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11 protocols using air objective

1

Confocal Microscopy Image Acquisition

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Images were acquired using a Nikon C2+ laser-scanning confocal microscope with a 60×/1.4 oil objective or a 20×/0.75 air objective (Nikon). Images were recorded as 1,024 × 1,024 square pixels. RGB images were assembled in ImageJ software (imagej.nih.gov), and panels were labeled in Adobe Illustrator CC.
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2

Confocal Imaging of Cellular Structures

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Images were acquired using a Nikon C2+ laser-scanning confocal microscope using a 60×/1.4 oil objective or a 20×/0.75 air objective (Nikon). Images were recorded as 1024×1024 square pixels. RGB images were assembled in ImageJ software (imagej.nih.gov), and panels were labelled in Adobe Illustrator CC.
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3

Confocal Imaging with Nikon C2+ Microscope

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Images were acquired with a Nikon C2+ laser-scanning confocal microscope using a 60×/1.4 oil objective or a 20×/0.75 air objective (Nikon). Images were recorded as 1024 × 1024 square pixels. RGB images were assembled in ImageJ software (imagej.nih.gov), and panels were labeled in Adobe Illustrator CC.
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4

Reflectivity Spectra Measurement Protocol

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Bright-field reflectivity spectra at normal incidence were collected using a 20× air objective (NIKON, NA = 0.45), directed to a fiber-coupled spectrometer and normalized with reflection from a standard dielectric-coated silver mirror.
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5

T Cell Tracking and Perturbations

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Cell tracking on the 2D and “2.5D” surfaces was performed with the TrackMate plugin in ImageJ. T cells were imaged with differential interference contrast microscopy at 10 s intervals using a ×20 air objective (Nikon Instruments, Japan) and tracking was later performed manually, one cell at a time, at each interval. Cells were maintained at 37 °C in 5% CO2 (Tokai Hit, Japan) for the duration of the live-cell imaging session. Images were captured at resolutions of 512 × 512 or 1024 × 1024 pixels. For phenotype perturbations, T cells were treated with either 70 nM Taxol or 10 µM Nocodazole.
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6

Cell Tracking via Automated Microscopy

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Cells were seeded in plates with poly-L-lysine–coated glass bottoms. Upon cell adhesion, each plate was positioned into a stage top incubator on an Eclipse Ti 2 inverted microscope (Nikon). Cells were automatically imaged over time using phase contrast microscopy at multiple positions per well using a 10× air objective (Nikon). Cell tracking was performed manually for all selected cells. Further details are given in SI Appendix, Extended Materials and Methods.
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7

Imaging of L-Scaffolds and L-Hydrogels

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Repopulated L-Scaffolds and L-Hydrogels were fixed in 4% formaldehyde for 45 min at room temperature and stored in PBS with 0.05% sodium azide (Sigma-Aldrich) at 4 °C until further processing. This included permeabilization in 0.1% Triton X-100 (Sigma-Aldrich) for 5 min at room temperature and staining with 1X Phalloidin-iFluor 555 (Abcam, Cambridge, UK) for F-actin staining and DAPI (nuclei staining) prepared in 1% BSA in PBS for 1 h at room temperature. The L-Scaffolds and L-Hydrogels were immersed in Ce3D (prepared as previously described [21 (link)]) in chambers built on top of slides using iSpacers (SunJin Lab) and glass coverslips. They were imaged in a resonant scanner A1RHD confocal microscope (Nikon) controlled with the NIS Elements AR software (Nikon) using a 10× air objective (Nikon) and laser excitation. Images were corrected for brightness and prepared for publication in NIS Elements AR Analysis software (Nikon).
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8

Raman Imaging of Biofilm Microstructure

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Raman analysis was performed using a laser scanning confocal Raman microscope (Alpha 300R, WITec, GMBH, Germany), equipped with 532 and 785 nm focused lasers. The laser radiation was delivered to the microscope using a polarization preserving single mode optical fiber, deflected through a dichroic beam-splitter and focused onto the sample through the microscope objectives. Raman images from biofilms were acquired using either a coverslip corrected Nikon water immersion 60× objective (NA = 1) or a 40× air objective (NA = 0.6). Images were obtained by acquiring a full Raman spectrum from each image pixel (150 × 150, 100×100 or 80×80 pixels) over a desired region on the sample with an integration time of 100 ms per spectrum. Data processing software WITec Project 2.10 was used to remove cosmic ray spikes from Raman images. Principal component analysis was performed on the Raman images in MATLAB using previously established procedures.23 (link)
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9

Microscopy Techniques for Cell Imaging

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All experiments were conducted 16–28 hr after seeding the cells on the sample. Then the cells were observed on an inverted Nikon Ti-E2 microscope with an Orca Flash 4.0 sCMOS camera (Hamamatsu), a temperature control system set at 37°C, a humidifier, and a CO 2 controller. For the opto-experiments on cell doublets and singlets, a Nikon ×60 oil objective was used and for the opto-experiments on tissues a Nikon ×40 air objective was used. The E-cadherin and vinculin staining images were taken with an Eclipse Ti inverted confocal microscope (Nikon France Instruments, Champigny sur Marne, France), equipped with sCMOS prime camera (Photometrics), a ×60 objective, and a CSU X1 spinning disk (Yokogawa, Roper Scientific, Lisses, France). MetaMorph software was used for controlling the microscope (Universal Imaging Corporation, Roper Scientific, Lisses, France). Unless otherwise stated, all photoactivations were done with one pulse per min for 10min , and each pulse had a duration of 200ms , a power density of 0.9mWmm-2 , and a wavelength of 470nm . The power density was measured with a power meter right after the objective by shining light on a surface of a given size and dividing the measured power by this size. Photoactivation regions were aligned with respect to the micropattern to ensure reproducibility.
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10

Confocal Raman Spectroscopy of Samples

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Confocal Raman spectroscopy measurements were conducted using a WITec Confocal Raman Microscope System Alpha 300R (WITec, Ulm, Germany) with a UHTS300 spectrometer and a DV401 CCD detector with 600/mm grating. The WITec spectrometer was calibrated with a Mercury—Argon lamp. A 532 nm wavelength Nd:YAG laser was used as the excitation source. A 100× air objective (NA 0.90; Nikon Instruments, Melville, NY) was used for focusing the 532 nm excitation laser to the sample. Laser power at the objective was 10 mW as measured by an optical power meter (THORLABS, New Jersey). Resolution of the microscope was approximately 0.3 μm based on Abbe’s diffraction formula for lateral resolution.
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