Physics:Solid-state nuclear magnetic resonance

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Solid-state 900 MHz (21.1 T[1]) NMR spectrometer at the Canadian National Ultrahigh-field NMR Facility for Solids

Solid-state NMR (ssNMR) spectroscopy is a technique for characterizing atomic level structure in solid materials e.g. powders, single crystals and amorphous samples and tissues using nuclear magnetic resonance (NMR) spectroscopy. The anisotropic part of many spin interactions are present in solid-state NMR, unlike in solution-state NMR where rapid tumbling motion averages out many of the spin interactions. As a result, solid-state NMR spectra are characterised by larger linewidths than in solution state NMR, which can be utilized to give quantitative information on the molecular structure, conformation and dynamics of the material. Solid-state NMR is often combined with magic angle spinning to remove anisotropic interactions and improve the resolution as well as the sensitivity of the technique.

Bruker MAS rotors. From left to right: 1.3 mm (up to 67 kHz), 2.5 mm (up to 35 kHz), 3.2 mm (up to 24 kHz), 4 mm (up to 15 kHz), 7 mm (up to 7 kHz)

Nuclear spin interactions

The resonance frequency of a nuclear spin depends on the strength of the magnetic field at the nucleus, which can be modified by isotropic (e.g. chemical shift, isotropic J-coupling) and anisotropic interactions (e.g. chemical shift anisotropy, dipolar interactions). In a classical liquid-state NMR experiment, molecular tumbling coming from Brownian motion averages anisotropic interactions to zero and they are therefore not reflected in the NMR spectrum. However, in media with no or little mobility (e.g. crystalline powders, glasses, large membrane vesicles, molecular aggregates), anisotropic local fields or interactions have substantial influence on the behaviour of nuclear spins, which results in the line broadening of the NMR spectra.

Chemical shielding

Main page: Physics:Chemical shift

Chemical shielding is a local property of each nuclear site in a molecule or compound, and is proportional to the applied external magnetic field. The external magnetic field induces currents of the electrons in molecular orbitals. These induced currents create local magnetic fields that lead to characteristic changes in resonance frequency. These changes can be predicted from molecular structure using empirical rules or quantum-chemical calculations.

In general, the chemical shielding is anisotropic because of the anisotropic distribution of molecular orbitals around the nuclear sites. Under sufficiently fast magic angle spinning, or under the effect of molecular tumbling in solution-state NMR, the anisotropic dependence of the chemical shielding is time-averaged to zero, leaving only the isotropic chemical shift.

Dipolar coupling

Vectors important for dipolar coupling between nuclear spins I1 and I2. θ is the angle between the vector connecting I1 and I2, and the magnetic field B.

Nuclear spins exhibit a magnetic dipole moment, which generates a magnetic field that interacts with the dipole moments of other nuclei (dipolar coupling). The magnitude of the interaction is dependent on the gyromagnetic ratio of the spin species, the internuclear distance r, and the orientation, with respect to the external magnetic field B, of the vector connecting the two nuclear spins (see figure). The maximum dipolar coupling is given by the dipolar coupling constant d,

[math]\displaystyle{ d = \hbar \left( \frac{\mu_0}{4 \pi} \right) \frac{1}{r^3}\gamma_1 \gamma_2 }[/math],

where γ1 and γ2 are the gyromagnetic ratios of the nuclei, [math]\displaystyle{ \hbar }[/math] is the reduced Planck's constant, and [math]\displaystyle{ \mu_0 }[/math] is the vacuum permeability. In a strong magnetic field, the dipolar coupling depends on the angle θ between the internuclear vector and the external magnetic field B (figure) according to

[math]\displaystyle{ D \propto 3\cos^2\theta - 1 }[/math].

D becomes zero for [math]\displaystyle{ \theta_m = \arccos \sqrt{1/3}= \arctan \sqrt{2} \simeq 54.7^\circ }[/math]. Consequently, two nuclei with a dipolar coupling vector at an angle of θm = 54.7° to a strong external magnetic field have zero dipolar coupling. θm is called the magic angle. Magic angle spinning is typically used to remove dipolar couplings weaker than the spinning rate.

Quadrupolar interaction

Nuclei with a spin quantum number >1/2 have a non-spherical charge distribution and an associated electric quadrupole moment tensor. The nuclear electric quadrupole moment couples with surrounding electric field gradients. The nuclear quadrupole coupling is one of the largest interactions in NMR spectroscopy, often comparable in size to the Zeeman coupling. When the nuclear quadrupole coupling is not negligible relative to the Zeeman coupling, higher order corrections are needed to describe the NMR spectrum correctly. In such cases, the first-order correction to the NMR transition frequency leads to a strong anisotropic line broadening of the NMR spectrum. However, all symmetric transitions, between [math]\displaystyle{ m_I }[/math] and [math]\displaystyle{ -m_I }[/math] levels are unaffected by the first-order frequency contribution. The second-order frequency contribution depends on the P4 Legendre polynomial, which has zero points at 30.6° and 70.1°. These anisotropic broadenings can be removed using DOR (DOuble angle Rotation) where you spin at two angles at the same time, or DAS (Double Angle Spinning)[2] where you switch quickly between the two angles. Both techniques were developed in the late 1980s, and require specialized hardware (probe). Multiple quantum magic angle spinning (MQMAS) NMR was developed in 1995 and has become a routine method for obtaining high resolution solid-state NMR spectra of quadrupolar nuclei.[3][4] A similar method to MQMAS is satellite transition magic angle spinning (STMAS) NMR developed in 2000.

