pipettes microscope slide holder Search Results


90
ibidi GmbH 8-well µ-slides (chambered coverslip)
8 Well µ Slides (Chambered Coverslip), supplied by ibidi GmbH, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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Average 90 stars, based on 1 article reviews
8-well µ-slides (chambered coverslip) - by Bioz Stars, 2026-09
90/100 stars
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90
Corning Life Sciences untreated microscope slide cls294775 × 25
Untreated Microscope Slide Cls294775 × 25, supplied by Corning Life Sciences, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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Average 90 stars, based on 1 article reviews
untreated microscope slide cls294775 × 25 - by Bioz Stars, 2026-09
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95
R&D Systems microscope slides
Microscope Slides, supplied by R&D Systems, used in various techniques. Bioz Stars score: 95/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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Average 95 stars, based on 1 article reviews
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95/100 stars
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90
anvajo GmbH acella 100 microscopic slide
Acella 100 Microscopic Slide, supplied by anvajo GmbH, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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Average 90 stars, based on 1 article reviews
acella 100 microscopic slide - by Bioz Stars, 2026-09
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99
Eppendorf AG air displacement pipette
Air Displacement Pipette, supplied by Eppendorf AG, used in various techniques. Bioz Stars score: 99/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
https://www.bioz.com/product/pipettes+microscope+slide+holder/Eppendorf/pmc12320928-51-17-20
Average 99 stars, based on 1 article reviews
air displacement pipette - by Bioz Stars, 2026-09
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86
Fisher Scientific microscope glass slide
( a ) Schematic of PFAM implemented in a widefield fluorescence <t>microscope.</t> A deformable mirror (DM, inset) is placed at a plane conjugate to the objective’s back pupil for both aberration measurement and correction. Inset: (Left) Enlarged view of the image plane at the widefield (WF) camera, showing N probe beamlets (gold) scanned around a stationary reference focus (gray) by controlling tip and tilt of their corresponding DM macro-segments; (Upper right) At each tip/tilt configuration, phase of probe beamlet is modulated at a unique frequency ωs ( ω 1 , ω 2 , …, ω N ) by controlling the piston of its corresponding macro-segment, modulating the fluorescence signal resulting from the interference between the probe beamlet and the reference focus at frequency ω s ; (Lower right) Interference strength between each probe beamlet and the reference focus is extracted by performing a Fourier transform (FT) on the fluorescence signal trace and identifying the Fourier magnitude at ω s . ( b ) DM grouping configuration. Modulated regions (gold) consist of macro-segments formed by grouping adjacent DM segments with piston, tip, and tilt control. Remaining segments (gray) are held static to generate the reference focus. To increase sampling density of phase gradient measurement, three DM groups are typically used sequentially (see other groupings in Supplementary Fig. 1 ). ( c ) Tip/tilt interference maps for macro-segments across three DM groups, from which phase gradients are measured. Inset: Example interference map (scaled to the sample plane) of a macro-segment. ( d ) Corrective wavefronts for system aberration measured using PFAM from a 0.5-μm-diameter fluorescent bead (left) and phase retrieval from a 0.2-μm-diameter fluorescent bead (right). Both PFAM and PR were iterated twice. ( e ) Maximum intensity projection (MIP) images in XZ of a 0.5-μm-diameter fluorescent bead acquired without adaptive optics (AO, left), with corrective wavefront from PFAM (middle), and with corrective wavefront from phase retrieval (right). ( f ) Axial fluorescence intensity profiles along dashed lines in ( e ).
Microscope Glass Slide, supplied by Fisher Scientific, used in various techniques. Bioz Stars score: 86/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
https://www.bioz.com/product/pipettes+microscope+slide+holder/glass+slides/bio_rxiv__2025__10__11__681535-220-42-46
Average 86 stars, based on 1 article reviews
microscope glass slide - by Bioz Stars, 2026-09
86/100 stars
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90
UHU GmbH Co KG super glue uhu sekundenkleber pipette
( a ) Schematic of PFAM implemented in a widefield fluorescence <t>microscope.