dataesr/scientific-paragraphs-categorization huggingface dataset:
Dating of the archaeological site During the excavation of the archaeological site, Beta Analytics™ realized 14 C datings on 13 samples, giving dates with 68. 3% probability (1σ) between 200 BCE and 5 AD. New 14 C dates were realized on collagen extracted from 7 human, 2 horse and 1 bovid bones. The protocol of the extraction of soluble collagen was based on the method described by  Longin (1971)  and has been previously described in detail by  Richardin et al. (2017). All measurements were performed with Accelerator Mass Spectrometry techniques from the Artemis AMS facility at Saclay (France)  (Moreau et al. , 2013). Calendar dates were determined using the OxCal v. 4. 2 procedure and the most recent calibration curve data for the Northern Hemisphere, IntCal13  (Reimer et al. , 2013). Calibration of radiocarbon ages was performed considering that the contribution of marine products to the diet of the Gauls remained marginal.
Oxygen isotope ratios of apatite phosphate Oxygen isotopic analyses were performed with stable isotope mass spectrometry techniques. Phosphate ions were extracted from the apatite using a wet chemistry procedure. After the dissolution of about 30 mg of each sample in 2 mL of 2 M HF at ambient temperature for 24 h, the CaF 2 precipitate was separated from the sample solution by centrifugation. The phosphate ions were neutralized with KOH and isolated using a strong anionic resin (Amberlite IRN 78) before being precipitated as silver phosphate following the method first described by  Crowson et al. (1991)  and slightly modified by  Lécuyer et al. (1993). The oxygen isotope data were obtained using a high-temperature pyrolysis continuous flow technique developed by  Lécuyer et al. (2007)  and  Fourel et al.
A large part of the child's diet consists of milk, which is 18 O-enriched from the mother's body water. The second and third molars, respectively M2 and M3, are considered postweaning teeth and do not record any breast-feeding. Although the M3 is not discernable from the oxygen isotope value of bones from TG-02 and is 18 O-depleted compared to the two other teeth for TG-03, the M2 has similar values than pre-weaning teeth (M1 for TG-01 and PM1 for TG-03). On the contrary, herbivore teeth are depleted in 18 O compared to bones: -1. 3‰ for bovids and -1. 4‰ for the horse TG-CH1. Herbivore hypsodont teeth, which grow continuously and are often used to study climate seasonality (e. g. Bernard et al. , 2009) , record a signal which is more limited in time than bones. For the last decade, the average interannual change in yearly MAT of Picardie, France, is ±1 • C (data from historique-meteo.
Therefore, we can apply one-way ANOVA analysis to test our hypothesis. The results of the test, as well as the summary statistics by groups (i. e. , count, mean, standard deviation) are presented in Table  2. Based on these results, we can conclude that our research hypothesis is validated. The participants that interacted with a robot that matched their regulatory focus type interacted with it for longer than the participants that interacted with a robot that did not match their regulatory focus type. This result is also represented graphically as a raincloud plot 6  in Figure  5. To further validate our results we have performed a power analysis for the one-way analysis of variance by applying the specific function from the pwr R package that implements the power analysis as outlined by  Cohen (2013).
Population Twenty-three patients with early-stage DLB and 20 healthy control subjects (CS), who were participating in a larger cohort study, AlphaLewyMA (http://clinicaltrials. gov/ct2/show/NCT01876459), were enrolled in the study. Patients were recruited from the tertiary memory clinic of the University Hospital of Strasbourg, France. Control subjects were recruited from the hospital's Clinical Investigation Centre. The patient group and the control group were matched for age and educational level (Table  1 ). Patients had to be in the prodromal or mild stages of the disease (Mini-Mental State Examination [MMSE] score ≥ 20), with probable DLB according to the current and formal criteria  [42, 43]  and to DSM-5 for the prodromal stage  [44]. Thus, in addition to the cognitive impairment, they had to fulfil a minimum of two of the following core criteria for the disease: fluctuations, parkinsonism, and hallucinations.
VBM analysis VBM analyses included image pre-processing and statistical analyses. These steps were carried out using the SPM12 software package (Wellcome Department of Imaging Neuroscience, London; http://www. fil. ion. ucl. ac. uk/) running on Matlab R2017 (MathWorks, Natick, MA, USA). Anatomical MRI images were spatially preprocessed using standard procedures  [55]. All T1weighted structural images were first segmented, biascorrected and spatially normalized to the Montreal Neurological Institute (MNI) space using an extension of the unified segmentation procedure  [56]  that includes six classes of tissue. The DARTEL registration toolbox was then used to build a study-specific template and to bring into alignment all of the segmentation images. The VBM analysis was done on modulated grey matter (GM) images; that is, the GM value in each voxel was multiplied by the Jacobian determinant derived from the spatial normalization.
