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Probing heteronuclear N-15-O-17 and C-13-O-17 connectivities and proximities by solid-state NMR spectroscopy

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Probing heteronuclear N-15-O-17 and C-13-O-17 connectivities and proximities by solid-state NMR spectroscopy. / Hung, Ivan; Uldry, Anne-Christine; Becker-Baldus, Johanna et al.
In: Journal of the American Chemical Society, Vol. 131, No. 5, 01.02.2009, p. 1820-1834.

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Harvard

Hung, I, Uldry, A-C, Becker-Baldus, J, Webber, AL, Wong, A, Smith, ME, Joyce, SA, Yates, JR, Pickard, CJ, Dupree, R & Brown, SP 2009, 'Probing heteronuclear N-15-O-17 and C-13-O-17 connectivities and proximities by solid-state NMR spectroscopy', Journal of the American Chemical Society, vol. 131, no. 5, pp. 1820-1834. https://doi.org/10.1021/ja805898d

APA

Hung, I., Uldry, A.-C., Becker-Baldus, J., Webber, A. L., Wong, A., Smith, M. E., Joyce, S. A., Yates, J. R., Pickard, C. J., Dupree, R., & Brown, S. P. (2009). Probing heteronuclear N-15-O-17 and C-13-O-17 connectivities and proximities by solid-state NMR spectroscopy. Journal of the American Chemical Society, 131(5), 1820-1834. https://doi.org/10.1021/ja805898d

Vancouver

Hung I, Uldry AC, Becker-Baldus J, Webber AL, Wong A, Smith ME et al. Probing heteronuclear N-15-O-17 and C-13-O-17 connectivities and proximities by solid-state NMR spectroscopy. Journal of the American Chemical Society. 2009 Feb 1;131(5):1820-1834. doi: 10.1021/ja805898d

Author

Hung, Ivan ; Uldry, Anne-Christine ; Becker-Baldus, Johanna et al. / Probing heteronuclear N-15-O-17 and C-13-O-17 connectivities and proximities by solid-state NMR spectroscopy. In: Journal of the American Chemical Society. 2009 ; Vol. 131, No. 5. pp. 1820-1834.

Bibtex

@article{616afeaaaca94ff6b4d1e86977c7e405,
title = "Probing heteronuclear N-15-O-17 and C-13-O-17 connectivities and proximities by solid-state NMR spectroscopy",
abstract = "Heteronuclear solid-state magic-angle spinning (MAS) NMR experiments for probing N-15-O-17 dipolar and J couplings are presented for [H-2(NH3),1-C-13,N-15,O-17(2)]glycine center dot(HCl)-H-2 and [N-15(2), O-17(2)]uracil. Two-dimensional N-15-O-17 correlation spectra are obtained using the R-3-HMQC experiment; for glycine center dot(HCl)-H-2, the intensity of the resolved peaks for the C=O and C-(OH)-H-2 O-17 resonances corresponds to the relative magnitude of the respective N-15-O-17 dipolar couplings. O-17-N-15 REDOR curves are presented for glycine center dot(HCl)-H-2; fits of the initial buildup (Delta S/S <0.2) yield effective dipolar couplings in agreement with (+/- 20%) the root-sum-squared dipolar couplings determined from the crystal structure. Experimental N-15-O-17 REAPDOR curves for the N-15 resonances in glycine center dot(HCl)-H-2 and uracil fit well to the universal curve presented by Goldbourt et al. (J. Am. Chem. Soc. 2003, 125,11194). Heteronuclear C-13-O-17 and N-15-O-17 J couplings were experimentally determined from fits of the quotient of the integrated intensity obtained in a heteronuclear and a homonuclear spin-echo experiment, S-Q(tau) = S-HET(tau)/S-HOM(tau). For glycine center dot(HCl)-H-2, (1)J(CO) was determined as 24.7 +/- 0.2 and 25.3 +/- 0.3 Hz for the C=O and C-(OH)-H-2 resonances, respectively, while for uracil, the average of the two NH center dot center dot center dot O hydrogen-bond-mediated J couplings was determined as 5.1 +/- 0.6 Hz. In addition, two-bond intramolecular J couplings, (2)J(OO) = 8.8 +/- 0.9 Hz and (2)J(N1,N3) = 2.7 +/- 0.1 Hz, were determined for glycine center dot(HCl)-H-2 and uracil, respectively. Excellent agreement was found with J couplings calculated using the CASTEP code using geometrically optimized crystal structures for glycine center dot HCl [(1)J(CO)(C=O) = 24.9 Hz, (1)J(CO)(C-OH) = 27.5 H Z, (2)J(OO) = 7.9 Hz] and uracil [(2h)J(N1,O4) = 6.1 Hz, (2h)J(N3,O4) = 4.6 Hz, (2)J(N1,N3) = 2.7 Hz].",
keywords = "DOUBLE-RESONANCE NMR, ANGLE-SPINNING NMR, INTEGER QUADRUPOLAR NUCLEI, QUANTUM CROSS-POLARIZATION, MEDIUM-RANGE ORDER, ROTATIONAL-ECHO, REAPDOR NMR, O-17 NMR, MAS NMR, DIPOLAR INTERACTIONS",
author = "Ivan Hung and Anne-Christine Uldry and Johanna Becker-Baldus and Webber, {Amy L.} and Alan Wong and Smith, {Mark E.} and Joyce, {Sin A.} and Yates, {Jonathan R.} and Pickard, {Chris J.} and Ray Dupree and Brown, {Steven P.}",
year = "2009",
month = feb,
day = "1",
doi = "10.1021/ja805898d",
language = "English",
volume = "131",
pages = "1820--1834",
journal = "Journal of the American Chemical Society",
issn = "1520-5126",
publisher = "AMER CHEMICAL SOC",
number = "5",

