2017
DOI: 10.1002/macp.201700329
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Rotational Dynamics of a Probe in Rubbery Polymers Characterized by Time‐Resolved Fluorescence Anisotropy Measurement

Abstract: The rotational relaxation time (τrot) of a fluorescent molecule, coumarin 153 (C153), dispersed in different rubbery polymers is characterized by time‐resolved fluorescence anisotropy measurement, and an attempt is made to quantitatively combine it with the segmental relaxation time (τseg) of the corresponding matrix polymer obtained by dielectric relaxation spectroscopy. This study here demonstrates that τseg extrapolated to higher temperatures using the Vogel–Fulcher–Tammann law can be superimposed on τrot, … Show more

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Cited by 6 publications
(12 citation statements)
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“…TRFA is effective for characterizing the segmental dynamics of polymers in a short time range from a few to tens of nanoseconds. 51 Thus, combining TRFA with DRS enables us to gain access to the segmental dynamics of adsorbed chains in a long time range. 51 In TRFA measurements, a small amount of fluorescent probes is dispersed into a polymer matrix and the fluorescence anisotropy, which is related to the polymer dynamics, is tracked as a function of time.…”
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confidence: 99%
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“…TRFA is effective for characterizing the segmental dynamics of polymers in a short time range from a few to tens of nanoseconds. 51 Thus, combining TRFA with DRS enables us to gain access to the segmental dynamics of adsorbed chains in a long time range. 51 In TRFA measurements, a small amount of fluorescent probes is dispersed into a polymer matrix and the fluorescence anisotropy, which is related to the polymer dynamics, is tracked as a function of time.…”
mentioning
confidence: 99%
“…51 Thus, combining TRFA with DRS enables us to gain access to the segmental dynamics of adsorbed chains in a long time range. 51 In TRFA measurements, a small amount of fluorescent probes is dispersed into a polymer matrix and the fluorescence anisotropy, which is related to the polymer dynamics, is tracked as a function of time. When exciting laser pulses were guided into a sample from the solid side at an incident angle (θ) smaller and larger than the critical angle (θ c ) related to the total reflection, respectively, they crossed the bulk region and totally reflected at the interface, as schematically illustrated in the inset of Figure 1a.…”
mentioning
confidence: 99%
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