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Dataset for published paper: Mode Conversion Trimming in Asymmetric Directional Couplers Enabled by Silicon Ion Implantation
<p>This dataset contains the measurement results described in the paper 'Mode Conversion Trimming in Asymmetric Directional Couplers Enabled by Silicon Ion Implantation'.</p>
Supporting data for increasing fire activity reinforces shrub conversion in Southwestern US forests
<p>Fire-exclusion in historically frequent-fire forests of the southwestern United States has altered forest structure and increased the probability of high-severity fire. Warmer and drier conditions, coupled with dispersal distance limitations are limiting tree seedling establishment and survival following high-severity fire. Post-fire conversion to non-forest vegetation can be reinforced by subsequent fire events. We sought to determine the influence of fire probability on post-fire vegetation development in a severely burned landscape in New Mexico, USA. We used LANDIS-II to simulate three fire probability scenarios—contemporary mean fire return interval (CMFRI), and 1.5 times and 2 times CMFRI—with contemporary climate. As fire probability increased, the mean size of the largest fires and the mean landscape fire severity increased. These changes in fire characteristics resulted in a net decrease in total above ground biomass and photosynthetic capacity on the landscape. Additionally, the distribution of individual species biomass shifted, with early successional species, especially those that resprout after fire, increasing as a fraction of total biomass with increasing fire occurrence. Continued increases in fire frequency are likely to favor resprouting species and result in a loss of forest biomass and ecosystem productivity in this southwestern forest landscape.</p>
On energy transfer of parametric resonance for wave energy conversion
<p>Parametric resonance has been observed, both numerically and experimentally, in various studies of wave energy converters (WECs). A large motion in heave induces a periodic variation in the metacentric height of a WEC body, and, consequently, causes a harmonic variation in pitch/roll restoring coefficients, which can parametrically excite the pitch/roll modes. Current studies have a specific focus to determine the occurrence conditions of parametric resonance, by detecting the boundaries between stable and unstable regions in the parameter space. In the literature, some studies aim to make use of parametric resonance for improving power capture. In contrast, some studies try to suppress the effect of parametric resonance, as it reduces power capture efficiency. However, how energy transfers from one mode to another is not fully understood. This study aims to analyse the energy transfer between heave and pitch/roll modes when parametric resonance occurs. A generic cylindrical point absorber is studied as a WEC floater to considering non-linear wave-structure interaction, including non-linear Froude-Krylov and viscous forces. A heave-pitch-roll three-degree-of-freedom model is derived for numerical study of the energy transfer between different operation modes.</p>
Thermally conductive honeycombs for chemical reactors with enhanced chemical conversion behavior
