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.2014 Aug 19;111(33):11955-60.
doi: 10.1073/pnas.1402015111. Epub 2014 Aug 4.

Scalable NMR spectroscopy with semiconductor chips

Affiliations

Scalable NMR spectroscopy with semiconductor chips

Dongwan Ha et al. Proc Natl Acad Sci U S A..

Abstract

State-of-the-art NMR spectrometers using superconducting magnets have enabled, with their ultrafine spectral resolution, the determination of the structure of large molecules such as proteins, which is one of the most profound applications of modern NMR spectroscopy. Many chemical and biotechnological applications, however, involve only small-to-medium size molecules, for which the ultrafine resolution of the bulky, expensive, and high-maintenance NMR spectrometers is not required. For these applications, there is a critical need for portable, affordable, and low-maintenance NMR spectrometers to enable in-field, on-demand, or online applications (e.g., quality control, chemical reaction monitoring) and co-use of NMR with other analytical methods (e.g., chromatography, electrophoresis). As a critical step toward NMR spectrometer miniaturization, small permanent magnets with high field homogeneity have been developed. In contrast, NMR spectrometer electronics capable of modern multidimensional spectroscopy have thus far remained bulky. Complementing the magnet miniaturization, here we integrate the NMR spectrometer electronics into 4-mm(2) silicon chips. Furthermore, we perform various multidimensional NMR spectroscopies by operating these spectrometer electronics chips together with a compact permanent magnet. This combination of the spectrometer-electronics-on-a-chip with a permanent magnet represents a useful step toward miniaturization of the overall NMR spectrometer into a portable platform.

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Conflict of interest statement

The authors declare no conflict of interest.

Figures

Fig. 1.
Fig. 1.
NMR spectrometer combining silicon spectrometer electronics chips and a 0.51-T NdFeB permanent magnet (W × D × H: 12.6 × 11.7 × 11.9 cm3; weight: 7.3 kg; Neomax Co.).
Fig. 2.
Fig. 2.
Spectrometer electronics chip architecture and measurements. (A) Free-induction decay (FID) experiments with ethylbenzene demonstrate multiphase generation; 32 FID signals excited by π/2 pulses with 32 different RF phases (Upper) are aligned (Lower), after shifting each signal by its respective excitation phase. These particular experiments were done before the magnet shimming. (B) Receiver input referred noise; and (C) receiver gain.
Fig. 3.
Fig. 3.
One-dimensional1H NMR spectroscopy. (A) Setup. (BH) The 1D spectra for deionized tap water (1 scan), ethanol (1 scan),l-alanine (64 scans), ethylbenzene (1 scan), aspirin (64 scans),l-serine (64 scans), andd-(+)-glucose (64 scans).l-alanine,l-serine, andd-(+)-glucose are dissolved in D2O (1.5 M). Aspirin is dissolved in DMSO-d6 (1.5 M).
Fig. 4.
Fig. 4.
Two-dimensional1H NMR spectroscopy. (A) Setup; 1D spectra of ethanol andl-alanine, identical to Fig. 3C andD. (B)J-resolved spectra of ethanol (Left) andl-alanine (Right); each takes 15 min to obtain (84 scans with a single scan/wait time of 11 s). In the pulse sequence, black (white) bar signifies a π/2 (π) pulse. Quadrature detection in thef1 domain is done by additional phase cycle with ϕ1 shifted by π/2 (41). (C) COSY spectra of ethanol (Left) andl-alanine (Right); each takes 73 min to acquire (400 scans with a single scan/wait time of 11 s).
Fig. 5.
Fig. 5.
Two-dimensional heteronuclear spectroscopy with methanol. (A) Setup. (B)1H-only 1D spectrum. (C) HSQC spectrum. A four-phase cycling to select the particular coherence pathway uses ϕ1∈{0,π,0,π}, ϕ2∈{0,0,π,π}, and ϕ3∈{0,π,π,0}. HSQC spectrum takes 17 min to obtain (168 scans including phase cycling with a single scan/wait time of 6 s). (D) HMQC spectrum. An eight-phase cycling to select the particular coherence pathway uses ϕ1∈{0,π,0,π,0,π,0,π}, ϕ2∈{0,0,π/2, π/2,π,π,3π/2,3π/2}, and ϕ3∈{0,π,π,0,0,π,π,0}. HMQC spectrum takes 34 min to acquire (336 scans including phase cycling with a single scan/wait time of 6 s). ForC andD, the13C π/2-pulse duration is obtained separately (Materials and Methods), and τ = 1/(4JC-H).
Fig. 6.
Fig. 6.
Raw,f2-calibrated, andf2- andf1-calibrated COSY ethanol spectrum; the final one is identical to Fig. 4C,Left.
Fig. 7.
Fig. 7.
1H NMR relaxometry for a crude oil sample. (A) Setup. (B) CPMG echo signal vs. echo time at 25 °C (blue) and 150 °C (red). (C,Left) Semilog plot of the echo decay at 25 °C (blue) and 150 °C (red). Echo spacing is 4 ms. (Right)T2 spectrum at 25 °C.
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