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Chapter 8 letter /5
https://www-keeler.ch.cam.ac.uk/lectures/Irvine/chapter8.pdf12 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. ( ) ( ) ( ) ( ). ( ) ( ) ( ) ( ). -
main.dvi
https://www-keeler.ch.cam.ac.uk/lectures/Irvine/chapter2.pdf5 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. -
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. -
Chapter 8 a4 /6
https://www-keeler.ch.cam.ac.uk/lectures/understanding/chapter_8.pdf24 Feb 2004: 13. 23 0 3. 11. 24 0 2. 112. 22 0 2. ... 11. 24 0 3. 24. 24 2 4. 23. 22 2 1. ( ) ( ) ( ) ( ). ( ) ( ) ( ) ( ). -
C:/Documents and Settings/jhk10/My Documents/NMR Course 2004/../NMR…
https://www-keeler.ch.cam.ac.uk/lectures/understanding/chapter_2.pdf24 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. -
Ch 6-9 probs /2
https://www-keeler.ch.cam.ac.uk/lectures/understanding/chapter_6_9_probs.pdf24 Feb 2004: 1 24 2 2 2+ ( )In a heteronuclear system a coherence order can be assigned to each spinseparately. -
Basis_Quante–
https://www-keeler.ch.cam.ac.uk/lectures/quant_letter.pdf1 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 -
relax_2
https://www-keeler.ch.cam.ac.uk/lectures/relax2_a4.pdf9 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. -
3–1 3 Basic concepts fortwo-dimensional NMR ���� ,QWURGXFWLRQ The ...
https://www-keeler.ch.cam.ac.uk/lectures/2d_a4.pdf1 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 -
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
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