effects related to the initial and final state of the collision system and also with previous measurements at $\sqrt{s_{_{\rm NN}}}=5.02$ TeV.
DOI: 10.3535/8zk-x4p-yaz
title: Dactylis glomerata L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/m05-5gm-z87
title: Vicia sativa subsp. nigra Ehrh.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.96029.v1/t12
title: "Table 12" of "Measurement of nuclear effects on $\psi\rm{(2S)}$ production in p-Pb collisions at $\sqrt{\textit{s}_{\rm NN}} = 8.16$ TeV"

description: Double ratio of $\psi$(2S) and J/$\psi$ cross sections in p--Pb and pp collisions as a function of $p_{\rm T}$, at $\sqrt{s_{\mathrm{NN}}} = 8.16$ TeV at backward rapidity. The first uncertainty is statistical, while the second is the systematic.
description: Inclusive $\psi(2{\rm S})$ production is measured in \ppb collisions at the centre-of-mass energy per nucleon--nucleon pair $\sqrt{s_{_{\rm NN}}}=8.16$ TeV, using the ALICE detector at the CERN LHC. The production of $\psi(2{\rm S})$ is studied at forward ($2.03 &lt; y_{\rm cms} &lt; 3.53$) and backward ($-4.46 &lt; y_{\rm cms} &lt; -2.96$) centre-of-mass rapidity and for transverse momentum \pt $&lt;$ 12 \gevc via the decay to muon pairs. In this paper, we report the integrated as well as the $y_{\rm cms}$- and $p_{\rm T}$-differential inclusive production cross sections. Nuclear effects on $\psi(2{\rm S})$ production are studied via the determination of the nuclear modification factor that shows a strong suppression at both forward and backward centre-of-mass rapidities. Comparisons with corresponding results for inclusive J$/psi$ show a similar suppression for the two states at forward rapidity (p-going direction), but a stronger suppression for $\psi(2{\rm S})$ at backward rapidity (Pb-going direction). As a function of $p_{\rm T}$, no clear dependence of the nuclear modification factor is found. The relative size of nuclear effects on $\psi(2{\rm S})$ production compared to J$/psi$ is also studied via the double ratio of production cross sections $[\sigma_{\psi({\rm 2S})}/\sigma_{{\rm J/}\psi}]_{\rm pPb}/[\sigma_{\psi({\rm 2S})}/\sigma_{{\rm J/}\psi}]_{\rm pp}$ between \ppb and \pp collisions. The results are compared with theoretical models that include various effects related to the initial and final state of the collision system and also with previous measurements at $\sqrt{s_{_{\rm NN}}}=5.02$ TeV.