Download Assessing the Functional Structure of Molecular Transporters by Matthias J.N.Junk PDF

By Matthias J.N.Junk

In his thesis, Matthias Junk takes an leading edge method of verify the neighborhood constitution and dynamics of organic and artificial amphiphilic macromolecules in a position to transporting small molecules. changing the latter with good radicals, he makes use of state of the art electron paramagnetic resonance (EPR) spectroscopy to explain the hugely proper shipping functionality from the point of view of the visitor molecules. Such, he demonstrates that the practical constitution of human serum albumin in answer considerably differs from its crystal constitution – a end result of the protein’s adaptability to host quite a few endogenous compounds and drug molecules. extra, he indicates that the thermal cave in of thermoresponsive hydrogels and dendronized polymers ends up in static and dynamic heterogeneities at the nanoscale. those heterogeneities undergo results for the material’s internet hosting homes and allow unexpected complicated catalytic functionalities.

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Extra info for Assessing the Functional Structure of Molecular Transporters by EPR Spectroscopy

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2 Hyperfine Sublevel Correlation (HYSCORE) Spectroscopy A modification of the 3-pulse ESEEM sequence is achieved by introduction of a non-selective p-pulse, which interchanges the nuclear coherences between the jai and jbi manifolds of the electron spin (Fig. 19a) [62]. The incrementation of both times prior to and after this pulse, t1 and t2 ; yields time-domain data in two dimensions which can be converted to 2D nuclear frequency spectra by Fourier transformation. This 2D EPR technique was invented in 1986 by Höfer et al.

During the time of free evolution s; spin packets with different Larmor frequencies gain a phase shift due to their different angular precession. In the rotating frame, the spin packets thus fan out according to their resonance offset XS and the magnitude of the magnetization vector is decreased. The second ðpÞx -pulse inverts the sign of the y-component. After the same evolution time s; the phases of the different spin packets are refocused and the magnetization vector is maximized. The same result is obtained in the framework of the product operator formalism (Eq.

After the time 2s; only magnetization from the initially inverted electron coherence gives rise to an echo. The redistributed magnetization has acquired a phase / and forms coherence transfer echoes that oscillate with cosð/Þ: For the two-spin system, the phase is given by / ¼ ðxkl À x13 Þs: The oscillations thus depend on the frequencies of the nuclear transitions x12 and x34 and the difference frequency xÀ : The spin density operator at the time of echo formation can be calculated by substituting the spin Hamiltonian in Eq.

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