cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.6084/m9.figshare.18270866.v1
title: Datasets to "Geography, climate and shifts in host plants distribution explain the genomic variation in the cactus moth"

description: The ten zipped folders contains input and output data used in this study, they are: 01) zip folder contains three datasets: A) a variant call file obtained after IPYRAD assembly B) a variant call file obtained after filtering steps and C) a genepop file used for genetic diversity estimation. 02) This dataset consist in 8 folders each one with inputs files and the SFS to demographic estimation using Fastsimcoal. 03) The folder contains occurrence points (latitude and longitude) of the cactus moth C. cactorum and five of its host plant species, Opuntia megapotamica, O. anacantha, O. quimilo, O. elata and O. rioplatense. 03a) The folder contains the raster files obtained with ecological niche modelling (ENM) of the cactus moth C. cactorum for present time (current) and Last Glacial Maximum (LGM) under the CCSM4 general atmospheric circulation model. 03b) The folder contains the raster files obtained with ecological niche modelling (ENM) of five host plants of the moth C. cactorum for present time (current) and Last Glacial Maximum (LGM) under the CCSM4 general atmospheric circulation model. 04) The dataset contains the pairwise genetic distance matrices of C. cactorum sampling sites based on nuclear (ddRAD) and mitochondrial (mtDNA) genetic data. 05a) This file contains a distance matrix using weighted topographic distances (WTopDis) of 28 sampling sites used in isolation by distance (IBD) analysis. 05b) This file contains a distance matrix using 15 bioclimatic variables of CHELSA (EnvDis) for 28 sampling sites used in isolation by environmental (IBE) analysis. 05c) The zip folder contains six isolation by resistance escenarios derived from current and LGM projections of ENMs as well as a Null model of flat landscape. Each scenario includes the input files to Circuitscape analysis. 06) The folder contains three climatic/habitat stability models resulting from ENMs for current and LGM projections.<br>
DOI: 10.21338/eosc-future-sp9
title: EOSC Future Science Project 'Climate Neutral and Smart Cities'
DOI: 10.34740/kaggle/dsv/6420466
title: posts and comments by kaggle in the questionanswer
DOI: 10.5519/qd.ocoonqh4
title: Query on the Natural History Museum Data Portal (data.nhm.ac.uk) (42 records)
DOI: 10.6084/m9.figshare.24085281
title: Do file replication material revision SP&A

description: Replication file <b>Welfare state regimes and social policy resistance to </b><b>fiscal consolidations</b>
DOI: 10.34770/wzgz-x526
title: CKavity Library: Next-Generation Sequencing
title: A library of novel genes with combinatorially diverse cavities, built on a stably folded structural template

