Magnetic resonance imaging and optical microscopy are key technologies in the life sciences. For microbiological studies, especially of the inner workings of single cells, optical microscopy is normally used because it easily achieves resolution close to the optical wavelength. But in conventional microscopy, diffraction limits the resolution to about half the wavelength. Recently, it was shown that this limit can be partly overcome by nonlinear imaging techniques 1,2 , but there is still a barrier to reaching the molecular scale. In contrast, in magnetic resonance imaging the spatial resolution is not determined by diffraction; rather, it is limited by magnetic field sensitivity, and so can in principle go well below the optical wavelength. The sensitivity of magnetic resonance imaging has recently been improved enough to image single cells 3,4 , and magnetic resonance force microscopy 5 has succeeded in detecting single electrons 6 and small nuclear spin ensembles 7 . However, this technique currently requires cryogenic temperatures, which limit most potential biological applications 8 . Alternatively, single-electron spin states can be detected optically 9,10 , even at room temperature in some systems [11][12][13][14] . Here we show how magneto-optical spin detection can be used to determine the location of a spin associated with a single nitrogen-vacancy centre in diamond with nanometre resolution under ambient conditions. By placing these nitrogen-vacancy spins in functionalized diamond nanocrystals, biologically specific magnetofluorescent spin markers can be produced. Significantly, we show that this nanometre-scale resolution can be achieved without any probes located closer than typical cell dimensions. Furthermore, we demonstrate the use of a single diamond spin as a scanning probe magnetometer to map nanoscale magnetic field variations. The potential impact of single-spin imaging at room temperature is far-reaching. It could lead to the capability to probe biologically relevant spins in living cells.The nitrogen-vacancy centre in diamond is a unique solid state system that allows ultrasensitive and rapid detection of single electronic spin states under ambient conditions 12 . The nitrogen-vacancy defect is a naturally occurring impurity that is responsible for the pink colouration of diamond crystals when present in high concentration. It was demonstrated that this colour centre can be produced in diamond nanocrystals by electron irradiation. Fluorescing nitrogen-vacancy diamond nanocrystals can be used as markers for bioimaging applications 15 . Such markers have attracted widespread interest because of their unprecedented photostability and non-toxicity 16,17 . It was recognized recently that the magnetic properties of such fluorescent labels can in principle be used for novel microscopy 18,19 . Here we demonstrate the realization of a magneto-optic microscope using nitrogen-vacancy diamond as the magnetic fluorescent label that moreover does not bleach or blink. Figure 1c and d show the fluorescenc...

Here we report the increase of the coherence time T 2 of a single electron spin at room temperature by using dynamical decoupling. We show that the Carr-Purcell-Meiboom-Gill (CPMG) pulse sequence can prolong the T 2 of a single Nitrogen-Vacancy center in diamond up to 2.44 ms compared to the Hahn echo measurement where T 2 = 390 µs. Moreover, by performing spin locking experiments we demonstrate that with CPMG the maximum possible T 2 is reached. On the other hand, we do not observe strong increase of the coherence time in nanodiamonds, possibly due to the short spin lattice relaxation time T 1 = 100 µs (compared to T 1 = 5.93 ms in bulk). An application for detecting low magnetic field is demonstrated, where we show that the sensitivity using the CPMG method is improved by about a factor of two compared to the Hahn echo method.

Low detection sensitivity stemming from the weak polarization of nuclear spins is a primary limitation of magnetic resonance spectroscopy and imaging. Methods have been developed to enhance nuclear spin polarization but they typically require high magnetic fields, cryogenic temperatures or sample transfer between magnets. Here we report bulk, room-temperature hyperpolarization of 13C nuclear spins observed via high-field magnetic resonance. The technique harnesses the high optically induced spin polarization of diamond nitrogen vacancy centres at room temperature in combination with dynamic nuclear polarization. We observe bulk nuclear spin polarization of 6%, an enhancement of ∼170,000 over thermal equilibrium. The signal of the hyperpolarized spins was detected in situ with a standard nuclear magnetic resonance probe without the need for sample shuttling or precise crystal orientation. Hyperpolarization via optical pumping/dynamic nuclear polarization should function at arbitrary magnetic fields enabling orders of magnitude sensitivity enhancement for nuclear magnetic resonance of solids and liquids under ambient conditions.