NMR experiments rely on creating a difference in population of nuclear spin energy levels, such that the net magnetic field they produce may be detected. This polarization, as it is called, is most commonly induced thermally by applying strong magnetic fields to establish an energetic preference for spins aligned with or against the applied field. Current magnetic resonance technologies have pushed towards increasingly stronger fields in order to overcome inherently poor nuclear polarization at thermal equilibrium, which remains as a limitation to sensitivity and scope of the capabilities of magnetic resonance. Even the most sophisticated instruments can achieve polarizations no greater than 0.01%, and such gains in sensitivity are nearly negated by the cost and impracticality of the resulting instruments. For this reason our group has focused part of its work on developing practical methods of producing nonequilibrium polarization – or hyperpolarization – for signal enhancement in magnetic resonance methods.


Nuclear polarization is poor because the energy required to align a nuclear spin against a magnetic field can be incredibly small – often ten or more orders of magnitude smaller than the energy required to break a chemical bond. This means that thermal fluctuations can easily overpower these transitions despite using large magnetic fields, i.e. 10,000 times larger than earth’s magnetic field. As a result, the polarization vector P in the figure to the left, arising from the slight excess of spins aligned with the magnetic field, is relatively small and thus difficult to detect.

A number of elegant solutions have been presented for hyperpolarizing nuclei either completely or on the order of parts per hundred rather than parts per million. These solutions generally transfer polarization to a nuclear ensemble from systems that can be easily polarized, using the interactions that couple the two. Due to their ease of polarization by magnetic fields, optical illumination, or chemical reaction, current sources for polarization transfer are electrons in solid-state systems and organic radicals, gaseous alkali atoms, and parahydrogen.

Alkali metal atoms are characterized by a single valence electron whose spin state is strongly coupled to the nuclear spin. By imparting the angular momentum of circularly polarized light to the electron during promotion to an excited electronic state, the spin state of the electron, and therefore the atom, may be selected (1). It was then demonstrated that polarization can be transferred to noble gas atoms such as Xenon-129 and Helium-3 during spin-exchange collisions of gaseous atoms (2). Our group currently applies hyperpolarized Xenon-129 for targeted cellular imaging as well as remotely detected imaging for chemical analysis.  

Another example is the nitrogen-vacancy (NV-) center, which is an electronic defect in diamond with total spin equal to 1. Upon optical excitation, the triplet spin state preferentially relaxes through intersystem crossing to the ground state, resulting in polarization to the 0 spin state with ~80% efficiency. This means that by simply pumping the NV- center with green light, the system can be nearly completely polarized to the spin-0 state.

Lastly, the symmetry of singlet states such as parahydrogen can be exploited to produce complete polarization in newly-formed bonds incorporating these systems, which can then be probed and manipulated for a number of purposes (3,4). 


Because magnetic resonance techniques universally and fundamentally rely on adequate polarization, members of the field have worked towards the development of hyperpolarization methods for decades. Early work was focused on the development of a body of techniques referred to as dynamic nuclear polarization, which is now implemented in commercial systems for application to solids and solutions, surfaces, materials, as well as micro- and macromolecular biological systems (5-11). The Pines group has purposed these techniques of hyperpolarization – DNP, optically-pumped systems, and parahydrogen – for a number of applications. A few examples include photochemical DNP for time-resolved magnetic resonance imaging, the use of alkali vapor magnetometry and PHIP for chemical analysis at zero-field, and the NV defect for sensitive magnetometry

Current Work

We are currently exploring three different mechanisms for hyperpolarization. This includes polarization transfer from the nitrogen vacancy defect in diamond to other nuclear spins in the lattice, the development of a microfabricated Xenon polarizer capable of both hyperpolarizing Xenon and detecting encoded Xenon with increased sensitivity, and testing the breadth of the SABRE (Signal Amplification by Reversible Exchange) method with parahydrogen and different catalysts.  We also hope to transfer hyperpolarization to liquids.

