I band

Hamm P, Urn M and Hochstrasser R M 1998 Structure of the amide I band of peptides measured by femtosecond nonlinear-infrared spectroscopy J. Phys. Chem. B 102 6123-38... 

The SMD simulations were based on an NMR structure of the Ig domain 127 of the cardiac titin I-band (Improta et ah, 1996). The Ig domains consist of two /9-sheets packed against each other, with each sheet containing four strands, as shown in Fig. 8b. After 127 was solvated and equilibrated, SMD simulations were carried out by fixing one terminus of the domain and applying a force to the other in the direction from the fixed terminus to the other terminus. Simulations were performed as described by Eq. (1) with V = 0.5 A/ps and if = 10 ksT/A 414 pN/A. The force-extension profile from the SMD trajectory showed a single force peak as presented in Fig. 8a. This feature agrees well with the sawtooth-shaped force profile exhibited in AFM experiments. 

Improta et al., 1996] Improta, S., Politou, A., and Pasture, A. Immunoglobulinlike modules from titin I-band extensible components of muscle elasticity. Structure. 4 (1996) 323-337... 

Such bands also obey the rotational selection rules in Equation (6.82) and appear similar to a U-I band of a linear molecule. 

FIGURE 17.12 Electron micrograph of a skeletal muscle myofibril (in longitndinal section). The length of one sarcomere is indicated, as are the A and I bands, the H zone, the M disk, and the Z lines. Cross-sections from the H zone show a hexagonal array of thick filaments, whereas the I band cross-section shows a hexagonal array of thin filaments. (Photo courtesy of Hugh Huxley, Brandeis University)... 

Regulatory proteins Major Tropomyosin 33 X 2 5 I band Binds to actin and... 

Figure 3. Structure of a muscle sarcomere. In a polarizing microscope muscle appears to have dark (A) and light (I) bands. The l-band region only contains thin filaments. The A-band region contains both thick and thin filaments. One sarcomere is the distance between two Z-lines. In cross section, the hexagonal packing of the thick and thin filaments can be seen.

Figure 11a shows a force-distance profile measnred for poly(L-glutamic acid) brushes (2C18PLGA(44)) in water (pH = 3.0, 10 M HNO3) deposited at 40 mN/m from the water subphase at pH = 3.0. The majority of peptides are in the forms of an a-helix (38% determined from the amide I band) and a random coil. Two major regions are clearly seen in... 

It is a supposition that the )9-sheet structure of neurotoxin is an essential structural element for binding to the receptor. The presence of -sheet structure was found by Raman spectroscopic analysis of a sea snake neurotoxin (2). The amide I band and III band for Enhydrina schistosa toxin were at 1672 cm and 1242 cm" respectively. These wave numbers are characteristic for anti-parallel -sheet structure. The presence of -sheet structure found by Raman spectroscopic study was later confirmed by X-ray diffraction study on Laticauda semifasciata toxin b. 

For the explicit calculations presented below, we have chosen a width wq = 10 e V for the ip-band, and a coupling strength A p =0.2 eV, and have varied the parameters for the (i-band. The level shift A(e) is obtained from the second part of (2.7). The resulting functions are illustrated in Fig. 2.12. 

Figure 2.13 shows the effect that a d-haaA has on the density of states of a level positioned at its center. When the interaction is weak, the level is just broadened. However, when the interaction is strong, the level is split into a bonding orbital (with respect to the metal) and an antibonding orbital, which lie below and above the (i-band, respectively. The same effects can be observed when the level lies originally above or below the (i-band (Fig. 2.14). For a weak interaction, the level just...

This allows a direct influence of the alloying component on the electronic properties of these unique Pt near-surface formations from subsurface layers, which is the crucial difference in these materials. In addition, the electronic and geometric structures of skin and skeleton were found to be different for example, the skin surface is smoother and the band center position with respect to the metallic Fermi level is downshifted for skin surfaces (Fig. 8.12) [Stamenkovic et al., 2006a] owing to the higher content of non-Pt atoms in the second layer. On both types of surface, the relationship between the specific activity for the oxygen reduction reaction (ORR) and the tf-band center position exhibits a volcano-shape, with the maximum... 

The key parameters of the electronic structure of these surfaces are summarized in Table 9.3. The calculated rf-band vacancy of Pt shows no appreciable increase. Instead, there is a shght charge transfer from Co to Pt, which may be attributable to the difference in electronegativity of Pt and Co, in apparent contradiction with the substantial increase in Pt band vacancy previously reported [Mukerjee et al., 1995]. What does change systematically across these surfaces is the J-band center (s ) of Pt, which, as Fig. 9.12 demonstrates, systematically affects the reactivity of the surfaces. This correlation is consistent with the previous successes [Greeley et al., 2002 Mavrikakis et al., 1998] of the band model in describing the reactivity of various bimetallic surfaces and the effect of strain. Compressive strain lowers s, which, in turn, leads to weaker adsorbate-surface interaction, whereas expansive strain has the opposite effect. 

This is the first experimental demonstration of changes in the strength of CO adsorption at Pt-based alloy electrodes. Nprskov and co-workers theoretically predicted a similar linear relation between changes in ads(CO) and shifts in the (i-band center [Hammer et al., 1996 Hammer and Nprskov, 2000 Ruban et al., 1997]. Because the Pt4/7/2 CL shift due to alloying can be more easily measured by XPS than the li-band center can, this should be one of the most important parameters to aid in discovering CO-tolerant anode catalysts among Pt-based alloys or composites. 

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