_id,doi,title
13266,10.1111/nph.19123,Tale of cAMP as a second messenger in auxin signaling and beyond
13267,10.1038/s41592-023-01936-6,Dense 4D nanoscale reconstruction of living brain tissue
13268,10.4310/mrl.2023.v30.n1.a6,On type II degenerations of hyperkähler manifolds
13269,10.1109/TIT.2023.3292219,Codes for the Z-channel
13270,10.1007/s00454-023-00500-5,Iterated medial triangle subdivision in surfaces of constant curvature
13271,10.1007/s00023-023-01345-7,Some convexity and monotonicity results of trace functionals
13274,10.1103/physrevlett.131.034002,Direct path from turbulence to time-periodic solutions
13275,10.21468/scipostphyscodeb.12-r1.0,Codebase release 1.0 for FermiFCI
13276,10.21468/scipostphyscodeb.12,A modular implementation of an effective interaction approach for harmonically trapped fermions in 1D
13277,10.21468/scipostphyscore.6.2.029,Stochastic representation of the quantum quartic oscillator
13278,10.21468/scipostphys.14.1.006,Magnetic impurity in a one-dimensional few-fermion system
13286,10.15479/at:ista:13286,Mesoscopic phenomena in hybrid semiconductor-superconductor nanodevices : From full-shell nanowires to two-dimensional hole gas in germanium
13292,10.4230/LIPIcs.ICALP.2023.129,Regular methods for operator precedence languages
13310,10.1007/978-3-031-37703-7_17,Monitoring algorithmic fairness
13312,10.48550/arXiv.2306.07109,Radio frequency driven superconducting diode and parity conserving  Cooper pair transport in a two-dimensional germanium hole gas
13314,10.1038/s41567-023-02218-w,Chiral and nematic phases of flexible active filaments
13315,10.1073/pnas.2302028120,Fundamental limits in structured principal component analysis and how to reach them
13316,10.7554/eLife.84850,The yeast endocytic early/sorting compartment exists as an independent sub-compartment within the trans-Golgi network
13317,10.1007/s10955-023-03132-4,Eigenstate thermalisation hypothesis for translation invariant spin systems
13318,10.1007/s00208-023-02680-0,"Noncommutative Bohnenblust–Hille inequalities"