cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.159489.v1/t64
title: "Fig3_3.9GeV_$p$" of "Observation of the Onset of Constituent Quark Number Scaling in Heavy-Ion Collisions at RHIC"

description: The number of constituent quarks $n_q$ scaled $v_2$ as a function of $n_q$ scaled transverse kinetic energy for $p$ at 3.9 GeV
description: Partonic collectivity is one of the necessary signatures for the formation of Quark-Gluon-Plasma in high-energy nuclear collisions. Number of Constituent Quarks (NCQ) scaling has been observed for light hadron elliptic flow $v_2$ in top energy nuclear collisions at RHIC and the LHC, and this has been theoretically suggested as strong evidence for partonic collectivity. In this letter, a systematic analysis of $v_2$ of $\pi^{\pm}$, $K^{\pm}$, $K^{0}_{S}$, $p$ and $\Lambda$ in Au+Au collisions at $\sqrt{s_{\text{NN}}}$ = 3.2, 3.5, 3.9, and 4.5 GeV, with the STAR experiment at RHIC, is presented. NCQ scaling is markedly violated at 3.2 GeV, consistent with a hadronic-interaction dominated equation of state. However, as the collision energy increases, a gradual evolution to NCQ scaling is observed. This beam-energy dependence of $v_2$ for all hadrons studied provides evidence for the onset of dominant partonic interactions by $\sqrt{s_{\text{NN}}}$ = 4.5 GeV.
DOI: 10.17182/hepdata.159489.v1/t65
title: "Fig3_4.5GeV_$p$" of "Observation of the Onset of Constituent Quark Number Scaling in Heavy-Ion Collisions at RHIC"

description: The number of constituent quarks $n_q$ scaled $v_2$ as a function of $n_q$ scaled transverse kinetic energy for $p$ at 4.5 GeV
description: Partonic collectivity is one of the necessary signatures for the formation of Quark-Gluon-Plasma in high-energy nuclear collisions. Number of Constituent Quarks (NCQ) scaling has been observed for light hadron elliptic flow $v_2$ in top energy nuclear collisions at RHIC and the LHC, and this has been theoretically suggested as strong evidence for partonic collectivity. In this letter, a systematic analysis of $v_2$ of $\pi^{\pm}$, $K^{\pm}$, $K^{0}_{S}$, $p$ and $\Lambda$ in Au+Au collisions at $\sqrt{s_{\text{NN}}}$ = 3.2, 3.5, 3.9, and 4.5 GeV, with the STAR experiment at RHIC, is presented. NCQ scaling is markedly violated at 3.2 GeV, consistent with a hadronic-interaction dominated equation of state. However, as the collision energy increases, a gradual evolution to NCQ scaling is observed. This beam-energy dependence of $v_2$ for all hadrons studied provides evidence for the onset of dominant partonic interactions by $\sqrt{s_{\text{NN}}}$ = 4.5 GeV.
DOI: 10.17182/hepdata.159489.v1/t66
title: "Fig3_3GeV_$\Lambda$" of "Observation of the Onset of Constituent Quark Number Scaling in Heavy-Ion Collisions at RHIC"

description: The number of constituent quarks $n_q$ scaled $v_2$ as a function of $n_q$ scaled transverse kinetic energy for $\Lambda$ at 3 GeV
description: Partonic collectivity is one of the necessary signatures for the formation of Quark-Gluon-Plasma in high-energy nuclear collisions. Number of Constituent Quarks (NCQ) scaling has been observed for light hadron elliptic flow $v_2$ in top energy nuclear collisions at RHIC and the LHC, and this has been theoretically suggested as strong evidence for partonic collectivity. In this letter, a systematic analysis of $v_2$ of $\pi^{\pm}$, $K^{\pm}$, $K^{0}_{S}$, $p$ and $\Lambda$ in Au+Au collisions at $\sqrt{s_{\text{NN}}}$ = 3.2, 3.5, 3.9, and 4.5 GeV, with the STAR experiment at RHIC, is presented. NCQ scaling is markedly violated at 3.2 GeV, consistent with a hadronic-interaction dominated equation of state. However, as the collision energy increases, a gradual evolution to NCQ scaling is observed. This beam-energy dependence of $v_2$ for all hadrons studied provides evidence for the onset of dominant partonic interactions by $\sqrt{s_{\text{NN}}}$ = 4.5 GeV.
DOI: 10.17182/hepdata.159489.v1/t67
title: "Fig3_3.2GeV_$\Lambda$" of "Observation of the Onset of Constituent Quark Number Scaling in Heavy-Ion Collisions at RHIC"

