%D8%AC%D9%88%D8%B1%D8%AC_%D8%B3%D9%88%D8%AF%D8%A7%D8%B1%D8%B4%D8%A7%D9%86%D8%AC%D9%88%D8%B1%D8%AC_%D8%B3%D9%88%D8%AF%D8%A7%D8%B1%D8%B4%D8%A7%D9%86%E0%A6%87_%E0%A6%9A%E0%A6%BF_%E0%A6%9C%E0%A7%B0%E0%A7%8D%E0%A6%9C_%E0%A6%B8%E0%A7%81%E0%A6%A6%E0%A7%B0%E0%A7%8D%E0%A6%B6%E0%A6%A8%D8%A7%DB%8C_%D8%B3%DB%8C_%D8%AC%D9%88%D8%B1%D8%AC_%D8%B3%D9%88%D8%AF%D8%A7%D8%B1%D8%B4%D8%A7%D9%86%D0%94%D0%B6%D0%BE%D1%80%D0%B4%D0%B6_%D0%A1%D1%83%D0%B4%D0%B0%D1%80%D1%88%D0%B0%D0%BDGeorge_SudarshanGeorge_SudarshanE._C._George_SudarshanE._C._George_SudarshanGeorge_Sudarshan%D8%A7%DB%8C_%D8%B3%DB%8C_%D8%AC%D9%88%D8%B1%D8%AC_%D8%B3%D9%88%D8%AF%D8%A7%D8%B1%D8%B4%D8%A7%D9%86George_Sudarshan%E0%A4%9C%E0%A5%89%E0%A4%B0%E0%A5%8D%E0%A4%9C_%E0%A4%B8%E0%A5%81%E0%A4%A6%E0%A4%B0%E0%A5%8D%E0%A4%B6%E0%A4%A8George_Sudarshan%D5%8B%D5%B8%D6%80%D5%BB_%D5%8D%D5%B8%D6%82%D5%A4%D5%A1%D6%80%D5%B7%D5%A1%D5%B6E._C._George_SudarshanGeorge_Sudarshan%E3%82%B8%E3%83%A7%E3%83%BC%E3%82%B8%E3%83%BB%E3%82%B9%E3%83%80%E3%83%AB%E3%82%B7%E3%83%A3%E3%83%B3%E0%B4%87.%E0%B4%B8%E0%B4%BF.%E0%B4%9C%E0%B4%BF._%E0%B4%B8%E0%B5%81%E0%B4%A6%E0%B5%BC%E0%B4%B6%E0%B5%BBGeorge_SudarshanGeorge_Sudarshan%D0%A1%D1%83%D0%B4%D0%B0%D1%80%D1%88%D0%B0%D0%BD,_%D0%94%D0%B6%D0%BE%D1%80%D0%B4%D0%B6E._C._George_Sudarshan%E0%AE%9C%E0%AE%BE%E0%AE%B0%E0%AF%8D%E0%AE%9C%E0%AF%8D_%E0%AE%9A%E0%AF%81%E0%AE%A4%E0%AE%B0%E0%AF%8D%E0%AE%9A%E0%AE%A9%E0%AF%8DQ1384866
about
P185
Equivalence of Semiclassical and Quantum Mechanical Descriptions of Statistical Light BeamsRelation between Quantum and Semiclassical Description of Optical CoherenceMonopole Topology and the Problem of ColorThe Zeno’s paradox in quantum theory“Meta” RelativityChirality Invariance and the Universal Fermi InteractionSpin‐s Spherical Harmonics and ðStochastic Dynamics of Quantum-Mechanical SystemsMarkov approximations encounter map domains: A hazard of open quantum dynamicsEntanglement increase from local interactions and not completely positive mapsLorentz transformations that entangle spins and entangle momentaOne qubit almost completely reveals the dynamics of twoMapping the Schrödinger picture of open quantum dynamicsMaps for Lorentz transformations of spinDynamics of initially entangled open quantum systemsRole of preparation in quantum process tomographyHow state preparation can affect a quantum experiment: Quantum process tomography for open systemsThe sense in which a "weak measurement" of a spin-½ particle's spin component yields a value 100Generalized tomographic maps
P50
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P50
description
India füüsik
@et
Indiaas natuurkundige
@nl
Indian physicist
@en
Indian physicist
@en-ca
Indian physicist
@en-gb
fisiceoir Indiach
@ga
fisico indiano
@it
fizician indian
@ro
fizikan indian
@sq
físic indi
@ca
name
E. C. George Sudarshan
@cy
E. C. George Sudarshan
@en
E. C. George Sudarshan
@ga
E. C. George Sudarshan
@id
E. C. George Sudarshan
@sl
E·C·乔治·苏达山
@zh-hans
George Sudarshan
@ca
George Sudarshan
@cs
George Sudarshan
@de
George Sudarshan
@es
type
label
E. C. George Sudarshan
@cy
E. C. George Sudarshan
@en
E. C. George Sudarshan
@ga
E. C. George Sudarshan
@id
E. C. George Sudarshan
@sl
E·C·乔治·苏达山
@zh-hans
George Sudarshan
@ca
George Sudarshan
@cs
George Sudarshan
@de
George Sudarshan
@es
altLabel
E. C. G. Sudarshan
@de
E.C.G. Sudarshan
@ml
E.C.G.スダルシャン
@ja
E.C.ジョージ・スダルシャン
@ja
E·C·乔治·苏达山
@zh
E·C·喬治·蘇達山
@zh-hant
George Sudarshan
@ml
Сударшан Эннакал Ченди Джордж
@ru
Сударшан, Джордж
@ru
Эннакал Ченди Джордж Сударшан
@ru
prefLabel
E. C. George Sudarshan
@cy
E. C. George Sudarshan
@en
E. C. George Sudarshan
@ga
E. C. George Sudarshan
@id
E. C. George Sudarshan
@sl
E·C·乔治·苏达山
@zh-hans
George Sudarshan
@ca
George Sudarshan
@cs
George Sudarshan
@de
George Sudarshan
@es