description: Protein sequence space is vast; nature uses only an infinitesimal fraction of possible sequences to sustain life. Are there solutions to biological problems other than those provided by nature? Can we create artificial proteins that sustain life? To investigate this question, the Hecht lab has created combinatorial collections, or libraries, of novel sequences with no homology to those found in living organisms. These libraries were subjected to screens and selections, leading to the identification of sequences with roles in catalysis, modulating gene regulation, and metal homeostasis. However, the resulting functional proteins formed dynamic rather than well-ordered structures. This impeded structural characterization and made it difficult to ascertain a mechanism of action. To address this, Christina Karas's thesis work focuses on developing a new model of libraries based on the de novo protein S-824, a four-helix bundle with a very stable three-dimensional structure. The first part of this research focused on mutagenesis of S-824 and characterization of the resulting proteins, revealing that this scaffold tolerates amino acid substitutions, including buried polar residues and the removal of hydrophobic side chains to create a putative cavity. Distinct from previous libraries, Karas targeted variability to a specific region of the protein, seeking to create a cavity and potential active site. The second part of this work details the design and creation of a library encoding 1.7 x 10^6 unique proteins, assembled from degenerate oligonucleotides. The third and fourth parts of this work cover the screening effort for a range of activities, both in vitro and in vivo. I found that this collection binds heme readily, leading to abundant peroxidase activity. Hits for lipase and phosphatase activity were also detected. This work details the development of a new strategy for creating de novo sequences geared toward function rather than structure.
DOI: 10.25346/s6/6vhdxs/svqwv2
title: plot_PSD_Q1=1.5_Q2=1.0472_interp.mat
DOI: 10.25346/s6/6vhdxs/f7fvdk
title: plot_PSD_Q1=2.5_Q2=1.3090_interp.mat
DOI: 10.25346/s6/6vhdxs/0cigjr
title: plot_PSD_Q1=0.3_Q2=0.7854_interp.mat
DOI: 10.25346/s6/6vhdxs/febmsv
title: plot_PSD_Q1=2.3_Q2=1.3090_interp.mat
DOI: 10.25346/s6/6vhdxs/knfce2
title: plot_PSD_Q1=0.7_Q2=1.0472_interp.mat
DOI: 10.25346/s6/6vhdxs/rkzrzk
title: plot_PSD_Q1=3.3_Q2=0.7854_interp.mat
DOI: 10.25346/s6/6vhdxs/1juiw0
title: plot_PSD_Q1=2.5_Q2=1.4835_interp.mat
DOI: 10.25346/s6/6vhdxs/qxa92v
title: plot_PSD_Q1=2.0_Q2=0.2618_interp.mat
DOI: 10.25346/s6/6vhdxs/ekeu89
title: plot_PSD_Q1=2.5_Q2=0.7854_interp.mat
DOI: 10.25346/s6/6vhdxs/jt5awe
title: plot_PSD_Q1=0.8_Q2=0.2618_interp.mat
DOI: 10.25346/s6/6vhdxs/wotq18
title: plot_PSD_Q1=3.0_Q2=1.0472_interp.mat
DOI: 10.25346/s6/6vhdxs/xkbvjt
title: plot_PSD_Q1=3.5_Q2=0.2618_interp.mat
DOI: 10.25346/s6/6vhdxs/jzxxjc
title: plot_PSD_Q1=4.2_Q2=1.4835_interp.mat
DOI: 10.25346/s6/6vhdxs/arh2lk
title: plot_PSD_Q1=2.5_Q2=0.5236_interp.mat
DOI: 10.25346/s6/6vhdxs/yshqru
title: plot_PSD_Q1=1.7_Q2=0.2618_interp.mat
DOI: 10.25346/s6/6vhdxs/mvpvcn
title: plot_PSD_Q1=1.75_Q2=1.0472_interp.mat
DOI: 10.25346/s6/6vhdxs/dibr3t
title: plot_PSD_Q1=2.7_Q2=0.5236_interp.mat
DOI: 10.25346/s6/6vhdxs/kfhn7k
title: plot_PSD_Q1=2.0_Q2=1.0472_interp.mat
DOI: 10.25346/s6/6vhdxs/x7ugw6
title: plot_PSD_Q1=3.3_Q2=1.3090_interp.mat
DOI: 10.25346/s6/6vhdxs/71uljf
title: plot_PSD_Q1=4.2_Q2=0.2618_interp.mat
DOI: 10.25346/s6/6vhdxs/4iwmdw
title: plot_PSD_Q1=1.0_Q2=0.5236_interp.mat
DOI: 10.25346/s6/6vhdxs/w8nykd
title: plot_PSD_Q1=0.9_Q2=0.5236_interp.mat
DOI: 10.25346/s6/6vhdxs/ijym8q
title: plot_PSD_Q1=1.5_Q2=1.3090_interp.mat
DOI: 10.25346/s6/6vhdxs/uxd9vd
title: plot_PSD_Q1=1.3_Q2=0.2618_interp.mat
DOI: 10.25346/s6/6vhdxs
title: PSD_Malaspina_et_al+Low_frequency_hiss_Simulation