description: The number of constituent quarks $n_q$ scaled $v_2$ as a function of $n_q$ scaled transverse kinetic energy for $\Lambda$ at 3.2 GeV
description: Partonic collectivity is one of the necessary signatures for the formation of Quark-Gluon-Plasma in high-energy nuclear collisions. Number of Constituent Quarks (NCQ) scaling has been observed for light hadron elliptic flow $v_2$ in top energy nuclear collisions at RHIC and the LHC, and this has been theoretically suggested as strong evidence for partonic collectivity. In this letter, a systematic analysis of $v_2$ of $\pi^{\pm}$, $K^{\pm}$, $K^{0}_{S}$, $p$ and $\Lambda$ in Au+Au collisions at $\sqrt{s_{\text{NN}}}$ = 3.2, 3.5, 3.9, and 4.5 GeV, with the STAR experiment at RHIC, is presented. NCQ scaling is markedly violated at 3.2 GeV, consistent with a hadronic-interaction dominated equation of state. However, as the collision energy increases, a gradual evolution to NCQ scaling is observed. This beam-energy dependence of $v_2$ for all hadrons studied provides evidence for the onset of dominant partonic interactions by $\sqrt{s_{\text{NN}}}$ = 4.5 GeV.
DOI: 10.17182/hepdata.159489.v1/t68
title: "Fig3_3.5GeV_$\Lambda$" of "Observation of the Onset of Constituent Quark Number Scaling in Heavy-Ion Collisions at RHIC"

description: The number of constituent quarks $n_q$ scaled $v_2$ as a function of $n_q$ scaled transverse kinetic energy for $\Lambda$ at 3.5 GeV
description: Partonic collectivity is one of the necessary signatures for the formation of Quark-Gluon-Plasma in high-energy nuclear collisions. Number of Constituent Quarks (NCQ) scaling has been observed for light hadron elliptic flow $v_2$ in top energy nuclear collisions at RHIC and the LHC, and this has been theoretically suggested as strong evidence for partonic collectivity. In this letter, a systematic analysis of $v_2$ of $\pi^{\pm}$, $K^{\pm}$, $K^{0}_{S}$, $p$ and $\Lambda$ in Au+Au collisions at $\sqrt{s_{\text{NN}}}$ = 3.2, 3.5, 3.9, and 4.5 GeV, with the STAR experiment at RHIC, is presented. NCQ scaling is markedly violated at 3.2 GeV, consistent with a hadronic-interaction dominated equation of state. However, as the collision energy increases, a gradual evolution to NCQ scaling is observed. This beam-energy dependence of $v_2$ for all hadrons studied provides evidence for the onset of dominant partonic interactions by $\sqrt{s_{\text{NN}}}$ = 4.5 GeV.
DOI: 10.17182/hepdata.159489.v1/t69
title: "Fig3_3.9GeV_$\Lambda$" of "Observation of the Onset of Constituent Quark Number Scaling in Heavy-Ion Collisions at RHIC"

description: The number of constituent quarks $n_q$ scaled $v_2$ as a function of $n_q$ scaled transverse kinetic energy for $\Lambda$ at 3.9 GeV
description: Partonic collectivity is one of the necessary signatures for the formation of Quark-Gluon-Plasma in high-energy nuclear collisions. Number of Constituent Quarks (NCQ) scaling has been observed for light hadron elliptic flow $v_2$ in top energy nuclear collisions at RHIC and the LHC, and this has been theoretically suggested as strong evidence for partonic collectivity. In this letter, a systematic analysis of $v_2$ of $\pi^{\pm}$, $K^{\pm}$, $K^{0}_{S}$, $p$ and $\Lambda$ in Au+Au collisions at $\sqrt{s_{\text{NN}}}$ = 3.2, 3.5, 3.9, and 4.5 GeV, with the STAR experiment at RHIC, is presented. NCQ scaling is markedly violated at 3.2 GeV, consistent with a hadronic-interaction dominated equation of state. However, as the collision energy increases, a gradual evolution to NCQ scaling is observed. This beam-energy dependence of $v_2$ for all hadrons studied provides evidence for the onset of dominant partonic interactions by $\sqrt{s_{\text{NN}}}$ = 4.5 GeV.
DOI: 10.17182/hepdata.159489.v1/t70
title: "Fig3_4.5GeV_$\Lambda$" of "Observation of the Onset of Constituent Quark Number Scaling in Heavy-Ion Collisions at RHIC"