ROI analysis Insular cortex volumes (Fig. 1 ) were extracted in the left and the right hemisphere using Freesurfer (http://surfer. nmr. mgh. harvard. edu/). Correlation analyses between insular volumes and behavioural data were carried out using a general linear model, with age and TGM as nuisance covariates, with the StatsModels python module (http://statsmodels. sourceforge. net/), using a statistical threshold of P = 0. 05. As in the VBM study, only negative correlations were considered, on the assumption that higher scores would be associated with more pronounced atrophy within the insular cortex. A more complex regression model involving additional explanatory variables, namely the MMSE score, the educational level and the volumes of the regions found outside the insular cortex with the VBM analyses (i.
We carried out measurements during the first minute of flow and during the last minute of flow over five minutes. Each profile measurement lasts for 30 s. In some cases, there is a slight evolution of Fig. 3. Dimensionless velocity (V/V max ) as a function of the radius for 7 wt. % of wax in oil. The symbols present the velocity profile during the increasing phase and the dashed lines present the velocity profile in the decreasing phase. the velocity profile during the five minutes of shearing, which is illustrated in Fig. 3  for one rotation velocity value. In the following we will leave apart this aspect and focus on the last velocity profile measured during the five minutes period at each rotation velocity. First, we focus on the data for the 7% concentration, which well illustrate different aspects.
The thickness and refractive index of the different layers were estimated by fitting the ellipsometry data using the Cauchy model. The refractive index was considered equal across all layers of the same material in the fitting. It should be pointed out that the reliability of ellipsometry data fitting is somewhat lower in comparison with single thin films due to large number of layers. The 10-layer BR fit yielded on average 230 nm thick Al 2 O 3 layers with a   refractive index of 1. 64 ± 0. 01 at 1. 55 µm, and 130 nm thick As 2 Se 3 layers with a refractive index of 2. 81 ± 0. 01 at 1. 55 µm. The 20-layer BR fit yielded on average 230 nm thick Al 2 O 3 layers with a refractive index of 1. 67 ± 0. 01 at 1. 55 µm, and 130 nm thick As 2 Se 3 layers with a refractive index of 2. 79 ± 0. 01 at 1.
Acknowledgments The project  of International Mobility of Researchers  at the  University of Pardubice , OP  RDE  project  CZ. 02. 2. 69/0. 0/0. 0/16_027/0008008 ; the  Czech Science Foundation  (project No. 19-24516S );  COST MP1401-STSM ;  Centre National de la Recherche Scientifique (CNRS) ;  Brittany Region. Equipment funding of  Institut Foton  was partly provided by the  CPER Sophie. Platform ScanMAT-CMEBA UMS CNRS 2001 at University of Rennes 1, FRANCE.
Electrophysiology Magnesium Inhibited Cation (MIC) currents were recorded using the whole-cell patch-clamp technique as previously published  (Rybarczyk et al. , 2017). The composition of the extracellular solution was (in mM): Na-gluconate 150; K-gluconate 5; Mg-gluconate 2; Ca-gluconate 2; HEPES 10; glucose 5; TEA-Cl 5; pH adjusted to 7. 4 with NaOH. The composition of intrapipette solution was (in mM): Na-gluconate 8; Cs-methanesulfonate 145; EGTA 10; HEPES 10; pH adjusted to 7. 2 with CsOH. Membrane potential was held at -40 mV and currents were elicited by a ramp depolarization from -100 mV to +100 mV for 350 ms at the frequency of 0. 1 Hz. Signals were filtered at 1 kHz and digitized at 5 kHz using an Axopatch 200B patch-clamp amplifier (Molecular Devices, Sunnyvale, CA, United States) combined with a 1322A digidata (Molecular Devices, Sunnyvale, CA, United States).
Immunofluorescence-labeled cell preparations were studied using a Zeiss LSM 710 R NLO confocal laser scanning microscope (Carl ZEISS SAS, Marly-le-Roi, France) with the 63× oil-immersion objective (ON 1. 4) coupled with CHAMELEON femtosecond Titanium-Sapphire Laser (Coherent, Santa Clara, CA, United States). Alexa 488 and 568 were sequentially excited by 488 nm line of Argon laser and diode laser 561 nm. Emitted signals were, respectively, collected with 493-560 nm and 570-700 bandpass filters. Image acquisitions were performed with ZEN Software (Carl ZEISS SAS, Marly-le-Roi, France) and all acquisition settings were constant between specimens. Colocalization analyses were made with ImageJ software (Colocalization Analysis plugin).
