Publication data of Zhang, Xilin: Link to Inspire

Created with Highcharts 9.0.1CitationsCitationsw/o self-citaionself-citaion20102012201420162018202020222024025050075010001250
Created with Highcharts 9.0.1Publicationspublications per yearPublicationsPublications per yearCumulative publications20102012201420162018202020222024010203040500246810
Created with Highcharts 9.0.1h-indexh-indexh-indexh-index w/o self-citaion201020122014201620182020202220240510152025
Created with Highcharts 9.0.1CitationsBreakdown of Most Cited PapersrestHard probe of geometry and fluctuations in heavy ion collisions at sNN=0.2 , 2.76, and 5.5 TeVHard probe of geometry and fluctuations in heavy ion collisions at sNN=0.2 ,…Coherent Neutrinoproduction of Photons and Pions in a Chiral Effective Field Theory for NucleiCoherent Neutrinoproduction of Photons and Pions in a Chiral Effective Field …$S$-factor and scattering-parameter extractions from ${}^{3}mathrm{He} +{}^{4}mathrm{He} ightarrow {}^{7}mathrm{Be} + gamma$$S$-factor and scattering-parameter extractions from ${}^{3}mathrm{He…Event-by-event azimuthal anisotropy of jet quenching in relativistic heavy ion collisionsEvent-by-event azimuthal anisotropy of jet quenching in relativistic heavy ion…Incoherent Neutrinoproduction of Photons and Pions in a Chiral Effective Field Theory for NucleiIncoherent Neutrinoproduction of Photons and Pions in a Chiral Effective Fiel…Jet Quenching and Its Azimuthal Anisotropy in AA and possibly High Multiplicity pA and dA CollisionsJet Quenching and Its Azimuthal Anisotropy in AA and possibly High Multiplici…Fast emulation of quantum three-body scatteringCan a protophobic vector boson explain the ATOMKI anomaly?Marrying ab initio calculations and Halo-EFT: the case of ${}^7{ m Li} + n ightarrow {}^8{ m Li} + gamma$Marrying ab initio calculations and Halo-EFT: the case of ${}^7{ m Li} + n …Can neutrino-induced photon production explain the low energy excess in MiniBooNE?Can neutrino-induced photon production explain the low energy excess in Mi…Fast & accurate emulation of two-body scattering observables without wave functionsFast & accurate emulation of two-body scattering observables without wave f…Combining ab initio calculations and low-energy effective field theory for halo nuclear systems: The case of ${}^7Be+p o {}^8B+gamma$Combining ab initio calculations and low-energy effective field theory for halo…Model reduction methods for nuclear emulatorsNeutrinoproduction of Photons and Pions From Nucleons in a Chiral Effective Field Theory for NucleiNeutrinoproduction of Photons and Pions From Nucleons in a Chiral Effective …Halo effective field theory constrains the solar $^7$Be + p → $^8$B + γ rateEfficient emulators for scattering using eigenvector continuationCan nuclear physics explain the anomaly observed in the internal pair production in the Beryllium-8 nucleus?Can nuclear physics explain the anomaly observed in the internal pair produ…Charge-dependent azimuthal correlations from AuAu to UU collisionsAzimuthally fluctuating magnetic field and its impacts on observables in heavy-ion collisionsAzimuthally fluctuating magnetic field and its impacts on observables in hea…20102012201420162018202020222024025050075010001250
Created with Highcharts 9.0.1Fraction [%]Breakdown of Most Cited Papers (Fraction)Hard probe of geometry and fluctuations in heavy ion collisions at sNN=0.2 , 2.76, and 5.5 TeVHard probe of geometry and fluctuations in heavy ion collisions at sNN=0.2 ,…Coherent Neutrinoproduction of Photons and Pions in a Chiral Effective Field Theory for NucleiCoherent Neutrinoproduction of Photons and Pions in a Chiral Effective Field …$S$-factor and scattering-parameter extractions from ${}^{3}mathrm{He} +{}^{4}mathrm{He} ightarrow {}^{7}mathrm{Be} + gamma$$S$-factor and scattering-parameter extractions from ${}^{3}mathrm{He…Event-by-event azimuthal anisotropy of jet quenching in relativistic heavy ion collisionsEvent-by-event azimuthal anisotropy of jet quenching in relativistic heavy ion…Incoherent Neutrinoproduction of Photons and Pions in a Chiral Effective Field Theory for NucleiIncoherent Neutrinoproduction of Photons and Pions in a Chiral Effective Fiel…Jet Quenching and Its Azimuthal Anisotropy in AA and possibly High Multiplicity pA and dA CollisionsJet Quenching and Its Azimuthal Anisotropy in AA and possibly High Multiplici…Fast emulation of quantum three-body scatteringCan a protophobic vector boson explain the ATOMKI anomaly?Marrying ab initio calculations and Halo-EFT: the case of ${}^7{ m Li} + n ightarrow {}^8{ m Li} + gamma$Marrying ab initio calculations and Halo-EFT: the case of ${}^7{ m Li} + n …Can neutrino-induced photon production explain the low energy excess in MiniBooNE?Can neutrino-induced photon production explain the low energy excess in Mi…Fast & accurate emulation of two-body scattering observables without wave functionsFast & accurate emulation of two-body scattering observables without wave f…Combining ab initio calculations and low-energy effective field theory for halo nuclear systems: The case of ${}^7Be+p o {}^8B+gamma$Combining ab initio calculations and low-energy effective field theory for halo…Model reduction methods for nuclear emulatorsNeutrinoproduction of Photons and Pions From Nucleons in a Chiral Effective Field Theory for NucleiNeutrinoproduction of Photons and Pions From Nucleons in a Chiral Effective …Halo effective field theory constrains the solar $^7$Be + p → $^8$B + γ rateEfficient emulators for scattering using eigenvector continuationCan nuclear physics explain the anomaly observed in the internal pair production in the Beryllium-8 nucleus?Can nuclear physics explain the anomaly observed in the internal pair produ…Charge-dependent azimuthal correlations from AuAu to UU collisionsAzimuthally fluctuating magnetic field and its impacts on observables in heavy-ion collisionsAzimuthally fluctuating magnetic field and its impacts on observables in hea…201020122014201620182020202220240255075100
Created with Highcharts 9.0.1Citations/1 YearCitations/PeriodCitations / 1 YearMoving average20102012201420162018202020222024050100150200250