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Charge giant

Figure 10.9 Video-microscopy images of positively charged CL/DNA complexes in the (A) iiand(B) phases, and interacting with negatively charged giant (G) vesicles (C and D). In all cases, complexes were viewed in (DIC) (left), lipid fluorescence (middle), and DNA fluorescence (right). The scale bar for DIC is 3 gpm for (A) (B), and 20 ppm... Figure 10.9 Video-microscopy images of positively charged CL/DNA complexes in the (A) iiand(B) phases, and interacting with negatively charged giant (G) vesicles (C and D). In all cases, complexes were viewed in (DIC) (left), lipid fluorescence (middle), and DNA fluorescence (right). The scale bar for DIC is 3 gpm for (A) (B), and 20 ppm...
I phases, and interacting with negatively charged giant (G) vesicles (C and D)... [Pg.493]

Labeit, S., and Kolmerer, B., 1995. Tidns Giant proteins in charge of muscle nltrastrnctnre and elasdcity. Science 270 293-296. [Pg.564]

During the red giant phase of stellar evolution, free neutrons are generated by reactions such as C(a,n) and Ne(a,n) Mg. (The (ot,n) notation signifies a nuclear reaction where an alpha particle combines with the first nucleus and a neutron is ejected to form the second nucleus.) The neutrons, having no charge, can interact with nuclei of any mass at the existing temperatures and can in principle build up the elements to Bi, the heaviest stable element. The steady source of neutrons in the interiors of stable, evolved stars produces what is known as the "s process," the buildup of heavy elements by the slow interaction with a low flux of neutrons. The more rapid "r process" occurs in... [Pg.18]

The dynamics of charge recombination from the giant CS states of syn-23 and anti-23, +An-DMN-DCV , were surprising (Figure 21).1371 The two molecules are diastereoisomers, the former possessing a... [Pg.283]

The photophysical results1391 for the giant porphyrin - dimethoxynaphthalene - naphthoquinone - vio -logen tetrad, P-DMN-NQ.-MV2, 24 (Figure 22), complement those obtained for 23. Photoinduced charge separation, to form the giant CS state, +P-DMN-NQ -MV+, readily occurs in the syn, syn isomer, but not in the anti,syn isomer. This result... [Pg.283]

A Schottky diode is always operated under depletion conditions flat-band condition would involve giant currents. A Schottky diode, therefore, models the silicon electrolyte interface only accurately as long as the charge transfer is limited by the electrode. If the charge transfer becomes reaction-limited or diffusion-limited, the electrode may as well be under accumulation or inversion. The solid-state equivalent would now be a metal-insulator-semiconductor (MIS) structure. However, the I-V characteristic of a real silicon-electrolyte interface may exhibit features unlike any solid-state device, as... [Pg.41]

This chapter is about molecules. A molecule is a collection of nuclei Z., Z/,... at rest (in the Bom-Oppenheimer approximation) in a sea of fast-moving electrons. The nuclei can be identified and thus provide convenient reference marks. Each nucleus found in the molecule, say, Z], can be viewed as the nucleus of a giant atom extending over the entire molecule is surrounded by charges, just as in an ordinary atom, with the difference that motionless positive point charges are now part of its environment. Of course, the electronic content is still described by its stationary density. [Pg.35]

Labeit S, Kolmerer B. Titins giant proteins in charge of muscle ultrastmcture and elasticity. Science 1995 270 293-296. [Pg.255]

Further, each composite dipole has its own scalar potential between its end charges. With the previously stated reservation (see Section III.A.l), this scalar potential decomposes per Whittaker [8] and thus initiates a giant negentropic reordering of the vacuum energy as previously discussed. So any charge is really an entire set of composite dipoles, composite negative resistors, and broken... [Pg.659]


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