RESUMEN
Radiologists today play a central role in making diagnostic decisions and labeling images for training and benchmarking artificial intelligence (AI) algorithms. A key concern is low inter-reader reliability (IRR) seen between experts when interpreting challenging cases. While team-based decisions are known to outperform individual decisions, inter-personal biases often creep up in group interactions which limit nondominant participants from expressing true opinions. To overcome the dual problems of low consensus and interpersonal bias, we explored a solution modeled on bee swarms. Two separate cohorts, three board-certified radiologists, (cohort 1), and five radiology residents (cohort 2) collaborated on a digital swarm platform in real time and in a blinded fashion, grading meniscal lesions on knee MR exams. These consensus votes were benchmarked against clinical (arthroscopy) and radiological (senior-most radiologist) standards of reference using Cohen's kappa. The IRR of the consensus votes was then compared to the IRR of the majority and most confident votes of the two cohorts. IRR was also calculated for predictions from a meniscal lesion detecting AI algorithm. The attending cohort saw an improvement of 23% in IRR of swarm votes (k = 0.34) over majority vote (k = 0.11). Similar improvement of 23% in IRR (k = 0.25) in 3-resident swarm votes over majority vote (k = 0.02) was observed. The 5-resident swarm had an even higher improvement of 30% in IRR (k = 0.37) over majority vote (k = 0.07). The swarm consensus votes outperformed individual and majority vote decision in both the radiologists and resident cohorts. The attending and resident swarms also outperformed predictions from a state-of-the-art AI algorithm.
Asunto(s)
Inteligencia Artificial , Radiólogos , Animales , Humanos , Consenso , Reproducibilidad de los Resultados , InteligenciaRESUMEN
Dual polarization interferometry (DPI) and quartz-crystal microgravimetry (QCM-D) were used to investigate the adsorption of DOPC vesicles to a solid hydrophilic surface. The layer of hydration formed between a self-assembled DOPC bilayer and a silica solid support was probed in assemblies constructed using H(2)O and D(2)O buffers. We used QCM-D to measure the mass of the bilayer, including the mass contribution of the coupled solvent that resides between the membrane-solid interface. The mass of only the DOPC in the bilayer was resolved using DPI. By comparing these two measurements, and also accounting for the bulk phase effects on mass, we have been able to determine the mass of water below the bilayer. The thickness of this hydration layer, calculated by relating its mass to the density of the layer, was determined to be 10.46 A +/- 0.15 A for trapped D(2)O and 10.21 A +/- 0.40 A for trapped H(2)O, in agreement with measurements obtained by other methods. This work establishes the feasibility of concurrently using DPI and QCM-D to gauge the extent of hydration in thin films.
RESUMEN
The electrostatically driven binding dynamics of a polyelectrolyte multilayer (PEMU) film was investigated in real-time using dual-beam polarization interferometry (DPI) and independently supported by quartz crystal microbalance with dissipation monitoring (QCM-D) studies. Multilayer assemblies of the polyanions poly[1-[4[(3-carboxy-4-hydroxyphenylazo)benzenesulfonamido]-1,2-ethanediyl sodium salt] (PAZO) and poly(styrene sulfonate) (PSS) were respectively constructed with the polycation poly(ethylenimine) (PEI) on anionic functionalized substrates using the layer-by-layer electrostatic self-assembly method. DPI measurements indicate that polyelectrolyte adsorption occurs in three distinct stages. In the first stage, for approximately 5 s, coil-like segments of polyanion partially tether to the surface of the oppositely charged PEI. In the second stage, these coils unfurl over a period of approximately 10 s to cover the surface resulting in an increase in average density of the film. During the final adsorption step, the surface-bound polyelectrolyte diffuses into the multilayer assembly, exposing the surface to further deposition. This last step occurs over a much longer time period and results in a highly interpenetrated film containing a charge-overcompensated region at the film surface.