J-coupling

The J-coupling or indirect nuclear spin-spin coupling (sometimes also called "scalar" coupling despite the fact that J is a tensor quantity) describes the interaction of nuclear spins through chemical bonds. J-couplings are not always resolved in solids owing to the typically large linewdiths observed in solid state NMR.

Other interactions

Paramagnetic substances are subject to the Knight shift.

Solid-state NMR line shapes

Powder pattern

Simulations of the shape of different powder patterns for different asymmetry [math]\displaystyle{ \eta }[/math] and chemical shift anisotropy [math]\displaystyle{ \Delta_{CS} }[/math]parameters.

A powder pattern arises in powdered samples where crystallites are randomly oriented relative to the magnetic field so that all molecular orientations are present. In presence of a chemical shift anisotropy interaction, each orientation with respect to the magnetic field gives a different resonance frequency. If enough crystallites are present, all the different contributions overlap continuously and lead to a smooth spectrum.

Fitting of the pattern in a static ssNMR experiment gives information about the shielding tensor, which are often described by the isotropic chemical shift [math]\displaystyle{ \delta_{iso} }[/math], the chemical shift anisotropy parameter [math]\displaystyle{ \Delta_{CS} }[/math], and the asymmetry parameter [math]\displaystyle{ \eta }[/math].[5]

Dipolar pattern

Further information: Pake doublet
Dipolar powder pattern (Pake pattern)

The dipolar powder pattern (also Pake pattern) has a very characteristic shape that arises when two nuclear spins are coupled together within a crystallite. The splitting between the maxima (the "horns") of the pattern is equal to the dipolar coupling constant [math]\displaystyle{ d }[/math].:[6]

[math]\displaystyle{ d = \hbar \left( \frac{\mu_0}{4 \pi} \right) \frac{1}{r^3}\gamma_1 \gamma_2 }[/math]

where γ1 and γ2 are the gyromagnetic ratios of the dipolar-coupled nuclei, [math]\displaystyle{ r }[/math] is the internuclear distance, [math]\displaystyle{ \hbar }[/math] is the reduced Planck's constant, and [math]\displaystyle{ \mu_0 }[/math] is the vacuum permeability.

Essential solid-state techniques

Magic angle spinning

Main page: Magic angle spinning
Simulation of an increasing MAS rate on the 13C solid-state NMR spectrum of 13C-Glycine at 9.4 T (400 MHz 1H frequency). MAS introduces a set of spinning sidebands separated from the isotropic frequency by a multiple of the spinning rate.

Magic angle spinning (MAS) is a technique routinely used in solid-state NMR to produce narrower NMR and more intense NMR lines. This is achieved by rotating the sample at the magic angle θm (ca. 54.74°, where cos2θm=1/3) with respect to the direction of the magnetic field, which has the effect to cancel, at least partially, anisotropic nuclear interactions such as dipolar, chemical shift anisotropy, and quadrupolar interactions. To achieve the complete averaging of these interactions, the sample needs to be spun at a rate that is at least higher than the largest anisotropy.

Spinning a powder sample at a slower rate than the largest component of the chemical shift anisotropy results in an incomplete averaging of the interaction, and produces a set of spinning sidebands in addition to the isotropic line, centred at the isotropic chemical shift. Spinning sidebands are sharp lines separated from the isotropic frequency by a multiple of the spinning rate. Although spinning sidebands can be used to measure anisotropic interactions, they are often undesirable and removed by spinning the sample faster or by recording the data points synchronously with the rotor period.

Cross-polarisation

Cross-polarization pulse sequence
The CP pulse sequence. The sequence starts with a 90º pulse on the abundant channel (typically H). Then CP contact pulses matching the Hartmann-Hahn condition are applied to transfer the magnetisation from H to X. Finally, the free induction decay (FID) of the X nuclei is detected, typically with 1H decoupling.

Cross-polarization (CP) if a fundamental RF pulse sequence and a building-block in many solid-state NMR. It is typically used to enhance the signal of a dilute nuclei with a low gyromagnetic ratio (e.g. 13C, 15N) by magnetization transfer from an abundant nuclei with a high gyromagnetic ratio (e.g. 1H), or as a spectral editing method to get through space information (e.g. directed 15N→13C CP in protein spectroscopy).

