2009
DOI: 10.1016/j.jmr.2009.01.028
|View full text |Cite
|
Sign up to set email alerts
|

Nuclear magnetic resonance in microfluidic environments using inductively coupled radiofrequency resonators

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
34
1

Year Published

2011
2011
2018
2018

Publication Types

Select...
3
2

Relationship

0
5

Authors

Journals

citations
Cited by 28 publications
(35 citation statements)
references
References 38 publications
0
34
1
Order By: Relevance
“…Equation [18] shows that the efficiency is close to 1 in the overcoupling regime: k k c . As k is of the order of the square root of the ratio of the coil's volumes V 1 and V 2 , the condition k k c is not very stringent and is realized if:…”
Section: Model Circuit and Definitionsmentioning
confidence: 91%
See 2 more Smart Citations
“…Equation [18] shows that the efficiency is close to 1 in the overcoupling regime: k k c . As k is of the order of the square root of the ratio of the coil's volumes V 1 and V 2 , the condition k k c is not very stringent and is realized if:…”
Section: Model Circuit and Definitionsmentioning
confidence: 91%
“…Resonant inductive coupling to a resonator has been introduced by Diodato et al (36) in the context of EPR. Applications to NMR and MRI have recently followed (1,(16)(17)(18). Here we present extensively an analysis to fully determine optimized performance for microNMR studies.…”
Section: Coupling To Rotating Coils By Resonant Inductive Couplingmentioning
confidence: 99%
See 1 more Smart Citation
“…However, in certain cases, as for example, for bench‐top NMR spectrometers, the detector is non‐changeable, and therefore, it is not feasible to replace such detector with one that exhibits a higher filling factor for small samples. A very good solution to such a problem is the use of a passive LC resonator 19. The inductor L c , in this case, is designed to achieve maximum filling factor of the sample, while the capacitor C c is chosen in a way to make the L c resonate at the Larmor frequency C c  = 1/( L c ω 2 ).…”
Section: Theorymentioning
confidence: 99%
“…(ii) The wireless transfer of energy (signal) from an MR detector, which is enabled by placing a pick‐up coil which is wired to the spectrometer in close proximity to a non‐wired MR detector. The signal recorded by the MR detector is transferred via inductive coupling to the spectrometer and is typically used to access samples within restricted areas,7, 8, 9, 10, 11, 12, 13 to locally enhance the signal‐to‐noise ratio (SNR),14, 15, 16 or to improve the handling comfort of MR probes 17, 18, 19, 20, 21, 22…”
Section: Introductionmentioning
confidence: 99%