cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1662152
title: Materials Data on Rb2U6Pd4Se17 by Materials Project

description: Rb2U6Pd4Se17 crystallizes in the tetragonal P4/mnc space group. The structure is three-dimensional. Rb1+ is bonded in a 9-coordinate geometry to nine Se2- atoms. There are a spread of Rb–Se bond distances ranging from 3.44–3.75 Å. There are two inequivalent U4+ sites. In the first U4+ site, U4+ is bonded to seven Se2- atoms to form a mixture of distorted face and corner-sharing USe7 pentagonal bipyramids. There are a spread of U–Se bond distances ranging from 2.80–2.94 Å. In the second U4+ site, U4+ is bonded in a 8-coordinate geometry to eight Se2- atoms. There are four shorter (2.89 Å) and four longer (3.04 Å) U–Se bond lengths. Pd2+ is bonded in a rectangular see-saw-like geometry to four Se2- atoms. There are two shorter (2.50 Å) and two longer (2.51 Å) Pd–Se bond lengths. There are three inequivalent Se2- sites. In the first Se2- site, Se2- is bonded to one Rb1+, two U4+, and one Pd2+ atom to form distorted SeRbU2Pd trigonal pyramids that share corners with two equivalent SeRb2U4 octahedra, corners with six equivalent SeRbU2Pd trigonal pyramids, and an edgeedge with one SeRbU2Pd trigonal pyramid. The corner-sharing octahedra tilt angles range from 39–70°. In the second Se2- site, Se2- is bonded in a 5-coordinate geometry to one Rb1+, three U4+, and one Pd2+ atom. In the third Se2- site, Se2- is bonded to two equivalent Rb1+ and four equivalent U4+ atoms to form distorted corner-sharing SeRb2U4 octahedra.
DOI: 10.17188/1662153
title: Materials Data on Na2FeH4C5(N2O)3 by Materials Project

description: Na2FeC5H4(N2O)3 crystallizes in the orthorhombic Pnnm space group. The structure is two-dimensional and consists of two Na2FeC5H4(N2O)3 sheets oriented in the (0, 0, 1) direction. there are two inequivalent Na1+ sites. In the first Na1+ site, Na1+ is bonded in a water-like geometry to two equivalent O2- atoms. Both Na–O bond lengths are 2.34 Å. In the second Na1+ site, Na1+ is bonded in a 4-coordinate geometry to two equivalent N3- and two equivalent O2- atoms. Both Na–N bond lengths are 2.73 Å. Both Na–O bond lengths are 2.82 Å. Fe2+ is bonded in a single-bond geometry to one C+3.20+ and one N3- atom. The Fe–C bond length is 2.01 Å. The Fe–N bond length is 1.81 Å. There are three inequivalent C+3.20+ sites. In the first C+3.20+ site, C+3.20+ is bonded in a linear geometry to two N3- atoms. There is one shorter (1.19 Å) and one longer (1.31 Å) C–N bond length. In the second C+3.20+ site, C+3.20+ is bonded in a 2-coordinate geometry to one Fe2+ and one C+3.20+ atom. The C–C bond length is 1.25 Å. In the third C+3.20+ site, C+3.20+ is bonded in a distorted T-shaped geometry to two N3- and one O2- atom. There is one shorter (1.35 Å) and one longer (1.38 Å) C–N bond length. The C–O bond length is 1.43 Å. There are four inequivalent N3- sites. In the first N3- site, N3- is bonded in a 2-coordinate geometry to two equivalent C+3.20+ and one N3- atom. The N–N bond length is 1.31 Å. In the second N3- site, N3- is bonded in a bent 120 degrees geometry to one C+3.20+ and one H1+ atom. The N–H bond length is 1.60 Å. In the third N3- site, N3- is bonded in a distorted trigonal planar geometry to one Na1+ and two C+3.20+ atoms. In the fourth N3- site, N3- is bonded in a distorted bent 120 degrees geometry to one Fe2+ and one N3- atom. There are two inequivalent H1+ sites. In the first H1+ site, H1+ is bonded in a distorted linear geometry to one N3- and one O2- atom. The H–O bond length is 1.02 Å. In the second H1+ site, H1+ is bonded in a single-bond geometry to one O2- atom. The H–O bond length is 0.98 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted water-like geometry to two Na1+ and two H1+ atoms. In the second O2- site, O2- is bonded in an L-shaped geometry to two equivalent C+3.20+ atoms.
DOI: 10.17188/1662155
title: Materials Data on TiSiC7NCl3 by Materials Project

