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  2. Chapter 8 letter /5

    https://www-keeler.ch.cam.ac.uk/lectures/Irvine/chapter8.pdf
    12 Mar 2002: 13. 23 0 3. 11. 24 0 2. 112. 22 0 2. ... 11. 24 0 3. 24. 24 2 4. 23. 22 2 1. ( ) ( ) ( ) ( ). ( ) ( ) ( ) ( ).
  3. main.dvi

    https://www-keeler.ch.cam.ac.uk/lectures/Irvine/chapter2.pdf
    5 Mar 2002: 2 3. 4. ν0,1 ν0,2. frequency. 13. 24. 12. 3424 1334 12. ... 13 57 24 68. spin 2spin 3. αα. α ββ α β.
  4. C:/Documents and Settings/jhk10/My Documents/NMR Course 2004/../NMR…

    https://www-keeler.ch.cam.ac.uk/lectures/understanding/chapter_2.pdf
    24 Feb 2004: ν0,1 ν0,2. frequency. 13. 24. 12. 3424 1334 12. spin 1flipsflips spin 2. ... 13 57 24 68. spin 2spin 3. αα. α ββ α β.
  5. Ch 6-9 probs /2

    https://www-keeler.ch.cam.ac.uk/lectures/understanding/chapter_6_9_probs.pdf
    24 Feb 2004: 1 24 2 2 2+ ( )In a heteronuclear system a coherence order can be assigned to each spinseparately.
  6. Basis_Quante–

    https://www-keeler.ch.cam.ac.uk/lectures/quant_letter.pdf
    1 Feb 2001: These details are summarized in thediagram below. 2 J122 J1213 24 12 34. ... 1–24. 1.6.1.2 Ensemble averages; bulk magnetization. In order to compute, say, the x-magnetization from the whole sample, it isnecessary to add up the individual contributions
  7. relax_2

    https://www-keeler.ch.cam.ac.uk/lectures/relax2_a4.pdf
    9 Aug 2003: 6. 320. 2 320. 24. ω ω. ω ω. τω τ. ... 6.3.4.4 Relaxation of IEvaluating. 6–24. [ ][ ] ( )( ) ( ) ( )12 A A I Jpq p qp q.
  8. 1 Feb 2001: 3–1. 3 Basic concepts fortwo-dimensional NMR. ,QWURGXFWLRQ. The basic ideas of two-dimensional NMR will be introduced by reference tothe appearance of a COSY spectrum; later in this lecture the productoperator formalism will be used to predict the
  9. 2d_3_12

    https://www-keeler.ch.cam.ac.uk/lectures/2d_letter.pdf
    1 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
  10. 4–1 4 Coherence Selection: Phase Cycling and Gradient Pulses ...

    https://www-keeler.ch.cam.ac.uk/lectures/phasen_a4.pdf
    1 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
  11. C:/Documents and Settings/jhk10/My Documents/NMR Course 2004/../NMR…

    https://www-keeler.ch.cam.ac.uk/lectures/understanding/chapter_5.pdf
    24 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.

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