Current Members:

Ashok Ajoy

Danila Barskiy

Tobias Sjolander

Jonathan King

Muller Gomes

Ashley Truxal

Xudong Lv


Dmitry Budker (UC-Berkeley, Physics)
Jeffrey Reimer (UC-Berkeley, Chemical Engineering)
John Kitching (NIST)


[1] Ajoy, A.; Liu, K.; Nazaryan, R.; Lv, X.; Zangara, PR; Safvati, B.; Wang, G.; Arnold, D.; Li, G.; Lin, A.; et al. "Orientation independent room-temperature optical 13C hyperpolarization in powdered diamond". Science Advances4(5), 2018.

[2] Kastler, A. “Optical Methods of Atomic Orientation and of Magnetic Resonance”. Journal of the Optical Society of America, 47(6), 460-465 (1957).


[3] Happer, W. “Optical Pumping”. Reviews of Modern Physics. 144(2), 170-250, 1972.

[4] Goodson, B. M. “Nuclear Magnetic Resonance of Laser-Polarized Noble Gas Nuclei in Molecules, Materials, and Organisms”. Journal of Magnetic Resonance, 155, 157-216 (2002). R. G. Walker, W. Happer. “Spin-exchange optical pumping of noble gas nuclei”. Reviews of Modern Physics, 69(2), 629-642 (1997).

[5] A. Abragam, The Principles of Nuclear Magnetism (Clarendon, Oxford, England, 1961); C.P. Slichter, Principles of Magnetic Resonance (Springer-Verlag, Berlin, 1989).

[6] Rossini, A. J.; Zagdoun, A.; Lelli, M.; Lesage, A.; Coperet, C.; and L. Emsley. Dynamic nuclear polarization surface enhanced NMR spectroscopy. Acc. Chem. Res. (2013).

[7] Duckett, S. B. and R. E. Mewis. Application of parahydrogen induced polarization techniques in NMR spectroscopy and imaging. Acc. Chem. Res. 45(8) 1247 (2012).

[8] R. Eisenberg. Parahydrogen-induced polarization: a new spin on reactions with molecular hydrogen. Acc. Chem. Res. 24(4), 110, (1991).

[9] Maly, T.; Debelouchina, G. T.; Bajaj, V. S.; Hu, K.; Joo, C.; Mak-Jurkauskas, M. L.; Sirigiri, J. R.; van der Wel, P. C.; Herzfeld, J.; Temkin, R. J.; and R. G. Griffin. Dynamic nuclear polarization at high magnetic fields. Journ. Chem. Phys. 128, 052211 (2008).

[10] Ardenkjaer-Larsen, J. H.; Fridlund, B.; Gram, A.; Hansson, G.; Hansson, L.; Lerche, M. H.; Servin, R.; Thaning, M.; and K. Golman. Increase in signal-noise ratio of >10,000 times in liquid state NMR. Proc. Natl. Acad. Sci. 100(18), 10158 (2003).

[11] Zhou, J.; Liyun, L.; Hongbing, H.; Yang, B.; Dan, Z.; Qiu, J.; Guo, J.; Chen, F. and C. Ye. Study of natural diamonds by dynamic nuclear polarization enhanced 13C nuclear magnetic resonance spectroscopy. Solid State Nucl. Magn. Reson. 3, 339 (1994).
Wind, R. A.; Duijvestijn, M. J.; van der Lugt, C.; Manenschijn, A.; and J. Vriend. Application of dynamic nuclear polarization in 13C NMR in solids. Prog. Nucl. Magn. Reson. Spectrosc. 17, 33 (1985).

[12] Afeworki, M.; McKay, R. A.; and J. Schaefer. Selective observation of the interface of heterogeneous polycarbonate/polystyrene blends by dynamic nuclear polarization carbon-13 NMR spectroscopy. Macromolecules 25, 4084 (1992).

[13] Zysmilich, M. G. and A. McDermott. Photochemically induced dynamic nuclear polarization in the solid-state 15N spectra of reaction centers from photosynthetic bacteria Rhodobacter sphaeroides R-26. J. Am. Chem. Soc. 116, 8362 (1994).