description: This folder contains the saved PSD files for the combination Malaspina et al. and low frequency hiss model for that respective energy and pitch angle. Energies range from 0.3 - 4.2 MeV, with pitch angles of: 15, 30, 45, 60, and 75 degrees. The files are saved as matlab files. The file naming convention is: "plot_PSD_Q1=(INSERT ENERGY IN MEV)_Q2=(INSERT PITCH ANGLE IN RADIANS)_interp.mat"
DOI: 10.25346/s6/6vhdxs/beuniv
title: plot_PSD_Q1=0.7_Q2=0.5236_interp.mat
DOI: 10.25346/s6/j5hqns/cnytvo
title: Log_Diff_E=2.0_75PA.fig
DOI: 10.25346/s6/j5hqns/wpk842
title: Comparison_Norm_Hiss_E=0.9_75PA.fig
DOI: 10.25346/s6/j5hqns/u6rh62
title: Log_Diff_E=2.8_30PA.fig
DOI: 10.25346/s6/j5hqns/yjmes0
title: Comparison_Norm_Hiss_E=1.5_60PA.fig
DOI: 10.25346/s6/j5hqns/kocjry
title: Log_Diff_E=5.0_75PA.fig
DOI: 10.25346/s6/j5hqns/rsybai
title: Log_Diff_E=0.3_75PA.fig
DOI: 10.25346/s6/j5hqns/haqwrr
title: Log_Diff_E=1.0_60PA.fig
DOI: 10.25346/s6/j5hqns/t85mj7
title: Log_Diff_E=3.9_30PA.fig
DOI: 10.25346/s6/j5hqns/xeilsy
title: Log_Diff_E=3.5_30PA.fig
DOI: 10.25346/s6/j5hqns/foktyg
title: Comparison_Norm_Hiss_E=0.8_75PA.fig
DOI: 10.25346/s6/j5hqns/jfepls
title: Comparison_Norm_Hiss_E=3.1_30PA.fig
DOI: 10.25346/s6/j5hqns/jrzxnv
title: Comparison_Norm_Hiss_E=4.4_75PA.fig
DOI: 10.25346/s6/j5hqns/f325vz
title: Comparison_Norm_Hiss_E=2.8_75PA.fig
DOI: 10.25346/s6/j5hqns/n00kol
title: Log_Diff_E=1.5_30PA.fig
DOI: 10.25346/s6/j5hqns/ttddub
title: Comparison_Norm_Hiss_E=2.8_30PA.fig
DOI: 10.25346/s6/j5hqns/zmgxf0
title: Log_Diff_E=4.4_30PA.fig
DOI: 10.25346/s6/j5hqns/op8yco
title: Comparison_Norm_Hiss_E=3.1_60PA.fig
DOI: 10.25346/s6/j5hqns/s8t0rv
title: Comparison_Norm_Hiss_E=5.0_60PA.fig
DOI: 10.25346/s6/j5hqns/vl4z7y
title: Log_Diff_E=5.0_60PA.fig
DOI: 10.25346/s6/j5hqns/nh58my
title: Comparison_Norm_Hiss_E=0.7_60PA.fig
DOI: 10.25346/s6/j5hqns/br2iot
title: Comparison_Norm_Hiss_E=2.2_30PA.fig
DOI: 10.25346/s6/j5hqns/jdjxfv
title: Comparison_Norm_Hiss_E=1.7_30PA.fig
DOI: 10.25346/s6/j5hqns/frc9ot
title: Log_Diff_E=1.3_30PA.fig
DOI: 10.25346/s6/j5hqns/rnvxnz
title: Log_Diff_E=0.8_75PA.fig
DOI: 10.25346/s6/j5hqns/7eypxr
title: Comparison_Norm_Hiss_E=1.7_60PA.fig
DOI: 10.25346/s6/j5hqns/5dfdw4
title: Log_Diff_E=0.8_60PA.fig
DOI: 10.25346/s6/j5hqns/ooci51
title: Log_Diff_E=1.5_60PA.fig
DOI: 10.25346/s6/j5hqns/w4b9oz
title: Comparison_Norm_Hiss_E=0.7_75PA.fig
DOI: 10.25346/s6/j5hqns/cvt5vd
title: Log_Diff_E=2.5_75PA.fig
DOI: 10.25346/s6/j5hqns/k2fsff
title: Log_Diff_E=0.7_75PA.fig
DOI: 10.25346/s6/j5hqns/1qoos2
title: Log_Diff_E=2.2_60PA.fig
DOI: 10.25346/s6/j5hqns/fx9ooc
title: Log_Diff_E=1.3_60PA.fig