<p><strong>Thermally conductive honeycombs for chemical reactors with enhanced chemical conversion behavior</strong></p> <p>Junjie Chen</p> <p>Department of Energy and Power Engineering, School of Mechanical and Power Engineering, Henan Polytechnic University, 2000 Century Avenue, Jiaozuo, Henan, 454000, P.R. China</p> <p>Contributor: Junjie Chen, ORCID: 0000-0001-5055-4309, E-mail address: komcjj@gmail.com</p> <p> </p> <p>It has been taught a method to produce a thermally conductive honeycombs for chemical reactors. It has been taught a technique to produce an extruded metal monolith and highlights how copper or copper alloys are particularly suitable for this application. It has been taught how catalysts may be attached to walls to produce an active catalyst matrix. It is claimed that thermally conductive monoliths reduce the likelihood of hot spot formation, as any hotter area conducts the energy via conduction through the monolith body to an area which is less hot. However, the method does not teach of the possibility of having different chemical reactions simultaneously occurring on opposing sides of the monolith substrate. Therefore, it is necessary to provide an improved chemical processor which is suitable for efficiently carrying out chemical reactions. Therefore, it is also necessary to provide a reactor which can be ready produced by suitable modification of a regular monolithic structure such that two reactions of different energetic nature can be catalytically performed on opposing sides of walls which divide the two sets of discrete flow channels.</p> <p>Streamwise distance (meter), Heterogeneous reaction rate along the length of the reactor (mole per square meter per second)</p> <p>0 13.075</p> <p>0.00025 13.1037</p> <p>0.0005 13.1253</p> <p>0.00075 13.0811</p> <p>0.001 12.9897</p> <p>0.00125 12.8713</p> <p>0.0015 12.7362</p> <p>0.00175 12.5895</p> <p>0.002 12.4345</p> <p>0.00225 12.2741</p> <p>0.0025 12.1101</p> <p>0.00275 11.9443</p> <p>0.003 11.7782</p> <p>0.00325 11.6128</p> <p>0.0035 11.4491</p> <p>0.00375 11.2879</p> <p>0.004 11.1299</p> <p>0.00425 10.9755</p> <p>0.0045 10.8253</p> <p>0.00475 10.6793</p> <p>0.005 10.5378</p> <p>0.00525 10.4009</p> <p>0.0055 10.2684</p> <p>0.00575 10.1406</p> <p>0.006 10.0173</p> <p>0.00625 9.89855</p> <p>0.0065 9.78406</p> <p>0.00675 9.6739</p> <p>0.007 9.56804</p> <p>0.00725 9.46615</p> <p>0.0075 9.36809</p> <p>0.00775 9.27394</p> <p>0.008 9.18373</p> <p>0.00825 9.09715</p> <p>0.0085 9.01421</p> <p>0.00875 8.9348</p> <p>0.009 8.85876</p> <p>0.00925 8.78593</p> <p>0.0095 8.71625</p> <p>0.00975 8.64929</p> <p>0.01 8.58508</p> <p>0.01025 8.52384</p> <p>0.0105 8.46504</p> <p>0.01075 8.4084</p> <p>0.011 8.35384</p> <p>0.01125 8.30147</p> <p>0.0115 8.25092</p> <p>0.01175 8.20203</p> <p>0.012 8.15488</p> <p>0.01225 8.10937</p> <p>0.0125 8.06514</p> <p>0.01275 8.02226</p> <p>0.013 7.98085</p> <p>0.01325 7.9406</p> <p>0.0135 7.90137</p> <p>0.01375 7.86316</p> <p>0.014 7.82602</p> <p>0.01425 7.78976</p> <p>0.0145 7.75459</p> <p>0.01475 7.72034</p> <p>0.015 7.68674</p> <p>0.01525 7.65366</p> <p>0.0155 7.6212</p> <p>0.01575 7.58953</p> <p>0.016 7.55833</p> <p>0.01625 7.52745</p> <p>0.0165 7.49677</p> <p>0.01675 7.46607</p> <p>0.017 7.43551</p> <p>0.01725 7.40508</p> <p>0.0175 7.37459</p> <p>0.01775 7.34397</p> <p>0.018 7.31357</p> <p>0.01825 7.28303</p> <p>0.0185 7.25215</p> <p>0.01875 7.22111</p> <p>0.019 7.19005</p> <p>0.01925 7.15883</p> <p>0.0195 7.12722</p> <p>0.01975 7.09539</p> <p>0.02 7.06334</p> <p>0.02025 7.03095</p> <p>0.0205 6.99814</p> <p>0.02075 6.96499</p> <p>0.021 6.93157</p> <p>0.02125 6.89773</p> <p>0.0215 6.86322</p> <p>0.02175 6.8282</p> <p>0.022 6.79267</p> <p>0.02225 6.7565</p> <p>0.0225 6.71985</p> <p>0.02275 6.6827</p> <p>0.023 6.64477</p> <p>0.02325 6.60607</p> <p>0.0235 6.56675</p> <p>0.02375 6.52675</p> <p>0.024 6.48581</p> <p>0.02425 6.4439</p> <p>0.0245 6.40125</p> <p>0.02475 6.35774</p> <p>0.025 6.31309</p> <p>0.02525 6.26742</p> <p>0.0255 6.22078</p> <p>0.02575 6.17321</p> <p>0.026 6.12453</p> <p>0.02625 6.07467</p> <p>0.0265 6.02388</p> <p>0.02675 5.97193</p> <p>0.027 5.91868</p> <p>0.02725 5.86423</p> <p>0.0275 5.80859</p> <p>0.02775 5.75169</p> <p>0.028 5.69341</p> <p>0.02825 5.63397</p> <p>0.0285 5.57294</p> <p>0.02875 5.51116</p> <p>0.029 5.45709</p> <p>0.02925 5.39358</p> <p>0.0295 5.3349</p> <p>0.02975 5.27843</p> <p>0.03 5.21054</p> <p>Contributor: Junjie Chen, ORCID: 0000-0001-5055-4309, E-mail address: komcjj@gmail.com, Department of Energy and Power Engineering, School of Mechanical and Power Engineering, Henan Polytechnic University, 2000 Century Avenue, Jiaozuo, Henan, 454000, P.R. China</p>
