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BCS relation

The inset of Fig. 2 shows that the generalization of the BCS relation Tc 0.57 A(T = 0. fiq) g(pq), between the critical temperature Tc of the superconducting phase transition and the pairing gap A at T = 0 is satisfactorily fulfilled in the domain of the phase diagram relevant for compact stars. [Pg.346]

It has recently been proposed that the Biopharmaceutical Classification System (BCS) can be used to predict intestinal drug disposition with regards to efflux transport and metabolism (339). Furthermore, on the basis of the key substrate BCS-related properties, permeability, and solubility, the system may be used to predict potential interactions mediated through changes in efflux and/or metabolism at the level of the intestine. [Pg.391]

Although for many Bechgaard salts the application of pressure, P, is necessary to observe superconductivity a further increase of the pressure results in a rather rapid decrease of Tc of, e. g., dPc/dP -8.7 x lO K/kbar in (TMTSF)2PF6 [100, 101]. In principle, this effect is nothing unusual (except for the magnitude) and very common in many conventional superconductors [102]. The effect can be explained with the BCS relation in its simplest form... [Pg.23]

Z o = 3.6 meV for (TMTSF)2PFe [114] and a similar value for (TMTSF)2-CIO4 [115]. Later refined experiments, however, stated for (TMTSF)2C104 at 0.5 K a much lower value of 2Aq = 0.4 meV for the gap in excellent agreement with the BCS relation and consistent with the above stated C value [116]. [Pg.27]

In the phonon-mediated BCS formalism, can simply be expressed by the BCS relation ... [Pg.314]

For diatomic molecules, Bo is the rotational constant to use with equation (10.125), while BQ applies to equation (10.124). They are related by Bo — Bc — ja. The moment of inertia /o/(kg-m2) is related to Z o/(cm ) through the relationship /o = A/(8 x 10 27r2 b< ) with h and c expressed in SI units. For polyatomic molecules, /a, /b, and Iq are the moments of inertia to use with Table A4.1 where the rigid rotator approximation is assumed. For diatomic molecules, /o is used with Table A4.1 to calculate the thermodynamic properties assuming the rigid rotator approximation. The anharmonicity and nonrigid rotator corrections are added to this value. [Pg.642]

Allen GC, Warren KD (1974) The Electronic Spectra of the Hexafluoro Complexes of the Second and Third Transition Series. 19 105-165 Alonso JA, Baibas LC (1993) Hardness of Metallic Clusters. 80 229-258 Alonso JA, Baibas LC (1987) Simple Density Functional Theory of the Electronegativity and Other Related Properties of Atoms and Ions. 66 41-78 Andersson LA, Dawson JH (1991) EXAFS Spectroscopy of Heme-Containing Oxygenases and Peroxidases. 74 1-40 Antanaitis BC, see Doi K (1988) 70 1-26... [Pg.241]

Dobias B (1984) Surfactant Adsorption on Minerals Related to Flotation. 56 91-147 Doi K, Antanaitis BC, Aisen P (1988) The Binuclear Iron Centres of Uteroferrin and the Purple Acid Phosphatases. 70 1-26 Domcke W, see Bradshaw AM (1975) 24 133-170 Dophin D, see Morgan B (1987) 64 115-204... [Pg.244]

Tofield BC (1975) The Study of Covalency by Magnetic Neutron Scattering. 21 1-87 Trautwein AX, Bill E, Bominaar EL, Winkler H (1991) Iron-Containing Proteins and Related Analogs-Complementary Mossbauer, EPR and Magnetic Susceptibility Studies. 78 1-96 Trautwein AX (1974) Mossbauer-Spectroscopy on Heme Proteins. 20 101-167 Tressaud A, Dance J-M (1982) Relationships Between Structure and Low-Dimensional Magnetism in Fluorides. 52 87-146... [Pg.256]

Binder, W.D., Mitchell, G.M. Ballantyne, D.J. (1974). Pollen viability testing, storage and related physiology. Canada Forestry Service, Pacific Forest Research Centre, Victoria, B.C. Report BC-X-105, pp. 1-37. [Pg.126]

