attoNVM
cryogenic NV microscope
unmatched magnetic field sensitivity & photon count rate
breakthrough in magnetic imaging & fully quantitative
ultra-low vibrations and drift tuned for quantum applications
ultimate stability over long measurement cycles
swiftly and safely exchangeable NV tips with integrated MW antenna
advanced user-friendliness for advanced scanning microscopy
The ability to measure magnetic fields at nanoscale in cryogenic environment is key for understanding magnetism on the quantum level and for designing materials for novel data storage devices or quantum computers. Nitrogen vacancy magnetometry (NVM) is a quantum sensing technique particularly suitable for applications where high magnetic field sensitivity is required.
attocube and QZabre combine forces to bring to the market the first commercial cryogenic scanning NV magnetometer in a dry cryostat. The seamless integration between attocube and QZabre state-of-the-art hardware and software enables users to efficiently perform magnetic imaging at various temperatures and truly quantitatively. There is no need for the calibration of the sensor, because of using its quantum properties for imaging.
Specifications
| General Specifications | |
|---|---|
| type of instrument | magnetometer based on Nitrogen-Vacancy (NV) Centers in Diamond, combining confocal (CFM) and atomic force microscope (AFM) with microwave excitation |
| NV tips | QZabre QST: fully integrated sensor chip with a single NV at the tip, AFM-compatible force feedback and integrated microwave antenna |
| Modes of Operation | |
| imaging modes | NV-based: ODMR, quench mode, iso-B mode, pulsed protocols. Others: AFM (engaged in shear mode and fixed height), CFM, MOKE, widefield (non-scanning) |
| slope compensation | 2 axis scan plane correction |
| pulsed protocols | Rabi, Ramsey, Spin-Echo, CPMG, XY4, XY8, customizable pulsed protocols |
| NVM performance | |
| ODMR contrast at base temperature | > 8 % |
| magnetic field sensitivity | < 10 µT/(Hz)^1/2 |
| lateral magnetic resolution | < 70 nm |
| microwave generator | 0.7 – 6 GHz |
| single photon detector | high quantum efficiency (typically 80% at 670 nm, guaranteed > 60%) |
| AFM performance | |
| z feedback | AM-AFM (amplitude modulation), FM-AFM (frequency modulation); using PID feedback loops and PLL |
| RMS z-noise (BW = 200 Hz) | < 0.4 nm @ RT, < 2.5 nm @ LT |
| z bit resolution @ 4 K | 25 pm at 2 µm range |
| Confocal Unit | |
| configuration | compact and modular design, two optical channels: one excitation and one detection channel |
| key benefits | motorized steering mirror for combined beams, long-term stability: drift of < 100 nm/24h (within deltaT=2K in lab) |
| confocal excitation | 515 nm (others on request) |
| compatible LT-objective | LT-APO/Raman532 |
| inspection unit | sample/tip imaging with large field of view: ~55 µm |
| Sample Positioning | |
| total travel range | 2 mm x 3 mm x 2.5 mm (closed loop via resistive encoder), 3 degrees of freedom each for tip and sample |
| fine scan range | 30 x 30 x 4.3 µm³ @ 300 K, 18 x 18 x 2 µm³ @ 4 K (open loop) |
| sample holder | Ti plate with integrated heater and calibrated temperature sensor |
| Suitable Operating Conditions | |
| temperature range | < 1.8 .. 300 K in quench mode (AFM scan with optical readout, MW off), < 4 .. 300 K in cw-ODMR |
| magnetic field range | 9/1/1 or 1/1/1 Tesla |
| atmosphere | designed for He exchange gas |
| Suitable Cooling Systems | |
| bore size requirement | designed for top-loading cryostat with 2" (50.8 mm) opening (Ti housing diameter of mic = 48 mm) |
| compatible cryostats | attoDRY2200 |
| Options and Upgrades | |
| MOKE | polar MOKE in H/V basis with a biased photodetector (BW=500 kHz), remotely controllable waveplate, integration into QS3 software |
| RF sample holder | 2 additional RF cables for the sample |