DOI: 10.25346/s6/j5hqns/r9y6xq
title: Log_Diff_E=2.8_60PA.fig
DOI: 10.25346/s6/j5hqns/jrfszw
title: Comparison_Norm_Hiss_E=2.8_60PA.fig
DOI: 10.25346/s6/j5hqns/j7wlmc
title: Comparison_Norm_Hiss_E=2.5_60PA.fig
DOI: 10.25346/s6/j5hqns/k5uwkz
title: Comparison_Norm_Hiss_E=1.5_75PA.fig
DOI: 10.25346/s6/j5hqns/jkcmkg
title: Log_Diff_E=1.5_75PA.fig
DOI: 10.25346/s6/j5hqns/nki87s
title: Log_Diff_E=0.5_75PA.fig
DOI: 10.25346/s6/j5hqns/nomqe9
title: Log_Diff_E=0.9_75PA.fig
DOI: 10.25346/s6/j5hqns/2p1myl
title: Log_Diff_E=1.0_30PA.fig
DOI: 10.25346/s6/j5hqns/ag37iy
title: Comparison_Norm_Hiss_E=5.0_75PA.fig
DOI: 10.25346/s6/j5hqns/ndrizz
title: Comparison_Norm_Hiss_E=0.9_60PA.fig
DOI: 10.25346/s6/j5hqns/gsgblp
title: Log_Diff_E=3.5_60PA.fig
DOI: 10.25346/s6/j5hqns/bqc8lw
title: Log_Diff_E=0.7_30PA.fig
DOI: 10.25346/s6/j5hqns/gmbvpw
title: Log_Diff_E=0.9_60PA.fig
DOI: 10.25346/s6/j5hqns/zxzh6j
title: Comparison_Norm_Hiss_E=1.7_75PA.fig
DOI: 10.25346/s6/j5hqns/gcmcid
title: Comparison_Norm_Hiss_E=0.5_75PA.fig
DOI: 10.25346/s6/j5hqns/pclkbf
title: Log_Diff_E=2.0_30PA.fig
DOI: 10.25346/s6/j5hqns/txuris
title: Comparison_Norm_Hiss_E=0.3_75PA.fig
DOI: 10.25346/s6/j5hqns/ag90km
title: Log_Diff_E=3.9_75PA.fig
DOI: 10.25346/s6/j5hqns/efmxjw
title: Log_Diff_E=2.8_75PA.fig
DOI: 10.25346/s6/j5hqns/qzms2d
title: Log_Diff_E=0.8_30PA.fig
DOI: 10.25346/s6/j5hqns/ygnf9a
title: Log_Diff_E=0.7_60PA.fig
DOI: 10.25346/s6/j5hqns/oh69ny
title: Comparison_Norm_Hiss_E=2.2_75PA.fig
DOI: 10.25346/s6/j5hqns/rytdtr
title: Comparison_Norm_Hiss_E=1.3_75PA.fig
DOI: 10.25346/s6/j5hqns/5zrsqp
title: Log_Diff_E=1.7_60PA.fig
DOI: 10.25346/s6/j5hqns/y6t1lm
title: Comparison_Norm_Hiss_E=3.9_30PA.fig
DOI: 10.25346/s6/j5hqns/ehiydg
title: Comparison_Norm_Hiss_E=1.0_60PA.fig
DOI: 10.25346/s6/j5hqns/k4zy85
title: Log_Diff_E=5.0_30PA.fig
DOI: 10.25346/s6/j5hqns/yzldpc
title: Log_Diff_E=3.5_75PA.fig
DOI: 10.25346/s6/j5hqns/eg0til
title: Comparison_Norm_Hiss_E=2.5_75PA.fig
DOI: 10.25346/s6/j5hqns/eybohf
title: Comparison_Norm_Hiss_E=2.2_60PA.fig
DOI: 10.25346/s6/j5hqns/fbrqzr
title: Log_Diff_E=2.5_30PA.fig
DOI: 10.25346/s6/j5hqns/8xvyjy
title: Comparison_Norm_Hiss_E=0.3_30PA.fig
DOI: 10.25346/s6/j5hqns/fxb0np
title: Comparison_Norm_Hiss_E=3.9_75PA.fig
DOI: 10.25346/s6/j5hqns/nu3qj2
title: Log_Diff_E=0.5_60PA.fig
DOI: 10.25346/s6/j5hqns/qs6wpu
title: Log_Diff_E=1.7_30PA.fig
DOI: 10.25346/s6/j5hqns/42tqol
title: Comparison_Norm_Hiss_E=3.5_60PA.fig
DOI: 10.25346/s6/j5hqns/esqc84
title: Comparison_Norm_Hiss_E=3.1_75PA.fig
DOI: 10.25346/s6/j5hqns/gu2cwn
title: Log_Diff_E=2.5_60PA.fig
DOI: 10.25346/s6/j5hqns/jibgr9
title: Comparison_Norm_Hiss_E=2.5_30PA.fig