description: TiSiC7NCl3 is Hg_xSn structured and crystallizes in the monoclinic P2_1/c space group. The structure is zero-dimensional and consists of two TiSiC7NCl3 clusters. Ti4+ is bonded to one N3- and four Cl1- atoms to form distorted edge-sharing TiNCl4 trigonal bipyramids. The Ti–N bond length is 2.05 Å. There are a spread of Ti–Cl bond distances ranging from 2.18–2.59 Å. Si4+ is bonded in a 1-coordinate geometry to three C+0.29- and one N3- atom. There are two shorter (2.04 Å) and one longer (2.07 Å) Si–C bond lengths. The Si–N bond length is 1.95 Å. There are seven inequivalent C+0.29- sites. In the first C+0.29- site, C+0.29- is bonded in a 2-coordinate geometry to two C+0.29- atoms. Both C–C bond lengths are 1.44 Å. In the second C+0.29- site, C+0.29- is bonded in a 2-coordinate geometry to one Si4+ and one C+0.29- atom. The C–C bond length is 1.34 Å. In the third C+0.29- site, C+0.29- is bonded in a 3-coordinate geometry to one Si4+ and two C+0.29- atoms. The C–C bond length is 1.34 Å. In the fourth C+0.29- site, C+0.29- is bonded in a 2-coordinate geometry to one Si4+ and one C+0.29- atom. In the fifth C+0.29- site, C+0.29- is bonded in a distorted single-bond geometry to two C+0.29- and one N3- atom. Both C–C bond lengths are 1.44 Å. The C–N bond length is 1.27 Å. In the sixth C+0.29- site, C+0.29- is bonded in a 3-coordinate geometry to three C+0.29- atoms. The C–C bond length is 1.55 Å. In the seventh C+0.29- site, C+0.29- is bonded in a 3-coordinate geometry to three C+0.29- atoms. N3- is bonded in a trigonal planar geometry to one Ti4+, one Si4+, and one C+0.29- atom. There are three inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a single-bond geometry to one Ti4+ atom. In the second Cl1- site, Cl1- is bonded in a single-bond geometry to one Ti4+ atom. In the third Cl1- site, Cl1- is bonded in a water-like geometry to two equivalent Ti4+ atoms.
DOI: 10.17188/1662157
title: Materials Data on BaMnSnSe4 by Materials Project