</t> A deformable mirror (DM, inset) is placed at a plane conjugate to the objective’s back pupil for both aberration measurement and correction. Inset: (Left) Enlarged view of the image plane at the widefield (WF) camera, showing N probe beamlets (gold) scanned around a stationary reference focus (gray) by controlling tip and tilt of their corresponding DM macro-segments; (Upper right) At each tip/tilt configuration, phase of probe beamlet is modulated at a unique frequency ωs ( ω 1 , ω 2 , …, ω N ) by controlling the piston of its corresponding macro-segment, modulating the fluorescence signal resulting from the interference between the probe beamlet and the reference focus at frequency ω s ; (Lower right) Interference strength between each probe beamlet and the reference focus is extracted by performing a Fourier transform (FT) on the fluorescence signal trace and identifying the Fourier magnitude at ω s . ( b ) DM grouping configuration. Modulated regions (gold) consist of macro-segments formed by grouping adjacent DM segments with piston, tip, and tilt control. Remaining segments (gray) are held static to generate the reference focus. To increase sampling density of phase gradient measurement, three DM groups are typically used sequentially (see other groupings in Supplementary Fig. 1 ). ( c ) Tip/tilt interference maps for macro-segments across three DM groups, from which phase gradients are measured. Inset: Example interference map (scaled to the sample plane) of a macro-segment. ( d ) Corrective wavefronts for system aberration measured using PFAM from a 0.5-μm-diameter fluorescent bead (left) and phase retrieval from a 0.2-μm-diameter fluorescent bead (right). Both PFAM and PR were iterated twice. ( e ) Maximum intensity projection (MIP) images in XZ of a 0.5-μm-diameter fluorescent bead acquired without adaptive optics (AO, left), with corrective wavefront from PFAM (middle), and with corrective wavefront from phase retrieval (right). ( f ) Axial fluorescence intensity profiles along dashed lines in ( e ).
Super Glue Uhu Sekundenkleber Pipette, supplied by UHU GmbH Co KG, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
https://www.bioz.com/product/pipettes+microscope+slide+holder/solvent+free+glue/pmc09864629-310-11-16
Average 90 stars, based on 1 article reviews
super glue uhu sekundenkleber pipette - by Bioz Stars, 2026-09
90/100 stars
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90
KEYENCE digital microscope
( a ) Schematic of PFAM implemented in a widefield fluorescence <t>microscope.</t> A deformable mirror (DM, inset) is placed at a plane conjugate to the objective’s back pupil for both aberration measurement and correction. Inset: (Left) Enlarged view of the image plane at the widefield (WF) camera, showing N probe beamlets (gold) scanned around a stationary reference focus (gray) by controlling tip and tilt of their corresponding DM macro-segments; (Upper right) At each tip/tilt configuration, phase of probe beamlet is modulated at a unique frequency ωs ( ω 1 , ω 2 , …, ω N ) by controlling the piston of its corresponding macro-segment, modulating the fluorescence signal resulting from the interference between the probe beamlet and the reference focus at frequency ω s ; (Lower right) Interference strength between each probe beamlet and the reference focus is extracted by performing a Fourier transform (FT) on the fluorescence signal trace and identifying the Fourier magnitude at ω s . ( b ) DM grouping configuration. Modulated regions (gold) consist of macro-segments formed by grouping adjacent DM segments with piston, tip, and tilt control. Remaining segments (gray) are held static to generate the reference focus. To increase sampling density of phase gradient measurement, three DM groups are typically used sequentially (see other groupings in Supplementary Fig. 1 ). ( c ) Tip/tilt interference maps for macro-segments across three DM groups, from which phase gradients are measured. Inset: Example interference map (scaled to the sample plane) of a macro-segment. ( d ) Corrective wavefronts for system aberration measured using PFAM from a 0.5-μm-diameter fluorescent bead (left) and phase retrieval from a 0.2-μm-diameter fluorescent bead (right). Both PFAM and PR were iterated twice. ( e ) Maximum intensity projection (MIP) images in XZ of a 0.5-μm-diameter fluorescent bead acquired without adaptive optics (AO, left), with corrective wavefront from PFAM (middle), and with corrective wavefront from phase retrieval (right). ( f ) Axial fluorescence intensity profiles along dashed lines in ( e ).
Digital Microscope, supplied by KEYENCE, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
https://www.bioz.com/product/pipettes+microscope+slide+holder/fluorescence+microscope+bz+9000/pmc10345981-173-16-15
Average 90 stars, based on 1 article reviews
digital microscope - by Bioz Stars, 2026-09
90/100 stars
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90
MATHESON fully frosted microscope slides
( a ) Schematic of PFAM implemented in a widefield fluorescence <t>microscope.</t> A deformable mirror (DM, inset) is placed at a plane conjugate to the objective’s back pupil for both aberration measurement and correction. Inset: (Left) Enlarged view of the image plane at the widefield (WF) camera, showing N probe beamlets (gold) scanned around a stationary reference focus (gray) by controlling tip and tilt of their corresponding DM macro-segments; (Upper right) At each tip/tilt configuration, phase of probe beamlet is modulated at a unique frequency ωs ( ω 1 , ω 2 , …, ω N ) by controlling the piston of its corresponding macro-segment, modulating the fluorescence signal resulting from the interference between the probe beamlet and the reference focus at frequency ω s ; (Lower right) Interference strength between each probe beamlet and the reference focus is extracted by performing a Fourier transform (FT) on the fluorescence signal trace and identifying the Fourier magnitude at ω s . ( b ) DM grouping configuration. Modulated regions (gold) consist of macro-segments formed by grouping adjacent DM segments with piston, tip, and tilt control. Remaining segments (gray) are held static to generate the reference focus. To increase sampling density of phase gradient measurement, three DM groups are typically used sequentially (see other groupings in Supplementary Fig. 1 ). ( c ) Tip/tilt interference maps for macro-segments across three DM groups, from which phase gradients are measured. Inset: Example interference map (scaled to the sample plane) of a macro-segment. ( d ) Corrective wavefronts for system aberration measured using PFAM from a 0.5-μm-diameter fluorescent bead (left) and phase retrieval from a 0.2-μm-diameter fluorescent bead (right). Both PFAM and PR were iterated twice. ( e ) Maximum intensity projection (MIP) images in XZ of a 0.5-μm-diameter fluorescent bead acquired without adaptive optics (AO, left), with corrective wavefront from PFAM (middle), and with corrective wavefront from phase retrieval (right). ( f ) Axial fluorescence intensity profiles along dashed lines in ( e ).
