0000000000951097

AUTHOR

S. Mandal

showing 12 related works from this author

The Large Hadron–Electron Collider at the HL-LHC

2021

The Large Hadron-Electron Collider (LHeC) is designed to move the field of deep inelastic scattering (DIS) to the energy and intensity frontier of particle physics. Exploiting energy-recovery technology, it collides a novel, intense electron beam with a proton or ion beam from the High-Luminosity Large Hadron Collider (HL-LHC). The accelerator and interaction region are designed for concurrent electron-proton and proton-proton operations. This report represents an update to the LHeC's conceptual design report (CDR), published in 2012. It comprises new results on the parton structure of the proton and heavier nuclei, QCD dynamics, and electroweak and top-quark physics. It is shown how the LH…

energy recoverylepton nucleus: scatteringparton: distribution functionhiukkasfysiikka7. Clean energy01 natural sciencesaccelerator physicsHigh Energy Physics - Phenomenology (hep-ph)HEAVY FLAVOR CONTRIBUTIONSenergy-recovery- linacNuclear Experimentcolliding beams [electron p]deep-inelastic scatteringtop and electroweak physicsnew physicsPhysicsSTRUCTURE-FUNCTION RATIOSMonte Carlo [numerical calculations]buildingsprimary [vertex]High Energy Physics - Phenomenologyelectron p: colliding beamskinematicsNuclear Physics - Theoryfinal state: hadronicp: distribution functionbeyond Standard Modelvertex: primarynumerical calculations: Monte Carlodistribution function [parton]High-lumiLHCSTRUCTURE-FUNCTION F-2(X[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]ion: beam[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]114 Physical sciencesNuclear Theory (nucl-th)deep inelastic scatteringquantum chromodynamicsddc:530010306 general physicsdeep-inelastic scattering; high-lumi LHC; QCD; Higgs; top and electroweak physics; nuclear physics; beyond standard Model; energy-recovery- linac; accelerator physics010308 nuclear & particles physicshigh-lumi LHCresolutionscattering [electron p]structure function [nucleus]sensitivitybeam [electron]energy-recovery-linacHiggsacceptanceNuclear TheoryHIGH-ENERGY FACTORIZATIONdistribution function [p]density [parton]Higgs; High-lumi LHCHigh Energy Physics - Experimentdesign [detector]High Energy Physics - Experiment (hep-ex)electron: linear acceleratorelectron hadron: scatteringCERN LHC Coll: upgrade[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]scattering [electron hadron]FCCelectron: beamNuclear Experiment (nucl-ex)linear accelerator [electron]Nuclear ExperimentlatticesuperconductivityEnergy-recoverylinacBeyond Standard ModeNuclear physics; QCDelectron nucleus: colliding beamsparton: densitycolliding beams [electron nucleus]Particle Physics - ExperimentNUCLEON STRUCTURE FUNCTIONSNuclear and High Energy Physicsscattering [lepton nucleus]beam [ion]FOS: Physical sciencesnucleus: structure functionhadronic [final state]electron p: scatteringTRANSVERSE-MOMENTUM DEPENDENCEnuclear physics0103 physical sciencesNuclear Physics - Experimentstructureupgrade [CERN LHC Coll]detector: designParticle Physics - PhenomenologyDEEP-INELASTIC-SCATTERINGelectroweak interaction3-LOOP SPLITTING FUNCTIONSCLASSICAL RADIATION ZEROScalibrationAccelerators and Storage RingsQCDmagnethigh [current]13. Climate action[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]LHeCPhysics::Accelerator PhysicsJET CROSS-SECTIONSHigh Energy Physics::Experimentcurrent: highJournal of Physics G: Nuclear and Particle Physics
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βdecay of102Y produced in projectile fission of238U

2012

The population of 102Zr following the β decay of 102Y produced in the projectile fission of 238U at the GSI facility in Darmstadt, Germany has been studied. 102Y is known to ß decay into 102Zr via two states, one of high spin and the other low spin. These states preferentially populate different levels in the 102Zr daughter. In this paper the intensities of transitions in 102Zr observed are compared with those from the decay of the low-spin level studied at the TRISTAN facility at Brookhaven National Laboratory and of the high-spin level studied at the JOSEF separator at the Kernforschungsanlage Jülich.

PhysicsHistoryeducation.field_of_studyCluster decayFissionProjectilePopulationBeta decayddc:Computer Science ApplicationsEducationNuclear physicsSubatomic PhysicsHigh Energy Physics::ExperimentAtomic physicsNuclear ExperimentSpin (physics)National laboratoryeducationJournal of Physics: Conference Series
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CCDC 920809: Experimental Crystal Structure Determination

2013

Related Article: S.Mandal, J.Mukherjee, F.Lloret, R.Mukherjee|2012|Inorg.Chem.|51|13148|doi:10.1021/ic3013848

Space GroupCrystallographyCrystal System(mu2-2-(((2-(Dimethylamino)ethyl)(methyl)amino)methyl)-6-(((2-(dimethylamino)ethyl)(methyl)amino)methyl)phenolato)-(mu2-hydroxo)-(perchlorato)-di-copper(ii) perchlorate acetonitrile solvateCrystal StructureCell ParametersExperimental 3D Coordinates
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CCDC 920807: Experimental Crystal Structure Determination

2013

Related Article: S.Mandal, J.Mukherjee, F.Lloret, R.Mukherjee|2012|Inorg.Chem.|51|13148|doi:10.1021/ic3013848

Space GroupCrystallography(mu2-N'-(3-(((2-(dimethylamino)ethyl)amino)methyl)benzyl)-NN-dimethylethane-12-diaminato)-bis((acetonitrile)-(triphenylphosphine))-di-copper diperchlorateCrystal SystemCrystal StructureCell ParametersExperimental 3D Coordinates
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CCDC 920808: Experimental Crystal Structure Determination