description: BaMnSnSe4 crystallizes in the orthorhombic Fdd2 space group. The structure is three-dimensional. there are three inequivalent Ba2+ sites. In the first Ba2+ site, Ba2+ is bonded in a 8-coordinate geometry to eight Se2- atoms. There are six shorter (3.44 Å) and two longer (3.45 Å) Ba–Se bond lengths. In the second Ba2+ site, Ba2+ is bonded in a 8-coordinate geometry to eight Se2- atoms. There are six shorter (3.44 Å) and two longer (3.45 Å) Ba–Se bond lengths. In the third Ba2+ site, Ba2+ is bonded in a 8-coordinate geometry to eight Se2- atoms. There are a spread of Ba–Se bond distances ranging from 3.41–3.47 Å. There are two inequivalent Mn2+ sites. In the first Mn2+ site, Mn2+ is bonded to four Se2- atoms to form MnSe4 tetrahedra that share corners with two equivalent SnSe4 tetrahedra and an edgeedge with one SnSe4 tetrahedra. There are a spread of Mn–Se bond distances ranging from 2.53–2.59 Å. In the second Mn2+ site, Mn2+ is bonded to four Se2- atoms to form MnSe4 tetrahedra that share corners with two equivalent SnSe4 tetrahedra and an edgeedge with one SnSe4 tetrahedra. There are a spread of Mn–Se bond distances ranging from 2.52–2.59 Å. There are two inequivalent Sn4+ sites. In the first Sn4+ site, Sn4+ is bonded to four Se2- atoms to form SnSe4 tetrahedra that share corners with two equivalent MnSe4 tetrahedra and an edgeedge with one MnSe4 tetrahedra. There are a spread of Sn–Se bond distances ranging from 2.56–2.59 Å. In the second Sn4+ site, Sn4+ is bonded to four Se2- atoms to form SnSe4 tetrahedra that share corners with two equivalent MnSe4 tetrahedra and an edgeedge with one MnSe4 tetrahedra. There are a spread of Sn–Se bond distances ranging from 2.56–2.59 Å. There are eight inequivalent Se2- sites. In the first Se2- site, Se2- is bonded in a 4-coordinate geometry to two Ba2+, one Mn2+, and one Sn4+ atom. In the second Se2- site, Se2- is bonded in a 4-coordinate geometry to two Ba2+, one Mn2+, and one Sn4+ atom. In the third Se2- site, Se2- is bonded in a 4-coordinate geometry to two Ba2+, one Mn2+, and one Sn4+ atom. In the fourth Se2- site, Se2- is bonded in a 4-coordinate geometry to two Ba2+, one Mn2+, and one Sn4+ atom. In the fifth Se2- site, Se2- is bonded in a 4-coordinate geometry to two Ba2+, one Mn2+, and one Sn4+ atom. In the sixth Se2- site, Se2- is bonded in a 4-coordinate geometry to two Ba2+, one Mn2+, and one Sn4+ atom. In the seventh Se2- site, Se2- is bonded in a 4-coordinate geometry to two Ba2+, one Mn2+, and one Sn4+ atom. In the eighth Se2- site, Se2- is bonded in a 4-coordinate geometry to two Ba2+, one Mn2+, and one Sn4+ atom.
DOI: 10.17188/1662158
title: Materials Data on Li6V3P8O29 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1662159
title: Materials Data on CaLaAu2 by Materials Project

description: CaLaAu2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ca is bonded in a body-centered cubic geometry to eight equivalent Au atoms. All Ca–Au bond lengths are 3.22 Å. La is bonded in a body-centered cubic geometry to eight equivalent Au atoms. All La–Au bond lengths are 3.22 Å. Au is bonded in a body-centered cubic geometry to four equivalent Ca and four equivalent La atoms.
DOI: 10.17188/1662160
title: Materials Data on PuMg by Materials Project

description: MgPu is beta-prime cadmium gold structured and crystallizes in the orthorhombic Pmma space group. The structure is three-dimensional. Mg is bonded to four equivalent Mg and eight equivalent Pu atoms to form MgPu8Mg4 cuboctahedra that share corners with eight equivalent PuPu4Mg8 cuboctahedra, corners with ten equivalent MgPu8Mg4 cuboctahedra, edges with six equivalent MgPu8Mg4 cuboctahedra, edges with twelve equivalent PuPu4Mg8 cuboctahedra, faces with eight equivalent PuPu4Mg8 cuboctahedra, and faces with twelve equivalent MgPu8Mg4 cuboctahedra. There are two shorter (3.05 Å) and two longer (3.20 Å) Mg–Mg bond lengths. There are four shorter (3.39 Å) and four longer (3.43 Å) Mg–Pu bond lengths. Pu is bonded to eight equivalent Mg and four equivalent Pu atoms to form PuPu4Mg8 cuboctahedra that share corners with eight equivalent MgPu8Mg4 cuboctahedra, corners with ten equivalent PuPu4Mg8 cuboctahedra, edges with six equivalent PuPu4Mg8 cuboctahedra, edges with twelve equivalent MgPu8Mg4 cuboctahedra, faces with eight equivalent MgPu8Mg4 cuboctahedra, and faces with twelve equivalent PuPu4Mg8 cuboctahedra. There are two shorter (3.05 Å) and two longer (3.20 Å) Pu–Pu bond lengths.
DOI: 10.17188/1662162
title: Materials Data on Mn5Ni8Sn3 by Materials Project

