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COSY R

Figure 3.10 Effect of different window functions (apodization functions) on the appearance of COSY plot (magnitude mode), (a) Sine-bell squared and (b) sine-bell. The spectrum is a portion of an unsymmetrized matrix of a H-COSY I.R experiment (400 MHz in CDCl, at 303 K) of vasicinone. (c) Shifted sine-bell squared with r/4. (d) Shifted sine-bell squared with w/8. (a) and (b) are virtually identical in the case of delayed COSY, whereas sine-bell squared multiplication gives noticeably better suppression of the stronger dispersion-mode components observed when no delay is used. A difference in the effective resolution in the two axes is apparent, with Fi having better resolution than F. The spectrum in (c) has a significant amount of dispersion-mode line shape. Figure 3.10 Effect of different window functions (apodization functions) on the appearance of COSY plot (magnitude mode), (a) Sine-bell squared and (b) sine-bell. The spectrum is a portion of an unsymmetrized matrix of a H-COSY I.R experiment (400 MHz in CDCl, at 303 K) of vasicinone. (c) Shifted sine-bell squared with r/4. (d) Shifted sine-bell squared with w/8. (a) and (b) are virtually identical in the case of delayed COSY, whereas sine-bell squared multiplication gives noticeably better suppression of the stronger dispersion-mode components observed when no delay is used. A difference in the effective resolution in the two axes is apparent, with Fi having better resolution than F. The spectrum in (c) has a significant amount of dispersion-mode line shape.
Figure 6.11 A 3D heteronuclear HMQC-COSY spectrum of a tripepiide. The o),-axis represents N chemical shifts, whereas the (Or and 88, copyright (1988), with permission from Academic Pre.ss, Inc.)... Figure 6.11 A 3D heteronuclear HMQC-COSY spectrum of a tripepiide. The o),-axis represents N chemical shifts, whereas the (Or and <i),-axes exhibit proton chemical shifts. The a.ssignment pathways are indicated in the top spectrum for reference purposes, not as part of the 3D experiment. (Reprinted from J. Mag. Reson. 78, S. W. Fesik and E. R. P. Zuiderweg, >88, copyright (1988), with permission from Academic Pre.ss, Inc.)...
Figure 7.25 Homoniiclear double-quantum filtered COSY spectrum (400 MHz) of 8-mMangiotensin II in H,0 recorded without phase cycling. Magnetic field gradient pulses have been used to select coherence transfer pathways. (Reprinted from J. Mag. Reson. 87, R. Hurd, 422, copyright (1990), with permission from Academic Press, Inc.)... Figure 7.25 Homoniiclear double-quantum filtered COSY spectrum (400 MHz) of 8-mMangiotensin II in H,0 recorded without phase cycling. Magnetic field gradient pulses have been used to select coherence transfer pathways. (Reprinted from J. Mag. Reson. 87, R. Hurd, 422, copyright (1990), with permission from Academic Press, Inc.)...
Baldini F., Bracci S., Cosi F., Falciai R., Italian Patent No FI 93 A125, July (1993). [Pg.381]

Falciai R., Baldini F., Cosi F., Bechi P., Pucciani F., Bile enterogastric reflux sensor using plastic optical fibres, Fiber and Integr. Opt. 1993 12 215. [Pg.432]


See other pages where COSY R is mentioned: [Pg.611]    [Pg.265]    [Pg.47]    [Pg.75]    [Pg.18]    [Pg.226]    [Pg.706]    [Pg.86]    [Pg.84]    [Pg.325]    [Pg.611]    [Pg.265]    [Pg.47]    [Pg.75]    [Pg.18]    [Pg.226]    [Pg.706]    [Pg.86]    [Pg.84]    [Pg.325]    [Pg.611]    [Pg.502]    [Pg.556]    [Pg.398]    [Pg.126]    [Pg.126]    [Pg.122]    [Pg.165]    [Pg.374]    [Pg.123]    [Pg.719]    [Pg.147]    [Pg.45]    [Pg.116]    [Pg.247]    [Pg.330]    [Pg.333]    [Pg.174]    [Pg.249]    [Pg.92]    [Pg.45]    [Pg.302]    [Pg.116]    [Pg.139]    [Pg.134]    [Pg.141]    [Pg.338]    [Pg.381]    [Pg.391]    [Pg.13]    [Pg.142]    [Pg.143]    [Pg.56]   
See also in sourсe #XX -- [ Pg.2 , Pg.108 ]




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