Fully Frosted Microscope Slides, supplied by MATHESON, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
https://www.bioz.com/product/pipettes+microscope+slide+holder/superfrost+plus+slides/pm09401076-46-27-31
Average 90 stars, based on 1 article reviews
fully frosted microscope slides - by Bioz Stars, 2026-09
90/100 stars
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90
Avantor microscope slide
( a ) Schematic of PFAM implemented in a widefield fluorescence <t>microscope.</t> A deformable mirror (DM, inset) is placed at a plane conjugate to the objective’s back pupil for both aberration measurement and correction. Inset: (Left) Enlarged view of the image plane at the widefield (WF) camera, showing N probe beamlets (gold) scanned around a stationary reference focus (gray) by controlling tip and tilt of their corresponding DM macro-segments; (Upper right) At each tip/tilt configuration, phase of probe beamlet is modulated at a unique frequency ωs ( ω 1 , ω 2 , …, ω N ) by controlling the piston of its corresponding macro-segment, modulating the fluorescence signal resulting from the interference between the probe beamlet and the reference focus at frequency ω s ; (Lower right) Interference strength between each probe beamlet and the reference focus is extracted by performing a Fourier transform (FT) on the fluorescence signal trace and identifying the Fourier magnitude at ω s . ( b ) DM grouping configuration. Modulated regions (gold) consist of macro-segments formed by grouping adjacent DM segments with piston, tip, and tilt control. Remaining segments (gray) are held static to generate the reference focus. To increase sampling density of phase gradient measurement, three DM groups are typically used sequentially (see other groupings in Supplementary Fig. 1 ). ( c ) Tip/tilt interference maps for macro-segments across three DM groups, from which phase gradients are measured. Inset: Example interference map (scaled to the sample plane) of a macro-segment. ( d ) Corrective wavefronts for system aberration measured using PFAM from a 0.5-μm-diameter fluorescent bead (left) and phase retrieval from a 0.2-μm-diameter fluorescent bead (right). Both PFAM and PR were iterated twice. ( e ) Maximum intensity projection (MIP) images in XZ of a 0.5-μm-diameter fluorescent bead acquired without adaptive optics (AO, left), with corrective wavefront from PFAM (middle), and with corrective wavefront from phase retrieval (right). ( f ) Axial fluorescence intensity profiles along dashed lines in ( e ).
Microscope Slide, supplied by Avantor, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
https://www.bioz.com/product/pipettes+microscope+slide+holder/microscope+slides/pmc07647122-293-9-11
Average 90 stars, based on 1 article reviews
microscope slide - by Bioz Stars, 2026-09
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92
Addgene inc blade • parafilm • microscope slide • transfer pipette
Microinjection setup for needle and droplet calibration . A . The length of the pulled needle before cutting. B . Needle selection: cutting the tip of a pre-pulled needle with a sharp blade on a scale micrometer slide wrapped by <t>parafilm</t> under the <t>microscope</t> to produce a slant needle with similar opening. C . Injection with a slant needle backfilled with phenol red to produce a droplet. Volume determination by injecting into mineral oil placed on a micrometer. D . Fertilized embryos aligned into the ramps of pre-casted injection plate.
Blade • Parafilm • Microscope Slide • Transfer Pipette, supplied by Addgene inc, used in various techniques. Bioz Stars score: 92/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
https://www.bioz.com/product/pipettes+microscope+slide+holder/CMV-mito-LAR-GECO1%2E2+(Plasmid+%2361245)/pmc08374492-4-105-120
Average 92 stars, based on 1 article reviews
blade • parafilm • microscope slide • transfer pipette - by Bioz Stars, 2026-09
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90
CITOTEST Labware microscope slide citotest haimen
Microinjection setup for needle and droplet calibration . A . The length of the pulled needle before cutting. B . Needle selection: cutting the tip of a pre-pulled needle with a sharp blade on a scale micrometer slide wrapped by <t>parafilm</t> under the <t>microscope</t> to produce a slant needle with similar opening. C . Injection with a slant needle backfilled with phenol red to produce a droplet. Volume determination by injecting into mineral oil placed on a micrometer. D . Fertilized embryos aligned into the ramps of pre-casted injection plate.
Microscope Slide Citotest Haimen, supplied by CITOTEST Labware, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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Average 90 stars, based on 1 article reviews
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Image Search Results


