Search

Search Funnelback University

Search powered by Funnelback
21 - 30 of 31 search results for :pc53 24 / |u:www-keeler.ch.cam.ac.uk where 0 match all words and 31 match some words.
  1. Results that match 1 of 2 words

  2. Chapter 7/3(A4)

    https://www-keeler.ch.cam.ac.uk/lectures/understanding/chapter_7.pdf
    24 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
  3. Chapter 9 letter

    https://www-keeler.ch.cam.ac.uk/lectures/Irvine/chapter9.pdf
    12 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
  4. select/ALL/5

    https://www-keeler.ch.cam.ac.uk/lectures/EMBOselect.pdf
    23 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
  5. Chapter 9 a4 /2

    https://www-keeler.ch.cam.ac.uk/lectures/understanding/chapter_9.pdf
    24 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
  6. main.dvi

    https://www-keeler.ch.cam.ac.uk/lectures/Irvine/chapter3.pdf
    5 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.
  7. Chapter 8 a4 /6

    https://www-keeler.ch.cam.ac.uk/lectures/understanding/chapter_8.pdf
    24 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. ( ) ( ) ( ) ( ). ( ) ( ) ( ) ( ).
  8. Development of a method for the measurement of long-range ...

    https://www-keeler.ch.cam.ac.uk/publications/lrjch.pdf
    7 Aug 2003: Development of a method for the. measurement of long-range 13C–1H coupling. constants from HMBC spectra. Richard A E Edden and James Keeler University of Cambridge, Department of Chemistry, Lensfield Rd, Cambridge,. CB2 1EW, U.K. Abstract. This
  9. relax_1

    https://www-keeler.ch.cam.ac.uk/lectures/relax1_a4.pdf
    9 Aug 2003: 13. 23 0 3. 11. 24 0 2. 112. 22 0 2. ... 11. 24 0 3. 24. 24 2 4. 23. 22 2 1. ( ) ( ) ( ) ( ). ( ) ( ) ( ) ( ).
  10. C:/Documents and Settings/jhk10/My Documents/NMR Course 2004/../NMR…

    https://www-keeler.ch.cam.ac.uk/lectures/understanding/chapter_3.pdf
    24 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.
  11. C:/Documents and Settings/jhk10/My Documents/Papers/broadband…

    https://www-keeler.ch.cam.ac.uk/publications/ProtonDecoupled.pdf
    9 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.

Refine your results

Search history

Recently clicked results

Recently clicked results

Your click history is empty.

Recent searches

Recent searches

Your search history is empty.