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Movement tracking with TrackMate

               Videos were recorded at 120 fps and then converted to files at 30 fps, cut to the area of interest
               and exported as uncompressed AVI files (8-bit, UYUY codec) with Premiere Pro (Adobe,

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               USA). Movement speed of the microscaffolds was tracked via TrackMate plugin v6.0.3  in
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               Fiji v 1.53c  . After importing, the files were converted to greyscale, the ROI was set around
               the central channel. Particles were detected using the Difference-of-Gaussian (DoG) detector

               using 20 px, 2 px thresholds and no filters as settings. Using the quality filter, unneeded dots
               were erased until only the main track was visible anymore. Using the Laplacian filter with a

               maximum distance of 20 px and a segment gap closing of 20 px and 5 frames, the tracks were
               generated. Filtering by track ID allowed to get the track speed of each microscaffold.





               Fluorescence spectrum analysis of microconstructs
               The fact that the produced microscaffolds are fluorescent, due to the presence of the PI in the

               material,  was  leveraged  for  the  on-the-fly  detection  and  analysis  process.  The  fluorescent
               spectrum  of  BBs  produced  from  ZrHyb  was  characterized  by  placing  around  100

               microscaffolds into a 96-well plate in 200 µl of 1-Propanol. The samples were excited at 360
               nm and their emission spectrum was analyzed on a photometer (Synergy H1, BioTek) from

               390 nm to 700 nm in intervals of 10 nm. The excitation wavelength was determined from

               literature values stating that the photoinitiator showed the highest absorption potential at 365
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               nm  . The emission values were subtracted from the background signal emitted from the well
               plate and the 1-Propanol.




               Optical Detection Device

               The optical detection mechanism was built using an excitation LED with a wavelength of 360-
               370 nm and (3W370380m, Avonec GmbH). The LED was powered with a constant current

               source  (LDD-700LW,  Mean  Well)  at  100%  output.  The  light  source  was  collimated  and
               focused using a condenser lens (ACL25416U, Thorlabs). Light splitting was performed via

               dichroic  mirror  (DMLP490R,  Thorlabs)  housed  in  a  metric  filter  mount  (CM1-DCH/M,

               Thorlabs). To distinguish between excitation and emission wavelength, a 500 nm long-pass
               filter (62983, Edmund Optics) and a short-pass filter at 475 nm (84705, Edmund Optics) was

               used. The LED light was positioned at a precise distance to the lens using a 3D printed holder.
               The fluorescent excitation signal was detected with a photodiode (PDA100A2, Thorlabs). The



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