PC71d: 1D double quantum excitation POST_C7 pulse program for TopSpin2.1

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Double-quantum excitation with PC7 pulse sequence

Since non-phase cycling is applied to the PC7 excitation pulse, four-phase cycling is applied to the detection pulse P1 for selecting the 0Q -> -1Q coherence order jump, and four-phase cycling is applied to the PC7 reconversion pulse for filtering DQ coherences.

*** Outline ***

Code for Avance III spectrometers with topSpin2.1 operating system

;pc71d (TopSpin 2.0)

;1D DQ excitation sequence POST_C7
;for setup of the 2D INADEQUATE type experiments
;Hohwy, M. Jakobsen, H.J. Eden, M. Levitt, M.H., Nielsen, N.C., 
;J. Chem. Phys. 108, 2686-2694 (1998)
;revised 09/09/03 JOS

;Avance II+ version
;parameters:
;d1  : recycle delay
;d20 : delay between saturation pulses

;pl1 : f1 power level for presaturation pulses and detection pulse
;pl7 : for POST C7 recoupling sequence, B1=7*cnst31 in Hz
;p1  : detection pulse at pl1

;cnst31 : spinning speed, make sure cnst31>1000
;l1  : number of composite C7 cycles for DQ excitation 
;l20 : # of pulses in saturation pulse train, 0 if undesired
;ns  : n*16
;zgoptns :-Dpresat or blank

;$COMMENT=DQ excitation sequence post-C7
;$CLASS=Solids
;$DIM=1D
;$TYPE=direct excitation
;$SUBTYPE=homonuclear correlation
;$OWNER=Bruker

define pulse tau1
  "tau1=((0.25s/cnst31)/7)"    ; 90° pulse
define pulse tau4
  "tau4=((1s/cnst31)/7)"       ;360° pulse
define pulse tau3
  "tau3=((0.75s/cnst31)/7)"    ;270° pulse

"d31=1s/cnst31"

;cnst11 : to adjust t=0 for acquisition, if digmod = baseopt
"acqt0=1u*cnst11"

#include <rot_prot.incl>
#include <Avancesolids.incl>

  ze                           ;acquire into a cleared memory
1 d31

#ifdef presat                  ;set with -Dpresat
pres, d20                      ;delay between saturation pulses
  (p1 pl1 ph1):f1              ;saturation loop if required
  lo to pres times l20
#endif /* presat */

2 d1
  1m rpp11                     ;reset the phase program ph11 pointer to the first element
  1m rpp12                     ;reset the phase program ph12 pointer to the first element
  1m rpp13                     ;reset the phase program ph13 pointer to the first element
  1m rpp14                     ;reset the phase program ph14 pointer to the first element
  10u reset:f1
  1u pl7:f1

3 tau1:f1 ph11 ipp13 ipp14     ;c7 excitation, 1 loop = 2*Tr/7, 
                               ;increment reconversion pulse phase ph13 and ph14 pointers
                               ;to the next phase in the lists
  tau4:f1 ph12 ipp12           ;increment phase ph12 pointer
  tau3:f1 ph11 ipp11           ;increment phase ph11 pointer
                               ;to the next phase in the lists
  lo to 3 times l1

  3u

6 tau1:f1 ph13                 ;c7 reconversion, 1 loop = 2*Tr/7,
  tau4:f1 ph14 ipp14           ;increment phase ph14 pointer
  tau3:f1 ph13 ipp13           ;increment phase ph13 pointer
                               ;to the next phase in the lists
  lo to 6 times l1

  p1:f1 ph5 pl1:f1             ;detection pulse
  2u 
  gosc ph31                    ;gosc does not loop to 1
                               ;start ADC with ph31 signal routing

                               ;DQ filtering (four phase cycling):
  1m ip13                      ;increments all phases of ph13 by 90°
  1m ip14                      ;increments all phases of ph14 by 90°
  ;1m ip13*16384                ;increments all phases of ph13 by 90°
  ;1m ip14*16384                ;increments all phases of ph14 by 90°

  lo to 1 times ns             ;next scan
  100m wr #0                   ;save data
HaltAcqu, 1m
exit

ph1= 0                         ;for saturation pulse

ph11 = (float,45.0)   0.00  51.43 102.86 154.29 205.71 257.14 308.57 
ph12 = (float,45.0) 180.00 231.43 282.86 334.29 385.71 437.14 488.57 
ph13 = (float,90.0)   0.00  51.43 102.86 154.29 205.71 257.14 308.57 
ph14 = (float,90.0) 180.00 231.43 282.86 334.29 385.71 437.14 488.57 