Statistical Analysis Data are presented as mean ± SEM and n refers to the number of independent repeat of experiment. Statistical analyses were made using Student's t-tests or Mann-Whitney rank sum test depending on sample normality or paired Wilcoxon signed rank test using Sigma-Stat 3. 0 (Systat Software, Inc. ). When more than two conditions were compared, a Kruskal-Wallis one-way ANOVA was used followed by post hoc Dunn's Method tests. Results were considered significant when *P < 0. 05, **P < 0. 01, and ***P < 0. 001.
AG-9 Stimulates TRPM7 Currents in Pancreatic Cancer Cells Firstly, TRPM7 expression was assessed by quantitative RT-PCR following the treatment with AG-9 or VG-6 for 24 h. TRPM7 expression was not modified by EDP treatment (n = 4; P < 0. 05; Figure  2A ) while TRPM7 silencing decreased TRPM7 expression by 90. 2 ± 0. 1% at mRNA level (n = 4; P < 0. 01; Figure  2B ), and by 30 ± 7% at protein level (n = 4; P < 0. 05; Figures  2C, D ) when compared to siControl. We previously showed that Magnesium-Inhibited Cation (MIC) currents are mainly due to TRPM7 channel activity in MIA PaCa-2 cells  (Rybarczyk et al. , 2017). MIC currents were recorded by using the conventional technique of patch-clamp in whole-cell configuration. Maximal MIC current intensity was reached after almost 15 min of intracellular media dialysis with EGTA (data not shown, see  Rybarczyk et al.
ACKNOWLEDGMENTS We thank  Aurélie Dupont-Deshorgues ,  Marie-Pierre Mabille , and  Louis-Victor Gaudet  for their technical help. This work was supported by  L'Université de Picardie Jules Verne (UPJV), L'Université de Reims Champagne-Ardenne (URCA), Le CHU Amiens-Picardie ,  Le Centre National de la Recherche Scientifique  ( UMR 7369 ),  La Ligue Contre le Cancer (Comité du Septentrion) , and  Le Cancéropôle Nord-Ouest (CNO).
01 eV is used for all cross sections entering in eq 8 for consistency. The statistical error in the ML cross section stems mainly from ML inaccuracy, while the error in TDDFT cross sectionfrom insufficient statistical sampling. Accuracy errors due to the quality of the TDDFT electronic structure and NEA approximations are out of the scope of this work and will not be discussed. The ML-NEA method proposed here does not aim at creating models transferable to other molecules, but rather to improve the existing NEA technique for a single system. Thus, an ML model must be trained for each new case. The cross section calculations using our ML-NEA approach can be performed by following the online tutorial available at http://mlatom. com/tutorial/tutorial-mlnea. This tutorial also contains the necessary scripts (open source) and links to the required free software packages.
■ COMPUTATIONAL DETAILS Absorption cross sections based on NEA were calculated with the Newton-X program package. 45, 46 Gaussian line shapes were used throughout. For benzene, we report new calculations done for this work, while for compound 2, we used the NEA spectrum from ref 47. In the case of benzene, the required geometry optimization and frequency calculations were performed at the B3LYP 48 /def2-TZVPP 49-51 level of theory. TDDFT at the CAM-B3LYP 52 /ma-TZVP  [49] [50] [51] 53  level of theory was used for calculating excitation energies and oscillator strengths. All electronic-structure calculations (geometry optimization, frequency, and excited-state calculations) for benzene were performed using the Gaussian 16 program package. 54  See ref 47 for computational details for compound 2.
■ CONCLUSIONS In this study, we developed a new ML approach to compute absorption cross sections within NEA. In this ML-NEA approach, a large ensemble with 50000 nuclear geometries is obtained by stochastically sampling a Wigner distribution for the quantum harmonic oscillator. The required electronic propertiesexcitation energies and oscillator strengthsare calculated only for a fraction of these points using the reference electronic structure method (here, we used linear-response TDDFT). The obtained data set is used as the training set for ML. We train individual ML models for each of the reference properties using the KREG model (KRR with the Gaussian kernel function and the RE descriptor) as implemented in MLatom to calculate the required properties for the remaining points in the large ensemble.