Catalytic reactors with enhanced chemical conversion behavior for conducting simultaneous endothermic and exothermic reactions
<p><strong>Catalytic reactors with enhanced chemical conversion behavior for conducting simultaneous endothermic and exothermic reactions</strong></p> <p>Junjie Chen</p> <p>Department of Energy and Power Engineering, School of Mechanical and Power Engineering, Henan Polytechnic University, 2000 Century Avenue, Jiaozuo, Henan, 454000, P.R. China</p> <p>Contributor: Junjie Chen, ORCID: 0000-0001-5055-4309, E-mail address: komcjj@gmail.com</p> <p> </p> <p>It has been taught methods which may be used to transform a monolithic structure into a co-current or countercurrent flow heat exchanger. The monolith is transformed by cutting or grinding the uppermost section of diving walls from rows of channels contained in the honeycomb. The top end of the newly formed groove is then sealed with suitable cement. The depth of the sealant is such that an opening still exists in the side wall of the structure. A manifold is attached to this inlet. A similar exercise is performed at the opposing end to produce an outlet section. Hot gas is passed through the inlet whilst cold coolant is passed through the open end. Efficient heat transfer occurs between the two streams. However, the possibility of using such an arrangement for coupling endothermic and exothermic catalytic processes on opposing sides of each dividing wall is not taught. It has been taught a method to efficiently transfer energy through a divider by contacting a catalyst to the wall and performing an exothermic reaction there. The energy is conducted through the wall and used to heat a gas stream on the opposing side of the wall. An apparatus is described where multiple layers are formed with alternating hot and cold channels to produce a gas heater. However, the method does not discuss the possibility of utilizing this concept for thermally coupling endothermic and exothermic reactions within a monolith reactor.</p> <p>Streamwise distance (meter), Heterogeneous reaction rate along the length of the reactor (mole per square meter per second)</p> <p>0 1.88478</p> <p>0.00025 1.92635</p> <p>0.0005 2.0243</p> <p>0.00075 2.14121</p> <p>0.001 2.26285</p> <p>0.00125 2.38391</p> <p>0.0015 2.5016</p> <p>0.00175 2.61386</p> <p>0.002 2.71933</p> <p>0.00225 2.81695</p> <p>0.0025 2.9061</p> <p>0.00275 2.98659</p> <p>0.003 3.05831</p> <p>0.00325 3.12146</p> <p>0.0035 3.17647</p> <p>0.00375 3.22385</p> <p>0.004 3.26403</p> <p>0.00425 3.29778</p> <p>0.0045 3.32579</p> <p>0.00475 3.34828</p> <p>0.005 3.36585</p> <p>0.00525 3.37923</p> <p>0.0055 3.38901</p> <p>0.00575 3.39569</p> <p>0.006 3.39964</p> <p>0.00625 3.40142</p> <p>0.0065 3.40139</p> <p>0.00675 3.39974</p> <p>0.007 3.39685</p> <p>0.00725 3.39304</p> <p>0.0075 3.38846</p> <p>0.00775 3.38332</p> <p>0.008 3.37786</p> <p>0.00825 3.37216</p> <p>0.0085 3.36657</p> <p>0.00875 3.36135</p> <p>0.009 3.35646</p> <p>0.00925 3.35185</p> <p>0.0095 3.34767</p> <p>0.00975 3.34403</p> <p>0.01 3.3408</p> <p>0.01025 3.33803</p> <p>0.0105 3.33572</p> <p>0.01075 3.33405</p> <p>0.011 3.33301</p> <p>0.01125 3.33242</p> <p>0.0115 3.33227</p> <p>0.01175 3.33256</p> <p>0.012 3.33329</p> <p>0.01225 3.33451</p> <p>0.0125 3.33619</p> <p>0.01275 3.33825</p> <p>0.013 3.34069</p> <p>0.01325 3.34347</p> <p>0.0135 3.34647</p> <p>0.01375 3.34978</p> <p>0.014 3.35347</p> <p>0.01425 3.35729</p> <p>0.0145 3.36123</p> <p>0.01475 3.36531</p> <p>0.015 3.36946</p> <p>0.01525 3.37365</p> <p>0.0155 3.37777</p> <p>0.01575 3.38195</p> <p>0.016 3.38636</p> <p>0.01625 