Boecking leads the Molecular Machines Group and is acting director of the EMBL Australia Node in Single Molecule Science. The group reconstitutes molecular machines — clathrin coat disassembly, HIV capsid assembly and uncoating, pore-forming toxins — and watches them work one molecule at a time by TIRF, interferometric scattering (mass photometry) and fluorescence fluctuation methods, resolving short-lived intermediates that ensemble kinetics averages into invisibility. He trained originally in surface chemistry and biosensors with Gooding, which gives the group unusual competence in engineering the surfaces these assays run on. Positioned against the established body of NV-ensemble quantum sensing work — DEER, nanoscale NMR and T1 relaxometry protocols operating at pT/sqrt(Hz) field sensitivity — the argument for single-molecule methods over ensemble ones is identical to the argument for pushing NV sensing below its pT/sqrt(Hz) ensemble regime: the interesting biology lives in heterogeneity and in transient states that averaging destroys. Strong methodological neighbour for a quantum-biosensing candidate.
Gooding is one of the world's most-cited biosensor scientists (inaugural editor-in-chief of ACS Sensors) and runs a group of over thirty researchers spanning surface chemistry, electrochemistry and nanomedicine. The sensing programme that matters here is the move from ensemble to digital, single-molecule-resolved detection: nanoparticle-tethered electrochemical sensors in which single binding events are counted rather than averaged, nanopore blockade sensors for protein biomarkers such as PSA, amplification-free nucleic-acid detection, and antifouling surface chemistries that make any of this work in real biological fluid. He has a strong commercialisation record (AgaMatrix glucose sensors). Positioned against the established body of NV-ensemble quantum sensing work — DEER, nanoscale NMR and T1 relaxometry protocols operating at pT/sqrt(Hz) field sensitivity — his single-molecule-counting philosophy is the biosensing analogue of moving from a pT/sqrt(Hz) NV ensemble to single-spin detection: in both cases the sensitivity gain comes from resolving individual events rather than improving an averaged signal. He is also the obvious collaborator for anyone trying to functionalise a diamond or nanoparticle quantum sensor for a real analyte.
Reece runs UNSW's optical trapping and nanophotonics laboratory. The group combines optical tweezers with spectroscopy and microfluidics to characterise individual nanoparticles and cells: trapping and spectroscopically interrogating plasmonic core-satellite assemblies (with Gooding and Tilley), measuring single-cell mechanics, and building porous-silicon and photonic-crystal resonant structures for label-free biosensing where the analyte shifts a cavity resonance. Positioned against the established body of NV-ensemble quantum sensing work — DEER, nanoscale NMR and T1 relaxometry protocols operating at pT/sqrt(Hz) field sensitivity — optical trapping is the standard way to hold a nanoscale sensor — including a nanodiamond hosting an NV ensemble at pT/sqrt(Hz) — at a controlled position inside a cell or fluid, and levitated-nanodiamond spin-mechanics is an active field that this group's capabilities map onto almost exactly. Strong practical fit for a bio-oriented quantum sensing candidate.
Whitesides' group pioneered soft lithography and paper-based microfluidics, and has long applied these tools to low-cost point-of-care diagnostic biosensors for global health settings. Included as a borderline, not-preferred biosensing case: the sensing target (colorimetric/electrochemical assays) is compelling but device-fabrication-centric rather than a cutting-edge-sensitivity physical sensor.