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34 results for “direct transition”

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zenodo48/100

Direct observation of electron density reconstruction at the metal-insulator transition in NaOsO3

<p>Open access data set for manuscript &quot;Direct observation of electron density reconstruction at the metal- insulator transition in NaOsO3&quot; published in Physical Review B, 98, 115116 (2018)</p>

opencc-by-4.0Sep 2018View details →
zenodo40/100

The optical absorption in semiconductor to semimetal PtSe2 arises from direct transitions - Supporting data

<p>Data supporting the findings of the work:</p> <p>M. Tharrault, S. Ayari, M. Arfaoui, E. Desgu&eacute;, R. Le Goff, P. Morfin, J. Palomo, M. Rosticher, S. Jaziri, B. Pla&ccedil;ais, P. Legagneux, F. Carosella, C. Voisin, R. Ferreira and E. Baudin,&nbsp;<strong>The optical absorption in semiconductor to semimetal PtSe2 arises from direct transitions</strong><em>, <a href="https://doi.org/10.48550/arXiv.2311.01847">arXiv:2311.01847 [cond-mat.mtrl-sci]</a></em>.</p> <p>&nbsp;</p> <p>The sample names in this study match those used in the <strong>Raman spectroscopy focused study</strong> <a href="https://doi.org/10.1088/2053-1583/ad1e79">https://doi.org/10.1088/2053-1583/ad1e79</a>. Data from that study can be accessed at <a href="https://doi.org/10.5281/zenodo.8256907">https://doi.org/10.5281/zenodo.8256907</a>.</p> <p>See the Supplemental Material for extra details.</p> <p>&nbsp;</p> <p>Files available:</p> <p><strong>Optical absorption spectroscopy.zip:</strong> reflectance, transmittance, real and imaginary 2D optical conductivity for exfoliated and MBE samples.</p> <p><strong>Differential reflectance with temperature.zip:</strong> differential reflectance Delta R / R pour 4 exfoliated thin samples and temperatures from 290K to 440K.</p> <p><strong>Layers label attribution.txt:</strong> number of layers for each sample.</p> <p><strong>Selected samples fig1.txt: </strong>list of samples displayed in the figure 1 of the publication.</p> <p><strong>Band diagrams.zip:</strong> Band diagrams for GGA-computed 1-12L and AB stacked bilayers as well as GW and HSE06 computed 1L and the k-points path used for the diagrams.</p> <p><strong>Optical conductivity DFT.zip:</strong> real 2D optical conductivity and jDOS computed using GGA-IPA for 1-12L and AB stacked bilayers.</p> <p><strong>Optical absorption 1L different models.csv:</strong> GGA-IPA, GW-IPA, GW-BSE and HSE06-IPA real 2D optical conductivities for the monolayer.</p> <p><strong>1L optical absorption with temperature DFT.csv</strong>: 2D real optical conductivity of 1L PtSe2 computed with EPW/ZG Quantum Espresso package for T = 0 K to 450 K.</p> <p><strong>1L electronic spectral function with temperature.zip:</strong> electronic spectral function for 1L PtSe2 for T = 0, 300 and 450 K.</p> <p><strong>Atomic orbitals decomposition.zip:</strong> band diagrams and the corresponding orbital components, as displayed in Supplemental Material.</p> <p><strong>Electronic bandgap correction.txt:</strong> GGA computed bandgaps and corrected by the energy shift.</p>

opencc-by-4.0Oct 2023View details →
zenodo40/100

FIGURE 2 in First direct archosauromorph remains from the Early-Middle Triassic transition of the Iberian Peninsula

FIGURE 2. Geological map and stratigraphic profile of the Port del Cantó locality where IPS-73757 and IPS-90188 were collected.

opencc-by-4.0Dec 2017View details →
zenodo40/100

FIGURE 1 in First direct archosauromorph remains from the Early-Middle Triassic transition of the Iberian Peninsula

FIGURE 1. Map of Catalonia showing the geographic occurrence of the archosauromorph teeth described here. Dashed lines indicate the boundary of each mountain range.