description: The number of constituent quarks $n_q$ scaled $v_2$ as a function of $n_q$ scaled transverse kinetic energy for $\Lambda$ at 4.5 GeV
description: Partonic collectivity is one of the necessary signatures for the formation of Quark-Gluon-Plasma in high-energy nuclear collisions. Number of Constituent Quarks (NCQ) scaling has been observed for light hadron elliptic flow $v_2$ in top energy nuclear collisions at RHIC and the LHC, and this has been theoretically suggested as strong evidence for partonic collectivity. In this letter, a systematic analysis of $v_2$ of $\pi^{\pm}$, $K^{\pm}$, $K^{0}_{S}$, $p$ and $\Lambda$ in Au+Au collisions at $\sqrt{s_{\text{NN}}}$ = 3.2, 3.5, 3.9, and 4.5 GeV, with the STAR experiment at RHIC, is presented. NCQ scaling is markedly violated at 3.2 GeV, consistent with a hadronic-interaction dominated equation of state. However, as the collision energy increases, a gradual evolution to NCQ scaling is observed. This beam-energy dependence of $v_2$ for all hadrons studied provides evidence for the onset of dominant partonic interactions by $\sqrt{s_{\text{NN}}}$ = 4.5 GeV.
DOI: 10.17182/hepdata.159489.v1/t71
title: "Fig4_a" of "Observation of the Onset of Constituent Quark Number Scaling in Heavy-Ion Collisions at RHIC"

description: The energy dependence of $p_T$ integrated $v_2$ for $\pi^{\pm}$, $K^{\pm}$, $K^{0}_{S}$, $p$, and $\Lambda$ in 10-40\% centrality from Au+Au collisions at $\sqrt{s_{\text{NN}}}$ = 3.0, 3.2, 3.5, 3.9, and 4.5 GeV.
description: Partonic collectivity is one of the necessary signatures for the formation of Quark-Gluon-Plasma in high-energy nuclear collisions. Number of Constituent Quarks (NCQ) scaling has been observed for light hadron elliptic flow $v_2$ in top energy nuclear collisions at RHIC and the LHC, and this has been theoretically suggested as strong evidence for partonic collectivity. In this letter, a systematic analysis of $v_2$ of $\pi^{\pm}$, $K^{\pm}$, $K^{0}_{S}$, $p$ and $\Lambda$ in Au+Au collisions at $\sqrt{s_{\text{NN}}}$ = 3.2, 3.5, 3.9, and 4.5 GeV, with the STAR experiment at RHIC, is presented. NCQ scaling is markedly violated at 3.2 GeV, consistent with a hadronic-interaction dominated equation of state. However, as the collision energy increases, a gradual evolution to NCQ scaling is observed. This beam-energy dependence of $v_2$ for all hadrons studied provides evidence for the onset of dominant partonic interactions by $\sqrt{s_{\text{NN}}}$ = 4.5 GeV.
DOI: 10.17182/hepdata.159489.v1/t72
title: "Fig4_b" of "Observation of the Onset of Constituent Quark Number Scaling in Heavy-Ion Collisions at RHIC"