description: Mn5Ni8Sn3 is Tungsten-derived structured and crystallizes in the trigonal R-3m space group. The structure is three-dimensional. there are four inequivalent Mn sites. In the first Mn site, Mn is bonded in a distorted body-centered cubic geometry to eight Ni and six Sn atoms. There are a spread of Mn–Ni bond distances ranging from 2.58–2.67 Å. There are three shorter (2.99 Å) and three longer (3.00 Å) Mn–Sn bond lengths. In the second Mn site, Mn is bonded in a distorted body-centered cubic geometry to eight Ni and three equivalent Sn atoms. There are a spread of Mn–Ni bond distances ranging from 2.44–2.64 Å. All Mn–Sn bond lengths are 3.00 Å. In the third Mn site, Mn is bonded in a body-centered cubic geometry to eight Ni atoms. There are two shorter (2.48 Å) and six longer (2.56 Å) Mn–Ni bond lengths. In the fourth Mn site, Mn is bonded in a distorted body-centered cubic geometry to eight Ni and six Sn atoms. There are a spread of Mn–Ni bond distances ranging from 2.58–2.67 Å. There are three shorter (2.99 Å) and three longer (3.00 Å) Mn–Sn bond lengths. There are five inequivalent Ni sites. In the first Ni site, Ni is bonded in a distorted body-centered cubic geometry to seven Mn and one Sn atom. There are a spread of Ni–Mn bond distances ranging from 2.44–2.59 Å. The Ni–Sn bond length is 2.63 Å. In the second Ni site, Ni is bonded in a distorted body-centered cubic geometry to four equivalent Mn and four Sn atoms. There are three shorter (2.58 Å) and one longer (2.63 Å) Ni–Sn bond lengths. In the third Ni site, Ni is bonded in a distorted body-centered cubic geometry to five Mn and three equivalent Sn atoms. All Ni–Sn bond lengths are 2.61 Å. In the fourth Ni site, Ni is bonded in a distorted body-centered cubic geometry to seven Mn and one Sn atom. The Ni–Sn bond length is 2.63 Å. In the fifth Ni site, Ni is bonded in a distorted body-centered cubic geometry to four Mn and four Sn atoms. All Ni–Sn bond lengths are 2.59 Å. There are two inequivalent Sn sites. In the first Sn site, Sn is bonded in a 8-coordinate geometry to six Mn and eight Ni atoms. In the second Sn site, Sn is bonded in a 8-coordinate geometry to six equivalent Mn and eight Ni atoms.
DOI: 10.17188/1662163
title: Materials Data on Cs3PrCl6 by Materials Project

description: Cs3PrCl6 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are three inequivalent Cs1+ sites. In the first Cs1+ site, Cs1+ is bonded in a 8-coordinate geometry to eight Cl1- atoms. There are a spread of Cs–Cl bond distances ranging from 3.36–4.08 Å. In the second Cs1+ site, Cs1+ is bonded in a 9-coordinate geometry to nine Cl1- atoms. There are a spread of Cs–Cl bond distances ranging from 3.56–4.13 Å. In the third Cs1+ site, Cs1+ is bonded in a 8-coordinate geometry to eight Cl1- atoms. There are a spread of Cs–Cl bond distances ranging from 3.47–3.94 Å. There are two inequivalent Pr3+ sites. In the first Pr3+ site, Pr3+ is bonded in an octahedral geometry to six Cl1- atoms. There are a spread of Pr–Cl bond distances ranging from 2.77–2.79 Å. In the second Pr3+ site, Pr3+ is bonded in an octahedral geometry to six Cl1- atoms. There are four shorter (2.75 Å) and two longer (2.79 Å) Pr–Cl bond lengths. There are six inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a 5-coordinate geometry to four Cs1+ and one Pr3+ atom. In the second Cl1- site, Cl1- is bonded in a 1-coordinate geometry to five Cs1+ and one Pr3+ atom. In the third Cl1- site, Cl1- is bonded in a 1-coordinate geometry to four Cs1+ and one Pr3+ atom. In the fourth Cl1- site, Cl1- is bonded in a 1-coordinate geometry to four Cs1+ and one Pr3+ atom. In the fifth Cl1- site, Cl1- is bonded in a 5-coordinate geometry to four Cs1+ and one Pr3+ atom. In the sixth Cl1- site, Cl1- is bonded in a 5-coordinate geometry to four Cs1+ and one Pr3+ atom.
DOI: 10.15468/qhv595
title: Neotype designation and redescription of Sicus indicus Kröber, 1940 (Diptera: Conopidae)

