Publication data of Wang, Xing: Link to Inspire

Created with Highcharts 9.0.1CitationsCitationsw/o self-citaionself-citaion20162017201820192020202120222023202420250200400600800
Created with Highcharts 9.0.1Publicationspublications per yearPublicationsPublications per yearCumulative publications20162018202020222024061218243001.534.567.5
Created with Highcharts 9.0.1h-indexh-indexh-indexh-index w/o self-citaion201620172018201920202021202220232024202505101520
Created with Highcharts 9.0.1CitationsBreakdown of Most Cited PapersrestRenormalization of the next-to-leading-power γγ → h and gg → h soft quark functionsRenormalization of the next-to-leading-power γγ → h and gg → h soft quark f…Invariant-mass distribution of top-quark pairs and top-quark mass determinationInvariant-mass distribution of top-quark pairs and top-quark mass determina…Factorization and Sudakov resummation in leptonic radiative B decay — a reappraisalFactorization and Sudakov resummation in leptonic radiative B decay — a re…A Calabi-Yau-to-curve correspondence for Feynman integralsε-factorized differential equations for two-loop non-planar triangle Feynman integrals with elliptic curvesε-factorized differential equations for two-loop non-planar triangle Feynman i…Radiative quark jet function with an external gluonTop quark pair production at complete NLO accuracy with NNLO+NNLL′ corrections in QCDTop quark pair production at complete NLO accuracy with NNLO+NNLL′ corr…Factorization at next-to-leading power and endpoint divergences in gg → h productionFactorization at next-to-leading power and endpoint divergences in gg → h p…One bump or two peaks: The 750 GeV diphoton excess and dark matter with a complex mediatorOne bump or two peaks: The 750 GeV diphoton excess and dark matter with…Top quark pair production near threshold: single/double distributions and mass determinationTop quark pair production near threshold: single/double distributions and ma…The three-loop equal-mass banana integral in ε-factorised form with meromorphic modular formsThe three-loop equal-mass banana integral in ε-factorised form with meromor…Renormalization and Scale Evolution of the Soft-Quark Soft FunctionTaming Calabi-Yau Feynman Integrals: The Four-Loop Equal-Mass Banana IntegralTaming Calabi-Yau Feynman Integrals: The Four-Loop Equal-Mass Banana Inte…Bananas of equal mass: any loop, any order in the dimensional regularisation parameterBananas of equal mass: any loop, any order in the dimensional regularisation…Resummation for (boosted) top-quark pair production at NNLO+NNLL' in QCDFactorization at subleading power and endpoint divergences in $h ogammagamma$ decay. Part II. Renormalization and scale evolutionFactorization at subleading power and endpoint divergences in $h ogammag…Resummed differential cross sections for top-quark pairs at the LHCFactorization at subleading power, Sudakov resummation, and endpoint divergences in soft-collinear effective theoryFactorization at subleading power, Sudakov resummation, and endpoint dive…Transverse Parton Distribution and Fragmentation Functions at NNLO: the Quark CaseTransverse Parton Distribution and Fragmentation Functions at NNLO: the Qu…20162017201820192020202120222023202420250200400600800
Created with Highcharts 9.0.1Fraction [%]Breakdown of Most Cited Papers (Fraction)Renormalization of the next-to-leading-power γγ → h and gg → h soft quark functionsRenormalization of the next-to-leading-power γγ → h and gg → h soft quark f…Invariant-mass distribution of top-quark pairs and top-quark mass determinationInvariant-mass distribution of top-quark pairs and top-quark mass determina…Factorization and Sudakov resummation in leptonic radiative B decay — a reappraisalFactorization and Sudakov resummation in leptonic radiative B decay — a re…A Calabi-Yau-to-curve correspondence for Feynman integralsε-factorized differential equations for two-loop non-planar triangle Feynman integrals with elliptic curvesε-factorized differential equations for two-loop non-planar triangle Feynman i…Radiative quark jet function with an external gluonTop quark pair production at complete NLO accuracy with NNLO+NNLL′ corrections in QCDTop quark pair production at complete NLO accuracy with NNLO+NNLL′ corr…Factorization at next-to-leading power and endpoint divergences in gg → h productionFactorization at next-to-leading power and endpoint divergences in gg → h p…One bump or two peaks: The 750 GeV diphoton excess and dark matter with a complex mediatorOne bump or two peaks: The 750 GeV diphoton excess and dark matter with…Top quark pair production near threshold: single/double distributions and mass determinationTop quark pair production near threshold: single/double distributions and ma…The three-loop equal-mass banana integral in ε-factorised form with meromorphic modular formsThe three-loop equal-mass banana integral in ε-factorised form with meromor…Renormalization and Scale Evolution of the Soft-Quark Soft FunctionTaming Calabi-Yau Feynman Integrals: The Four-Loop Equal-Mass Banana IntegralTaming Calabi-Yau Feynman Integrals: The Four-Loop Equal-Mass Banana Inte…Bananas of equal mass: any loop, any order in the dimensional regularisation parameterBananas of equal mass: any loop, any order in the dimensional regularisation…Resummation for (boosted) top-quark pair production at NNLO+NNLL' in QCDFactorization at subleading power and endpoint divergences in $h ogammagamma$ decay. Part II. Renormalization and scale evolutionFactorization at subleading power and endpoint divergences in $h ogammag…Resummed differential cross sections for top-quark pairs at the LHCFactorization at subleading power, Sudakov resummation, and endpoint divergences in soft-collinear effective theoryFactorization at subleading power, Sudakov resummation, and endpoint dive…Transverse Parton Distribution and Fragmentation Functions at NNLO: the Quark CaseTransverse Parton Distribution and Fragmentation Functions at NNLO: the Qu…20162017201820192020202120222023202420250255075100
Created with Highcharts 9.0.1Citations/1 YearCitations/PeriodCitations / 1 YearMoving average2016201720182019202020212022202320242025050100150200250300