Microwave characterization For the microwave behavior, the ferrimagnetic composite used to fabricate the coplanar transmission line is the sample deposited at -1. 2 V due to a large internal magnetic field and a minimum roughness emphasized by SQUID and AFM measurements, respectively. The saturation magnetization (: -) for a filled membrane is close to 0. 18 T. As a matter of fact, for the CoFe2O4 nanowires, the < = value is approximately equal to 0. 36 T since the porosity of the AAO template is around 50 %. This value is quite close to this generally attributed to bulk material which is 0. 48 T. In addition, an effective permittivity of 11 as the average value between alumina Al2O3 and CoFe2O4 nanowires was introduced into HFSS during the simulations. As shown in Fig. 8 , the 3D design of the CPW line and the numerical studies at high-frequency are performed using the three dimensional software HFSS based on the finite elements method (FEM).
Conclusions The dynamical properties of plasticized cellulose acetate have been examined by dynamical mechanical analysis, structural properties and crystallinity were investigated by X-ray diffraction for a more detailed description of blends. For octanoic acid, a decrease of the glass transition temperature followed by an unmixing of the system, as a function of plasticizer content, was observed. Although it is not a good plasticizer at high content, at low concentration 10 wt% allowed a drop in Tg of approximately 150 °C. Through the correlation between DMA and WAXS/SAXS results, the plasticizing effect of lactates on cellulose acetate were studied in detail. We interpreted data and with the help of the literature, it allowed us to highlight mechanisms regarding miscibility and phase separation in the strongly H-bonded of cellulose acetate blends with the increasing plasticizer content.
Acknowledgments: The authors appreciatively thank the  FUI FOR-TUNE, and more particularly Bpi France , the  DGE (Directorate General for Enterprise) , the  Minister for Enterprises , the  Auvergne Rhône-Alpes Region , and the  FEDER European Funds , for their financial support and more particularly  Olivier Chaubet  from  Solvay  for the fruitful discussions. The authors also thank  RHODIA Acetow  for their supply of commercial cellulose acetate and  Carlos Fernandez de Alba  from the  ICL polymeric NMR service  ( IMP / CNRS / UMR 5223 ) for his kind welcome and help. They acknowledge all the project partners.
Here, ε 0 = 8. 85 × 10 -12 C V -1 m -1 is the vacuum permittivity, and ε b 10 is the background dielectric constant of the non-polar ions  40. The last term of (2) emulates the interaction of the ferroelectric polarization with the material chirality fluctuation, described by the parameter Λ. In most simulations, we took Λ = 0. The local fluctuation, defining the direction of the chirality jumps naturally arise due to the random mesh configuration. To calibrate the effect of the mesh fluctuations we swept the value of Λ and found that at the threshold value Λ c 7 × 10 -5 C -2 m 3 N, the direction of the chirality jump 2-3 at Fig. 2d  changes to the opposite one. The phase-field simulations were performed using the FERRET package  40  , designed for the multi-physics simulation environment MOOSE  41.
Acknowledgements. This work was supported by the  US Department of Energy, Office of Science, Basic Energy Sciences, Materials Sciences and Engineering Division  (O. H. V. M. V and partly I. L); by the  H2020 RISE-ENGIMA , RISE-MELON and ITN-MANIC actions (Y. T. , A. R. and I. L. ),  French goverment for Bourse Ostrogradski  (Y. T. ), and by the  Southern Federal University, Russia  (A. R. and Y. T. ).
11-1. 91×10 6 ixels 2 each) regularly spaced from one another by 1 micron. The corresponding voxel size is of 1 micron. The total volume of each sample corresponds to huge datasets of 557-958 x 10 6 voxels 3 , linearly scaled into a 16-bit format, corresponding to sample volumes of 0. 557-0. 958mm 3 able4). Image analysis. Image analysis is performed with the ImageJ software, allowing to use the whole image datasets. Filtering and thresholding procedures are tuned in order to get as close as possible to the imposed %oil of 20 or 40% The greylevel histogram of the whole stack is calculated, and filtering aims at allowing the histogram to span the whole available grayscale (0-255), and to separate the existing peaks (one corresponds to darker pores and the other to lighter solids). While controlling the stack histogram at each step of the procedure, the contrast of the image stack is enhanced (with the Enhance Composition of the raw materials used to make the two GP cement pastes, either with 100% MK OR 80%MK, 20%GGBFS, obtained by X Ray fluorescence.
Acknowledgments We gratefully acknowledge the  French Centre National de la Recherche Scientifique (CNRS)  for funding the one year délégation of  Prof. C. A. Davy  at  Sorbonne Université ,  Campus de Jussieu , laboratoire METIS, UMR 7619, Paris, France. Scientific input by  Dr Christel Pierlot ,  UCCS , is also gratefully acknowledged.
