Search results for "DT"

showing 10 items of 2454 documents

The DNA-binding subunit p140 of replication factor C is upregulated in cycling cells and associates with G 1 phase cell cycle regulatory proteins

1999

The DNA-binding subunit of replication factor C (RFCp140) plays an important role in both DNA replication and DNA repair. The mechanisms regulating activation of RFCp140 thereby controlling replication and cellular proliferation are largely unknown. We analyzed protein expression of RFCp140 during cell cycle progression and investigated the association of RFCp140 with cell cycle regulatory proteins in cell lines of various tissue origin and in primary hematopoietic cells. Western and Northern blot analyses of RFCp140 from synchronized cells showed downregulation of RFCp140 when cells enter a G0-like quiescent state and upregulation of RFCp140 in cycling cells. Translocation from the cytopla…

CytoplasmSaccharomyces cerevisiae ProteinsT-LymphocytesCyclin ACell Cycle ProteinsEukaryotic DNA replicationCell LineMinor Histocompatibility AntigensDNA replication factor CDT1MiceReplication factor CControl of chromosome duplicationDrug DiscoveryAnimalsHumansReplication Protein CGenetics (clinical)Cell NucleusHomeodomain ProteinsbiologyG1 PhaseS-phase-promoting factor3T3 CellsCell cycleMolecular biologyUp-RegulationCell biologyDNA-Binding ProteinsRepressor ProteinsProto-Oncogene Proteins c-bcl-2biology.proteinMolecular MedicineOrigin recognition complexJournal of Molecular Medicine
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High Reynolds number Navier-Stokes solutions and boundary layer separation induced by a rectilinear vortex

2013

Abstract We compute the solutions of Prandtl’s and Navier–Stokes equations for the two dimensional flow induced by a rectilinear vortex interacting with a boundary in the half plane. For this initial datum Prandtl’s equation develops, in a finite time, a separation singularity. We investigate the different stages of unsteady separation for Navier–Stokes solution at different Reynolds numbers Re = 103–105, and we show the presence of a large-scale interaction between the viscous boundary layer and the inviscid outer flow. We also see a subsequent stage, characterized by the presence of a small-scale interaction, which is visible only for moderate-high Re numbers Re = 104–105. We also investi…

D'Alembert's paradoxGeneral Computer SciencePrandtl numberMathematics::Analysis of PDEsFOS: Physical sciencesPhysics::Fluid Dynamicssymbols.namesakeMathematics - Analysis of PDEsHagen–Poiseuille flow from the Navier–Stokes equationsFOS: MathematicsSettore MAT/07 - Fisica MatematicaMathematical PhysicsMathematicsMathematical analysisGeneral EngineeringFluid Dynamics (physics.flu-dyn)Reynolds numberPhysics - Fluid DynamicsMathematical Physics (math-ph)Non-dimensionalization and scaling of the Navier–Stokes equationsBoundary layersymbolsTurbulent Prandtl numberReynolds-averaged Navier–Stokes equationsBoundary layer Unsteady separation Navier Stokes solutions Prandtl’s equation High Reynolds number flows.Analysis of PDEs (math.AP)
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"Table 28" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

2017

Beam helicity dependent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.

D4SIG/DQ**2/DX/DT/DPHIDeeply Virtual Compton ScatteringE- P --> E- GAMMA PBeam helicity dependent cross sectionExclusive
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"Table 36" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

2017

Beam helicity dependent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.

D4SIG/DQ**2/DX/DT/DPHIDeeply Virtual Compton ScatteringE- P --> E- GAMMA PBeam helicity dependent cross sectionExclusive
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"Table 22" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

2017

Beam helicity dependent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.

D4SIG/DQ**2/DX/DT/DPHIDeeply Virtual Compton ScatteringE- P --> E- GAMMA PBeam helicity dependent cross sectionExclusive
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"Table 34" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

2017

Beam helicity dependent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.

D4SIG/DQ**2/DX/DT/DPHIDeeply Virtual Compton ScatteringE- P --> E- GAMMA PBeam helicity dependent cross sectionExclusive
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"Table 6" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

2017

Beam helicity dependent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.

D4SIG/DQ**2/DX/DT/DPHIDeeply Virtual Compton ScatteringE- P --> E- GAMMA PBeam helicity dependent cross sectionExclusive
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"Table 2" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

2017

Beam helicity dependent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.

D4SIG/DQ**2/DX/DT/DPHIDeeply Virtual Compton ScatteringE- P --> E- GAMMA PBeam helicity dependent cross sectionExclusive
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"Table 32" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

2017

Beam helicity dependent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.

D4SIG/DQ**2/DX/DT/DPHIDeeply Virtual Compton ScatteringE- P --> E- GAMMA PBeam helicity dependent cross sectionExclusive
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"Table 16" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

2017

Beam helicity dependent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.

D4SIG/DQ**2/DX/DT/DPHIDeeply Virtual Compton ScatteringE- P --> E- GAMMA PBeam helicity dependent cross sectionExclusive
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