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The spectrophotometric recording of the kinetics of peroxidase complex II at 390 m i and the disappearance of donor .

The spectroscopic called V4.

The spectroscopic experiments on the hyperfine structure of muonium and the Is-2s energy interval are closely related to a precise measurement of the muon muon magnetic anomaly. The measurements put a stringent test on the internal consistency of the theory of electroweak interaction and on the set of the involved fundamental constants

The spectroscopic experiments on the hyperfine structure of muonium and the ls-2s energy interval are closely related to a precise measurement of the muon muon magnetic anomaly. The measurements put a stringent test on the internal consistency of the theory of electroweak interaction and on the set of the involved fundamental constants

The spectroscopic values of the complex reflection ratio p for three samples of Si02 films grown on silicon as measured by spectroscopic ellipsometry. The three different thicknesses are 321 nm.

The spectroscopically confirmed cage structures of the first three fuUerenes to be isolated in macroscopic amounts A-Ceo, Dsi, -C70, and the chiral fullerene D2 -C76

The spectroscopically cxjnfitmed cage structures of the first three fullerenes to be isolated inmacroscopic amounts A-Ceo, Dsh-Cjo, and the chiral fullerene D2-C76

The spectroscopically detectable metabolic intermediate . The arrow shows the nitrogen that is involved in the reaetion in TAO.

The spectroscopically determined change of the extension of theH-bonded water molecules from 0.5 m added ions as a function of the T

The Spectroscopically Effective Active Site of hemocyanln and tyrosinase.

The spectroscopy of pyrene, PRODAN and DCM. Effects of probe structure, PLLA concentration and preparation method on the local microenvironment that surrounds pyrene, PRODAN, and DCM in PLLA P104-based BPs

The spectrum

The spectrum as a function of wavelength. The fact that the polarized flux does not vary across the lines indicates that the lines are unpolarized, and, therefore, arise in a region unobscured by dust .

The spectrum at 4-2 K of a sample of 3.9H20 showing the unequally spaced lines of the paramagnetic hyperfine spectrum caused by a breakdown of e effective-field approximation. Ref. 138,

The spectrum at the off-diagonal bar shows the strong interaction between a- and b-type protons. This shows that a- and b-type protons are in close proximity in the polymer.

The spectrum Ba J 1 state observed by ICE

The spectrum calculated from the two mode example illustrated in

The spectrum contains three arcs.

The spectrum corresponds to the dry material .

The spectrum demonstrates the presence of an equilibrium between two conformational isomers.

The spectrum due to sample L showing the relatively large line on the low-field side of the dating signal.

The spectrum estimated using the equation I 0.60 is shown as curve 1 the steady-state fluorescence emission spectrum of iPS gel after annealing for 30 min at 318 K as curve 2 comp.2 and comp.3 correspond to spectra 2 and 3 in

The spectrum for styrene consists of 12 lines. Theoretically, the hyperfine structure for the growing chain radical should reflect the interaction of the unpaired

The spectrum has not been source normalized . The interferogram was based on samples taken at 256 equally spaced mirror positions. The

The spectrum is tentatively assigned to a compound related to propenyl-heptaisobutyl-POSS.



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