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1 - 20 of 31 search results for katalk: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. The Keeler Group - Downloads

    https://www-keeler.ch.cam.ac.uk/utilities/index.html
    10 Dec 2007: Broadband proton-decoupled proton spectra. Author:. Version:. Posted:. Andrew Pell. October 24, 2006.

  3. Chapter 7/2 Letter

    https://www-keeler.ch.cam.ac.uk/lectures/Irvine/chapter7.pdf
    5 Mar 2002: 7–1. 7 Two-dimensional NMR†. 7.1 Introduction. The basic ideas of two-dimensional NMR will be introduced by reference to theappearance of a COSY spectrum; later in this chapter the product operatorformalism will be used to predict the form of

  4. doi:10.1016/j.jmr.2007.09.002

    https://www-keeler.ch.cam.ac.uk/publications/absjspectra.pdf
    17 Sep 2007: 13. 14. 1516. 17. 18. 19. 20. 21. 22. 23. 24.

  5. EMBO problems/2

    https://www-keeler.ch.cam.ac.uk/lectures/EMBOprobs.pdf
    1 Feb 2001: 1 24 2 2 2+ ( )In a heteronuclear system a coherence order can be assigned to each spinseparately.

  6. doi:10.1016/S1090-7807(03)00186-1

    https://www-keeler.ch.cam.ac.uk/publications/1DT1.pdf
    7 Oct 2003: and refocusing. Different slices were excited by stepping. the frequency offset for the selective pulses from 24 to.

  7. 4–1 4 Coherence Selection: Phase Cycling and Gradient Pulses ...

    https://www-keeler.ch.cam.ac.uk/lectures/phasen_letter.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

  8. 55th Experimental Nuclear Magnetic Resonance Conference Boston, 2014…

    https://www-keeler.ch.cam.ac.uk/lectures/ENC_handout.pdf
    25 Mar 2014: gives considerable flexibility. Spin echoes 24. Spin echoes: summary. I in homonuclear systems spin echoes allow the coupling toevolve while effectively suppressing the evolution due to theoffset (shift).

  9. EUROMAR Zürich, 2014 Introduction toRelaxation Theory James Keeler…

    https://www-keeler.ch.cam.ac.uk/lectures/Keeler_EUROMAR_handout.pdf
    26 Jun 2014: n0α). I rate depends on deviation from equilibrium population. Relaxation in terms of populations 24.

  10. Ch 6-9 probs letter /1

    https://www-keeler.ch.cam.ac.uk/lectures/Irvine/ch6-9probs.pdf
    5 Mar 2002: 1 24 2 2 2+ ( )In a heteronuclear system a coherence order can be assigned to each spin.

  11. main.dvi

    https://www-keeler.ch.cam.ac.uk/lectures/Irvine/chapter5.pdf
    5 Mar 2002: Is the magnet sufficientlyhomogeneous to be of use? E 5–2A careful pulse calibration experiment determines that the 180 pulse is 24.8µs.

  12. 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.

  13. 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.

  14. 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. ( ) ( ) ( ) ( ). ( ) ( ) ( ) ( ).

  15. 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.

  16. 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. ( ) ( ) ( ) ( ). ( ) ( ) ( ) ( ).

  17. 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

  18. 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. ( ) ( ) ( ) ( ). ( ) ( ) ( ) ( ).

  19. 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

  20. 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.

  21. 3–1 3 Basic concepts fortwo-dimensional NMR ���� ,QWURGXFWLRQ The ...

    https://www-keeler.ch.cam.ac.uk/lectures/2d_a4.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 tothe appearance of a COSY spectrum; later in this lecture the productoperator formalism will be used to predict the

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