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1. Impact of physical parameterizations on wind simulation with WRF V3.9.1.1 under stable conditions at planetary boundary layer gray-zone resolution: a case study over the coastal regions of North China

2. Experimentally Accessible Scheme for a Fractional Chern Insulator in Rydberg Atoms

3. First co-infection case of melioidosis and Japanese encephalitis in China

7. Gene expression profile in white alpaca (Vicugna pacos) skin

35. Multichannel room response equalization with a broadened control region using a linearly constrained approach and sensor interpolation

38. Acoustic modal analysis of room responses from the perspective of state-space balanced realization with application to field interpolation

40. Measurement of beauty production via non-prompt charm hadrons in p–Pb collisions at s NN $$ \sqrt{s_{\textrm{NN}}} $$ = 5.02 TeV

41. Measurement of the B s 0 → J / ψK S 0 $$ {\textrm{B}}_{\textrm{s}}^0\to \textrm{J}/{\uppsi \textrm{K}}_{\textrm{S}}^0 $$ effective lifetime from proton-proton collisions at s $$ \sqrt{s} $$ = 13 TeV

42. Measurement of differential ZZ + jets production cross sections in pp collisions at s $$ \sqrt{s} $$ = 13 TeV

43. Measurement of beauty-quark production in pp collisions at s $$ \sqrt{s} $$ = 13 TeV via non-prompt D mesons

44. Observation of the $${{{\Lambda }} _{\text {b}}^{{0}}} \rightarrow {{\text {J}/\uppsi }} {{{\Xi }} ^{{-}}} {{\text {K}} ^{{+}}} $$ Λ b 0 → J / ψ Ξ - K + decay

45. Multiplicity dependence of charged-particle intra-jet properties in pp collisions at $$\sqrt{{{\varvec{s}}}}$$ s = 13 TeV

46. Search for Higgs boson pair production with one associated vector boson in proton-proton collisions at s $$ \sqrt{s} $$ = 13 TeV

48. Short-Range Structural Connections Are More Severely Damaged in Early-Stage MS

49. Theoretical investigations on the superhydrophobicity of intrinsic hydrophilic surfaces with overhang microstructures

50. Global feedforward active noise control using a linearly constrained loudspeaker beamformer and a sensor interpolation approach

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