To establish magnetization transfer, RF pulses ("contact pulses") are simultaneously applied on both frequency channels to produce [math]\displaystyle{ B_1 }[/math] fields whose strength fulfil the Hartmann–Hahn condition:[7][8]

[math]\displaystyle{ \gamma_H B_1(^{1}\text{H}) = \gamma_X B_1(\text{X}) \pm n \omega_R }[/math]

where [math]\displaystyle{ \gamma }[/math] are the gyromagnetic ratios, [math]\displaystyle{ \omega_R }[/math] is the spinning rate, and [math]\displaystyle{ n }[/math] is an integer. In practice, the pulse power, as well as the length of the contact pulse are experimentally optimised. The power of one contact pulse is typically ramped to achieve a more broadband and efficient magnetisation transfer.

Decoupling

Spin interactions can be removed (decoupled) to increase the resolution of NMR spectra during the detection, or to extend the lifetime of the nuclear magnetization.

Heteronuclear decoupling is achieved by radio-frequency irradiation on at the frequency of the nucleus to be decoupled, which is often 1H. The irradiation can be continuous (continuous wave decoupling[9]), or a series of pulses that extend the performance and the bandwidth of the decoupling (TPPM,[10] SPINAL-64,[11] SWf-TPPM[12])

Homonuclear decoupling is achieved with multiple-pulse sequences (WAHUHA,[13] MREV-8,[14] BR-24,[15] BLEW-12,[16] FSLG[17]), or continuous wave modulation (DUMBO,[18] eDUMBO[19]). Dipolar interactions can also be removed with magic angle spinning. Ultra fast MAS (from 60 kHz up to above 111 kHz) is an efficient way to average all dipolar interactions, including 1H-1H homonuclear dipolar interactions, which extends the resolution of 1H spectra and enables the usage of pulse sequences used in solution state NMR.[20][21]

Advanced solid-state NMR spectroscopy

Rotational Echo DOuble Resonance (REDOR)

Rotational Echo DOuble Resonance (REDOR) pulse sequence. The first excitation step (90º pulse or CP step) puts the magnetisation in the transverse plane. Then two trains of 180º pulses synchronised with the rotor half period are applied on the Y channel to reintroduce X-Y heteronuclear dipolar interactions. The trains of pulses are interrupted by a 180º pulse on the X channel that allows the refocussing of the X magnetisation for the X-detection (spin echo). The delay between the 90º pulse and the beginning of the acquisition is referred to as the "rephrasing time".

Rotational Echo DOuble Resonance (REDOR) experiment,[22][23] are a type of heteronuclear dipolar recoupling experiment which enable one to re-introduce heteronuclear dipolar couplings averaged by MAS. The reintroduction of such dipolar coupling reduce the intensity of the NMR signal intensity compared to a reference spectrum where no dephasing pulse is used. REDOR can be used to measure heteronuclear distances, and are the basis of NMR crystallographic studies.

Ultra Fast MAS for 1H NMR

The strong 1H-1H homonuclear dipolar interactions associated with broad NMR lines and short T2 relaxation time effectively relegate proton for bimolecular NMR. Recent developments of faster MAS, and reduction of dipolar interactions by deuteration have made proton ssNMR as versatile as in solution. This includes spectral dispersion in multi-dimensional experiments[24] as well as structurally valuable restraints and parameters important for studying material dynamics.[25]

Ultra-fast NMR and the associated sharpening of the NMR lines enables NMR pulse sequences to capitalize on proton-detection to improve the sensitivity of the experiments compared to the direct detection of a spin-1/2 system (X). Such enhancement factor [math]\displaystyle{ \xi }[/math] is given by:

[math]\displaystyle{ \xi \propto \left(\frac{\gamma_H}{\gamma_X}\right)^{3/2} \left(\frac{W_X}{W_H}\right)^{1/2} \left(\frac{Q_H}{Q_X}\right)^{1/2} }[/math]

where [math]\displaystyle{ \gamma }[/math] are the gyromagnetic ratios, [math]\displaystyle{ W }[/math] represent the NMR line widths, and [math]\displaystyle{ Q }[/math] represent the quality factor of the probe resonances.[26]

MAS-Dynamic Nuclear Polarisation (MAS-DNP)

Further information: Dynamic nuclear polarization

Magic angle spinning Dynamic Nuclear Polarization (MAS-DNP) is a technique that increases the sensitivity of NMR experiments by several orders of magnitude.[27][28] It involves the transfer of the very high electron polarisation from unpaired electrons to nearby nuclei. This is achieved at cryogenic temperatures by the means of a continuous microwave irradiation coming from a klystron or a Gyrotron, with a frequency close to the corresponding electron paramagnetic resonance (EPR) frequency.