;ph11=(65536)     0  9362 18725 28087 37449 46811 56174 
;ph12=(65536) 32768 42130 51493 60855  4681 14043 23406 
;ph13=(65536)     0  9362 18725 28087 37449 46811 56174 
;ph14=(65536) 32768 42130 51493 60855  4681 14043 23406 


ph5=   0 0 0 0 2 2 2 2 1 1 1 1 3 3 3 3
ph31 = 0 2 0 2 2 0 2 0 1 3 1 3 3 1 3 1    ;ph31 = ph5 + 2*ph13
  

References

  1. N. Chandrakumar
    1D double quantum filter NMR studies,
    in Annual Reports on NMR Spectroscopy, Graham A. Webb (Ed.), Elsevier, Amsterdam, vol. 67, pages 265-329 (2009).
    Abstract
  2. Giuseppe Pileio, Maria Concistrè, Neville McLean, Axel Gansmüller, Richard C. D. Brown, and Malcolm H. Levitt
    Analytical theory of γ-encoded double-quantum recoupling sequences in solid-state nuclear magnetic resonance,
    J. Magn. Reson. 186, 65-74 (2007).
    Abstract
  3. M. J. Potrzebowski, J. Gajda, W. Ciesielski, and I. M. Montesinos
    Distance measurements in disodium ATP hydrates by means of 31P double quantum two-dimensional solid-state NMR spectroscopy, (PC7, asymmetric peaks)
    J. Magn. Reson. 179, 173-181 (2006).
    Abstract
  4. Sebastian Olejniczak, Pawel Napora, Jaroslaw Gajda, Wlodzimierz Ciesielski, Marek J. Potrzebowski
    31P double-quantum solid-state NMR study of phosphoroorganic compounds with (O)P-O-P-(O), (S)P-O-P(S) and (S)P-S-P(O) unit, (PC7)
    Solid State Nucl. Magn. Reson. 30, 141-149 (2006).
    Abstract
  5. Colan E. Hughes and Marc Baldus
    Magic-angle-spinning solid-state NMR applied to polypeptides and proteins,
    in Annual Reports on NMR Spectroscopy, Graham A. Webb (Ed.), Elsevier, Amsterdam, vol. 55, pages 121-158 (2005).
    Abstract
  6. Ingo Schnell
    Dipolar recoupling in fast-MAS solid-state NMR spectroscopy,
    Prog. Nucl. Magn. Reson. Spectrosc. 45, 145-207 (2004).
    Abstract
  7. Yoh Matsuki, Hideo Akutsu, and Toshimichi Fujiwara
    Precision 1H-1H distance measurement via 13C NMR signals: utilization of 1H-1H double-quantum dipolar interactions recoupled under magic angle spinning conditions,
    Magn. Reson. Chem. 42, 291-300 (2004).
    Abstract
  8. T. Karlsson, J. M. Popham, J. R. Long, N. Oyler, and G. P. Drobny
    A study of homonuclear dipolar recoupling pulse sequences in solid-state nuclear magnetic resonance, (DRAWS, PC7, SPC5, R1426, R2246; phase cycling)
    J. Am. Chem. Soc. 125, 7394-7407 (2003).
    Abstract
  9. M. Bjerring, T. Vosegaard, A. Malimendal, and N.C. Nielsen
    Methodological development of solid-state NMR for characterization of membrane proteins, (PC7, C7)
    Concepts Magn. Reson. A 18, 111-129 (2003).
    Abstract
  10. G. P. Drobny, J. R. Long, T. Karlsson, W. Shaw, J. Popham, N. Oyler, P. Bower, J. Stringer, D. Gregory, M. Mehta, and P. S. Stayton
    Structural studies of biomateriaux using double-quantum solid-state NMR spectroscopy,
    Annu. Rev. Phys. Chem. 54, 531-571 (2003).
    Abstract
  11. Wyndham Bolling Blanton
    High Performance Computations in NMR,
    Berkeley, 2002.
    Ph.D
  12. Juraj Pivarč
    Application of the Multiple Quantum NMR Spectroscopy for Investigation of the Dipole-Dipole Couplings in Amorphous Polymers,
    Halle, 4 July 2000.
    Dissertation
  13. Andreas Brinkmann, Mattias Edén, and Malcolm H. Levitt
    Synchronous helical pulse sequences in magic-angle spinning nuclear magnetic resonance: Double quantum recoupling of multiple-spin systems, (CNnν: C721, C1445, C144-5, SC1445; phase cycling)
    J. Chem. Phys. 112, 8539-8554 (2000).
    Abstract
  14. Mattias Edén, Andreas Brinkmann, Henrik Luthman, Lars Eriksson, and Malcolm H. Levitt
    Determination of molecular geometry by high-order multiple-quantum evolution in solid-state NMR,
    J. Magn. Reson. 144, 266-279 (2000).
    Abstract
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    Multiple-quantum relaxation in the magic-angle-spinning NMR of 13C spin pairs, (C7, phase cycling)
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  16. Mei Hong
    Solid-state dipolar INADEQUATE NMR spectroscopy with a large double-quantum spectral width,
    J. Magn. Reson. 136, 86–91 (1999).
    Abstract
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    Efficient multispin homonuclear double-quantum recoupling for magic-angle spinning NMR: 13C-13C correlation spectroscopy of U-13C-erythromycin A, (combined MLEV refocusing and C7: CMR7; dependence of DQF efficiency on 1H CW decoupling field strength during mixing; sample size)
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    Abstract
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    Chem. Phys. Lett. 293, 173-179 (1998).
    Abstract
  19. M. Hohwy, H. J. Jakobsen, M. Edén, M. H. Levitt, and N. C. Nielsen
    Broadband dipolar recoupling in the nuclear magnetic resonance of rotating solids: A compensated C7 pulse sequence,
    J. Chem. Phys. 108, 2686-2694 (1998).
    Abstract
    PC7 pulse sequence