3.39101</p> <p>0.0165 3.3956</p> <p>0.01675 3.40005</p> <p>0.017 3.40456</p> <p>0.01725 3.40915</p> <p>0.0175 3.41362</p> <p>0.01775 3.41806</p> <p>0.018 3.42267</p> <p>0.01825 3.42714</p> <p>0.0185 3.43145</p> <p>0.01875 3.43582</p> <p>0.019 3.44022</p> <p>0.01925 3.44451</p> <p>0.0195 3.44872</p> <p>0.01975 3.45302</p> <p>0.02 3.45739</p> <p>0.02025 3.46153</p> <p>0.0205 3.46548</p> <p>0.02075 3.4695</p> <p>0.021 3.47355</p> <p>0.02125 3.47744</p> <p>0.0215 3.4811</p> <p>0.02175 3.48467</p> <p>0.022 3.48808</p> <p>0.02225 3.49137</p> <p>0.0225 3.49463</p> <p>0.02275 3.49784</p> <p>0.023 3.50085</p> <p>0.02325 3.50358</p> <p>0.0235 3.50617</p> <p>0.02375 3.50872</p> <p>0.024 3.51116</p> <p>0.02425 3.51353</p> <p>0.0245 3.51592</p> <p>0.02475 3.51817</p> <p>0.025 3.52004</p> <p>0.02525 3.52161</p> <p>0.0255 3.52305</p> <p>0.02575 3.52439</p> <p>0.026 3.52547</p> <p>0.02625 3.52614</p> <p>0.0265 3.52658</p> <p>0.02675 3.5265</p> <p>0.027 3.52593</p> <p>0.02725 3.5252</p> <p>0.0275 3.52428</p> <p>0.02775 3.52285</p> <p>0.028 3.52091</p> <p>0.02825 3.51866</p> <p>0.0285 3.51596</p> <p>0.02875 3.51277</p> <p>0.029 3.50899</p> <p>0.02925 3.5048</p> <p>0.0295 3.4992</p> <p>0.02975 3.4806</p> <p>0.03 3.46548</p> <p>Contributor: Junjie Chen, ORCID: 0000-0001-5055-4309, E-mail address: komcjj@gmail.com, Department of Energy and Power Engineering, School of Mechanical and Power Engineering, Henan Polytechnic University, 2000 Century Avenue, Jiaozuo, Henan, 454000, P.R. China</p>
Figure 14. Right-side mating Brettus cingulatus near a in Conversion of the egg nest to a brood nest by the female Brettus cingulatus (Araneae: Salticidae: Spartaeini)
Figure 14. Right-side mating Brettus cingulatus near a brood that has already molted to instar II. Photographed by Hemanth Kumar H M at Belur, Hassan district, Karnataka.
Figure 13 in Conversion of the egg nest to a brood nest by the female Brettus cingulatus (Araneae: Salticidae: Spartaeini)
Figure 13. Cambodian Brettus cingulatus feeding on a large ant. Attribution and ©: 1-2, mark spicer.
Figure 10. Adult male Brettus cingulatus. 1 in Conversion of the egg nest to a brood nest by the female Brettus cingulatus (Araneae: Salticidae: Spartaeini)
Figure 10. Adult male Brettus cingulatus. 1, Display with pedipalps extended to the sides. 2, Grooming, with fangs extended and chelicerae separated to reveal the endites and rostrum to the rear. Attribution and ©: 1-2, acharya_mr.
Figure 8 in Conversion of the egg nest to a brood nest by the female Brettus cingulatus (Araneae: Salticidae: Spartaeini)
Figure 8. Sequence of selected (not consecutive) frames from a 30 fps video of the brooding female Brettus cingulatus shown in Figure 5. These represent a series of positions at which this female attached silk lines, mostly around the periphery of the nest. This entire sequence of attachment positions is diagrammed in frame 1410 (yellow circle to yellow circle). Note that the number of young in the nest at this stage was considerably smaller than the ~43 eggs deposited by this female.
Figure 6 in Conversion of the egg nest to a brood nest by the female Brettus cingulatus (Araneae: Salticidae: Spartaeini)
Figure 6. Sequence of frames from a 30 fps video of the brooding female Brettus cingulatus shown in Figure 5. Here, as in Figures 7-8, total elapsed time is shown after frame number at the lower right of each frame. 1-5, The female removes remnants of the eggshell from an instar I spiderling (yellow arrow). 275-279, 682-686, The female masticated eggshell remnants (white arrow) with her chelicerae. 772-781, The female finished masticating the eggshell remnants, and then quickly flicked these remnants out of her nest with her feathery pedipalps. The high speed of this flick is indicated by the blurred image of the expelled material in frame 780 (streak marked by white arrow).
