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T point

Simply doing electronic structure computations at the M, K, X, and T points in the Brillouin zone is not necessarily sufficient to yield a band gap. This is because the minimum and maximum energies reached by any given energy band sometimes fall between these points. Such limited calculations are sometimes done when the computational method is very CPU-intensive. For example, this type of spot check might be done at a high level of theory to determine whether complete calculations are necessary at that level. [Pg.267]

Furthermore (f) 1 2 dichloroethene has a center of symmetry located at the mid t point of the carbon-carbon double bond This too tells us the molecule is achiral... [Pg.286]

A T) point group contains a C axis and n C2 axes. The C2 axes are perpendicular to C and at equal angles to each other. It also contains other elements which may be generated from these. [Pg.83]

Direct and Indirect Energy Gap. The radiative recombination rate is dramatically affected by the nature of the energy gap, E, of the semiconductor. The energy gap is defined as the difference in energy between the minimum of the conduction band and the maximum of the valence band in momentum, k, space. Eor almost all semiconductors, the maximum of the valence band occurs where holes have zero momentum, k = 0. Direct semiconductors possess a conduction band minimum at the same location, k = O T point, where electrons also have zero momentum as shown in Eigure la. Thus radiative transitions that occur in direct semiconductors satisfy the law of conservation of momentum. [Pg.115]

Operating Lines The McCabe-Thiele method is based upon representation of the material-balance equations as operating lines on the y-x diagram. The lines are made straight (and the need for the energy balance obviated) by the assumption of constant molar overflow. The liqmd-phase flow rate is assumed to be constant from tray to tray in each sec tiou of the column between addition (feed) and withdrawal (produc t) points. If the liquid rate is constant, the vapor rate must also be constant. [Pg.1265]

FIG. 26-9 Incident overpressure vs. scaled distance, surface hurst. The t points are from Kingery and PanniU, Memo Report ISIS BRL. Adapted fr am Department of Army, Navy, and Air- For ce TM5-1300, NAVFAC P-397, AFM 88-22.)... [Pg.2280]

Similarly, it can be shown that the nanotube modes at the T-point obtained from the zone-folding eqn by setting Ai = 1), where 0 < ri < N/2, transform according to the , irreducible representation of the symmetry group e. Thus, the vibrational modes at the T-point of a chiral nanotube can be decomposed according to the following eqn... [Pg.136]

Using the calculated phonon modes of a SWCNT, the Raman intensities of the modes are calculated within the non-resonant bond polarisation theory, in which empirical bond polarisation parameters are used [18]. The bond parameters that we used in this chapter are an - aj = 0.04 A, aji + 2a = 4.7 A and an - a = 4.0 A, where a and a are the polarisability parameters and their derivatives with respect to bond length, respectively [12]. The Raman intensities for the various Raman-active modes in CNTs are calculated at a phonon temperature of 300K which appears in the formula for the Bose distribution function for phonons. The eigenfunctions for the various vibrational modes are calculated numerically at the T point k=Q). [Pg.55]

Anspannung, /. Meek.) stress tension, strain, anspielen, v.i. hint, allude begin to play, anspitzen, v.t. point, sharpen. [Pg.29]

Anwartschaft, /. expectancy, anw ssern, v.t. moisten slightly, anweichen, v.t. soften soak slightly, aflweisen, v.t. point out, show assign direct instruct. [Pg.31]

Punkt, in. point dot spot, speck period. Punktcben, n. dot, speck, punkten, v.t. dot spot-weld, punkt-formig, a. in the form of points or a point, point-like, punctiform. -frei, a. (Dyeing) free from spots or specks, punktieren, v.t. point dot pimctuate speckle, spot, stipple. [Pg.350]

Spitze,/. point tip top, apex, vertex, peak, crest, summit, cusp lace, spitzeo, t-t. point, sharpen (to a point) tip. — 71.i. (of grain), sprout, spire, chit. [Pg.419]

Table 1 Time per iteration (in seconds) for the RMM-DIIS and CGa algorithms applied to Fe-ensembles with Natom atoms and using Nkpointa -points for Brillouin-zone integrations. The calculations performed at the T-point only where performed with a version of the code using real wave-functions. Table 1 Time per iteration (in seconds) for the RMM-DIIS and CGa algorithms applied to Fe-ensembles with Natom atoms and using Nkpointa -points for Brillouin-zone integrations. The calculations performed at the T-point only where performed with a version of the code using real wave-functions.
Figure 8.20 (Solid + liquid) phase equilibria for [.viQHf, +. yl.4-C6H4(CH,)2 - The circles are the experimental results the solid lines are the fit of the experimental results to equation (8.31) the dashed lines are the ideal solution predictions using equation (8.30) the solid horizontal line is at the eutectic temperature and the diamonds are (.v, T) points referred to in the text. Figure 8.20 (Solid + liquid) phase equilibria for [.viQHf, +. yl.4-C6H4(CH,)2 - The circles are the experimental results the solid lines are the fit of the experimental results to equation (8.31) the dashed lines are the ideal solution predictions using equation (8.30) the solid horizontal line is at the eutectic temperature and the diamonds are (.v, T) points referred to in the text.
It is important to understand the distinction between the implications of points [3] and [5], Point [3] implies that there is instantaneous mixing at the point of entry between the input stream and the contents of the vessel that is, the input stream instantaneously blends with what is already in the vessel. This does not mean that any reaction taking place in the fluid inside the vessel occurs instantaneously. The time required for the change in composition from input to output stream is t, point [5], which may be small or large. [Pg.31]

