How to Make Diamond Dust Glow in a Magnetic Field ✛ ✎

Original: "Microwave-Free $$^{13}$$C Hyperpolarization of Diamond Particles Enabled by Magic Angle Spinning and NV Centers"
arXiv:2609.07653v1 · 2026-09-07 · CC BY-NC-SA 4.0 · independent analysis · 1 min
Spinning diamond particles at 54.74° to the magnetic field boosted the carbon-13 signal 411-fold without microwaves.

Inside every diamond are tiny magnetic needles: the nuclei of carbon atoms. Normally they point in random directions, so their signal is very weak. But if you spin diamond dust at an angle of 54.74° to the magnetic field while shining a green laser on it, the needles start to align. The signal gets hundreds of times stronger.

The secret lies in diamond defects where a nitrogen atom sits next to a vacancy. These defects, called NV centers, become polarized under light, meaning their electrons all get the same spin direction. This polarization then transfers to neighboring carbon-13 nuclei. Previously, this transfer required microwave pulses, but now the spinning sample does all the work.

The angle 54.74° is called the magic angle because it cancels out interactions between nuclei. At this tilt, almost all defects pass through special points twice per rotation, where polarization transfer is especially efficient.

In the experiment, two types of diamond particles were used: small ones enriched in carbon-13 and larger ones with natural abundance. They were spun at up to 6000 revolutions per second and illuminated with a laser. The signal was amplified 411-fold for the natural sample and 280-fold for the enriched one. That is nearly ten times better than previous attempts.

Now the researchers want to transfer this polarization to molecules attached to the diamond particle surfaces. For that, they need particles smaller than 30 nanometers. Then diamond dust could amplify signals not only from its own nuclei but also from any substance applied to it.

The angle of 54.74° between the rotation axis and the magnetic field is called the magic angle because it nullifies dipole-dipole interactions between nuclei. It is this angle that made more than 99.9% of NV centers pass through the required level crossing points twice per rotor revolution.

\nu_{0,\pm1}(\theta) = |\bar{\gamma}_{\rm NV}| B \pm \frac{1}{2}(3\cos^2\theta - 1)D
The frequency depends on the angle θ between the NV axis and the field; at θ = 54.74° the term with D vanishes, which creates the conditions for level crossing
l_d \sim \sqrt{D T_{\rm pol}}
Polarization spreads from the paramagnetic center over a distance determined by the diffusion coefficient D and the pumping time T_pol
Concepts
diamond nv center spectroscopy diamond quantum memory nitrogen vacancy center ionization nuclear fusion