AI Article Synopsis

  • Parahydrogen can significantly amplify magnetic resonance signals, enhancing them by up to 10,000 times compared to normal thermal signals at around 10 Tesla.
  • The main issue with using parahydrogen is the rapid decay of the hyperpolarized signals, but research has found that signal decay can be controlled and extended when using specific techniques at microtesla fields.
  • The study reveals two mechanisms for polarization transfer: one where the carbon pair binds directly to the catalyst, and another where polarization is transferred through protons in the molecules surrounding the carbon pairs.

Article Abstract

Parahydrogen is an inexpensive and readily available source of hyperpolarization used to enhance magnetic resonance signals by up to four orders of magnitude above thermal signals obtained at ∼10 T. A significant challenge for applications is fast signal decay after hyperpolarization. Here we use parahydrogen-based polarization transfer catalysis at microtesla fields (first introduced as SABRE-SHEATH) to hyperpolarize C spin pairs and find decay time constants of 12 s for magnetization at 0.3 mT, which are extended to 2 min at that same field, when long-lived singlet states are hyperpolarized instead. Enhancements over thermal at 8.5 T are between 30 and 170 fold (0.02 to 0.12% polarization). We control the spin dynamics of polarization transfer by choice of microtesla field, allowing for deliberate hyperpolarization of either magnetization or long-lived singlet states. Density functional theory calculations and experimental evidence identify two energetically close mechanisms for polarization transfer: First, a model that involves direct binding of the C pair to the polarization transfer catalyst and, second, a model transferring polarization through auxiliary protons in substrates.

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http://www.ncbi.nlm.nih.gov/pmc/articles/PMC5580346PMC
http://dx.doi.org/10.1021/acs.jpclett.7b00987DOI Listing

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