DOI: 10.25346/s6/j5hqns/zfb6tg
title: Comparison_Norm_Hiss_E=0.8_60PA.fig
DOI: 10.25346/s6/j5hqns/hagmb2
title: Comparison_Norm_Hiss_E=0.8_30PA.fig
DOI: 10.25346/s6/j5hqns/igdlc5
title: Comparison_Norm_Hiss_E=2.0_75PA.fig
DOI: 10.25346/s6/j5hqns/ms2mrz
title: Comparison_Norm_Hiss_E=0.9_30PA.fig
DOI: 10.25346/s6/j5hqns/ibytdf
title: Log_Diff_E=1.7_75PA.fig
DOI: 10.25346/s6/j5hqns/3bxnad
title: Log_Diff_E=1.3_75PA.fig
DOI: 10.25346/s6/j5hqns/sdgbr8
title: Comparison_Norm_Hiss_E=1.5_30PA.fig
DOI: 10.25346/s6/j5hqns/icarw7
title: Log_Diff_E=1.0_75PA.fig
DOI: 10.25346/s6/j5hqns/ty1ikm
title: Log_Diff_E=2.2_30PA.fig
DOI: 10.25346/s6/j5hqns/0uvlfk
title: Log_Diff_E=3.1_30PA.fig
DOI: 10.25346/s6/j5hqns/3tcscf
title: Comparison_Norm_Hiss_E=1.3_30PA.fig
DOI: 10.25346/s6/j5hqns/vcdw4i
title: Comparison_Norm_Hiss_E=1.3_60PA.fig
DOI: 10.25346/s6/j5hqns/gxeqf8
title: Comparison_Norm_Hiss_E=0.7_30PA.fig
DOI: 10.25346/s6/j5hqns/goebak
title: Log_Diff_E=3.9_60PA.fig
DOI: 10.25346/s6/j5hqns/nbna9n
title: Comparison_Norm_Hiss_E=3.5_75PA.fig
DOI: 10.25346/s6/j5hqns/8mwz24
title: Log_Diff_E=2.2_75PA.fig
DOI: 10.25346/s6/j5hqns/y5unj1
title: Log_Diff_E=2.0_60PA.fig
DOI: 10.25346/s6/j5hqns/hd0ytt
title: Comparison_Norm_Hiss_E=0.5_60PA.fig
DOI: 10.25346/s6/j5hqns/rh9ytn
title: Log_Diff_E=3.1_75PA.fig
DOI: 10.25346/s6/j5hqns/kuddj1
title: Comparison_Norm_Hiss_E=3.5_30PA.fig
DOI: 10.25346/s6/j5hqns/wpq2mn
title: Log_Diff_E=0.5_30PA.fig
DOI: 10.25346/s6/j5hqns/0aa8xa
title: Comparison_Norm_Hiss_E=1.0_30PA.fig
DOI: 10.25346/s6/j5hqns/8ecs6o
title: Log_Diff_E=0.3_60PA.fig
DOI: 10.25346/s6/j5hqns/zkhhux
title: Comparison_Norm_Hiss_E=4.4_30PA.fig
DOI: 10.25346/s6/j5hqns/2fjejf
title: Comparison_Norm_Hiss_E=5.0_30PA.fig
DOI: 10.25346/s6/j5hqns/urgovg
title: Log_Diff_E=3.1_60PA.fig
DOI: 10.25346/s6/j5hqns/up41yn
title: Log_Diff_E=4.4_60PA.fig
DOI: 10.25346/s6/j5hqns/vi4ceh
title: Log_Diff_E=4.4_75PA.fig
DOI: 10.25346/s6/j5hqns/xll8wq
title: Comparison_Norm_Hiss_E=1.0_75PA.fig
DOI: 10.25346/s6/j5hqns/ahego0
title: Comparison_Norm_Hiss_E=0.3_60PA.fig
DOI: 10.25346/s6/j5hqns/zufb2k
title: Log_Diff_E=0.9_30PA.fig
DOI: 10.25346/s6/j5hqns/lh05yb
title: Log_Diff_E=0.3_30PA.fig
DOI: 10.25346/s6/j5hqns/btscaz
title: Comparison_Norm_Hiss_E=0.5_30PA.fig
DOI: 10.25346/s6/j5hqns/chgau5
title: Comparison_Norm_Hiss_E=2.0_60PA.fig
DOI: 10.25346/s6/j5hqns/z6ybq2
title: Comparison_Norm_Hiss_E=2.0_30PA.fig
DOI: 10.25346/s6/j5hqns/bixolp
title: Comparison_Norm_Hiss_E=3.9_60PA.fig
DOI: 10.25346/s6/j5hqns/rgyfnp
title: Comparison_Norm_Hiss_E=4.4_60PA.fig
DOI: 10.25346/s6/j5hqns
title: Figures_made_from_simulations_Flux_Norm_Log_Difference

