Matches in SemOpenAlex for { <https://semopenalex.org/work/W2595018192> ?p ?o ?g. }
Showing items 1 to 81 of
81
with 100 items per page.
- W2595018192 endingPage "1232" @default.
- W2595018192 startingPage "1226" @default.
- W2595018192 abstract "With the experimental examination in the past few decades, the Standard Model (SM), which describes the building blocks of matter and the fundamental forces in the universe, is considered to be the most successful theoretical model to describe the subatomic world. In particular, after the discovery of Higgs particle in 2012 at Large Hadron Collider (LHC), the success of SM reaches to an unprecedented level. However, it does leave a lot of phenomena unexplained questions, such as, what are the dark matter and dark energy? what happened to the anti-matter matter asymmetric in the world? why are there three generations of quarks and lepton with such a different mass scale? and so on. At present, it is believed that there exists a more general theory hidden deeply in the subatomic world, which includes the new physics, and can solve the all unexplained questions, and the SM is its appromiximation in the current reached energy region experimentally. On the other hand, as one of two parts of SM, Quantum chromodynamics (QCD) theory, which is theory of strong interactions, a fundamental force describing the interactions between quarks and gluons, and have been tested precisely in the high energy range, but there is still some fundamental questions unsolved in row energy region. Therefore, it is urgent for us to have the experiments beyond current level to explore and reveal the mysteries of the subatomic world. At present, the studies of particle physics based on accelerator is one of most powerful approach to investigate the subatomic world, and can be classed into two frontiers, i.e. the high energy frontiers and the high intensitive fronitiers. A super tau-charm factory, which is expected to have luminosity of 0.5 ´ 1035–1.0 ´ 1035 cm - 2 s - 1 and with center of mass energy at 2–7 GeV, is one of typical high intersitive frontiers experiment. It can produce all there generation leptons and first and secondary generation quarks and have several unique features, e.g., running on the energy at the transition between the perturbative and non-perturbative QCD, producing rich resonances, charmonium and charmed mesons, having threshold characteristics which provides clean environment for the signals, etc. The super tau-charm factory is regarded as an ideal platform to explore the hadronic physics and search for the new physics beyond the SM. In this letter, we present the key science questions and physics topics are desired on a super tau-charm factory, and discuss the feasibility and necessity to build a new generation high intensive Electron Position Accelerator Facility (HIEPA) at 2–7 GeV in China. The current international and internal situations for particle physics progress, the key technologies in both accelaerator and detector, and the driving force for science and technology to build the tau-charm factory in China are also illustrated. We conclude that HIEPA is an excellent option from all aspects for the future accelerator programs in China based on its current scale of particle physics community and the expertise reserve, and call for the start and support from the government of R&D for this project." @default.
- W2595018192 created "2017-03-23" @default.
- W2595018192 creator A5001000231 @default.
- W2595018192 creator A5001767533 @default.
- W2595018192 creator A5005449631 @default.
- W2595018192 creator A5012341807 @default.
- W2595018192 creator A5016816712 @default.
- W2595018192 creator A5022598327 @default.
- W2595018192 creator A5022734422 @default.
- W2595018192 creator A5026144834 @default.
- W2595018192 creator A5037040891 @default.
- W2595018192 creator A5047886846 @default.
- W2595018192 creator A5055319187 @default.
- W2595018192 creator A5058566561 @default.
- W2595018192 creator A5061132254 @default.
- W2595018192 creator A5077178417 @default.
- W2595018192 creator A5080010006 @default.
- W2595018192 creator A5083902118 @default.
- W2595018192 date "2017-03-07" @default.
- W2595018192 modified "2023-10-13" @default.
- W2595018192 title "Physics on the high intensive electron position accelerator at 2–7 GeV" @default.
- W2595018192 doi "https://doi.org/10.1360/n972016-00398" @default.
- W2595018192 hasPublicationYear "2017" @default.
- W2595018192 type Work @default.
- W2595018192 sameAs 2595018192 @default.
- W2595018192 citedByCount "3" @default.
- W2595018192 countsByYear W25950181922021 @default.
- W2595018192 countsByYear W25950181922023 @default.
- W2595018192 crossrefType "journal-article" @default.
- W2595018192 hasAuthorship W2595018192A5001000231 @default.
- W2595018192 hasAuthorship W2595018192A5001767533 @default.
- W2595018192 hasAuthorship W2595018192A5005449631 @default.
- W2595018192 hasAuthorship W2595018192A5012341807 @default.
- W2595018192 hasAuthorship W2595018192A5016816712 @default.
- W2595018192 hasAuthorship W2595018192A5022598327 @default.
- W2595018192 hasAuthorship W2595018192A5022734422 @default.
- W2595018192 hasAuthorship W2595018192A5026144834 @default.
- W2595018192 hasAuthorship W2595018192A5037040891 @default.
- W2595018192 hasAuthorship W2595018192A5047886846 @default.
- W2595018192 hasAuthorship W2595018192A5055319187 @default.
- W2595018192 hasAuthorship W2595018192A5058566561 @default.
- W2595018192 hasAuthorship W2595018192A5061132254 @default.
- W2595018192 hasAuthorship W2595018192A5077178417 @default.
- W2595018192 hasAuthorship W2595018192A5080010006 @default.
- W2595018192 hasAuthorship W2595018192A5083902118 @default.
- W2595018192 hasBestOaLocation W25950181921 @default.
- W2595018192 hasConcept C10138342 @default.
- W2595018192 hasConcept C109214941 @default.
- W2595018192 hasConcept C121332964 @default.
- W2595018192 hasConcept C144133560 @default.
- W2595018192 hasConcept C147120987 @default.
- W2595018192 hasConcept C185544564 @default.
- W2595018192 hasConcept C198082294 @default.
- W2595018192 hasConceptScore W2595018192C10138342 @default.
- W2595018192 hasConceptScore W2595018192C109214941 @default.
- W2595018192 hasConceptScore W2595018192C121332964 @default.
- W2595018192 hasConceptScore W2595018192C144133560 @default.
- W2595018192 hasConceptScore W2595018192C147120987 @default.
- W2595018192 hasConceptScore W2595018192C185544564 @default.
- W2595018192 hasConceptScore W2595018192C198082294 @default.
- W2595018192 hasIssue "12" @default.
- W2595018192 hasLocation W25950181921 @default.
- W2595018192 hasOpenAccess W2595018192 @default.
- W2595018192 hasPrimaryLocation W25950181921 @default.
- W2595018192 hasRelatedWork W1422493571 @default.
- W2595018192 hasRelatedWork W2008720822 @default.
- W2595018192 hasRelatedWork W2022301573 @default.
- W2595018192 hasRelatedWork W2035773682 @default.
- W2595018192 hasRelatedWork W2058525002 @default.
- W2595018192 hasRelatedWork W2064957847 @default.
- W2595018192 hasRelatedWork W2082691513 @default.
- W2595018192 hasRelatedWork W2084289794 @default.
- W2595018192 hasRelatedWork W2399261606 @default.
- W2595018192 hasRelatedWork W3106441232 @default.
- W2595018192 hasVolume "62" @default.
- W2595018192 isParatext "false" @default.
- W2595018192 isRetracted "false" @default.
- W2595018192 magId "2595018192" @default.
- W2595018192 workType "article" @default.