Young In any calculation you allow for a number of variables in terms of trying to model the system of action potential propagation. We know that action potentials have to travel within a fasciculus, which is a macroscopic 1—2 mm connective tissue grouping of bundles. Those do not follow a very tortuous route, at the most they wind once or twice over 30 cm, but not much larger than that. The best simulation that s been done using action potential alone used around nine parameters and was totally unrealistic. I probably didn t point it out but the dashed line that overlayed my clinical contraction was where I actually assumed a 350 /tm size bundle. I assumed an intracellular Ca2+ wave and cell activity for 20 s, and I was able to fit it except for the foot at the end (Young 1997). [Pg.187]

The second location of interest is the Tg associated with a maximally freeze-concentrated solute matrix, T (point E), which is important to the processing and stability of frozen foods. The freezing of most foods results in the formation of an amorphous freeze-concentrated phase that is plasticized... [Pg.67]

The frequency of the MS7 mode is well suited to give some fix points for the lattice dynamical calculation. This is obvious by inspection of Fig. 19 which shows the displacement pattern of this mode at the T point (at T the MS7 phonon corresponds to the A, symmetry group). The motions of the atoms being shear vertical, the lattice layers remain rigid planes i.e. the frequency of... [Pg.237]

Figure 26 shows the dispersion curve of the Kr monolayer obtained from a large number of spectra like those in Fig. 25. The hybridization splitting around the crossing with the substrate Rayleigh wave (solid line) is clearly observed. Also the predicted tiny frequency upshift close to the T point due to the coupling to the substrate vibrations is seen. The observed linewidth broadening is also shown in Fig. 26. As a measure of the broadening, the quantity Ae = [( ) — with dE the FWHM of the major loss feature... Figure 26 shows the dispersion curve of the Kr monolayer obtained from a large number of spectra like those in Fig. 25. The hybridization splitting around the crossing with the substrate Rayleigh wave (solid line) is clearly observed. Also the predicted tiny frequency upshift close to the T point due to the coupling to the substrate vibrations is seen. The observed linewidth broadening is also shown in Fig. 26. As a measure of the broadening, the quantity Ae = [( ) — with dE the FWHM of the major loss feature...
I can t point to anything other than the publicity and the news surrounding the atomic bomb and atomic energy. The things that I heard a lot about piqued my curiosity. First, I became interested in physics, then in chemistry. What most piqued my curiosity were the discussions about how atomic energy was going to revolutionize our society and the world. [Pg.54]

If the heat capacity functions of the various terms in the reaction are known and their molar enthalpy, molar entropy, and molar volume at the 2) and i). of reference (and their isobaric thermal expansion and isothermal compressibility) are also all known, it is possible to calculate AG%x at the various T and P conditions of interest, applying to each term in the reaction the procedures outlined in section 2.10, and thus defining the equilibrium constant (and hence the activity product of terms in reactions cf eq. 5.272 and 5.273) or the locus of the P-T points of univariant equilibrium (eq. 5.274). If the thermodynamic data are fragmentary or incomplete—as, for instance, when thermal expansion and compressibility data are missing (which is often the case)—we may assume, as a first approximation, that the molar volume of the reaction is independent of the P and T intensive variables. Adopting as standard state for all terms the state of pure component at the P and T of interest and applying... [Pg.396]

Tn some situations such as examining electronic structure, it can be important to include a k point at the T point. [Pg.57]


See other pages where T point is mentioned: [Pg.808]    [Pg.2894]    [Pg.531]    [Pg.101]    [Pg.185]    [Pg.348]    [Pg.131]    [Pg.538]    [Pg.115]    [Pg.1209]    [Pg.561]    [Pg.756]    [Pg.498]    [Pg.725]    [Pg.178]    [Pg.69]    [Pg.296]    [Pg.24]    [Pg.7]    [Pg.404]    [Pg.139]    [Pg.28]    [Pg.118]    [Pg.53]    [Pg.57]    [Pg.186]    [Pg.207]    [Pg.208]    [Pg.136]   
See also in sourсe #XX -- [ Pg.67 ]

See also in sourсe #XX -- [ Pg.31 ]




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Percentage points, Student’s t-distribution

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