}

RIS

TY - JOUR

T1 - Probing heteronuclear N-15-O-17 and C-13-O-17 connectivities and proximities by solid-state NMR spectroscopy

AU - Hung, Ivan

AU - Uldry, Anne-Christine

AU - Becker-Baldus, Johanna

AU - Webber, Amy L.

AU - Wong, Alan

AU - Smith, Mark E.

AU - Joyce, Sin A.

AU - Yates, Jonathan R.

AU - Pickard, Chris J.

AU - Dupree, Ray

AU - Brown, Steven P.

PY - 2009/2/1

Y1 - 2009/2/1

N2 - Heteronuclear solid-state magic-angle spinning (MAS) NMR experiments for probing N-15-O-17 dipolar and J couplings are presented for [H-2(NH3),1-C-13,N-15,O-17(2)]glycine center dot(HCl)-H-2 and [N-15(2), O-17(2)]uracil. Two-dimensional N-15-O-17 correlation spectra are obtained using the R-3-HMQC experiment; for glycine center dot(HCl)-H-2, the intensity of the resolved peaks for the C=O and C-(OH)-H-2 O-17 resonances corresponds to the relative magnitude of the respective N-15-O-17 dipolar couplings. O-17-N-15 REDOR curves are presented for glycine center dot(HCl)-H-2; fits of the initial buildup (Delta S/S <0.2) yield effective dipolar couplings in agreement with (+/- 20%) the root-sum-squared dipolar couplings determined from the crystal structure. Experimental N-15-O-17 REAPDOR curves for the N-15 resonances in glycine center dot(HCl)-H-2 and uracil fit well to the universal curve presented by Goldbourt et al. (J. Am. Chem. Soc. 2003, 125,11194). Heteronuclear C-13-O-17 and N-15-O-17 J couplings were experimentally determined from fits of the quotient of the integrated intensity obtained in a heteronuclear and a homonuclear spin-echo experiment, S-Q(tau) = S-HET(tau)/S-HOM(tau). For glycine center dot(HCl)-H-2, (1)J(CO) was determined as 24.7 +/- 0.2 and 25.3 +/- 0.3 Hz for the C=O and C-(OH)-H-2 resonances, respectively, while for uracil, the average of the two NH center dot center dot center dot O hydrogen-bond-mediated J couplings was determined as 5.1 +/- 0.6 Hz. In addition, two-bond intramolecular J couplings, (2)J(OO) = 8.8 +/- 0.9 Hz and (2)J(N1,N3) = 2.7 +/- 0.1 Hz, were determined for glycine center dot(HCl)-H-2 and uracil, respectively. Excellent agreement was found with J couplings calculated using the CASTEP code using geometrically optimized crystal structures for glycine center dot HCl [(1)J(CO)(C=O) = 24.9 Hz, (1)J(CO)(C-OH) = 27.5 H Z, (2)J(OO) = 7.9 Hz] and uracil [(2h)J(N1,O4) = 6.1 Hz, (2h)J(N3,O4) = 4.6 Hz, (2)J(N1,N3) = 2.7 Hz].