The coefficients of Equation 1 were determined by ordinary least square regression using the eight design points (Experiments 1 to 8 in Table  2 ). Four replicated experiments were also carried out at the centre of the experimental domain and used as check points in order to evaluate the predictive performance of the developed models (Experiments A to D in Table  2 ). Multiple linear regression analyses were performed using NEMRODW® software (LPRAI, Marseille, France).
Clay minerals were identified based on the position of the (001) series of basal reflections on the curve with the MacDiff software  (Petschick, 2000)  using the main X-ray diffraction peaks of each mineral (mixed-layers illite-smectite: 12-17Å; illite: 10Å and kaolinite/chlorite: 7Å). Relative proportions of kaolinite and chlorite were determined using the 3. 57 and 3. 54Å peaks respectively. Measurements of illite layers in mixedlayered (I-S) were performed following the procedure of  Moore and Reynolds (1997). Analytical uncertainties are estimated to be 5%.
Conclusion New mineralogical data from the Pueblo, Hot Springs, Elm and Lohali Point sections were documented for the Western Interior Basin during the Cenomanian-Turonian boundary time interval, which includes the OAE2. It appears that the mineralogical trends reflect a primary signal. During the Cenomanian-Turonian eustatic rise the incursion of warm oxygenated water masses into seaway corresponds exactly to a major change in clay mineralogical assemblage with a significant rise in R0 I-S up to 90% and a decrease in kaolinite contents at Pueblo. In this interval the mineralogical distribution in the south-central region of the basin is mainly influenced by sea-level fluctuations. In the WIB the large distribution of bentonite horizons and volcanic ash layers in sediments indicates very important volcanic activity.
Acknowledgments We are grateful to  Bernard Beaudoin  ( Mines-ParisTech ) and  Danièle Grosheny  ( University of Lorraine ) for their advice, help, and collecting the samples. We would like to thank the Navajo tribes for permission to conduct field work on their tribal lands. We would also like to acknowledge the editorial assistance of  Eduardo Koutsoukos. Mark Leckie  and an anonymous reviewer are acknowledged for their helpful and very constructive reviews.
Mechanical properties The static bending strength (MOR) and modulus of elasticity (MOE) were tested based on the EN 310 standard  [19]. The samples for this test were prepared to align the wood fiber course parallel to the long edge of the test specimen. Internal bonding was determined through the tensile test perpendicular to the surface of the board, according to EN 319 standard  [20]. The analysis of screw withdrawal strength was done according to EN 320 standard  [21]. All tests were done with an INSTRON 3369 universal testing machine and conducted at least ten times. The results of the determination of the physical and mechanical properties of plywood were statistically analyzed using Statistica version 13 (TIBCO Software Inc. ). For significant differences between factors, analysis of variance (ANOVA) at a 0.
Cutting force The cutting force was determined during the milling of samples with dimensions 100 mm × 150 mm × 6 mm. The panels were placed in a measuring platform with a piezoelectric transducer (Kistler 9601), with an amplifier (Kistler 5036), and a data acquisition card (National Instruments PCI-6111). Measurements were made in the X-and Y-axes with a frequency of 50 kHz. For the milling process, a single-blade mandrel head (Faba SA) with a cemented carbide blade was used (FTS-07. 01) for formatting and rebating. The measurements were carried out at a spindle speed of 18000 rpm and a feed rate of 3. 6 m min -1. The milling process was carried out throughout the entire thickness of the composite panels. Recorded measurements were analyzed in LabVIEW software. The cutting force index was calculated from the following equations (3 and 4): F ¼ RMS X 2 þ RM Y 2 À Á 0:5 ð3Þ CFI ¼ F RE F n À1 ð4Þ In which F RE is the average resulting force of the reference sample, F n is the average resulting force of each sample, and RMS is the root mean square of each axis.
Acknowledgments Eduardo Robles wants to acknowledge the support by  E2S UPPAResearch Chair Partnership (BOIS)  supported by the  Excellence Initiative of the University of Pau and Pays de l'Adour  and the  I-Site E2S. The tests of shear strength and in-wood damage have been completed within the activity of the  Student Furniture Research Group (Koło Naukowe Meblarstwa) at the Faculty of Wood Technology of the Warsaw University of Life Sciences -SGGW.
Data availability The raw data required to reproduce these findings are available to download from https://data. mendeley. com/datasets/hkgstm9sxg/dra ft?a = 01cff086-a35f-4542-9f44-b78194cd5db4. The processed data required to reproduce these findings are available to download from https://data. mendeley. com/datasets/hkgstm9 sxg/draft?a = 01cff086-a35f-4542-9f44-b78194cd5db4.