J Phys Chem B (submitted) Plato M, Lubitz W, Möbius K (1981) A so

J Phys Chem B (submitted) Plato M, Lubitz W, Möbius K (1981) A solution ENDOR sensitivity study of various nuclei in organic radicals. J Phys Chem 85:1202–1219. doi:10.​1021/​j150609a024 CrossRef Poluektov OG, Utschig LM, Dubinskij AA, Thurnauer MC (2005) Electron transfer pathways and protein response to charge separation in photosynthetic reaction centers: time-resolved high-field ENDOR of the PI3K Inhibitor Library spin-correlated radical pair P 865 •+ Q A •+ . J Am Chem Soc 127:4049–4059. doi:10.​1021/​ja043063g CrossRefPubMed Poole CP Jr (1983) Electron spin resonance. A comprehensive

treatise on experimental techniques. Wiley Intersience, New York, USA Rigby SEJ, Evans MCW, Heathcote P (2001) Electron nuclear double resonance (ENDOR) spectroscopy of radicals in photosystem I and related Type 1 photosynthetic reaction centres. Biochim Biophys Acta 1507:247–259. doi:10.​1016/​S0005-2728(01)00211-0 CrossRefPubMed Schweiger A, Jeschke G (2001) Principles of pulse electron paramagnetic resonance. Oxford University Press, UK Sinnecker S, Koch W, Lubitz W (2000) Bacteriochlorophyll a radical cation and anion—calculation of isotropic hyperfine coupling constants by density functional methods. Phys Chem Chem Phys 2:4772–4778.

doi:10.​1039/​b004370m CrossRef Sinnecker S, Flores M, Lubitz M (2006) Protein-cofactor interactions in bacterial reaction centers from Rhodobacter sphaeroides R 26: effect of hydrogen selleck kinase inhibitor bonding on the electronic and geometric structure of the primary quinone. A density functional theory study. Phys Chem Chem Phys 8:5659–5670. doi:10.​1039/​b612568a CrossRefPubMed”
“Introduction Direct information about the three-dimensional (3D) structure of a protein complex is essential for understanding its functional organization. At present, electron microscopy (EM) is a widely applied technique for studying the structure of proteins and membranes, but it is still less common than X-ray Dinaciclib diffraction where solving the 3D structure of proteins became almost routine, once

suitable crystals have 4��8C been obtained. On the other hand, X-ray diffraction has two disadvantages in comparison to EM. First, the main disadvantage is the problem of getting well-ordered, large enough crystals. The interaction of electrons with material is stronger than for X-rays by a factor of about 10,000. This makes EM a useful technique for imaging single-layer 2D crystals or single protein molecules on a thin support film, in contrast to the thicker specimens in the (sub) micron range, used in X-ray diffraction. A second reason is that only diffraction patterns are obtained, whereas EM results in direct information in the form of images. Imaging of thin metal foils or gold clusters by EM will easily provide projections with atomic details, but obtaining structures of proteins at high resolution is much harder work.

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