Parallel detection and spatial mapping of large nuclear spin clusters.

Nuclear magnetic resonance imaging (MRI) at the atomic scale offers exciting prospects for determining the structure and function of individual molecules and proteins. Quantum defects in diamond have recently emerged as a promising platform towards reaching this goal, and allowed for the detection and localization of single nuclear spins under ambient conditions. Here, we present an efficient strategy for extending imaging to large nuclear spin clusters, fulfilling an important requirement towards a single-molecule MRI technique. Our method combines the concepts of weak quantum measurements, phase encoding and simulated annealing to detect three-dimensional positions from many nuclei in parallel. Detection is spatially selective, allowing us to probe nuclei at a chosen target radius while avoiding interference from strongly-coupled proximal nuclei. We demonstrate our strategy by imaging clusters containing more than 20 carbon-13 nuclear spins within a radius of 2.4 nm from single, near-surface nitrogen-vacancy centers at room temperature. The radius extrapolates to 5-6 nm for 1H. Beside taking an important step in nanoscale MRI, our experiment also provides an efficient tool for the characterization of large nuclear spin registers in the context of quantum simulators and quantum network nodes.

Broadband radio-frequency transmitter for fast nuclear spin control.

The active manipulation of nuclear spins with radio-frequency (RF) coils is at the heart of nuclear magnetic resonance (NMR) spectroscopy and spin-based quantum devices. Here, we present a miniature RF transmitter designed to generate strong RF pulses over a broad bandwidth, allowing for fast spin rotations on arbitrary nuclear species. Our design incorporates (i) a planar multilayer geometry that generates a large field of 4.35 mT per unit current, (ii) a 50 Ω transmission circuit with a broad excitation bandwidth of ∼20 MHz, and (iii) an optimized thermal management leading to minimal heating at the sample location. Using individual 13C nuclear spins in the vicinity of a diamond nitrogen-vacancy center as a test system, we demonstrate Rabi frequencies exceeding 70 kHz and nuclear π/2 rotations within 3.4 µs. The extrapolated values for 1H spins are about 240 kHz and 1 µs, respectively. Beyond enabling fast nuclear spin manipulations, our transmitter system is ideally suited for the incorporation of advanced pulse sequences into micro- and nanoscale NMR detectors operating at a low (<1 T) magnetic field.

Tracking the precession of single nuclear spins by weak measurements.

Nuclear magnetic resonance (NMR) spectroscopy is a powerful technique for analysing the structure and function of molecules, and for performing three-dimensional imaging of their spin densities. At the heart of NMR spectrometers is the detection of electromagnetic radiation, in the form of a free induction decay signal1, generated by nuclei precessing around an applied magnetic field. Whereas conventional NMR requires signals from 1012 or more nuclei, recent advances in sensitive magnetometry2,3 have dramatically lowered the required number of nuclei to a level where a few or even individual nuclear spins can be detected4-6. It is unclear whether continuous detection of the free induction decay can still be applied at the single-spin level, or whether quantum back-action (the effect that a detector has on the measurement itself) modifies or suppresses the NMR response. Here we report the tracking of single nuclear spin precession using periodic weak measurements7-9. Our experimental system consists of nuclear spins in diamond that are weakly interacting with the electronic spin of a nearby nitrogen vacancy centre, acting as an optically readable meter qubit. We observe and minimize two important effects of quantum back-action: measurement-induced decoherence10 and frequency synchronization with the sampling clock11,12. We use periodic weak measurements to demonstrate sensitive, high-resolution NMR spectroscopy of multiple nuclear spins with a priori unknown frequencies. Our method may provide a useful route to single-molecule NMR13,14 at atomic resolution.

Three-Dimensional Nuclear Spin Positioning Using Coherent Radio-Frequency Control.

Distance measurements via the dipolar interaction are fundamental to the application of nuclear magnetic resonance (NMR) to molecular structure determination, but they provide information on only the absolute distance r and polar angle θ between spins. In this Letter, we present a protocol to also retrieve the azimuth angle ϕ. Our method relies on measuring the nuclear precession phase after the application of a control pulse with a calibrated external radio-frequency coil. We experimentally demonstrate three-dimensional positioning of individual ^{13}C nuclear spins in a diamond host crystal relative to the central electronic spin of a single nitrogen-vacancy center. The ability to pinpoint three-dimensional nuclear locations is central for realizing a nanoscale NMR technique that can image the structure of single molecules with atomic resolution.