description: These are the VERB simulation result .fig (Matlab) files for: -Comparison_Hiss (the plotted flux for each simulation at that respective energy and pitch angle), -Log_Difference (the difference between the simulation and the Van Allen Probe-A observations). -Normalized Difference (the normalized between the simulation and the Van Allen Probe-A observations). The file name is organized such as: "Figure_(INSERT ENERGY)_meV_(INSERT PITCH ANGLE)_PA.fig"
DOI: 10.6084/m9.figshare.17232491
title: The global map of tree species richness

description: <strong>Estimated tree species richness per hectare. </strong> This map can be downloaded in two formats. One is a geoTIFF file (S_mean_raster.tif) containing the fully geo-referenced map of tree species richness worldwide at a 0.025°×0.025° resolution. The other is a comma-separated file (S_mean_grid.csv) with the following attributes: <em>S</em> is local average tree species richness per hectare <em>x, y</em> are centroid coordinates of all 0.025°×0.025° pixels;
DOI: 10.5281/zenodo.6505273
title: Data Release: "No evidence that the majority of black holes in binaries have zero spin"

description: This dataset contains the results presented in "<em>No evidence that the majority of black holes in binaries have zero spin</em>". In this paper, we systematically explored the effective and component spin distributions of binary black holes among the LIGO/Virgo GWTC-3 catalog. In particular, we tried to answer the following core questions, which have been the subject of active exploration and some debate in the literature: <em>1. Is there an excess of binary black holes with vanishing spin, as predicted by some theories of angular momentum transport in stellar cores?</em> <strong>We find no evidence for an excess of vanishing spin systems.</strong> This finding is confirmed by three complementary analyses: one relying only on the Bayes factors between spinning and non-spinning priors for each BBH observation, one that seeks to model the distribution of effective aligned spins, and one modeling the distribution of component spin magnitudes and misalignment angles. Instead, we find BBH spin magnitudes to be consistent with a single, continuous distribution that remains finite at magnitude zero. <em>2. Do there exist binaries with component spins misaligned by more than 90 degrees relative to their orbits?</em> <strong>We find a strong preference for the existence of such strongly misaligned spins.</strong> Our analysis of the BBH component spin distribution indicates that at least some component spins are misaligned from their orbits by more than 90 degrees. This result is robust under a variety of modeling choices regarding both the distribution of component spin magnitudes and tilts. The code used to generate this data can be found in the repository https://github.com/tcallister/gwtc3-spin-studies/. This repository includes jupyter notebooks that can be used to open, explore, and plot the files contained in this data set. Additional information about reproducing and/or using this dataset can be found in our associated documentation.
DOI: 10.13011/m3-9qka-t722
title: Mohammadreza Yaghoobi
DOI: 10.6084/m9.figshare.16646020.v7
title: Network: czo, Domain: boulder