Figure 3. Three brooding Brettus cingulatus females. 1, Female guarding recently deposited eggs. 2 in Conversion of the egg nest to a brood nest by the female Brettus cingulatus (Araneae: Salticidae: Spartaeini)
Figure 3. Three brooding Brettus cingulatus females. 1, Female guarding recently deposited eggs. 2, Female with first instar young, still with little pigmentation of the opisthosoma. Note that almost all covering silk, white flecks, and eggshell fragments were absent at this stage. 3, Later first instar young with full pigmentation of the prosoma and opisthosoma, as well as pigmentation of each femur I. The female (not shown) was still guarding the brood at this stage. Photographs by Arundathi Sambayya taken at Bhimanakone, Sangara Taluk, Shimoga District, Karnataka, India.
Figure 1. Brooding female Brettus cingulatus Thorell 1895. 1 in Conversion of the egg nest to a brood nest by the female Brettus cingulatus (Araneae: Salticidae: Spartaeini)
Figure 1. Brooding female Brettus cingulatus Thorell 1895. 1, Guarding recently deposited cluster of eggs covered with silk fibers and white flecks. 2, Ten days later, guarding hatchlings (first instar). Larger white flecks represent eggshell fragments. 3, Three days later. All silk, white flecks, and eggshell fragments are gone, and except for their legs, the first instar young are now pigmented. Photographs by Abhijith A. P. C. at his Indraprastha Organic Farm, Kalalwadi Village, Karnataka, India.
Figure 7 in Conversion of the egg nest to a brood nest by the female Brettus cingulatus (Araneae: Salticidae: Spartaeini)
Figure 7. Sequence of frames from a 30 fps video of the brooding female Brettus cingulatus shown in Figure 5. 1-15, Female masticating eggshell remnants with her chelicerae. 550-559, Female flicking eggshell remnant (red arrow) away from the nest with her pedipalps.
Figure 12 in Conversion of the egg nest to a brood nest by the female Brettus cingulatus (Araneae: Salticidae: Spartaeini)
Figure 12. Immature Brettus cingulatus feeding on late instar I (fully pigmented) B. cingulatus spiderlings in an untended nest. It appears that the female left this brood without converting the egg nest to a brood nest, and the instar I spiderlings, now exposed and vulnerable outside of that nest, had no guardian. At this stage (instar I) it is likely that the spiderlings were still completely blind. Photographs by Hemanth Kumar H M.
Second-line drug resistance markers as proxy indicators of sputum culture conversion for samples tested in Uganda
<p>Increased TB disease burden arises as a result of low treatment success rates stemming from the emergence of second-line drug (SLD) resistance. We aimed at determining the usefulness of SLD resistance markers as proxy indicators of time to sputum culture conversion; a renowned predictor of Tuberculosis (TB) treatment outcome, among SLD-resistant TB patients tested at the Uganda National TB Reference Laboratory (NTRL). A cross-sectional study was conducted on 72 bacteriologically confirmed SLDR TB patients with datasets including culture conversion time and second-line probe assay mutation profiles between 01/06/2017 and 31/12/2019. The data were then imported into STATA v15 for descriptive statistical analysis, Univariate cox proportional hazard model analysis and Kaplan-Meier survival curves at a 5% level of significance; p-value ≤ 0.05. Results indicate the median time was achieved at 3 (0–12) months across the studied patients. The <em>rrs</em> G1484T mutation associated with conferring drug resistance to aminoglycosides was observed to have the shortest median conversion time of 1.5 months and the longest by the <em>gryB</em> E540D at 5 months. A single mutation in the <em>gryA</em> gene locus showed higher converted proportions 70.8% (58.9–81.0) than those that had two 8.3% (3.1–17.3) or three 2.7% (0.3–10.0) mutations. We conclude that the studied second-line drug resistance markers had no statistically significant association with the time to sputum culture conversion, although increased drug resistance levels reduced the converted proportions and stressed the need to utilize molecular diagnostics data to better comprehend proxy indicators of SLD-resistant tuberculosis management.</p>
Argument-seeking conversations in german
<p>This data set consists of ten conversations. The text files are the unedited transcripts of the conversations. The pdf files contain the conversations divided into their respective subtopics.</p>
Effect of temperature in methanol conversion to dimethyl ether (DME) and light hydrocarbons with beta zeolite
