_id,title
14224,Clustering meets implicit generative models
14284,Structure and mechanism of the two-component α-helical pore-forming toxin YaxAB
143,Efficient algorithms for asymptotic bounds on termination time in VASS
14306,Genetically encoding the spatial arrangement of DNA and proteins in self-assembling nanostructures
9053,Diffusiophoretic design of self-spinning microgears from colloidal microswimmers
9062,Targeted assembly and synchronization of self-spinning microgears
913,PATELLINS are regulators of auxin mediated PIN1 relocation and plant development in Arabidopsis thaliana
9134,Internal tide dissipation at topography: Triadic resonant instability equatorward and evanescent waves poleward of the critical latitude
9135,Acceleration of tropical cyclogenesis by self-aggregation feedbacks
9136,Scaling precipitation extremes with temperature in the Mediterranean: Past climate assessment and projection in anthropogenic scenarios
9229,Diffraction-unlimited optical imaging for synaptic physiology
9471,FACT complex is required for DNA demethylation at heterochromatin during reproduction in Arabidopsis
95,Collisional charging of individual submillimeter particles: Using ultrasonic levitation to initiate and track charge transfer
9565,Counting Hamilton cycles in sparse random directed graphs
9567,"The random k‐matching‐free process"
9568,Intercalates and discrepancy in random Latin squares
9587,Non-trivially intersecting multi-part families
9659,Communication: Computing the Tolman length for solid-liquid interfaces
9665,Hydrogen diffusion and trapping in α-iron: The role of quantum and anharmonic fluctuations
9668,Theoretical prediction of the homogeneous ice nucleation rate: Disentangling thermodynamics and kinetics