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A Phylogenetic Approach to Delimitate Species in a Probabilistic Way. [PDF]
Hua X, Moritz C.
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Development of a Microsurgical Simulator for Laryngeal Surgery: A Novel Training Device. [PDF]
Wen Y, Deng J, Lei W.
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Scaling Excellence: How Kaiser Permanente's Nurse Scholars Academy Transformed Nursing Workforce Strategy. [PDF]
Fuller RM, Kielty-Swinford M.
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3DLF-Scan dataset: Multi-sensor 3D light-field and structured-light scans of 3D-printed Stanford figures. [PDF]
Vodianyk B, Popov A, Nava-Baro E.
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Interactive 3D Model Completion
9th Biennial Conference of the Australian Pattern Recognition Society on Digital Image Computing Techniques and Applications (DICTA 2007), 2007A common problem when using automated structure from motion techniques is that the object to be modelled can only be partially reconstructed from the video. This can occur because not all of the object is visible in the video, or because of featureless or ambiguous regions on the object's surface.
van den Hengel, A +4 more
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Nearly Model Complete Theories
Mathematical Logic Quarterly, 1999AbstractA theory T of a language L is 1‐model complete (nearly model complete) iff for every formula ρ of L there is a formula ϕ (χ) of L which is a ∀∃‐formula (a Boolean combination of universal formulas) such that T ⊨ ∀x[ϕ↔θ]. The main results of the paper give characterizations of nearly model complete theories and of 1‐model complete theories. As a
Kueker, David W., Turnquist, Brian P.
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COUNTABLE MODELS OF COMPLETE ORDERED THEORIES
Доклады Российской академии наук. Математика, информатика, процессы управления, 2023The article consists of observations regarding complete theories of countable signatures and their countable models. We provide a construction of a countable linearly ordered theory which has the same number of countable non-isomorphic models as the given countable, not necessarily linearly ordered, theory.
Zambarnaya, T. S., Baizhanov, B. S.
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Completely ununified standard model
Physical Review D, 1990A model of electroweak interactions is presented in which quarks transform under the quark-matter electroweak symmetry {ital G}{sup {ital q}}=SU(2){sub {ital L}}{sup {ital q}}{times}U(1){sub {ital Y}}{sup {ital q}} and leptons transform under the leptonic-matter electroweak symmetry {ital G}{sup {ital l}}=SU(2){sub {ital L}}{sup {ital l}}{times}U(1 ...
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