Search results for "DT"

showing 10 items of 2454 documents

Raman spectroscopy of synthetic, geological and biological vaterite: a Raman spectroscopic study

2009

Raman spectroscopy was used to study vaterite samples of biological, geological and synthetic origin. The Raman band positions and the full width at half-maximum (FWHM) of the lattice modes and the internal modes of the carbonate ion of all specimens show no significant differences between vaterites of different origin. With increasing Mg concentrations, synthetic vaterite samples show increasing FWHM in the region of the lattice modes and the three ν1 bands, whereas no change in luminescence was detected. In contrast, in situ measurements of vaterite areas in freshwater cultured pearls (FWCPs) by laser ablation inductively coupled plasma mass spectrometry (LA-ICP-MS) together with the Rama…

In situMagnesiumchemistry.chemical_elementFull width at half maximumCrystallographychemistry.chemical_compoundsymbols.namesakechemistryVateritesymbolsCarbonate IonCarbonateGeneral Materials ScienceLuminescenceRaman spectroscopySpectroscopyJournal of Raman Spectroscopy
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A Split-Window Algorithm for Estimating LST From Meteosat 9 Data: Test and Comparison With Data and MODIS LSTs

2009

The main purpose of this letter is to give an operational algorithm for retrieving the land surface temperature (LST) using the Spinning Enhanced Visible and Infrared Imager data onboard the Meteosat Second Generation (MSG2) satellite. The algorithm is a split-window method using the two thermal infrared channels IR10.8 and IR12.0. The MODTRAN 4.0 code was used to obtain numerical coefficients of the algorithm proposed. The results show that for viewing angles lower than 50deg the algorithm is capable of producing LST with a standard deviation of 0.7 K and a root-mean-square error (rmse) of 1.3 K. The algorithm has been applied to a series of MSG2 images obtained from an MSG antenna system …

In situMeteorologyLand surface temperatureMean squared errorMODTRANGeotechnical Engineering and Engineering GeologyStandard deviationEnvironmental scienceSatelliteElectrical and Electronic EngineeringSplit windowImage retrievalAlgorithmRemote sensingIEEE Geoscience and Remote Sensing Letters
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In vitro evaluation of poloxamer in situ forming gels for bedaquiline fumarate salt and pharmacokinetics following intramuscular injection in rats

2019

Graphical abstract

In situPO Propylene oxideIV IntravenousP338 Poloxamer 338lcsh:RS1-441Pharmaceutical Sciencechemistry.chemical_compoundn Sample sizeSD Standard deviationIM Intramuscularchemistry.chemical_classificationC0 Analyte plasma concentration at time zeroDoE Design of experimentsUV UltravioletPharmacology. TherapyK2.EDTA Potassium ethylenediaminetetraacetic acidLC–MS/MS Liquid chromatography-tandem mass spectrometryH&E Hematoxylin and eosintmax Sampling time to reach the maximum observed analyte plasma concentrationIn situ forming gelsCMC Critical micellar concentrationCmax Maximum observed analyte plasma concentrationIntramuscular injectionDN Dose normalizedGPT Gel point temperaturePLGA Poly-(DL-lactic-co-glycolic acid)TFA Trifluoroacetic acidCAN AcetonitrileATP Adenosine 5′ triphosphateSalt (chemistry)Polyethylene glycolPoloxamerArticlelcsh:Pharmacy and materia medicaPharmacokineticsIn vivoUHPLC Ultra-high performance liquid chromatographyPharmacokineticsAUClast Area under the analyte concentration versus time curve from time zero to the time of the last measurable (non-below quantification level) concentrationEO Ethylene oxideNMP N-methyl-2-pyrrolidoneComputingMethodologies_COMPUTERGRAPHICSAUC∞ Area under the analyte concentration vs time curve from time zero to infinite timeP407 Poloxamer 407In vitro releasePoloxamerCMT Critical micellar temperatureGel erosionIn vitrot1/2 Apparent terminal elimination half-lifechemistryMDR-TB Multi-drug resistant tuberculosisAUC80h Area under the analyte concentration versus time curve from time zero to 80 htlast Sampling time until the last measurable (non-below quantification level) analyte plasma concentrationMRM Multiple reaction monitoringNuclear chemistrySustained releaseInternational Journal of Pharmaceutics: X
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"Table 11" of "Measurement of event shape and inclusive distributions at s**(1/2) = 130-GeV and 136-GeV."

