_id,doi,title
834,10.1103/PhysRevB.96.104201,Thouless energy and multifractality across the many-body localization transition
835,10.1038/ncomms15990,Regulation of Drosophila hematopoietic sites by Activin-β from active sensory neurons
836,10.1007/978-3-319-56932-1_8,Finding eigenvalues of self-maps with the Kronecker canonical form
837,10.15479/AT:ISTA:th_858,Reactivation of the hippocampal cognitive map in goal-directed spatial tasks
838,10.15479/AT:ISTA:th_828,(The exact security of) Message authentication codes
839,10.15479/AT:ISTA:th_855,Brittle fracture simulation with boundary elements for computer graphics
84,10.1201/9781315119601,Computational topology for structural molecular biology
840,10.1021/acs.nanolett.7b02627,Fast hole tunneling times in germanium hut wires probed by single-shot reflectometry
8423,10.1215/00127094-2017-0038,On the marked length spectrum of generic strictly convex billiard tables
8427,10.4007/annals.2017.186.1.7,Dynamical spectral rigidity among Z2-symmetric strictly convex domains close to a circle
8444,10.1016/j.bpj.2017.09.019,Mitochondrial ADP/ATP carrier in dodecylphosphocholine binds cardiolipins with non-native affinity
8445,10.1038/s41467-017-00165-8,Slow conformational exchange and overall rocking motion in ubiquitin protein crystals
8446,10.1002/cphc.201700572,"Solid‐state NMR H–N–(C)–H and H–N–C–C 3D/4D correlation experiments for resonance assignment of large proteins"
8447,10.1016/j.ssnmr.2017.04.002,"Protein conformational dynamics studied by 15N and 1HR1ρ relaxation dispersion: Application to wild-type and G53A ubiquitin crystals"
8448,10.1016/j.jmr.2017.05.016,Optimized fast mixing device for real-time NMR applications
8449,10.1093/nar/gkx044,RNA binding and chaperone activity of the E.coli cold-shock protein CspA
8450,10.1007/978-1-4939-7151-0_6,Methyl-specific isotope labeling strategies for NMR studies of membrane proteins
8451,10.1002/anie.201610441,Proton-detected solid-state NMR spectroscopy of a Zinc diffusion facilitator protein in native nanodiscs
169,10.1093/imrn/rnx116,Twisted Linnik implies optimal covering exponent for S3
172,10.1093/imrn/rnx252,Strong approximation and a conjecture of Harpaz and Wittenberg