description: The energy dependence of $n_{q}$ scaled $v_{2}$ ratios of $v_{2}^{q}(\pi^{+}) / v_{2}^{q}(K^{+})$ and $v_{2}^{q}(p) / v_{2}^{q}(K^{+})$ at ($m_T - m_0$)/$n_q$ = 0.4 GeV/$c^2$
description: Partonic collectivity is one of the necessary signatures for the formation of Quark-Gluon-Plasma in high-energy nuclear collisions. Number of Constituent Quarks (NCQ) scaling has been observed for light hadron elliptic flow $v_2$ in top energy nuclear collisions at RHIC and the LHC, and this has been theoretically suggested as strong evidence for partonic collectivity. In this letter, a systematic analysis of $v_2$ of $\pi^{\pm}$, $K^{\pm}$, $K^{0}_{S}$, $p$ and $\Lambda$ in Au+Au collisions at $\sqrt{s_{\text{NN}}}$ = 3.2, 3.5, 3.9, and 4.5 GeV, with the STAR experiment at RHIC, is presented. NCQ scaling is markedly violated at 3.2 GeV, consistent with a hadronic-interaction dominated equation of state. However, as the collision energy increases, a gradual evolution to NCQ scaling is observed. This beam-energy dependence of $v_2$ for all hadrons studied provides evidence for the onset of dominant partonic interactions by $\sqrt{s_{\text{NN}}}$ = 4.5 GeV.
DOI: 10.5281/zenodo.18275460
title: Erigeron bonariensis L. In: Marchesi E., Mailhos A. & Bonifacino J.M. (Eds.). Flora Uruguaya: Flora Vascular del Uruguay. ISSN 3121-2050, V. 1.0.

description: Citable snapshot. Includes PDF and CSV of collections. Date: January 13th, 2026 at 16:46
DOI: 10.5281/zenodo.18275461
title: Erigeron bonariensis L. In: Marchesi E., Mailhos A. & Bonifacino J.M. (Eds.). Flora Uruguaya: Flora Vascular del Uruguay. ISSN 3121-2050, V. 1.0.

description: Citable snapshot. Includes PDF and CSV of collections. Date: January 13th, 2026 at 16:46
DOI: 10.5281/zenodo.18275465
title: Erigeron caespitosus Nutt. In: Marchesi E., Mailhos A. & Bonifacino J.M. (Eds.). Flora Uruguaya: Flora Vascular del Uruguay. ISSN 3121-2050, V. 1.0.

description: Citable snapshot. Includes PDF and CSV of collections. Date: January 13th, 2026 at 16:46
DOI: 10.5281/zenodo.18275464
title: Erigeron caespitosus Nutt. In: Marchesi E., Mailhos A. & Bonifacino J.M. (Eds.). Flora Uruguaya: Flora Vascular del Uruguay. ISSN 3121-2050, V. 1.0.

description: Citable snapshot. Includes PDF and CSV of collections. Date: January 13th, 2026 at 16:46
DOI: 10.15468/dl.b2s4yp
title: Occurrence Download

description: A dataset containing 37219 species occurrences available in GBIF matching the query:
{
 "and" : [
 "Country is Belgium",
 "TaxonKey is one of (Crassula helmsii, Lithobates catesbeianus, Misgurnus mohoity, Myriophyllum aquaticum, Procambarus clarkii, Procambarus virginalis, Xenopus laevis, Zizania latifolia)",
 "OccurrenceStatus is Present",
 "Year is greater than or equal to 2000"
 ]
}

 The dataset includes 37219 records from 39 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015727-260108223611665/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.5281/zenodo.18275466
title: Erigeron canadensis  L. In: Marchesi E., Mailhos A. & Bonifacino J.M. (Eds.). Flora Uruguaya: Flora Vascular del Uruguay. ISSN 3121-2050, V. 1.0.

description: Citable snapshot. Includes PDF and CSV of collections. Date: January 13th, 2026 at 16:46
DOI: 10.5281/zenodo.18275467
title: Erigeron canadensis  L. In: Marchesi E., Mailhos A. & Bonifacino J.M. (Eds.). Flora Uruguaya: Flora Vascular del Uruguay. ISSN 3121-2050, V. 1.0.

description: Citable snapshot. Includes PDF and CSV of collections. Date: January 13th, 2026 at 16:46
DOI: 10.15468/dl.jswbta
title: Occurrence Download

description: A dataset containing 18 species occurrences available in GBIF matching the query:
{
 "TaxonKey" : [
 "is Protobothrops trungkhanhensis"
 ]
}