AB - Heteronuclear solid-state magic-angle spinning (MAS) NMR experiments for probing N-15-O-17 dipolar and J couplings are presented for [H-2(NH3),1-C-13,N-15,O-17(2)]glycine center dot(HCl)-H-2 and [N-15(2), O-17(2)]uracil. Two-dimensional N-15-O-17 correlation spectra are obtained using the R-3-HMQC experiment; for glycine center dot(HCl)-H-2, the intensity of the resolved peaks for the C=O and C-(OH)-H-2 O-17 resonances corresponds to the relative magnitude of the respective N-15-O-17 dipolar couplings. O-17-N-15 REDOR curves are presented for glycine center dot(HCl)-H-2; fits of the initial buildup (Delta S/S <0.2) yield effective dipolar couplings in agreement with (+/- 20%) the root-sum-squared dipolar couplings determined from the crystal structure. Experimental N-15-O-17 REAPDOR curves for the N-15 resonances in glycine center dot(HCl)-H-2 and uracil fit well to the universal curve presented by Goldbourt et al. (J. Am. Chem. Soc. 2003, 125,11194). Heteronuclear C-13-O-17 and N-15-O-17 J couplings were experimentally determined from fits of the quotient of the integrated intensity obtained in a heteronuclear and a homonuclear spin-echo experiment, S-Q(tau) = S-HET(tau)/S-HOM(tau). For glycine center dot(HCl)-H-2, (1)J(CO) was determined as 24.7 +/- 0.2 and 25.3 +/- 0.3 Hz for the C=O and C-(OH)-H-2 resonances, respectively, while for uracil, the average of the two NH center dot center dot center dot O hydrogen-bond-mediated J couplings was determined as 5.1 +/- 0.6 Hz. In addition, two-bond intramolecular J couplings, (2)J(OO) = 8.8 +/- 0.9 Hz and (2)J(N1,N3) = 2.7 +/- 0.1 Hz, were determined for glycine center dot(HCl)-H-2 and uracil, respectively. Excellent agreement was found with J couplings calculated using the CASTEP code using geometrically optimized crystal structures for glycine center dot HCl [(1)J(CO)(C=O) = 24.9 Hz, (1)J(CO)(C-OH) = 27.5 H Z, (2)J(OO) = 7.9 Hz] and uracil [(2h)J(N1,O4) = 6.1 Hz, (2h)J(N3,O4) = 4.6 Hz, (2)J(N1,N3) = 2.7 Hz].

KW - DOUBLE-RESONANCE NMR

KW - ANGLE-SPINNING NMR

KW - INTEGER QUADRUPOLAR NUCLEI

KW - QUANTUM CROSS-POLARIZATION

KW - MEDIUM-RANGE ORDER

KW - ROTATIONAL-ECHO

KW - REAPDOR NMR

KW - O-17 NMR

KW - MAS NMR

KW - DIPOLAR INTERACTIONS

U2 - 10.1021/ja805898d

DO - 10.1021/ja805898d

M3 - Journal article

VL - 131

SP - 1820

EP - 1834

JO - Journal of the American Chemical Society

JF - Journal of the American Chemical Society

SN - 1520-5126

IS - 5

ER -