description: This dataset contains the digitized treatments in Plazi based on the original journal article Maqbool, Amir, Wachkoo, Aijaz Ahmad, Stuke, Jens-Hermann, Akbar, Shahid Ali, Clements, David K. (2021): Neotype designation and redescription of Sicus indicus Kröber, 1940 (Diptera: Conopidae). Zoosystema 43 (11): 197-203, DOI: 10.5252/zoosystema2021v43a11
DOI: 10.5281/zenodo.4727847
title: Atomic resolution HOLZ-STEM imaging of atom position modulation in oxide heterostructures

description: <strong>Dataset and python processing scripts for the journal article "Atomic resolution HOLZ-STEM imaging of atom position modulation in oxide heterostructures"</strong> DOI for the journal article: https://doi.org/10.1016/j.ultramic.2021.113296 There are two types of data in this deposit, experimental and simulated: The simulated is contained in the sim_data_deposit.zip file The experimental is in the "root" folder. This is in the form of the raw data files themselves, the python scripts and the intermediate files. <strong>The experimental data</strong> The raw, original, dataset is 011_big_film_512x512.emd. Which is a hdf5-file following the EMD (NCEM) standard. In addition, a reconverted version of this file, with a more optimized internal structure, which can be loaded directly in HyperSpy and pyXem is included (011_big_film_512x512_updated.hspy). The python processing files are intended to be run from the first, a000, to the last b010. In the order a000, a001, a002, .... b000, b001, ... The python library and version requirements are found in requirements.txt. The most important ones being HyperSpy and pixStem. Note that pixStem has been merged with the pyXem project, but the pixStem code will remain available for the foreseeable future. The <strong>011_big_film_512x512_updated.hspy</strong> is included for convenience, to make it easier to explore the data with more recent versions of HyperSpy and pyXem. In addition, it has a more optimized internal structure (via more optimized chunking). To view it, install HyperSpy and load the data: <pre><code class="language-python">import hyperspy.api as hs s = hs.load("011_big_film_512x512_updated.hspy") s.plot()</code></pre>
DOI: 10.5281/zenodo.4061715
title: Atomic resolution HOLZ-STEM imaging of atom position modulation in oxide heterostructures

description: <strong>Dataset and python processing scripts for the journal article "Atomic resolution HOLZ-STEM imaging of atom position modulation in oxide heterostructures"</strong> DOI for the journal article: https://doi.org/10.1016/j.ultramic.2021.113296 There are two types of data in this deposit, experimental and simulated: The simulated is contained in the sim_data_deposit.zip file The experimental is in the "root" folder. This is in the form of the raw data files themselves, the python scripts and the intermediate files. <strong>The experimental data</strong> The raw, original, dataset is 011_big_film_512x512.emd. Which is a hdf5-file following the EMD (NCEM) standard. In addition, a reconverted version of this file, with a more optimized internal structure, which can be loaded directly in HyperSpy and pyXem is included (011_big_film_512x512_updated.hspy). The python processing files are intended to be run from the first, a000, to the last b010. In the order a000, a001, a002, .... b000, b001, ... The python library and version requirements are found in requirements.txt. The most important ones being HyperSpy and pixStem. Note that pixStem has been merged with the pyXem project, but the pixStem code will remain available for the foreseeable future. The <strong>011_big_film_512x512_updated.hspy</strong> is included for convenience, to make it easier to explore the data with more recent versions of HyperSpy and pyXem. In addition, it has a more optimized internal structure (via more optimized chunking). To view it, install HyperSpy and load the data: <pre><code class="language-python">import hyperspy.api as hs s = hs.load("011_big_film_512x512_updated.hspy") s.plot()</code></pre>
DOI: 10.5281/zenodo.4733966
title: Assessing the Impact of Code Samples Evolution on Developers' Doubts

description: Scripts to run all features from the article and the results of each step.
DOI: 10.5281/zenodo.4728233
title: Assessing the Impact of Code Samples Evolution on Developers' Doubts

description: Scripts to run all features from the article and the results of each step.
DOI: 10.3886/e130562v1-85580
title: biological living standards of Korea during the port-opening period, 1876-1910

description: Hangryu Deceased data
DOI: 10.5281/zenodo.4733220
title: Andricus quercuslanigera SPAdes preassembly

description: Andricus quercuslanigera SPAdes preassembly
DOI: 10.5281/zenodo.4733219
title: Andricus quercuslanigera SPAdes preassembly

