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BUNSENMAGAZIN - Deutsche Bunsengesellschaft für ...

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DEUTSCHE BUNSEN-GESELLSCHAFT<br />

troscopy. The basic pulse sequence for a 1 H- 13 C Heteronuclear<br />

Multiple-Quantum Correlation (HMQC) experiment is depicted<br />

in Figure 11. 48 As in homonuclear DQ-NMR, the fi rst half of the<br />

REDOR recoupling is identifi ed as the excitation period, and<br />

the second as the reconversion period. In between, HMQC evolution<br />

occurs during t 1 . Evolution due to the 13 C chemical shift<br />

that would lead to additional signal losses is fully refocused<br />

by p-pulses during excitation, evolution and reconversion (in<br />

simple words: its effect is undone).<br />

Figure 11: Basic pulse sequence of REPT-HMQC. The I-channel is usually 1 H,<br />

while the S-channel often refers to 13 C, 15 N or 31 P. REPT means recoupled<br />

polarisation transfer and indicates that the pulse sequence works on initial<br />

I-channel magnetisation, and thus does not require cross-polarisation. Setting<br />

n = 0 corresponds to a recoupling time of 2t R . 48<br />

Indeed, the absence of coherent line-narrowing pulse schemes,<br />

which are often rather sensitive to experimental imperfections,<br />

renders this experiment fairly robust. The recoupled polarisation<br />

transfer (REPT) technique is highly versatile in that it<br />

either allows recording of rotor-synchronized 1 H- 13 C chemical<br />

shift correlation spectra or the determination of even weak 1 H-<br />

13 C dipolar coupling constants by means of spinning sideband<br />

analysis in the indirect dimension of the experiment. Again,<br />

these sidebands are generated by rotor encoding of the reconversion<br />

Hamiltonian. 46<br />

3. SELECTED APPLICATIONS<br />

The versatility of solid-state NMR spectroscopy to elucidate<br />

both the structure and dynamics of (self-)organized possibly<br />

functional aggregates is demonstrated based on selected examples<br />

mainly taken from our laboratory. The rather recent<br />

applications are sorted with respect to the major interaction<br />

or driving force that governs the assembly into macro- or supramolecular<br />

systems.<br />

3.1. HYDROGEN-BONDING<br />

Currently, much interest is focussed on the controlled, rational<br />

design of well-ordered structures that are based on fairly weak<br />

non-covalent interactions such as hydrogen bonds. Though<br />

this approach in principle includes crystals (e.g. in the context<br />

of crystal engineering), many hydrogen-bonded aggregates<br />

crystallize rather poorly rendering single-crystal X-ray structure<br />

analysis diffi cult. In contrast, ultrafast magic-angle-spinning<br />

solid-state NMR is a useful and sensitive tool for the study<br />

of such materials. In particular, the proton chemical shift allows<br />

for a direct detection of local structural environments<br />

UNTERRICHT<br />

and facilitates an estimation of hydrogen-bonding strengths. 50<br />

Indeed, protons involved in hydrogen-bonded structures typically<br />

exhibit well-resolved 1 H chemical shifts, mainly between 8<br />

and 20 ppm. Moreover, correlations between the 1 H isotropic<br />

chemical shifts and the hydrogen-bond strength specifi ed by<br />

O•••H or O•••O distances from single-crystal analyses have<br />

been established. 51 Further resolution may be obtained from<br />

1 H double-quantum 1 H NMR methods (see above) that not<br />

only provide precise information on proton-proton distances on<br />

length scales of up to 0.35 nm but also identify proton positions<br />

in arrays of multiple hydrogen bonds. In this way, dynamic<br />

processes involving molecular recognition 52 or formation of hydrogen-bonded<br />

complexes 50 as well as proton conducting materials<br />

53 can be investigated in detail.<br />

In a rather early case-study, both the thermodynamics and<br />

kinetics of the tautomeric rearrangements of ureidopyrimidinone-based<br />

supramolecular polymers with quadruple hydrogen<br />

bonds was elucidated. The thermally induced and irreversible<br />

transition from pyrimidinone to pyrimidinol could be monitored<br />

via temperature-dependent 2D- 1 H double-quantum spectra<br />

since the two tautomeric structures are involved in different<br />

arrays of quadruple hydrogen-bonds that can be distinguished<br />

by their characteristic DQ peak pattern, thus facilitating an extraction<br />

of the keto/enol ratio present in the sample. It was<br />

found that the rearrangement is associated with an Arrhenius<br />

activation energy of 145 � 15 kJ mol -1 , which contains contributions<br />

from the breaking of hydrogen-bonds and subsequent<br />

reorientation of the polymer chain. 54<br />

Figure 12: Schematic representation of the thermally induced, irreversible<br />

transition from pyrimidin-one to pyrimidin-ol and their characteristic distinguishable<br />

DQ peak pattern. 54<br />

Artifi cial chromophoric receptors for biologically active molecules<br />

have attracted considerable attention from the viewpoint<br />

of molecular recognition. Indeed, barbiturates show very selective<br />

affi nities to binding adenine or its derivatives rendering<br />

them of interest for possible diagnostic applications. By means<br />

of 1 H- 1 H double-quantum and 1 H- 13 C chemical shift correlation<br />

NMR, we obtained detailed insights into packing and (self-)aggregation<br />

of the enolizable chromophor 1-n-butyl-5-(4-nitrophenyl)<br />

barbituric acid that offers adjustable hydrogen-bonding<br />

sites. While in solution, depending on the solvent, up to four<br />

67

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