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Typically, the feature of the decay of the PL intensity for QDs is a universal occurrence of a biexponential time distribution in the radiative lifetime, as shown in the following equation, where S and L represent the shorter lifetime and longer lifetime, respectively, and A i (i = S, L) is the amplitude of the components at t = 0

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Kullanlan maskeyi scak suda zndrn , oda scaklna gelince kapakl bir kavanozda buzdolabnda saklayn

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