( a ) Schematic of PFAM implemented in a widefield fluorescence microscope. A deformable mirror (DM, inset) is placed at a plane conjugate to the objective’s back pupil for both aberration measurement and correction. Inset: (Left) Enlarged view of the image plane at the widefield (WF) camera, showing N probe beamlets (gold) scanned around a stationary reference focus (gray) by controlling tip and tilt of their corresponding DM macro-segments; (Upper right) At each tip/tilt configuration, phase of probe beamlet is modulated at a unique frequency ωs ( ω 1 , ω 2 , …, ω N ) by controlling the piston of its corresponding macro-segment, modulating the fluorescence signal resulting from the interference between the probe beamlet and the reference focus at frequency ω s ; (Lower right) Interference strength between each probe beamlet and the reference focus is extracted by performing a Fourier transform (FT) on the fluorescence signal trace and identifying the Fourier magnitude at ω s . ( b ) DM grouping configuration. Modulated regions (gold) consist of macro-segments formed by grouping adjacent DM segments with piston, tip, and tilt control. Remaining segments (gray) are held static to generate the reference focus. To increase sampling density of phase gradient measurement, three DM groups are typically used sequentially (see other groupings in Supplementary Fig. 1 ). ( c ) Tip/tilt interference maps for macro-segments across three DM groups, from which phase gradients are measured. Inset: Example interference map (scaled to the sample plane) of a macro-segment. ( d ) Corrective wavefronts for system aberration measured using PFAM from a 0.5-μm-diameter fluorescent bead (left) and phase retrieval from a 0.2-μm-diameter fluorescent bead (right). Both PFAM and PR were iterated twice. ( e ) Maximum intensity projection (MIP) images in XZ of a 0.5-μm-diameter fluorescent bead acquired without adaptive optics (AO, left), with corrective wavefront from PFAM (middle), and with corrective wavefront from phase retrieval (right). ( f ) Axial fluorescence intensity profiles along dashed lines in ( e ).