The development in the MAS-DNP instrumentation, as well as the improvement of polarising agents (TOTAPOL, AMUPOL, TEKPOL, etc.[29]) to achieve a more efficient transfer of polarisation has dramatically reduced experiments times which enabled the observation of surfaces,[30] insensitive isotopes,[31] and multidimensional experiments on low natural abundance nuclei,[32] and diluted species.[33]

Applications

Solid-state NMR spectroscopy serves as an effective analytical tool in biological, organic, and inorganic chemistry due to its close resemblance to liquid-state spectra while providing additional insights into anisotropic interactions.[34]

It is used to characterize chemical composition, supramolecular structure, local motions, kinetics, and thermodynamics, with the special ability to assign the observed behavior to specific sites in a molecule. It is also crucial in the area of surface and interfacial chemistry.[35]

Biology and Medicine

Proteins and bioaggregates

Solid-state NMR is used to study insoluble proteins and proteins very sensitive to their environment such as membrane proteins[36] and amyloid fibrils.[37] The latter topic relates to protein aggregation diseases such as Alzheimer's disease and Parkinson's disease. Solid-state NMR spectroscopy complements solution-state NMR spectroscopy and beam diffraction methods (e.g. X-ray crystallography, electron microscopy). Despite often requiring isotopic enrichment,[38] ssNMR has the advantage that little sample preparation is required and can be used on not just dry or frozen samples, but also fully hydrated samples or native non-crystalline tissues.[39] Solid-state NMR structure elucidation of proteins has traditionally been based on secondary chemical shifts and spatial contacts between nuclei.

Biomaterials

Solid-state NMR has also been successfully used to study biomaterials such as bone,[40][41] teeth,[42][43] hair,[44] silk,[45] wood,[46] as well as viruses,[47][48] plants,[49][50] cells,[51][52] biopsies,[53] and even live animals.[54]

Drugs and drug delivery systems

Other ssNMR applications are in the field of pharmaceutical research.[55]

Firstly, it plays a pivotal role in the characterizatio of drug polymorphs and solid dispersions. This is useful to minimize risks linked with solid-state form changes: the determination of the solid form of an active pharmaceutical ingredient plays a pivotal role in ensuring controlled bioavailability and stability; alterations can impact the efficacy of drugs profoundly. Analysis of molecular-level interactions facilitates also the formulation development of amorphous solid dispersions, targeting enhanced solubility.

Furthermore, ssNMR aids in characterizing porous materials tailored for drug delivery systems, thus enhabling scientists to design carriers and formulations that heighten drug efficacy. [56]

Materials science

Solid-state NMR has been successfully used to study metal organic frameworks (MOFS),[57] batteries,[58][59][60] surfaces of nanoporous materials,[61] polymers.[62]

Art conservation

NMR can also be applied to art conservation. Different salts and moisture levels can be detected through the use of solid state NMR. However, sampling sizes retrieved from works of art in order to run through these large conducting magnets typically exceed levels deemed acceptable. Unilateral NMR techniques use portable magnets that are applied to the object of interest, bypassing the need for sampling.[63]