    Definition of PC7 excitation pulse.

  20. Helen Geen, Johannes Gottwald, Robert Graf, Ingo Schnell, Hans W. Spiess, and Jeremy J. Titman
    Elucidation of dipolar coupling networks under magic-angle spinning,
    J. Magn. Reson. 125, 224-227 (1997).
    Abstract
  21. W. A. Dollase, M. Feike, H. Förster, T. Schaller, I. Schnell, A. Sebald, and S. Steuernagel
    A 2D 31P MAS NMR study of polycrystalline Cd3(PO4)2,
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    Abstract
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    Efficient dipolar recoupling in the NMR of rotating solids. A sevenfold symmetric radiofrequency pulse sequence, (C7, phase cycling)
    Chem. Phys. Lett. 242, 304-309 (1995).
    Abstract
    C7 pulse sequence

    Definition of C7 excitation pulse.

  23. Yoshitaka Ishii, Jun Ashida, and Takehiko Terao
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    Chem. Phys. Lett. 246, 439-445 (1995).
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Solid-state NMR bibliography for:

Aluminum-27
Antimony-121/123
Arsenic-75
Barium-135/137
Beryllium-9
Bismuth-209
Boron-11
Bromine-79/81
Calcium-43
Cesium-133
Chlorine-35/37
Chromium-53
Cobalt-59
Copper-63/65
Deuterium-2
Gallium-69/71
Germanium-73
Gold-197
Hafnium-177/179
Indium-113/115
Iodine-127
Iridium-191/193
Krypton-83
Lanthanum-139
Lithium-7
Magnesium-25
Manganese-55
Mercury-201
Molybdenum-95/97
Neon-21
Nickel-61
Niobium-93
Nitrogen-14
Osmium-189
Oxygen-17
Palladium-105
Potassium-39/41
Rhenium-185/187
Rubidium-85/87
Ruthenium-99/101
Scandium-45
Sodium-23
Strontium-87
Sulfur-33
Tantalum-181
Titanium-47/49
Vanadium-51
Xenon-131
Zinc-67
Zirconium-91
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