Figure 9.14 shows a typical approach force curve along with schematic drawings of the relative positions of the SPM tip and the sample surface, as related to the force curve. At the start of the experiment, i.e., position A on the right-hand side of the figure, the tip is above the surface of the sample. As it approaches the surface the Z value decreases until at position B the tip contacts the surface. With further downward movement of the piezo the cantilever starts to be deflected by the force imposed on it by the surface. If the surface is much stiffer than the cantilever, we get a straight line with a slope of — 1, i.e., for every 1 nm of Z travel we get 1 nm of deflection (Une BC in Figure 9.14). If the surface has stiffness similar to that of the cantilever, the tip wUl penetrate the surface and we get a nonlinear curve with a decreased slope (line BD in Figure 9.14). The horizontal distance between the curve BD and the line BC is equal to the penetration at any given cantilever deflection or force. The piezo continues downward until a preset cantilever deflection is reached, the so-called trigger. The piezo is then retracted a predetermined distance, beyond the point at which the tip separates from the sample. Figure 9.14 shows a typical approach force curve along with schematic drawings of the relative positions of the SPM tip and the sample surface, as related to the force curve. At the start of the experiment, i.e., position A on the right-hand side of the figure, the tip is above the surface of the sample. As it approaches the surface the Z value decreases until at position B the tip contacts the surface. With further downward movement of the piezo the cantilever starts to be deflected by the force imposed on it by the surface. If the surface is much stiffer than the cantilever, we get a straight line with a slope of — 1, i.e., for every 1 nm of Z travel we get 1 nm of deflection (Une BC in Figure 9.14). If the surface has stiffness similar to that of the cantilever, the tip wUl penetrate the surface and we get a nonlinear curve with a decreased slope (line BD in Figure 9.14). The horizontal distance between the curve BD and the line BC is equal to the penetration at any given cantilever deflection or force. The piezo continues downward until a preset cantilever deflection is reached, the so-called trigger. The piezo is then retracted a predetermined distance, beyond the point at which the tip separates from the sample.
Z is a coefficient which relates the concentration of the analyte in the unknown sample to the concentration in the calibration standard, where = bc. R is a residual matrix which contains the measurement error. Its rows represent null spectra. However, in the presence of other (interfering) compounds, the residual matrix R is not random, but contains structure. Therefore the rank of R is greater than zero. A PCA of R, after retaining the significant PCs, gives ... [Pg.300]

Wilkes BC, Schiller, PW. Comparative analysis of various proposed models of the receptor-bound conformation of TIP(P)-related opioid antagonists. Biopolymers (Peptide Sci) 1995 37 391-400. [Pg.178]

Wilkes BC, Nguyen TM-D, Weltrowska G, Carpenter KA, Lemieux C, Chung NN, Schiller PW. The receptor-bound conformation of H-Tyr-Tic-(Phe-Phe)-OH related -opioid antagonists contains all trans peptide bonds. J Peptide Res 1998 51 386-394. [Pg.178]

The most well-known and dramatic manifestation of an INR is the appearance of a narrow feature in the integral cross-section (ICS), cr(E) at total energy E = Er of width T. Obviously the resonance peak is closely related to the existence of the resonance pole in the S-matrix. Using the normal body-fixed representation for an A + BC v,j) — AB(v, j ) + C reaction, the ICS is related to the S-matrix by... [Pg.52]


See other pages where BCS relation is mentioned: [Pg.193]    [Pg.342]    [Pg.25]    [Pg.454]    [Pg.322]    [Pg.193]    [Pg.342]    [Pg.25]    [Pg.454]    [Pg.322]    [Pg.30]    [Pg.644]    [Pg.422]    [Pg.390]    [Pg.378]    [Pg.59]    [Pg.61]    [Pg.1108]    [Pg.547]    [Pg.207]    [Pg.564]    [Pg.769]    [Pg.199]    [Pg.337]    [Pg.88]    [Pg.128]    [Pg.299]    [Pg.2]    [Pg.247]    [Pg.316]    [Pg.37]    [Pg.180]    [Pg.245]    [Pg.159]    [Pg.208]    [Pg.499]    [Pg.500]    [Pg.524]    [Pg.124]    [Pg.223]   
See also in sourсe #XX -- [ Pg.193 ]




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