References

  1. ↑ "National Ultrahigh-Field NMR Facility for Solids". http://nmr900.ca/instrument_e.html. Retrieved 2014-09-22. 
  2. ↑ Qian, Chunqi; Pines, Alex; Martin, Rachel W. (2007-09-01). "Design and construction of a contactless mobile RF coil for double resonance variable angle spinning NMR" (in en). Journal of Magnetic Resonance 188 (1): 183–189. doi:10.1016/j.jmr.2007.06.006. ISSN 1090-7807. PMID 17638585. Bibcode: 2007JMagR.188..183Q. https://www.sciencedirect.com/science/article/abs/pii/S109078070700198X. 
  3. ↑ Frydman Lucio; Harwood John S (1995). "Isotropic Spectra of Half-Integer Quadrupolar Spins from Bidimensional Magic-Angle Spinning NMR". J. Am. Chem. Soc. 117 (19): 5367–5368. doi:10.1021/ja00124a023. 
  4. ↑ Massiot D.; Touzo B.; Trumeau D.; Coutures J. P.; Virlet J.; Florian P.; Grandinetti P. J. (1996). "Two-dimensional Magic-Angle Spinning Isotropic Reconstruction Sequences for Quadrupolar Nuclei". Solid-State NMR 6 (1): 73–83. doi:10.1016/0926-2040(95)01210-9. PMID 8925268. 
  5. ↑ Duer, Melinda J. (2004). Introduction to solid-state NMR spectroscopy. Oxford, UK: Blackwell. ISBN 1-4051-0914-9. OCLC 53178681. https://www.worldcat.org/oclc/53178681. 
  6. ↑ Duer, Melinda J. (2004). Introduction to solid-state NMR spectroscopy. Oxford, UK: Blackwell. ISBN 1-4051-0914-9. OCLC 53178681. https://www.worldcat.org/oclc/53178681. 
  7. ↑ Hartmann, S. R.; Hahn, E. L. (1962). "Nuclear Double Resonance in the Rotating Frame". Phys. Rev. 128 (5): 2042–2053. doi:10.1103/PhysRev.128.2042. Bibcode: 1962PhRv..128.2042H. http://astrophysics.fic.uni.lodz.pl/100yrs/pdf/09/065.pdf. 
  8. ↑ Stejskal, E.O; Schaefer, Jacob; Waugh, J.S (October 1977). "Magic-angle spinning and polarization transfer in proton-enhanced NMR" (in en). Journal of Magnetic Resonance 28 (1): 105–112. doi:10.1016/0022-2364(77)90260-8. Bibcode: 1977JMagR..28..105S. https://linkinghub.elsevier.com/retrieve/pii/0022236477902608. 
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  19. ↑ Paruzzo, Federico M.; Emsley, Lyndon (December 2019). "High-resolution 1H NMR of powdered solids by homonuclear dipolar decoupling" (in en). Journal of Magnetic Resonance 309: 106598. doi:10.1016/j.jmr.2019.106598. PMID 31586820. Bibcode: 2019JMagR.30906598P. https://linkinghub.elsevier.com/retrieve/pii/S109078071930237X. 
  20. ↑ Zhang, Rongchun; Mroue, Kamal H.; Ramamoorthy, Ayyalusamy (2017-04-18). "Proton-Based Ultrafast Magic Angle Spinning Solid-State NMR Spectroscopy" (in en). Accounts of Chemical Research 50 (4): 1105–1113. doi:10.1021/acs.accounts.7b00082. ISSN 0001-4842. PMID 28353338. 
  21. ↑ Struppe, Jochem; Quinn, Caitlin M.; Sarkar, Sucharita; Gronenborn, Angela M.; Polenova, Tatyana (2020-01-13). "Ultrafast 1 H MAS NMR Crystallography for Natural Abundance Pharmaceutical Compounds" (in en). Molecular Pharmaceutics 17 (2): 674–682. doi:10.1021/acs.molpharmaceut.9b01157. ISSN 1543-8384. PMID 31891271. 
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  25. ↑ Schanda, P.; Meier, B. H.; Ernst, M. (2010). "Quantitative Analysis of Protein Backbone Dynamics in Microcrystalline Ubiquitin by Solid-State NMR Spectroscopy". J. Am. Chem. Soc. 132 (45): 15957–15967. doi:10.1021/ja100726a. PMID 20977205. 
  26. ↑ Ishii, Yoshitaka; Wickramasinghe, Ayesha; Matsuda, Isamu; Endo, Yuki; Ishii, Yuji; Nishiyama, Yusuke; Nemoto, Takahiro; Kamihara, Takayuki (2018). "Progress in proton-detected solid-state NMR (SSNMR): Super-fast 2D SSNMR collection for nano-mole-scale proteins" (in en). Journal of Magnetic Resonance 286: 99–109. doi:10.1016/j.jmr.2017.11.011. PMID 29223566. Bibcode: 2018JMagR.286...99I. 
  27. ↑ Lilly Thankamony, Aany Sofia; Wittmann, Johannes J.; Kaushik, Monu; Corzilius, Björn (November 2017). "Dynamic nuclear polarization for sensitivity enhancement in modern solid-state NMR" (in en). Progress in Nuclear Magnetic Resonance Spectroscopy 102-103: 120–195. doi:10.1016/j.pnmrs.2017.06.002. PMID 29157490. https://linkinghub.elsevier.com/retrieve/pii/S0079656517300201. 