Comparison of bone scintigraphy with bone markers in the diagnosis of bone metastasis in lung carcinoma patients.

This study was designed to evaluate the utility of the bone markers total alkaline phosphatase (TAP), bone-specific alkaline phosphatase (BAP), aminoterminal propeptide of type I collagen (PINP), carboxyterminal propeptide of type I collagen (PICP), pyridinoline crosslinks (PYD), deoxypyridinoline crosslinks (DPD), cross-linked carboxyterminal telopeptide of type I collagen (ICTP), cross-linked carboxyterminal telopeptide of type I collagen (CTx, beta-CrossLaps) and tartrate-resistant acid phosphatase 5b (TRAP 5b) in comparison with bone scintigraphy for the diagnosis of bone metastasis in lung carcinoma patients. The study population consisted of 49 patients with bone metastasis confirmed by plain radiography and/or computed tomography, 89 patients without bone metastasis, 12 patients with benign lung diseases and 18 healthy persons. All patients were of male gender. The bone markers were measured using commercially available tests. Serum and urine were collected from fasting patients at the time of bone scan between 7.00 and 8.00 a.m. The sensitivity of bone scintigraphy was 100%, its specificity 76.4%, resulting in a diagnostic efficiency of 84.8%. The positive predictive value was calculated to be 70% and the negative one to be 100%. The concentrations of the bone markers TAP, BAP, PINP, PYD, DPD and ICTP were significantly higher in patients with bone metastasis than in those without bone metastasis (p<0.01). The levels of PICP and CTx only tended to be higher in the patients with bone metastasis compared to those without bone metastasis. There was no significant difference in the TRAP 5b levels between the two groups. There was also no difference in the marker levels between osteoblastic, osteolytic and mixed osteoblastic-osteolytic lesions. Contrary to BAP, PICP, CTx and TRAP 5b, the markers TAP, PINP, PYD, DPD and ICTP were found to be higher (p<0.01-0.05) in patients with bone metastasis than in patients with benign lung diseases. In addition, PYD, DPD and ICTP differentiated patients with benign lung diseases from the healthy controls. Based on cut-off values that correspond to 95% specificity in the group of healthy persons, the sensitivity of the marker assays were as follows (specificity in brackets): TAP 33.3% (97.5%), BAP 22% (100%), PINP 18.4% (97.5%), PICP 2.1% (95.2%), PYD 91.8% (24.1%), DPD 83.7% (34.5%), ICTP 75.5% (44.6%), CTx 45.8% (77.5%) and TRAP 5b 14% (84%). The corresponding data for the diagnostic efficiency were as follows: TAP 73.6%, BAP 77.1%, PINP 67.7%, PICP 61.1%, PYD 48.5%, DPD 55.2%, ICTP 56.1%, CTx 65.6% and TRAP 5b 58.7%, respectively. The positive predictive values ranged from 20% (PICP) to 100% (BAP) and the negative values from 62.7% (PICP) to 84% (PYD). In the ROC analysis, TAP, followed by RAP, PINP and PYD, showed the best performance. The levels of TAP, BAP, PINP, PYD, DPD and ICTP were found to be higher in the patients with bone metastasis compared to those with metastastic lesions in other sites (p<0.01, except for ICTP having a p value of < 0.05). The levels of TAP, BAP, PYD, DPD and ICTP increased significantly with the number of metastases. There was also a steady increase in T scores of the markers PINP, PYD, DPD and ICTP with the extent of the metastatic bone disease. It is concluded that the currently available bone markers cannot replace bone scintigraphy, either for screening or in the diagnosis of bone metastasis, in lung carcinoma patients. However, a panel consisting of TAP, BAP, PINP, PYD, DPD and ICTP may be of some value as an adjunct tool to bone scintigraphy for this purpose.