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Gauss pulse

A Gauss pulse and a polynomial multiplied by a Gauss pulse satisfy the requirements of rapid fall-off in both the time and the frequency domains. A pulse the shape of which is determined by a product of a Hermitian polynomial and a Gauss function is a Hermite pulse [Sill, War2]. Its width can be more narrow than that of a Gauss pulse. A fairly uniform rotation of z magnetization can be generated if the sum of a zeroth- and a... [Pg.155]

Fig. 9. Pulse sequences for 3D- and 2D- H, X, Y correlations. The same notation as in Fig. 1 is used, (a) HNCA-analogue 3D experiment. (b) HNCO-analogue 3D experiment. (c) gs-SELTRIP with a selective 180° gauss pulse the gradient strength (for the case H. C. P) is +/-2S, —/+25,22.7 for echo/antiecho selection. ... Fig. 9. Pulse sequences for 3D- and 2D- H, X, Y correlations. The same notation as in Fig. 1 is used, (a) HNCA-analogue 3D experiment. (b) HNCO-analogue 3D experiment. (c) gs-SELTRIP with a selective 180° gauss pulse the gradient strength (for the case H. C. P) is +/-2S, —/+25,22.7 for echo/antiecho selection. ...
Calculate Angle (Radians) = [beta/[2 hbar]] g Attenuation (Bl, Gauss) pulse length (ns)... [Pg.146]

The const value depends on the shape of the pulse envelope. For the Gauss pulse const = 0.44. The pulse with a duration of 10 s has a spectral width of 1100 cm. This implies that the femtosecond light pulse can simultaneously excite several vibrational states. [Pg.92]

Tesla 1 T = lO gauss Pulse width (length, duration)... [Pg.616]

Figure 2. Spin-echo -NMR spectra from a diffusion experiment with a cubic phase of dDAVP (10%), MO (60%) and 2H20 (40%). Temperature 40 C, t=20 ms, A=24 ms, g=l 19 gauss/cm and 8=1.0,2.0..., 9.0 ms. The inset shows the aromatic region originating from dDAV P at a higher amplification. Also shown is the pulse sequence used in the NMR-diffusion method (see text for details). Figure 2. Spin-echo -NMR spectra from a diffusion experiment with a cubic phase of dDAVP (10%), MO (60%) and 2H20 (40%). Temperature 40 C, t=20 ms, A=24 ms, g=l 19 gauss/cm and 8=1.0,2.0..., 9.0 ms. The inset shows the aromatic region originating from dDAV P at a higher amplification. Also shown is the pulse sequence used in the NMR-diffusion method (see text for details).
Fig. 18. The pulse sequence of a ID ge-NOESY-TOCSY experiment, tnoe is the NOE mixing time, 5 are optional delays which can be used for z-filtration [81] or for suppression of ROE effects in macromolecules (2 x (5 + Tgrad) = 0.5 x mixing time). DIPSI-2 [78] sequence was used for isotropic mixing. Phases were cycled as follows 0i = 2x, 2(—x) (j)2 = X, —x Ip = X, 2 —x), X. Rectangular PFGs, G = 6 Gauss/cm and Gi = 7 Gauss/cm, were applied along the axis for Xpad = 1 ms. Fig. 18. The pulse sequence of a ID ge-NOESY-TOCSY experiment, tnoe is the NOE mixing time, 5 are optional delays which can be used for z-filtration [81] or for suppression of ROE effects in macromolecules (2 x (5 + Tgrad) = 0.5 x mixing time). DIPSI-2 [78] sequence was used for isotropic mixing. Phases were cycled as follows 0i = 2x, 2(—x) (j)2 = X, —x Ip = X, 2 —x), X. Rectangular PFGs, G = 6 Gauss/cm and Gi = 7 Gauss/cm, were applied along the axis for Xpad = 1 ms.
Loading the file ch4321.cfg set the Calculation mode to Shaped pulse in the Calculate I Setup dialog box and in the SPNAMO filename box enter the filename. .. wave gauss.shp. Close the dialog box OK. In the Calculate I Time... [Pg.167]

Clearly this will produce magnetization components which do not focus properly in the x-y plane. In order to avoid these problems, the condition H >G 2R should be met. Typically, this will limit continuous gradient diffusion measurements to G of 30 gauss/cm or less. One can do an approximate evaluation of G from the echo duration and of from the duration t of a 71/2 pulse, where yHjX=n/2, to check the above condition. The pulsed gradient method described in the... [Pg.201]

Several laboratories are experimenting with pulsed magnetic fields of sufficient strength (10 —10 gauss) to provide useful track curvature measurements in emulsions. [Pg.479]

The basic feature of time domain spectroscopy (TDS) is the application of a broad bandwidth signal containing all the frequencies togeflier. A typical signal with broad bandwidth is the square wave (Teorell, 1946). Other popular signals are the Dirac pulse, the multisinusoidal excitation, and the Gauss burst or wavelets. [Pg.309]


See other pages where Gauss pulse is mentioned: [Pg.155]    [Pg.155]    [Pg.157]    [Pg.155]    [Pg.155]    [Pg.157]    [Pg.735]    [Pg.116]    [Pg.111]    [Pg.32]    [Pg.338]    [Pg.202]    [Pg.286]    [Pg.94]    [Pg.302]    [Pg.189]    [Pg.709]    [Pg.296]    [Pg.28]    [Pg.116]    [Pg.114]    [Pg.106]    [Pg.30]    [Pg.156]    [Pg.114]    [Pg.653]    [Pg.140]    [Pg.168]    [Pg.169]    [Pg.170]    [Pg.171]    [Pg.267]    [Pg.269]    [Pg.52]    [Pg.85]    [Pg.26]    [Pg.336]    [Pg.80]    [Pg.198]    [Pg.614]    [Pg.40]   
See also in sourсe #XX -- [ Pg.155 , Pg.157 ]




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