_id,doi,title
10652,10.1103/PhysRevResearch.4.013023,Constraints on probing quantum coherence to infer gravitational entanglement
10653,10.1029/2021GL095184,Shear-convection interactions and orientation of tropical squall lines
10654,10.1103/PhysRevLett.128.014502,Phase transition to turbulence in spatially extended shear flows
11808,10.4230/LIPIcs.SAND.2022.1,Recent advances in fully dynamic graph algorithms
11812,10.4230/LIPIcs.SAND.2022.18,Fully dynamic four-vertex subgraph counting
11839,10.1007/978-3-031-19803-8_21,Almost-orthogonal layers for efficient general-purpose Lipschitz networks
11841,10.1073/pnas.2109718119,Adsorption free energy predicts amyloid protein nucleation rates
11842,10.1007/s00021-022-00722-2,"Weak-strong uniqueness for the Navier–Stokes equation for two fluids with ninety degree contact angle and same viscosities"
11843,10.7554/eLife.78995,Type 1 piliated uropathogenic Escherichia coli hijack the host immune response by binding to CD14
11844,10.1145/3519270.3538435,Near-optimal leader election in population protocols on graphs
11858,10.1007/s00028-022-00786-7,Nonlinear parabolic stochastic evolution equations in critical spaces part II
11879,10.15479/at:ista:11879,Modulation of auxin transport via ZF proteins adjust plant response to high ambient temperature
11916,10.1007/s43036-022-00199-w,Kac regularity and domination of quadratic forms
11917,10.1007/s10955-022-02940-4,Large deviation estimates for weakly interacting bosons
11918,10.1137/1.9781611977073.23,The complexity of average-case dynamic subgraph counting
11930,10.1137/1.9781611977042.2,Practical fully dynamic minimum cut algorithms
11932,10.15479/at:ista:11932,"On the encoding, transfer, and consolidation of spatial memories"
11937,10.1038/s41467-022-32374-1,Thermodynamics of high-pressure ice phases explored with atomistic simulations
11938,10.7155/jgaa.00591,On compatible matchings
11943,10.1101/2022.03.16.484431,Saturated reconstruction of living brain tissue