 The dataset includes 18 records from 4 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015728-260108223611665/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.5281/zenodo.18275471
title: Erigeron chilensis (Spreng.) D.Don ex G.Don. In: Marchesi E., Mailhos A. & Bonifacino J.M. (Eds.). Flora Uruguaya: Flora Vascular del Uruguay. ISSN 3121-2050, V. 1.0.

description: Citable snapshot. Includes PDF and CSV of collections. Date: January 13th, 2026 at 16:46
DOI: 10.5281/zenodo.18275472
title: Erigeron chilensis (Spreng.) D.Don ex G.Don. In: Marchesi E., Mailhos A. & Bonifacino J.M. (Eds.). Flora Uruguaya: Flora Vascular del Uruguay. ISSN 3121-2050, V. 1.0.

description: Citable snapshot. Includes PDF and CSV of collections. Date: January 13th, 2026 at 16:46
DOI: 10.34740/kaggle/dsv/14522695
title: SOLANA Price Data Binance API (2020–Now)
DOI: 10.5281/zenodo.18274885
title: SuperDARN data in netCDF format (1996-Mar)

description: 1996-Mar SuperDARN radar data in netCDF format. These files were produced using version 3.0 of the public FitACF algorithm, using the AACGM v2 coordinate system. Cite this dataset if using our data in a publication.


The RST is available here: https://github.com/SuperDARN/rst



The research enabled by SuperDARN is due to the efforts of teams of scientists and engineers working in many countries to build and operate radars, process data and provide access, develop and improve data products, and assist users in interpretation.
Users of SuperDARN data and data products are asked to acknowledge this support in presentations and publications.
A brief statement on how to acknowledge use of SuperDARN data is provided below.




Users are also asked to consult with a SuperDARN PI prior to submission of work intended for publication.
A listing of radars and PIs with contact information can be found here:
(SuperDARN Radar Overview)



Recommended form of acknowledgement for the use of SuperDARN data:



'The authors acknowledge the use of SuperDARN data. SuperDARN is a collection of radars funded by national scientific funding agencies of Australia, Canada, China, France, Italy, Japan, Norway, South Africa, United Kingdom and the United States of America.'
DOI: 10.5281/zenodo.6809373
title: SuperDARN data in netCDF format (1996-Mar)

description: 1996-Mar SuperDARN radar data in netCDF format. These files were produced using version 3.0 of the public FitACF algorithm, using the AACGM v2 coordinate system. Cite this dataset if using our data in a publication.


The RST is available here: https://github.com/SuperDARN/rst



The research enabled by SuperDARN is due to the efforts of teams of scientists and engineers working in many countries to build and operate radars, process data and provide access, develop and improve data products, and assist users in interpretation.
Users of SuperDARN data and data products are asked to acknowledge this support in presentations and publications.
A brief statement on how to acknowledge use of SuperDARN data is provided below.




Users are also asked to consult with a SuperDARN PI prior to submission of work intended for publication.
A listing of radars and PIs with contact information can be found here:
(SuperDARN Radar Overview)



Recommended form of acknowledgement for the use of SuperDARN data:



'The authors acknowledge the use of SuperDARN data. SuperDARN is a collection of radars funded by national scientific funding agencies of Australia, Canada, China, France, Italy, Japan, Norway, South Africa, United Kingdom and the United States of America.'
DOI: 10.5281/zenodo.18275476
title: Erigeron chrysopsidis A.Gray. In: Marchesi E., Mailhos A. & Bonifacino J.M. (Eds.). Flora Uruguaya: Flora Vascular del Uruguay. ISSN 3121-2050, V. 1.0.

description: Citable snapshot. Includes PDF and CSV of collections. Date: January 13th, 2026 at 16:46
DOI: 10.5281/zenodo.18275477
title: Erigeron chrysopsidis A.Gray. In: Marchesi E., Mailhos A. & Bonifacino J.M. (Eds.). Flora Uruguaya: Flora Vascular del Uruguay. ISSN 3121-2050, V. 1.0.

description: Citable snapshot. Includes PDF and CSV of collections. Date: January 13th, 2026 at 16:46
DOI: 10.5281/zenodo.18275481
title: Erigeron compositus Pursh. In: Marchesi E., Mailhos A. & Bonifacino J.M. (Eds.). Flora Uruguaya: Flora Vascular del Uruguay. ISSN 3121-2050, V. 1.0.

