Visual evoked potentials to a diamond pattern can predict accommodation power more accurately than those to a checkerboard pattern. [PDF]
Yamamoto R +3 more
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A Chiral Saddle‐Shaped Nanographene With Two Heptagon‐Embedded [4]Helicenes
We present a novel synthetic strategy toward a chiral saddle‐shaped nanographene (cSNG) via a two‐step oxidation of a prochiral anthracene precursor. The Scholl‐type oxidation first yields a key intermediate with sp3‐defect heptagons, and subsequent oxidative dehydrogenation affords fully conjugated cSNG.
Felix Trautner +11 more
wiley +1 more source
Geometry of the cumulant series in diffusion MRI. [PDF]
Coelho S +4 more
europepmc +1 more source
Cross-site harmonization of diffusion MRI data without matched training subjects. [PDF]
De Luca A +8 more
europepmc +1 more source
Moiré Folded Helical States at the Interfaces of Heterostructures
This manuscript explores a minimal ladder model of a graphene‐topological‐insulator heterostructure where moiré superlattices modulate Rashba spin‐orbit coupling. The study reveals that SOC lifs spin degeneracy, halves spectral periodicity, and induces “helicity fragmentation” across moiré minibands.
Paula Mellado
wiley +1 more source
Spectral decomposition unlocks ascidian morphogenesis. [PDF]
Dokmegang J +4 more
europepmc +1 more source
High-resolution Bayesian Virtual Epileptic Patient using neural field models. [PDF]
Vattikonda AN +6 more
europepmc +1 more source
Attosecond high-harmonic interferometry probes orbital- and band-dependent dipole phase in magnesium oxide. [PDF]
Kuzkova N +6 more
europepmc +1 more source
High-Precision Calibration Technology and Experimental Verification for Dual-Axis Laser Communication Systems. [PDF]
Li W +6 more
europepmc +1 more source
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On the Relation Between Spherical Harmonics and Simplified Spherical Harmonics Methods
Transport Theory and Statistical Physics, 2010The purpose of the paper is, first, to recall the proof that the AN method and, therefore, the SP2N−1 method (of which AN was shown to be a variant) are equivalent to the odd order P2N−1, at least for a particular class of multi-region problems; namely the problems for which the total cross section has the same value for all the regions and the ...
G G M Coppa, V Giusti, B Montagnini
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