HiSOR SR-VUVCD
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[SR-VUVCD spectrophotometer] Optical device SR-VUVCD spectrophotometer consists of two separate vacuum chambers (at10-4 Pa; a polarization modulation chamber and a sample chamber). All optical devices of the spectrophotometer are set up under a high vacuum (10-6 Torr), in order to avoid the light absorption in the VUV region by air and water vapor. The SR light is separated into two orthogonal linearly polarized light beams by a linear polarizer (POL, MgF2). Both linearly polarized light beams are modulated into circularly polarized light at 50 kHz by a photo-elastic modulator (PEM, LiF). The main light beam is led to the sample cell and the CD signal is detected by a photomultiplier tube (Main-PM), which is covered by an MgF2 window. The CD signal is rectified and amplified by the lock-in amplifier (LIA), and finally recorded on a personal computer. Another light beam from the PEM is detected as a reference signal by another photomultiplier tube (Ref-PM) after being modulated into a linearly polarization light beam at 100 kHz by a linear polarizer (ANA, MgF2), to obtain optimal driving voltages for the PEM. Further, this reference signal is used to enhance the stabilization of the LIA through the synchronization and rectification of the CD signal detected by the Main-PM. |
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Picture and Block diagram of SR-VUVCD ANA, analyzer; G, grating; GV, gate valve; LIA, lock-in amplifier; MON, monochromator; MR, mirror; PEM, photoelastic modulator; PM, photomultiplier tube; POL, polarizer; S, shutter; SR, synchrotron radiation. |
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Sample cell Sample cell consists of a stainless-steel container with a cylindrical screw, two CaF2 (or MgF2) crystal windows of 20-mm diameter and 1-mm thickness, and three fluoride-rubber O-rings. The optical path length can be adjusted over the range from 1.3 μm (without a spacer) to 100 μm (with donut-shaped Teflon spacers). The sample solution in the cell is sealed with three fluoride-rubber O-rings. The temperature of the sample is controlled between –20°C and 70°C by a Peltier thermoelectric element fixed to the copper jacket in which coolant from a thermostatic bath is circulated through flexible stainless-steel tubes. |
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Picture of optical cell BLock diagrams of optical cell and temperature control unit | |||
[Applications to structural analysis of biomolecules] |
Structural analysis of sugars D-Glucose and D-mannose, and D-galactose exhibit markedly different VUVCD spectra despite having very similar structures. The spectra of D-glucose and D-mannose show positive peaks around 168 and 170 nm, respectively. In contrast to these two monosaccharides, D-galactose shows two negative CD peaks around 177 and 162 nm. The spectra in the range 160–180 nm can be assigned to the n-s* transition of lone-pair oxygen electrons of hydroxy groups and acetal bonds, based on simple quantum mechanical considerations at the molecular orbital level. These VUVCD spectra were significantly affected by the a- and β-anomers at C-1, and the trans (T) and gauche (G) configurations of hydroxymethyl group at C-5. |
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UVCD spectra of D-glucose, D-mannose, and D-galactose Component spectra of D-glucose | |||
Structural analysis of proteins VUVCD spectra of proteins sensitively reflect secondary structures such as a-helices, β-sheets, turns, and unordered structures. Therefore, we can estimate the contents and the numbers of segments of these secondary structures of an unknown protein from its VUVCD spectra using some analytical programs (e.g. SELCOM 3 program). These secondary-structure data can be further combined with bioinformatics to improve the sequence-based predictions (VUVCD-NN method). The scheme for the secondary-structure analysis of proteins by VUVCD spectroscopy is depicted in the following illustration. |
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Scheme for the secondary-structure analysis of proteins by SR-VUVCD spectroscopy
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