description: Citable snapshot. Includes PDF and CSV of collections. Date: January 13th, 2026 at 16:46
DOI: 10.5281/zenodo.18275480
title: Erigeron compositus Pursh. In: Marchesi E., Mailhos A. & Bonifacino J.M. (Eds.). Flora Uruguaya: Flora Vascular del Uruguay. ISSN 3121-2050, V. 1.0.

description: Citable snapshot. Includes PDF and CSV of collections. Date: January 13th, 2026 at 16:46
DOI: 10.15468/dl.vudzg5
title: Occurrence Download

description: A dataset containing 62705 species occurrences available in GBIF matching the query:
{
 "TaxonKey" : [
 "is Opisthocomus hoazin"
 ]
}

 The dataset includes 62705 records from 196 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015710-260108223611665/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.15468/dl.9ybhc7
title: Occurrence Download

description: A dataset containing 199546 species occurrences available in GBIF matching the query:
{
 "and" : [
 "TaxonKey is Sus scrofa",
 "Country is France",
 "HasCoordinate is true"
 ]
}

 The dataset includes 199546 records from 2621 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015718-260108223611665/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.13130/rd_unimi/a1knyh/7q8a4e
title: d1_mean_5am_96t.csv
DOI: 10.13130/rd_unimi/a1knyh/qdwl6b
title: ener_prod_m0_flinear_d4_mean_5am_periodic_eucl_dist_p12.tab
DOI: 10.13130/rd_unimi/a1knyh/fabzsq
title: d6_mean_5am_periodic_eucl_dist_p12.tab
DOI: 10.13130/rd_unimi/a1knyh/pkaknv
title: ener_prod_m0_flinear_d4_mean_5am_periodic_cos_dist_p48.csv
DOI: 10.13130/rd_unimi/a1knyh/dd75pp
title: d2_mean_5am_periodic_cos_dist_p24.tab
DOI: 10.13130/rd_unimi/a1knyh/h4coih
title: d3_mean_5am_periodic_cos_dist_p48.csv
DOI: 10.13130/rd_unimi/a1knyh/fw1kci
title: ener_prod_m0_flinear_d0_mean_5am_periodic_eucl_dist_p48.csv
DOI: 10.13130/rd_unimi/a1knyh/qt7rzr
title: ener_prod_m0_flinear_d5_mean_5am_periodic_cos_dist_p12.tab
DOI: 10.13130/rd_unimi/a1knyh/lmlly8
title: ener_store_max_m0_flinear_d4_mean_5am_periodic_sum_dist_p12.csv
DOI: 10.13130/rd_unimi/a1knyh/s4rdjg
title: ener_store_max_m0_flinear_d2_mean_5am_periodic_cos_dist_p48.csv
DOI: 10.13130/rd_unimi/a1knyh/hrildz
title: ener_prod_m0_flinear_d6_mean_5am_periodic_cos_dist_p48.tab
DOI: 10.13130/rd_unimi/a1knyh/ikeutn
title: ener_store_max_m0_flinear_d0_mean_5am_periodic_sum_dist_p12.csv
DOI: 10.13130/rd_unimi/a1knyh/gmlwfe
title: d2_mean_5am_periodic_sum_dist_p12.tab
DOI: 10.13130/rd_unimi/a1knyh/tfhjfq
title: ener_prod_m0_flinear_d2_mean_5am_periodic_eucl_dist_p24.tab
DOI: 10.13130/rd_unimi/a1knyh/5shekh
title: ener_prod_m0_flinear_d5_mean_5am_periodic_eucl_dist_p24.tab
DOI: 10.13130/rd_unimi/a1knyh/stbusg
title: ener_prod_m0_flinear_d2_mean_5am_periodic_cos_dist_p12.tab