description: Andricus quercuslanigera SPAdes preassembly
DOI: 10.5517/ccdc.csd.cc1px7b5
title: CCDC 1576267: Experimental Crystal Structure Determination

description: Related Article: David Miklík, S. Fatemeh Mousavi, Zuzana Burešová, Anna Middleton, Yoshitaka Matsushita, Jan Labuta, Aisha Ahsan, Luiza Buimaga-Iarinca, Paul A. Karr, Filip Bureš, Gary J. Richards, Pavel Švec, Toshiyuki Mori, Katsuhiko Ariga, Yutaka Wakayama, Cristian Morari, Francis D’Souza, Thomas A. Jung, Jonathan P. Hill|2021|Communications Chemistry|4|29|doi:10.1038/s42004-021-00470-w
DOI: 10.5517/ccdc.csd.cc27mml3
title: CCDC 2074445: Experimental Crystal Structure Determination

description: Related Article: Brian W. Skelton, Keith A. Stubbs, Siobhan Wills|2021|CSD Communication|||
DOI: 10.5517/ccdc.csd.cc27n558
title: CCDC 2074959: Experimental Crystal Structure Determination

description: Related Article: Brian W. Skelton, Allan H. White, Eric J. Chan, Alexandre N. Sobolev|2021|CSD Communication|||
DOI: 10.5517/ccdc.csd.cc27pfyb
title: CCDC 2076192: Experimental Crystal Structure Determination

description: Related Article: Brian W. Skelton, Effendy, Allan H. White|2021|CSD Communication|||
DOI: 10.5517/ccdc.csd.cc27pt2v
title: CCDC 2076537: Experimental Crystal Structure Determination

description: Related Article: Arnold L. Rheingold|2021|CSD Communication|||
DOI: 10.5517/ccdc.csd.cc27pwxr
title: CCDC 2076625: Experimental Crystal Structure Determination

description: Related Article: W. Clegg, G.S. Nichol|2021|CSD Communication|||
DOI: 10.5281/zenodo.4734036
title: Performant implementation of the atomic cluster expansion (PACE): Application tocopper and silicon

description: This collection contains files associated with npj Comp.Mat. "Performant implementation of the atomic cluster expansion (PACE): Application tocopper and silicon" (2021) paper: - ACE potentials for copper - Copper DFT-PBE dataset computed with FHI-aims and that was used for fitting Atomic Cluster Expansion potential for copper. - Jupyter notebook for Copper dataset overview - ACE potentials for silicon
DOI: 10.5281/zenodo.4734035
title: Performant implementation of the atomic cluster expansion (PACE): Application tocopper and silicon

description: This collection contains files associated with npj Comp.Mat. "Performant implementation of the atomic cluster expansion (PACE): Application tocopper and silicon" (2021) paper: - ACE potentials for copper - Copper DFT-PBE dataset computed with FHI-aims and that was used for fitting Atomic Cluster Expansion potential for copper. - Jupyter notebook for Copper dataset overview - ACE potentials for silicon
DOI: 10.6084/m9.figshare.12129540.v1
title: The benefits and risks of beetroot juice consumption: a systematic review

description: Beetroot juice (BRJ) has become increasingly popular amongst athletes aiming to improve sport performances. BRJ contains high concentrations of nitrate, which can be converted into nitric oxide (NO) after consumption. NO has various functions in the human body, including a vasodilatory effect, which reduces blood pressure and increases oxygen- and nutrient delivery to various organs. These effects indicate that BRJ may have relevant applications in prevention and treatment of cardiovascular disease. Furthermore, the consumption of BRJ also has an impact on oxygen delivery to skeletal muscles, muscle efficiency, tolerance and endurance and may thus have a positive impact on sports performances. Aside from the beneficial aspects of BRJ consumption, there may also be potential health risks. Drinking BRJ may easily increase nitrate intake above the acceptable daily intake, which is known to stimulate the endogenous formation of <i>N-</i>nitroso compounds (NOC’s), a class of compounds that is known to be carcinogenic and that may also induce several other adverse effects. Compared to studies on the beneficial effects, the amount of data and literature on the negative effects of BRJ is rather limited, and should be increased in order to perform a balanced risk assessment.