description: MacroSheds timeseries data, shapefiles, and metadata for domain: boulder, within network: czo
DOI: 10.6084/m9.figshare.16646020.v6
title: Network: czo, Domain: boulder

description: MacroSheds timeseries data, shapefiles, and metadata for domain: boulder, within network: czo
DOI: 10.6084/m9.figshare.16646095.v5
title: Network: czo, Domain: calhoun

description: MacroSheds timeseries data, shapefiles, and metadata for domain: calhoun, within network: czo
DOI: 10.6084/m9.figshare.16646095.v4
title: Network: czo, Domain: calhoun

description: MacroSheds timeseries data, shapefiles, and metadata for domain: calhoun, within network: czo
DOI: 10.6084/m9.figshare.16646179.v3
title: Network: czo, Domain: catalina_jemez

description: MacroSheds timeseries data, shapefiles, and metadata for domain: catalina_jemez, within network: czo
DOI: 10.6084/m9.figshare.16648402.v3
title: Network: czo, Domain: shale_hills

description: MacroSheds timeseries data, shapefiles, and metadata for domain: shale_hills, within network: czo
DOI: 10.5517/ccdc.csd.cc29xjlc
title: CCDC 2142583: Experimental Crystal Structure Determination

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DOI: 10.5517/ccdc.csd.cc29xjmd
title: CCDC 2142584: Experimental Crystal Structure Determination

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DOI: 10.5517/ccdc.csd.cc29xjnf
title: CCDC 2142585: Experimental Crystal Structure Determination

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DOI: 10.5517/ccdc.csd.cc29xjpg
title: CCDC 2142586: Experimental Crystal Structure Determination

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DOI: 10.5517/ccdc.csd.cc29xjqh
title: CCDC 2142587: Experimental Crystal Structure Determination

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DOI: 10.5517/ccdc.csd.cc29zj83
title: CCDC 2144495: Experimental Crystal Structure Determination

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title: CCDC 2144615: Experimental Crystal Structure Determination

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title: Network: doe, Domain: east_river

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DOI: 10.6084/m9.figshare.16649734.v3
title: Network: walker_branch, Domain: walker_branch

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title: Raw data of article "Substantial organic impurities at the surface of synthetic ammonium sulfate particles"

description: Raw data of article "Substantial organic impurities at the surface of synthetic ammonium sulfate particles"
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title: Network: krycklan, Domain: krycklan

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title: Network: lter, Domain: arctic

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title: Network: lter, Domain: bonanza

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title: Query on the Natural History Museum Data Portal (data.nhm.ac.uk) (175 records)