opencc-by-4.0Dec 2017View details →
zenodo40/100

FIGURE 3 in First direct archosauromorph remains from the Early-Middle Triassic transition of the Iberian Peninsula

FIGURE 3. Isolated crocopodan archosauromorph teeth from the Early−Middle Triassic of Catalonia. 1, IPS-90631 in apical (top) and lingual (bottom) views and close up of distal denticles; 2, IPS-73757 in labial view and close up of distal denticles; 3, IPS-90188 in side view and close up of distal denticles. Abbreviations: cr, crown; ro, root. Scale bars equal 2 mm in (1), 5 mm in (2, 3), 0.2 mm in close up of (1), 0.5 mm in close up of (2), and 1 mm in close ups of (3).

opencc-by-4.0Dec 2017View details →
zenodo36/100

Direct observation of a dynamical glass transition in a nanomagnetic artificial Hopfield network

<p>Source files used to produce the publication &quot;Direct observation of a dynamical glass transition in a nanomagnetic artificial Hopfield network.&quot;</p>

opencc-by-4.0Jan 2022View details →
zenodo36/100

Dataset for "Quantifying the effects of bed roughness on transit time distributions via direct numerical simulations of turbulent hyporheic exchange"

<p>This dataset contains the sediment models, DNS flow field data, subsurface path data, and calculated transit time distributions for both the regular- and random-interface cases used in the paper: &quot;Quantifying the effects of bed roughness on transit time distributions via direct numerical simulations of turbulent hyporheic exchange&quot; by Guangchen Shen, Junlin Yuan, and Mantha S. Phanikumar (Submitted to Water Resources Research).&nbsp;<br> Detailed introduction of each data file is as follows.</p> <p>1. DNS flow field data</p> <p>Flowfield_Reg.h5 and Flowfield_Ran.h5 contains the following fields for the regular and random cases, respectively. &#39;ni&#39;, &#39;nj&#39;, &#39;nk&#39; are the numbers of grid points along x, y, and z directions. &#39;xc&#39;, &#39;yc&#39;, &#39;zc&#39; are the cell center locations. &#39;u3d&#39;,&#39;v3d&#39;,&#39;w3d&#39; are the three-dimensional time-averaged velocities at each grid point. &#39;vof&#39; is the volume-of-fluid field used by the immersed-boundary method to prescribe the fluid-solid interface (vof=1 in fluid and 0 in solid), at each grid point. &#39;vof&#39; contains the information of sediment grain distribution and bed roughness geometry. Only the subsurface data (those below the sediment crest) are shared due to dataset size limit.</p> <p>2. Particle-tracked subsurface flow paths and corresponding transit time distributions</p> <p>The mat files &ldquo;xxx_pathline&rdquo; store the (x,y,z) location of each point (saved as &#39;StrX&#39;, &#39;StrY, &#39;StrZ&#39;) along the subsurface paths, discretized by uniform steps of travel time (with time intervals of 0.1 for &#39;A&#39; and 0.01 for &#39;MD&#39; cases, normalized by channel height and friction velocity). The files &ldquo;xxx_TT&rdquo; store the array of transit times corresponding to the tracked paths, where the 1d array T is the transit time. &#39;A&#39; denotes calculations based on time-mean advection only, while &#39;MD&#39; denotes calculations accounting for additional molecular diffusion. &#39;Interface&#39; and &#39;3DiameterBelow&#39; indicate that the particles were released at the interface and -3 D below the interface, respectively.</p>

opencc-by-4.0Jan 2022View details →
zenodo36/100

Direct Observation of the Transitional Stage of Mixing-State- Related Absorption Enhancement for Atmospheric Black Carbon

<p>Data for article <em>Direct Observation of the Transitional Stage of Mixing-State-Related Absorption Enhancement for Atmospheric Black&nbsp;Carbon.</em></p>

opencc-by-4.0Sep 2022View details →
dryad36/100

Direct observation of phase transitions in truncated tetrahedral microparticles under quasi-2D confinement

Open the record for dataset details and reuse information.