  28. ↑ Rankin, Andrew G.M.; Trébosc, Julien; Pourpoint, Frédérique; Amoureux, Jean-Paul; Lafon, Olivier (2019-09-01). "Recent developments in MAS DNP-NMR of materials" (in en). Solid State Nuclear Magnetic Resonance 101: 116–143. doi:10.1016/j.ssnmr.2019.05.009. ISSN 0926-2040. PMID 31189121. https://www.sciencedirect.com/science/article/abs/pii/S092620401930030X. 
  29. ↑ Rankin, Andrew G.M.; Trébosc, Julien; Pourpoint, Frédérique; Amoureux, Jean-Paul; Lafon, Olivier (September 2019). "Recent developments in MAS DNP-NMR of materials" (in en). Solid State Nuclear Magnetic Resonance 101: 116–143. doi:10.1016/j.ssnmr.2019.05.009. PMID 31189121. https://linkinghub.elsevier.com/retrieve/pii/S092620401930030X. 
  30. ↑ Rossini, Aaron J.; Zagdoun, Alexandre; Lelli, Moreno; Lesage, Anne; Copéret, Christophe; Emsley, Lyndon (2013-09-17). "Dynamic Nuclear Polarization Surface Enhanced NMR Spectroscopy". Accounts of Chemical Research 46 (9): 1942–1951. doi:10.1021/ar300322x. ISSN 0001-4842. PMID 23517009. https://doi.org/10.1021/ar300322x. 
  31. ↑ Perras, Frédéric A.; Kobayashi, Takeshi; Pruski, Marek (2015-07-08). "Natural Abundance 17 O DNP Two-Dimensional and Surface-Enhanced NMR Spectroscopy" (in en). Journal of the American Chemical Society 137 (26): 8336–8339. doi:10.1021/jacs.5b03905. ISSN 0002-7863. PMID 26098846. https://pubs.acs.org/doi/10.1021/jacs.5b03905. 
  32. ↑ Smith, Adam N.; Märker, Katharina; Hediger, Sabine; De Paëpe, Gaël (2019-08-15). "Natural Isotopic Abundance 13 C and 15 N Multidimensional Solid-State NMR Enabled by Dynamic Nuclear Polarization" (in en). The Journal of Physical Chemistry Letters 10 (16): 4652–4662. doi:10.1021/acs.jpclett.8b03874. ISSN 1948-7185. PMID 31361489. https://pubs.acs.org/doi/10.1021/acs.jpclett.8b03874. 
  33. ↑ Rossini, Aaron J.; Widdifield, Cory M.; Zagdoun, Alexandre; Lelli, Moreno; Schwarzwälder, Martin; Copéret, Christophe; Lesage, Anne; Emsley, Lyndon (2014-02-12). "Dynamic Nuclear Polarization Enhanced NMR Spectroscopy for Pharmaceutical Formulations" (in en). Journal of the American Chemical Society 136 (6): 2324–2334. doi:10.1021/ja4092038. ISSN 0002-7863. PMID 24410528. https://pubs.acs.org/doi/10.1021/ja4092038. 
  34. ↑ Laws, David D. Laws; Bitter, Hans-Marcus L.; Jerschow, Alexej (30 August 2002). "Solid-State NMR Spectroscopic Methods in Chemistry". Angewandte Chemie 41 (17): 3096. doi:10.1002/1521-3773(20020902)41:17<3096::AID-ANIE3096>3.0.CO;2-X. https://onlinelibrary.wiley.com/doi/10.1002/1521-3773(20020902)41:17%3C3096::AID-ANIE3096%3E3.0.CO;2-X. 
  35. ↑ Marchetti, Alessandro; Chen, Juner; Pang, Zhenfeng; Li, Shenhui; Ling, Daishun; Deng, Feng; Kong, Xueqian (April 11, 2017). "Understanding Surface and Interfacial Chemistry in Functional Nanomaterials via Solid-State NMR". Advanced Materials 29 (14): 1605895. doi:10.1002/adma.201605895. https://onlinelibrary.wiley.com/doi/abs/10.1002/adma.201605895. Retrieved 20 December 2023. 
  36. ↑ McDermott, Ann (June 2009). "Structure and Dynamics of Membrane Proteins by Magic Angle Spinning Solid-State NMR" (in en). Annual Review of Biophysics 38 (1): 385–403. doi:10.1146/annurev.biophys.050708.133719. ISSN 1936-122X. PMID 19245337. http://www.annualreviews.org/doi/10.1146/annurev.biophys.050708.133719. 
  37. ↑ Tycko, Robert (2011-05-05). "Solid-State NMR Studies of Amyloid Fibril Structure" (in en). Annual Review of Physical Chemistry 62 (1): 279–299. doi:10.1146/annurev-physchem-032210-103539. ISSN 0066-426X. PMID 21219138. Bibcode: 2011ARPC...62..279T. 
  38. ↑ Demers, Jean-Philippe; Fricke, Pascal; Shi, Chaowei; Chevelkov, Veniamin; Lange, Adam (December 2018). "Structure determination of supra-molecular assemblies by solid-state NMR: Practical considerations". Progress in Nuclear Magnetic Resonance Spectroscopy 109: 51-78. https://www.sciencedirect.com/science/article/abs/pii/S0079656518300128?via%3Dihub. Retrieved 20 December 2023. 
  39. ↑ Chow, W. Y.; Rajan, R.; Muller, K. H.; Reid, D. G.; Skepper, J. N.; Wong, W. C.; Brooks, R. A.; Green, M. et al. (2014-05-16). "NMR Spectroscopy of Native and in Vitro Tissues Implicates PolyADP Ribose in Biomineralization" (in en). Science 344 (6185): 742–746. doi:10.1126/science.1248167. ISSN 0036-8075. PMID 24833391. Bibcode: 2014Sci...344..742C. https://www.science.org/doi/10.1126/science.1248167. 
