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C:/Documents and Settings/jhk10/My Documents/NMR Course 2004/../NMR…
https://www-keeler.ch.cam.ac.uk/lectures/understanding/chapter_5.pdf24 Feb 2004: Is the magnet sufficientlyhomogeneous to be of use? E 5–2A careful pulse calibration experiment determines that the 180 pulse is 24.8µs. -
2d_3_12
https://www-keeler.ch.cam.ac.uk/lectures/2d_letter.pdf1 Feb 2001: 3–1. 3 Basic concepts fortwo-dimensional NMR. ,QWURGXFWLRQ. The basic ideas of two-dimensional NMR will be introduced by reference to theappearance of a COSY spectrum; later in this lecture the product operatorformalism will be used to predict the -
4–1 4 Coherence Selection: Phase Cycling and Gradient Pulses ...
https://www-keeler.ch.cam.ac.uk/lectures/phasen_a4.pdf1 Feb 2001: 4–1. 4 Coherence Selection: Phase Cycling and Gradient Pulses. A multiple-pulse NMR experiment is designed to manipulate the spins in a certain carefully defined way so as to produce a particular spectrum. However, a given pulse sequence usually -
Chapter 7/3(A4)
https://www-keeler.ch.cam.ac.uk/lectures/understanding/chapter_7.pdf24 Feb 2004: 7–1. 7 Two-dimensional NMR†. 7.1 Introduction. The basic ideas of two-dimensional NMR will be introduced by reference tothe appearance of a COSY spectrum; later in this chapter the productoperator formalism will be used to predict the form of -
Chapter 9 letter
https://www-keeler.ch.cam.ac.uk/lectures/Irvine/chapter9.pdf12 Mar 2002: 9–1. 9 Coherence Selection:Phase Cycling and Gradient Pulses†. 9.1 Introduction. The pulse sequence used in an NMR experiment is carefully designed toproduce a particular outcome. For example, we may wish to pass the spinsthrough a state of -
select/ALL/5
https://www-keeler.ch.cam.ac.uk/lectures/EMBOselect.pdf23 Jul 2002: 4–1. 4. Coherence Selection:Phase Cycling and Gradient Pulses. 4.1 Introduction. The pulse sequence used in an NMR experiment is carefully designed toproduce a particular outcome. For example, we may wish to pass the spinsthrough a state of -
main.dvi
https://www-keeler.ch.cam.ac.uk/lectures/Irvine/chapter3.pdf5 Mar 2002: increasing τ. Fig. 3.24 Visualization of the outcome of an inversion recovery experiment. ... 3.24. 3.11 Off-resonance effects and soft pulses. -y. z. xb. c. -
Chapter 9 a4 /2
https://www-keeler.ch.cam.ac.uk/lectures/understanding/chapter_9.pdf24 Feb 2004: 9–1. 9 Coherence Selection:Phase Cycling and Gradient Pulses†. 9.1 Introduction. The pulse sequence used in an NMR experiment is carefully designed toproduce a particular outcome. For example, we may wish to pass the spinsthrough a state of -
C:/Documents and Settings/jhk10/My Documents/NMR Course 2004/../NMR…
https://www-keeler.ch.cam.ac.uk/lectures/understanding/chapter_3.pdf24 Feb 2004: increasing τ. Fig. 3.24 Visualization of the outcome of an inversion recovery experiment. ... Thewhole process is visualized in Fig. 3.24. 3.11 Off-resonance effects and soft pulses. -
C:/Documents and Settings/jhk10/My Documents/Papers/broadband…
https://www-keeler.ch.cam.ac.uk/publications/ProtonDecoupled.pdf9 Jan 2007: field strength of1.7 kHz, which was swept through an offset range of 24 kHz in 24 ms. ... 24. (a). (b). 2.6 2.2 1.8 1.4 ppm1.0. 0. -100. -200. -
Basis_Quante–
https://www-keeler.ch.cam.ac.uk/lectures/quant_a4.pdf1 Feb 2001: These details aresummarized in the diagram below. 2 J122 J1213 24 12 34. ... 1–24. The corresponding equation for cβ is found by left multiplying by 〈β|.
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