publicFeb 2024View details →
zenodo32/100

Directed percolation and puff jamming near the transition to pipe turbulence

<p>The onset of turbulence in pipe flow has defied detailed understanding ever since Reynolds' first observations revealed the spatially-heterogeneous nature of the transition. While recent theoretical studies and experiments in simpler, shear-driven flows suggest that the onset of turbulence is a directed percolation non-equilibrium phase transition, whether these findings are generic and apply also to open or pressure-driven flows is unknown. In pipe flow, the extremely long time scales near the transition make direct observations of critical behavior virtually impossible. Here, we circumvent these limitations by experimentally characterizing all pairwise interactions between localized patches of turbulence ("puffs"), and using these interactions as input to renormalization group and computer simulations of minimal models that extrapolate to long length and time scales. We show that the universality class of the transition is directed percolation, from which emerges a jammed phase of puffs above the critical point. The stronger interactions in the jamming regime enable us to explicitly measure the turbulent fraction and confirm model predictions. Our work shows that directed percolation scaling applies beyond simple closed shear flows, and underscores how statistical mechanics can lead to profound, quantitative and predictive insights on turbulent flows and their phases.</p>

opencc-by-4.0Dec 2023View details →
geo24/100

The atypical KRASQ22K mutation directs TGF-β response towards partial epithelial-to-mesenchymal transition in patient-derived colorectal cancer tumoroids

GEO Series GSE270815. Homo sapiens. 12 samples. Type: Expression profiling by high throughput sequencing.

openGEO-OpenMar 2025View details →
geo24/100

Adventitial fibroblasts direct smooth muscle cell-state transition in pulmonary vascular disease

GEO Series GSE262069. Homo sapiens. 16 samples. Type: Expression profiling by high throughput sequencing.

openGEO-OpenApr 2025View details →
geo24/100

Bi-directional interaction between mesenchymal stem cells and transit amplifying cells in mesenchymal tissue homeostasis [MSCTAC]

GEO Series GSE109876. Mus musculus. 6 samples. Type: Expression profiling by high throughput sequencing.

openGEO-OpenJan 2019View details →
geo24/100

Sorghum SbGhd7 is a major regulator of floral transition and directly represses genes crucial for flowering activation

GEO Series GSE238094. Sorghum bicolor. 4 samples. Type: Genome binding/occupancy profiling by high throughput sequencing.

openGEO-OpenJan 2024View details →
geo24/100

Chromatinized PKC-q directly regulates inducible genes in epithelial to mesenchymal transition and breast cancer stem cells

GEO Series GSE53320. Homo sapiens. 4 samples. Type: Genome binding/occupancy profiling by high throughput sequencing.

openGEO-OpenJun 2014View details →
geo24/100

Sorghum SbGhd7 is a major regulator of floral transition and directly represses genes crucial for flowering activation

GEO Series GSE237989. Sorghum bicolor. 6 samples. Type: Expression profiling by high throughput sequencing.

openGEO-OpenJan 2024View details →
geo24/100

Persister state-directed transitioning and vulnerability in melanoma

GEO Series GSE118529. Homo sapiens. 30 samples. Type: Expression profiling by high throughput sequencing.

openGEO-OpenMar 2022View details →
geo24/100

Sorghum SbGhd7 is a major regulator of floral transition and directly represses genes crucial for flowering activation

GEO Series GSE238095. Sorghum bicolor. 10 samples. Type: Expression profiling by high throughput sequencing; Genome binding/occupancy profiling by high throughput sequencing.

openGEO-OpenJan 2024View details →
geo24/100

Persister state-directed transitioning and vulnerability in melanoma

GEO Series GSE168192. Homo sapiens. 6 samples. Type: Expression profiling by high throughput sequencing.

openGEO-OpenMar 2022View details →
geo24/100

Selective RNA sequestration in biomolecular condensates directs cell fate transitions

GEO Series GSE302363. Homo sapiens; Mus musculus. 40 samples. Type: Expression profiling by high throughput sequencing.

openGEO-OpenSep 2025View details →

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International Brain Laboratory public data

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