<p><span>Crystalline beta zeolite molecular sieve with SiO<sub>2</sub>/Al2O<sub>3</sub> molar ratio of 28.5 was synthesized by the hydrothermal crystallization method and examined for the methanol dehydration reaction. The micro-mesoporous beta zeolite was active between 250 and 450°C. Dimethyl ether (DME) was observed as the predominant product at all reaction temperatures, with a maximum selectivity of 47.9% at 300°C and a methanol turnover frequency (TOF<sub>MeOH</sub>) of 741.9 h-1. At increased reaction temperatures, the beta zeolite showed enhanced strong acid site fraction, promoting higher hydrocarbon formation following the olefin-based cycle. It was revealed that the crystallinity, porosity, and acidity of the beta zeolite change in the reaction environment. Amorphous carbon deposition occurred on beta zeolite, which involved the loss in crystallinity to some extent. The temperature increase showed a pore-broadening phenomenon at elevated temperature regions. The regeneration cycle test showed stable activity of regenerated beta zeolite for 280 h time-on-stream.</span></p>
Raw data for manuscript Semantic context can mask intelligibility declines at above-conversational speech levels in normal-hearing listeners
<p>Raw data for the manuscript in doc file. <br> Copied from the Matlab .m file. used for the analysis.</p> <p>To be updated.</p> <p>For details, contact me at mfer@health.sdu.dk</p>
Fabrication of low loss III-V Bragg-reflection waveguides for parametric down-conversion
<p>Measurements of sidewall roughness (AFM), optical losses (transmission) and photon pair coincidence counts (coinc) of Bragg-reflection waveguides.</p> <p>Data are contained in .csv files. Example plots are .pdf or .png format.</p> <p>RF: with reflow step</p> <p>No RF: without reflow step</p> <p>Coinc: Coincidence Counts</p>
GRAND-SLAM analysis of simulated nucleotide conversion in Illumina TruSeq data sets for grandRescue
<p>These are processed data sets from the simulation of nucleotide conversions (T>C) in single-end and paired-end Illumina TruSeq reads for the purpose of investigating 4sU-induced mapping impairment by read lengths and library preparation methods and the potential of grandRescue to alleviate these effects.</p> <p>The original data set is from: Sarantopoulou, D. <em>et al. </em>(https://doi.org/10.1038/s41598-019-49889-1)</p> <p>GEO Accession:GSE124167 (samples: GSM3523316 - GSM3523318)</p> <p> </p> <p>The zip files contain the full output from the processing pipeline (including the mapped reads, the scripts to run the pipeline and the output) for single-end (R1) and paired-end before and after rescue. The *.tsv.gz files are the GRAND-SLAM output tables.</p> <p><br> To generate the GRAND-SLAM output yourself, first prepare the mouse genomes. Then run the following command with the respective cit-files, prefixes (*.cit) and genome:</p> <p>gedi -e Slam -trim5p 15 -reads *.cit -genomic m.ens102 -prefix grandslam_t15/* -plot -D -modelall</p> <p>To generate the cit file you have to modify the first lines in start.bash to match the paths on your file system, and then run it.</p> <p> </p> <p>Software versions:</p> <p> gedi toolkit 1.0.5<br> GRAND-SLAM 2.0.7<br> STAR version 2.7.10b</p>
ScienceDex guides
Understand access before you commit
These curated guides explain access requirements, typical timelines, costs, and reuse considerations for widely used research datasets.
Allen Brain Atlas
Allen Brain Atlas is an Allen Institute collection of brain map atlases, datasets, APIs, and analysis tools covering mouse, human, and non-human primate brain resources.
Annotated Behaviour and Observability Dataset (ABODe)
ABODe is a University of Edinburgh DataShare dataset for behavior classification in group-housed mice using home-cage video, identities, bounding boxes, ground-plate positions, and annotator labels.
DANDI Archive for NWB datasets
DANDI is a BRAIN Initiative archive for publishing and sharing neurophysiology data, including electrophysiology, optophysiology, and behavioral data packaged as NWB and related standards.
International Brain Laboratory public data
The International Brain Laboratory public data releases expose standardized mouse decision-making experiments, including Neuropixels recordings, widefield calcium imaging, behavior, and session metadata accessed through the ONE API.
OpenNeuro
OpenNeuro is a free, open platform for sharing neuroimaging datasets, with public search, dataset pages, and download paths for web, S3, DataLad, and the OpenNeuro CLI.