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The Keeler Group - Downloads
https://www-keeler.ch.cam.ac.uk/utilities/index.html10 Dec 2007: Broadband proton-decoupled proton spectra. Author:. Version:. Posted:. Andrew Pell. October 24, 2006. -
Chapter 7/2 Letter
https://www-keeler.ch.cam.ac.uk/lectures/Irvine/chapter7.pdf5 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 -
doi:10.1016/j.jmr.2007.09.002
https://www-keeler.ch.cam.ac.uk/publications/absjspectra.pdf17 Sep 2007: 13. 14. 1516. 17. 18. 19. 20. 21. 22. 23. 24. -
EMBO problems/2
https://www-keeler.ch.cam.ac.uk/lectures/EMBOprobs.pdf1 Feb 2001: 1 24 2 2 2+ ( )In a heteronuclear system a coherence order can be assigned to each spinseparately. -
doi:10.1016/S1090-7807(03)00186-1
https://www-keeler.ch.cam.ac.uk/publications/1DT1.pdf7 Oct 2003: and refocusing. Different slices were excited by stepping. the frequency offset for the selective pulses from 24 to. -
4–1 4 Coherence Selection: Phase Cycling and Gradient Pulses ...
https://www-keeler.ch.cam.ac.uk/lectures/phasen_letter.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 -
55th Experimental Nuclear Magnetic Resonance Conference Boston, 2014…
https://www-keeler.ch.cam.ac.uk/lectures/ENC_handout.pdf25 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). -
EUROMAR Zürich, 2014 Introduction toRelaxation Theory James Keeler…
https://www-keeler.ch.cam.ac.uk/lectures/Keeler_EUROMAR_handout.pdf26 Jun 2014: n0α). I rate depends on deviation from equilibrium population. Relaxation in terms of populations 24. -
Ch 6-9 probs letter /1
https://www-keeler.ch.cam.ac.uk/lectures/Irvine/ch6-9probs.pdf5 Mar 2002: 1 24 2 2 2+ ( )In a heteronuclear system a coherence order can be assigned to each spin. -
main.dvi
https://www-keeler.ch.cam.ac.uk/lectures/Irvine/chapter5.pdf5 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. -
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. -
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. -
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. -
relax_1
https://www-keeler.ch.cam.ac.uk/lectures/relax1_a4.pdf9 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. ( ) ( ) ( ) ( ). ( ) ( ) ( ) ( ). -
Development of a method for the measurement of long-range ...
https://www-keeler.ch.cam.ac.uk/publications/lrjch.pdf7 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 -
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. ( ) ( ) ( ) ( ). ( ) ( ) ( ) ( ). -
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 -
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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