DOI: 10.13130/rd_unimi/a1knyh/7so38f
title: d3_mean_5am_periodic_eucl_dist_p24.tab
DOI: 10.13130/rd_unimi/a1knyh/tnw50a
title: ener_store_max_m0_flinear_d5_mean_5am_periodic_sum_dist_p48.csv
DOI: 10.13130/rd_unimi/a1knyh/c1ol3x
title: ener_prod_m0_flinear_d1_mean_5am_periodic_cos_dist_p48.csv
DOI: 10.13130/rd_unimi/a1knyh/tudhev
title: coord_AP_degree.tab
DOI: 10.13130/rd_unimi/a1knyh/famw12
title: ener_store_max_m0_flinear_96t.csv
DOI: 10.13130/rd_unimi/a1knyh/k0q2wr
title: d3_mean_5am_periodic_eucl_dist_p48.csv
DOI: 10.13130/rd_unimi/a1knyh/3xbxsm
title: d4_mean_5am_periodic_eucl_dist_p48.csv
DOI: 10.13130/rd_unimi/a1knyh/kumbtf
title: d4_mean_5am_periodic_cos_dist_p24.tab
DOI: 10.13130/rd_unimi/a1knyh/rkm6ij
title: d1_mean_5am_24t.tab
DOI: 10.13130/rd_unimi/a1knyh/gy5yoh
title: ener_prod_m0_flinear_d3_mean_5am_periodic_eucl_dist_p24.tab
DOI: 10.13130/rd_unimi/a1knyh/qnjxjw
title: ener_prod_m0_flinear_d0_mean_5am_periodic_cos_dist_p12.tab
DOI: 10.13130/rd_unimi/a1knyh/0pk4hr
title: d1_mean_5am_periodic_cos_dist_p48.csv
DOI: 10.13130/rd_unimi/a1knyh/rt2dhs
title: ener_prod_m0_flinear_d5_mean_5am_periodic_eucl_dist_p48.csv
DOI: 10.13130/rd_unimi/a1knyh/jkxybz
title: d4_mean_5am_periodic_sum_dist_p12.tab
DOI: 10.13130/rd_unimi/a1knyh/leauml
title: ener_prod_m0_flinear_d4_mean_5am_periodic_eucl_dist_p24.tab
DOI: 10.13130/rd_unimi/a1knyh/kakpty
title: ener_store_max_m0_flinear_d4_mean_5am_periodic_cos_dist_p24.csv
DOI: 10.13130/rd_unimi/a1knyh/kyukqh
title: d5_mean_5am_periodic_eucl_dist_p12.tab
DOI: 10.13130/rd_unimi/a1knyh/ahgkzd
title: ener_store_max_m0_flinear_d3_mean_5am_periodic_sum_dist_p24.csv
DOI: 10.13130/rd_unimi/a1knyh/ipkacy
title: ener_store_max_m0_flinear_d5_mean_5am_periodic_eucl_dist_p48.csv
DOI: 10.13130/rd_unimi/a1knyh/50ntjf
title: ener_prod_m0_flinear_d6_mean_5am_periodic_sum_dist_p12.tab
DOI: 10.13130/rd_unimi/a1knyh/clpwms
title: ener_prod_m0_flinear_12t.tab
DOI: 10.13130/rd_unimi/a1knyh/ula2ya
title: d2_mean_5am_periodic_eucl_dist_p12.tab
DOI: 10.13130/rd_unimi/a1knyh/nmnult
title: ener_prod_m0_flinear_d4_mean_5am_periodic_sum_dist_p48.tab
DOI: 10.13130/rd_unimi/a1knyh/s6fhfm
title: ener_store_max_m0_flinear_d2_mean_5am_periodic_sum_dist_p24.csv
DOI: 10.13130/rd_unimi/a1knyh/a8wlxv
title: ener_store_max_m0_flinear_d5_mean_5am_periodic_sum_dist_p24.csv
DOI: 10.13130/rd_unimi/a1knyh/i9v9et
title: ener_prod_m0_flinear_d3_mean_5am_periodic_cos_dist_p48.csv
DOI: 10.13130/rd_unimi/a1knyh/inogjc
title: CU.tab
DOI: 10.13130/rd_unimi/a1knyh/mfifuy
title: ener_prod_m0_flinear_d2_mean_5am_periodic_cos_dist_p48.csv
DOI: 10.13130/rd_unimi/a1knyh/dg7zzj
title: ener_store_max_m0_flinear_d5_mean_5am_periodic_eucl_dist_p24.csv