000843949 001__ 843949 000843949 005__ 20210129232737.0 000843949 0247_ $$2doi$$a10.1088/1367-2630/aa649e 000843949 0247_ $$2Handle$$a2128/17495 000843949 0247_ $$2WOS$$aWOS:000398085100002 000843949 0247_ $$2altmetric$$aaltmetric:18193369 000843949 037__ $$aFZJ-2018-01472 000843949 082__ $$a530 000843949 1001_ $$0P:(DE-HGF)0$$aWang, L. M.$$b0$$eCorresponding author 000843949 245__ $$aNon-Fermi-liquid to Fermi-liquid transports in iron-pnictide Ba(Fe 1− x Co x ) 2 As 2 and the electronic correlation strength in superconductors newly probed by the normal-state Hall angle 000843949 260__ $$a[Bad Honnef]$$bDt. Physikalische Ges.$$c2017 000843949 3367_ $$2DRIVER$$aarticle 000843949 3367_ $$2DataCite$$aOutput Types/Journal article 000843949 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1519658312_3047 000843949 3367_ $$2BibTeX$$aARTICLE 000843949 3367_ $$2ORCID$$aJOURNAL_ARTICLE 000843949 3367_ $$00$$2EndNote$$aJournal Article 000843949 520__ $$aElectrical transports in iron-pnictide Ba(Fe1−x Co x )2As2 (BFCA) single crystals are heavily debated in terms of the hidden Fermi-liquid (HFL) and holographic theories. Both HFL and holographic theories provide consistent physic pictures and propose a universal expression of resistivity to describe the crossover of transports from the non-Fermi-liquid (FL) to FL behavior in these so-called 'strange metal' systems. The deduced spin exchange energy J and model-dependent energy scale W in BFCA are almost the same, or are of the same order of several hundred Kelvin for over-doped BFCA, which is in agreement with the HFL theory. Moreover, a drawn line of W/3.5 for BFCA in the higher-doping region up to the right demonstrates the crossover from non-FL-like behavior to FL-like behavior at high doping, and shows a new phase diagram of BFCA. The electronic correlation strength in superconductors has been newly probed by the normal-state Hall angle, which found that, for the first time, correlation strength can be characterized by the ratios of T c to the Fermi temperature T F, J/T F, and the transverse mass to longitudinal mass. 000843949 536__ $$0G:(DE-HGF)POF3-6G15$$a6G15 - FRM II / MLZ (POF3-6G15)$$cPOF3-6G15$$fPOF III$$x0 000843949 536__ $$0G:(DE-HGF)POF3-6G4$$a6G4 - Jülich Centre for Neutron Research (JCNS) (POF3-623)$$cPOF3-623$$fPOF III$$x1 000843949 588__ $$aDataset connected to CrossRef 000843949 65027 $$0V:(DE-MLZ)SciArea-120$$2V:(DE-HGF)$$aCondensed Matter Physics$$x0 000843949 65027 $$0V:(DE-MLZ)SciArea-170$$2V:(DE-HGF)$$aMagnetism$$x1 000843949 65017 $$0V:(DE-MLZ)GC-1604-2016$$2V:(DE-HGF)$$aMagnetic Materials$$x0 000843949 693__ $$0EXP:(DE-MLZ)External-20140101$$5EXP:(DE-MLZ)External-20140101$$eMeasurement at external facility$$x0 000843949 7001_ $$0P:(DE-HGF)0$$aWang, Chih-Yi$$b1 000843949 7001_ $$0P:(DE-HGF)0$$aZen, Sha-Min$$b2 000843949 7001_ $$0P:(DE-HGF)0$$aChang, Jin-Yuan$$b3 000843949 7001_ $$0P:(DE-HGF)0$$aKuo, C. N.$$b4 000843949 7001_ $$0P:(DE-HGF)0$$aLue, C. S.$$b5 000843949 7001_ $$0P:(DE-HGF)0$$aChang, L. 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