1997

1-Thrust distribution. Axis definition is from corrected charged plus neutral particles.

Inclusive133.0E+ E- --> NEUTRAL XE+ E- ScatteringPhysics::Space PhysicsHigh Energy Physics::ExperimentE+ E- --> CHARGED XDN/DTHRUSTSingle Differential Distribution
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"Table 41" of "Comparison of large-angle production of charged pions with incident protons on cylindrical long and short targets"

2009

Differential cross section for PI+ production with a PB target in the angular range 1.15 to 1.35 radians.. The errors are the square root of the diagonal elements of the covariant matrix.

InclusiveAstrophysics::High Energy Astrophysical PhenomenaAstrophysics::Solar and Stellar AstrophysicsPhysics::Accelerator PhysicsD2SIG/DP/DTHETADouble Differential Cross SectionAngular DependenceAstrophysics::Galaxy AstrophysicsP PB --> PI+ X
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"Table 42" of "Comparison of large-angle production of charged pions with incident protons on cylindrical long and short targets"

2009

Differential cross section for PI+ production with a PB target in the angular range 1.35 to 1.55 radians.. The errors are the square root of the diagonal elements of the covariant matrix.

InclusiveAstrophysics::High Energy Astrophysical PhenomenaD2SIG/DP/DTHETADouble Differential Cross SectionAngular DependenceP PB --> PI+ X
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"Table 5" of "Comparison of large-angle production of charged pions with incident protons on cylindrical long and short targets"

2009

Differential cross section for PI+ production with a C target in the angular range 1.15 to 1.35 radians.. The errors are the square root of the diagonal elements of the covariant matrix.

InclusiveAstrophysics::High Energy Astrophysical PhenomenaP C --> PI+ XAstrophysics::Solar and Stellar AstrophysicsPhysics::Accelerator PhysicsD2SIG/DP/DTHETADouble Differential Cross SectionAngular DependenceAstrophysics::Galaxy Astrophysics
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"Table 6" of "Comparison of large-angle production of charged pions with incident protons on cylindrical long and short targets"

2009

Differential cross section for PI+ production with a C target in the angular range 1.35 to 1.55 radians.. The errors are the square root of the diagonal elements of the covariant matrix.

InclusiveAstrophysics::High Energy Astrophysical PhenomenaP C --> PI+ XD2SIG/DP/DTHETADouble Differential Cross SectionAngular Dependence
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"Table 23" of "Comparison of large-angle production of charged pions with incident protons on cylindrical long and short targets"

2009

Differential cross section for PI+ production with a TA target in the angular range 1.15 to 1.35 radians.. The errors are the square root of the diagonal elements of the covariant matrix.

InclusiveAstrophysics::High Energy Astrophysical PhenomenaP TA --> PI+ XAstrophysics::Solar and Stellar AstrophysicsPhysics::Accelerator PhysicsD2SIG/DP/DTHETADouble Differential Cross SectionAngular DependenceAstrophysics::Galaxy Astrophysics
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"Table 24" of "Comparison of large-angle production of charged pions with incident protons on cylindrical long and short targets"

2009

Differential cross section for PI+ production with a TA target in the angular range 1.35 to 1.55 radians.. The errors are the square root of the diagonal elements of the covariant matrix.

InclusiveAstrophysics::High Energy Astrophysical PhenomenaP TA --> PI+ XD2SIG/DP/DTHETADouble Differential Cross SectionAngular Dependence
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