  40. ↑ New techniques in solid-state NMR. Jacek Klinowski. Berlin: Springer. 2005. ISBN 978-3-540-22168-5. OCLC 56697027. https://www.worldcat.org/oclc/56697027. 
  41. ↑ Duer, Melinda J. (2015). "The contribution of solid-state NMR spectroscopy to understanding biomineralization: Atomic and molecular structure of bone" (in en). Journal of Magnetic Resonance 253: 98–110. doi:10.1016/j.jmr.2014.12.011. PMID 25797009. Bibcode: 2015JMagR.253...98D. https://linkinghub.elsevier.com/retrieve/pii/S1090780714003590. 
  42. ↑ Mohammed, N.R.; Kent, N.W.; Lynch, R.J.M.; Karpukhina, N.; Hill, R.; Anderson, P. (2013). "Effects of Fluoride on in vitro Enamel Demineralization Analyzed by 19F MAS-NMR" (in en). Caries Research 47 (5): 421–428. doi:10.1159/000350171. ISSN 0008-6568. PMID 23712030. https://www.karger.com/Article/FullText/350171. 
  43. ↑ Ferizoli, Bajram; Cresswell-Boyes, Alexander J.; Anderson, Paul; Lynch, Richard J. M.; Hill, Robert G. (2023-05-24). "Effects of fluoride on in vitro hydroxyapatite demineralisation analysed by 19F MAS-NMR". Frontiers in Dental Medicine 4. doi:10.3389/fdmed.2023.1171827. ISSN 2673-4915. 
  44. ↑ Kricheldorf, H. R.; Müller, D. (1984-11-01). "Secondary structure of peptides 16th. Characterization of proteins by means of13C NMR CP/MAS spectroscopy" (in en). Colloid and Polymer Science 262 (11): 856–861. doi:10.1007/BF01452215. ISSN 1435-1536. https://doi.org/10.1007/BF01452215. 
  45. ↑ Zhao, Chenhua; Asakura, Tetsuo (2001-12-14). "Structure of Silk studied with NMR" (in en). Progress in Nuclear Magnetic Resonance Spectroscopy 39 (4): 301–352. doi:10.1016/S0079-6565(01)00039-5. ISSN 0079-6565. https://www.sciencedirect.com/science/article/abs/pii/S0079656501000395. 
  46. ↑ Gil, A.M.; Neto, C. Pascoal (1999), "Solid-State Nmr Studies Of Wood And Other Lignocellulosic Materials" (in en), Annual Reports on NMR Spectroscopy (Elsevier) 37: pp. 75–117, doi:10.1016/s0066-4103(08)60014-9, ISBN 978-0-12-505337-2, https://linkinghub.elsevier.com/retrieve/pii/S0066410308600149, retrieved 2021-09-13 
  47. ↑ Quinn, Caitlin M.; Lu, Manman; Suiter, Christopher L.; Hou, Guangjin; Zhang, Huilan; Polenova, Tatyana (2015). "Magic angle spinning NMR of viruses" (in en). Progress in Nuclear Magnetic Resonance Spectroscopy 86-87: 21–40. doi:10.1016/j.pnmrs.2015.02.003. PMID 25919197. 
  48. ↑ Mandala, Venkata S.; McKay, Matthew J.; Shcherbakov, Alexander A.; Dregni, Aurelio J.; Kolocouris, Antonios; Hong, Mei (2020). "Structure and drug binding of the SARS-CoV-2 envelope protein transmembrane domain in lipid bilayers" (in en). Nature Structural & Molecular Biology 27 (12): 1202–1208. doi:10.1038/s41594-020-00536-8. ISSN 1545-9993. PMID 33177698. 
  49. ↑ Wang, Tuo; Hong, Mei (2016). "Solid-state NMR investigations of cellulose structure and interactions with matrix polysaccharides in plant primary cell walls" (in en). Journal of Experimental Botany 67 (2): 503–514. doi:10.1093/jxb/erv416. ISSN 0022-0957. PMID 26355148. 
  50. ↑ Zhao, Wancheng; Fernando, Liyanage D.; Kirui, Alex; Deligey, Fabien; Wang, Tuo (2020). "Solid-state NMR of plant and fungal cell walls: A critical review" (in en). Solid State Nuclear Magnetic Resonance 107: 101660. doi:10.1016/j.ssnmr.2020.101660. PMID 32251983. https://linkinghub.elsevier.com/retrieve/pii/S0926204020300229. 
  51. ↑ Renault, M.; Tommassen-van Boxtel, R.; Bos, M. P.; Post, J. A.; Tommassen, J.; Baldus, M. (2012-03-27). "Cellular solid-state nuclear magnetic resonance spectroscopy" (in en). Proceedings of the National Academy of Sciences 109 (13): 4863–4868. doi:10.1073/pnas.1116478109. ISSN 0027-8424. PMID 22331896. 
  52. ↑ Renault, Marie; Pawsey, Shane; Bos, Martine P.; Koers, Eline J.; Nand, Deepak; Tommassen-van Boxtel, Ria; Rosay, Melanie; Tommassen, Jan et al. (2012-03-19). "Solid-State NMR Spectroscopy on Cellular Preparations Enhanced by Dynamic Nuclear Polarization" (in en). Angewandte Chemie International Edition 51 (12): 2998–3001. doi:10.1002/anie.201105984. PMID 22298470. https://onlinelibrary.wiley.com/doi/10.1002/anie.201105984. 
