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The nearly monoexponential 6T decay observed for nonresonant pumping at 392 nm was qualitatively interpreted as the convolution between the impulse decay function (obtained upon 6T resonant excitation) and the activation response function related to RET.
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The nearly monoexponential 6T decay observed for nonresonant pumping at 392 nm was qualitatively interpreted as the convolution between the impulse decay function (obtained upon 6T resonant excitation) and the activation response function related to RET.
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