2013

Related Article: S.Mandal, J.Mukherjee, F.Lloret, R.Mukherjee|2012|Inorg.Chem.|51|13148|doi:10.1021/ic3013848

Space GroupCrystallographyCrystal SystemCrystal Structure(mu2-2-(((2-(dimethylamino)ethyl)amino)methyl)-6-(((2-(dimethylamino)ethyl)amino)methyl)phenolato)-(mu2-hydroxo)-bis(acetonitrile)-di-copper(ii) diperchlorateCell ParametersExperimental 3D Coordinates
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CCDC 750006: Experimental Crystal Structure Determination

2011

Related Article: S.Banerjee, M.Nandy, S.Sen, S.Mandal, G.M.Rosair, A.M.Z.Slawin, C.J.G.Garcia, J.M.Clemente-Juan, E.Zangrando, N.Guidolin, S.Mitra|2011|Dalton Trans.|40|1652|doi:10.1039/c0dt00923g

Space GroupCrystallographybis(mu~3~-Methanolato)-bis(mu~3~-22'-((2-oxidopropane-13-diyl)bis(nitriloeth-1-yl-1-ylidene))diphenolato-NN'OOO'O'O'')-diaqua-(nitrato-OO')-di-cobalt(ii)-di-cobalt(iii) nitrate dihydrateCrystal SystemCrystal StructureCell ParametersExperimental 3D Coordinates
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CCDC 751685: Experimental Crystal Structure Determination

2010

Related Article: S.Mandal, V.Balamurugan, F.Lloret, R.Mukherjee|2009|Inorg.Chem.|48|7544|doi:10.1021/ic8018937

Space GroupCrystallographyCrystal SystemCrystal StructureCell Parametersbis(mu~2~-Acetato)-(mu~2~-4-methyl-2-((3-(pyridin-2-yl)-1H-pyrazol-1-yl)methyl)-6-((3-(pyridin-2-yl)-1H-pyrazol-1-yl)methyl)phenolato)-aqua-methanol-di-nickel tetraphenylborate methanol solvate monohydrateExperimental 3D Coordinates
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CCDC 751684: Experimental Crystal Structure Determination

2010

Related Article: S.Mandal, V.Balamurugan, F.Lloret, R.Mukherjee|2009|Inorg.Chem.|48|7544|doi:10.1021/ic8018937

Space GroupCrystallographyCrystal SystemCrystal StructureCell Parameters(mu~2~-26-bis[N-methyl-N-(2-pyridylethyl)amino]-4-methylphenolato)-bis(acetato)-diaqua-di-nickel(ii) hexafluorophosphate methanol solvate trihydrateExperimental 3D Coordinates
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CCDC 658242: Experimental Crystal Structure Determination

2009

Related Article: S.Mandal, F.Lloret, R.Mukherjee|2009|Inorg.Chim.Acta|362|27|doi:10.1016/j.ica.2008.02.072

Space GroupCrystallographyCrystal SystemCrystal StructureCell Parameterscatena-((mu~2~-13-bis(N-(2-(2-pyridyl)ethyl)-N-(2-pyridylmethyl)amino)-m-xylene)-bis(mu~2~-chloro)-di-copper(ii) diperchlorate tetrahydrofuran acetonitrile solvate)Experimental 3D Coordinates
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CCDC 687036: Experimental Crystal Structure Determination

2011

Related Article: S.Banerjee, M.Nandy, S.Sen, S.Mandal, G.M.Rosair, A.M.Z.Slawin, C.J.G.Garcia, J.M.Clemente-Juan, E.Zangrando, N.Guidolin, S.Mitra|2011|Dalton Trans.|40|1652|doi:10.1039/c0dt00923g

(mu~2~-22'-((2-Oxidopropane-13-diyl)bis(nitriloeth-1-yl-1-ylidene))diphenolato-NN'OOO'O'')-aqua-(22'-((2-oxidopropane-13-diyl)bis(nitriloeth-1-yl-1-ylidene))diphenolato-NN'OO'O'')-di-cobalt(iii)Space GroupCrystallographyCrystal SystemCrystal StructureCell ParametersExperimental 3D Coordinates
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CCDC 720540: Experimental Crystal Structure Determination

2011

Related Article: S.Banerjee, M.Nandy, S.Sen, S.Mandal, G.M.Rosair, A.M.Z.Slawin, C.J.G.Garcia, J.M.Clemente-Juan, E.Zangrando, N.Guidolin, S.Mitra|2011|Dalton Trans.|40|1652|doi:10.1039/c0dt00923g

bis(mu~3~-Methanolato)-bis(mu~3~-22'-((2-oxidopropane-13-diyl)bis(nitriloeth-1-yl-1-ylidene))diphenolato-NN'OOO'O'O'')-diaqua-tetra-nickel(ii) dihydrateSpace GroupCrystallographyCrystal SystemCrystal StructureCell ParametersExperimental 3D Coordinates
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CCDC 658243: Experimental Crystal Structure Determination

2009

Related Article: S.Mandal, F.Lloret, R.Mukherjee|2009|Inorg.Chim.Acta|362|27|doi:10.1016/j.ica.2008.02.072

Space GroupCrystallographyCrystal SystemCrystal StructureCell Parameterscatena-((mu~2~-NN'-(13-Phenylenebis(methylene))bis(N-(1H-pyrazol-1-ylmethyl)-2-(2-pyridinyl)ethanamino))-bis(mu~2~-chloro)-di-copper(ii) diperchlorate acetonitrile solvate)Experimental 3D Coordinates
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