  53. ↑ Martínez-Bisbal, M. Carmen; Martí-Bonmatí, Luis; Piquer, José; Revert, Antonio; Ferrer, Pilar; Llácer, José L.; Piotto, Martial; Assemat, Olivier et al. (2004). "1H and13C HR-MAS spectroscopy of intact biopsy samplesex vivo andin vivo1H MRS study of human high grade gliomas" (in en). NMR in Biomedicine 17 (4): 191–205. doi:10.1002/nbm.888. ISSN 0952-3480. PMID 15229932. https://onlinelibrary.wiley.com/doi/10.1002/nbm.888. 
  54. ↑ Sarou-Kanian, Vincent; Joudiou, Nicolas; Louat, Fanny; Yon, Maxime; Szeremeta, Frédéric; Même, Sandra; Massiot, Dominique; Decoville, Martine et al. (2015). "Metabolite localization in living drosophila using High Resolution Magic Angle Spinning NMR" (in en). Scientific Reports 5 (1): 9872. doi:10.1038/srep09872. ISSN 2045-2322. PMID 25892587. Bibcode: 2015NatSR...5E9872S. 
  55. ↑ Li, Mingyue; Xu, Wei; Su, Yongchao; Su, Yongchao (December 2020). "Solid-state NMR Spectroscopy in Pharmaceutical Sciences". TrAC Trends in Analytical Chemistry 135 (4): 116152. doi:10.1016/j.trac.2020.116152. 
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  57. ↑ Hoffmann, Herbert; Debowski, Marta; Müller, Philipp; Paasch, Silvia; Senkovska, Irena; Kaskel, Stefan; Brunner, Eike (2012-11-28). "Solid-State NMR Spectroscopy of Metal–Organic Framework Compounds (MOFs)" (in en). Materials 5 (12): 2537–2572. doi:10.3390/ma5122537. ISSN 1996-1944. Bibcode: 2012Mate....5.2537H. 
  58. ↑ Blanc, Frédéric; Leskes, Michal; Grey, Clare P. (2013-09-17). "In Situ Solid-State NMR Spectroscopy of Electrochemical Cells: Batteries, Supercapacitors, and Fuel Cells" (in en). Accounts of Chemical Research 46 (9): 1952–1963. doi:10.1021/ar400022u. ISSN 0001-4842. PMID 24041242. https://pubs.acs.org/doi/10.1021/ar400022u. 
  59. ↑ Haber, Shira; Leskes, Michal (2018). "What Can We Learn from Solid State NMR on the Electrode-Electrolyte Interface?" (in en). Advanced Materials 30 (41): 1706496. doi:10.1002/adma.201706496. PMID 29889328. Bibcode: 2018AdM....3006496H. https://onlinelibrary.wiley.com/doi/10.1002/adma.201706496. 
  60. ↑ Griffin, John M.; Forse, Alexander C.; Grey, Clare P. (2016). "Solid-state NMR studies of supercapacitors" (in en). Solid State Nuclear Magnetic Resonance 74-75: 16–35. doi:10.1016/j.ssnmr.2016.03.003. PMID 26974032. https://linkinghub.elsevier.com/retrieve/pii/S0926204016300042. 
  61. ↑ Pinto, Moisés L.; Mafra, Luís; Guil, José M.; Pires, João; Rocha, João (2011-03-22). "Adsorption and Activation of CO 2 by Amine-Modified Nanoporous Materials Studied by Solid-State NMR and 13 CO 2 Adsorption" (in en). Chemistry of Materials 23 (6): 1387–1395. doi:10.1021/cm1029563. ISSN 0897-4756. https://pubs.acs.org/doi/10.1021/cm1029563. 
  62. ↑ Schmidt-Rohr, K. (1994). Multidimensional solid-state NMR and polymers. Hans Wolfgang Spiess. London: Academic Press. ISBN 0-12-626630-1. OCLC 31785818. https://www.worldcat.org/oclc/31785818. 
  63. ↑ Del Federico, Eleonora; Centeno, Silvia A; Kehlet, Cindie; Currier, Penelope; Stockman, Denise; Jerschow, Alexej (2009). "Unilateral NMR applied to the conservation of works of art". Analytical and Bioanalytical Chemistry 396 (1): 213–220. doi:10.1007/s00216-009-3128-7. PMID 19787343. 

Suggested readings for beginners

General NMR

Solid-state NMR

  • Laws David D., Hans- , Bitter Marcus L., Jerschow Alexej (2002). "Solid-State NMR Spectroscopic Methods in Chemistry". Angewandte Chemie International Edition 41 (17): 3096–3129. doi:10.1002/1521-3773(20020902)41:17<3096::AID-ANIE3096>3.0.CO;2-X. PMID 12207374. 
  • Reif, Bernd; Ashbrook, Sharon E.; Emsley, Lyndon; Hong, Mei (2021). "Solid-state NMR spectroscopy". Nature Reviews Methods Primers 1. doi:10.1038/s43586-020-00002-1. PMID 34368784. 
  • Levitt, Malcolm H., Spin Dynamics: Basics of Nuclear Magnetic Resonance, Wiley, Chichester, United Kingdom, 2001. ISBN:978-0470511176 (NMR basics, including solids)
  • Duer, Melinda J., Introduction to Solid-State NMR Spectroscopy, Blackwell, Oxford, 2004. (Some detailed examples of ssNMR spectroscopy)
  • Schmidt-Rohr, K. and Spiess, H.-W., Multidimensional Solid-State NMR and Polymers, Academic Press, San Diego, 1994.

External links



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