High-resolution liquid- and solid-state nuclear magnetic resonance of nanoliter sample volumes using microcoil detectors

被引:116
作者
Kentgens, A. P. M. [1 ]
Bart, J. [2 ]
van Bentum, P. J. M. [1 ]
Brinkmann, A. [1 ]
Van Eck, E. R. H. [1 ]
Gardeniers, J. G. E. [2 ]
Janssen, J. W. G. [1 ]
Knijn, P. [1 ]
Vasa, S. [1 ]
Verkuijlen, M. H. W. [1 ]
机构
[1] Radboud Univ Nijmegen, Inst Mol & Mat, NL-6525 ED Nijmegen, Netherlands
[2] Univ Twente, MESA, Inst Nanotechnol, NL-7500 AE Enschede, Netherlands
关键词
D O I
10.1063/1.2833560
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The predominant means to detect nuclear magnetic resonance (NMR) is to monitor the voltage induced in a radiofrequency coil by the precessing magnetization. To address the sensitivity of NMR for mass-limited samples it is worthwhile to miniaturize this detector coil. Although making smaller coils seems a trivial step, the challenges in the design of microcoil probeheads are to get the highest possible sensitivity while maintaining high resolution and keeping the versatility to apply all known NMR experiments. This means that the coils have to be optimized for a given sample geometry, circuit losses should be avoided, susceptibility broadening due to probe materials has to be minimized, and finally the B-1-fields generated by the rf coils should be homogeneous over the sample volume. This contribution compares three designs that have been miniaturized for NMR detection: solenoid coils, flat helical coils, and the novel stripline and microslot designs. So far most emphasis in microcoil research was in liquid-state NMR. This contribution gives an overview of the state of the art of microcoil solid-state NMR by reviewing literature data and showing the latest results in the development of static and micro magic angle spinning (microMAS) solenoid-based probeheads. Besides their mass sensitivity, microcoils can also generate tremendously high rf fields which are very useful in various solid-state NMR experiments. The benefits of the stripline geometry for studying thin films are shown. This geometry also proves to be a superior solution for microfluidic NMR implementations in terms of sensitivity and resolution. (c) 2008 American Institute of Physics.
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页数:17
相关论文
共 155 条
[91]   Solenoidal microcoil design - Part II: Optimizing winding parameters for maximum signal-to-noise performance [J].
Minard, KR ;
Wind, RA .
CONCEPTS IN MAGNETIC RESONANCE, 2001, 13 (03) :190-210
[92]  
Minard KR, 2001, CONCEPT MAGNETIC RES, V13, P128, DOI 10.1002/1099-0534(2001)13:2<128::AID-CMR1002>3.0.CO
[93]  
2-8
[94]   Photo-CIDNP NMR methods for studying protein folding [J].
Mok, KH ;
Hore, PJ .
METHODS, 2004, 34 (01) :75-87
[95]  
Neuhoff PS, 2002, AM MINERAL, V87, P1307
[96]  
NIELSEN NC, 1995, J BIOMOL NMR, V5, P311, DOI 10.1007/BF00211758
[97]   Microflow NMR: Concepts and capabilities [J].
Olson, DL ;
Norcross, JA ;
O'Neil-Johnson, M ;
Molitor, PF ;
Detlefsen, DJ ;
Wilson, AG ;
Peck, TL .
ANALYTICAL CHEMISTRY, 2004, 76 (10) :2966-2974
[98]   High-resolution microcoil NMR for analysis of mass-limited, nanoliter samples [J].
Olson, DL ;
Lacey, ME ;
Sweedler, JV .
ANALYTICAL CHEMISTRY, 1998, 70 (03) :645-650
[99]   HIGH-RESOLUTION MICROCOIL H-1-NMR FOR MASS-LIMITED, NANOLITER-VOLUME SAMPLES [J].
OLSON, DL ;
PECK, TL ;
WEBB, AG ;
MAGIN, RL ;
SWEEDLER, JV .
SCIENCE, 1995, 270 (5244) :1967-1970
[100]  
OVERHAUSER AW, 1953, PHYS REV, V92, P411, DOI 10.1103/PhysRev.92.411