Journal: bioRxiv

Article Title: Parallel frequency-multiplexed aberration measurement for widefield fluorescence microscopy

doi: 10.1101/2025.10.11.681535

Figure Lengend Snippet: ( a ) Schematic of PFAM implemented in a widefield fluorescence microscope. A deformable mirror (DM, inset) is placed at a plane conjugate to the objective’s back pupil for both aberration measurement and correction. Inset: (Left) Enlarged view of the image plane at the widefield (WF) camera, showing N probe beamlets (gold) scanned around a stationary reference focus (gray) by controlling tip and tilt of their corresponding DM macro-segments; (Upper right) At each tip/tilt configuration, phase of probe beamlet is modulated at a unique frequency ωs ( ω 1 , ω 2 , …, ω N ) by controlling the piston of its corresponding macro-segment, modulating the fluorescence signal resulting from the interference between the probe beamlet and the reference focus at frequency ω s ; (Lower right) Interference strength between each probe beamlet and the reference focus is extracted by performing a Fourier transform (FT) on the fluorescence signal trace and identifying the Fourier magnitude at ω s . ( b ) DM grouping configuration. Modulated regions (gold) consist of macro-segments formed by grouping adjacent DM segments with piston, tip, and tilt control. Remaining segments (gray) are held static to generate the reference focus. To increase sampling density of phase gradient measurement, three DM groups are typically used sequentially (see other groupings in Supplementary Fig. 1 ). ( c ) Tip/tilt interference maps for macro-segments across three DM groups, from which phase gradients are measured. Inset: Example interference map (scaled to the sample plane) of a macro-segment. ( d ) Corrective wavefronts for system aberration measured using PFAM from a 0.5-μm-diameter fluorescent bead (left) and phase retrieval from a 0.2-μm-diameter fluorescent bead (right). Both PFAM and PR were iterated twice. ( e ) Maximum intensity projection (MIP) images in XZ of a 0.5-μm-diameter fluorescent bead acquired without adaptive optics (AO, left), with corrective wavefront from PFAM (middle), and with corrective wavefront from phase retrieval (right). ( f ) Axial fluorescence intensity profiles along dashed lines in ( e ).

Article Snippet: Fluorescent beads with diameters of 0.2 μm, 0.5 μm, 1 μm, 2 μm (FluoSpheresTM Carboxylate-Modified Microspheres, yellow-green 505/515; ThermoFisher Scientific) or 4 μm (ThermoFisher Scientific TetraSpeck Microspheres, fluorescent blue/green/orange/dark red) were diluted 1:1000 to 1:3000 in deionized water and pipetted onto a microscope glass slide (12-550-12, Fisher Scientific).

Techniques: Fluorescence, Microscopy, Control, Sampling

( a ) (Left) Schematic of structured illumination (SI); (Right) Simulated illumination pattern at the back pupil plane of the microscope objective and the periodic hexagonal SI pattern at the objective focal plane. Yellow dashed circle: cutoff frequency; ( b ) (Left) Example image of a fluorescence film of 0.8 μm thickness under SI; (Middle) Power spectrum (PS) of the Fourier Transform (FT) of the image in logarithmic scale; (Right) Profile along the dashed white line in PS image. Yellow dashed circle: 0.5k 0 ; k 0 : cutoff frequency; Red dashed lines: spatial frequency of SI. ( c ) Same as in ( b ) but for a 2-µm-diameter fluorescent bead. ( d ) PFAM-SIFT calculates the average PS values within regions containing modulated in-focus signals (red boxes) in each frame to obtain the PS trace, which is then Fourier transformed and Fourier magnitudes corresponding to the interference strength between each probe beamlet and the reference focus are extracted for phase gradient measurement. ( e ) Example tip/tilt interference maps obtained using PS values with two-group DM configuration. ( f ) (From left to right) Ground-truth (GT) corrective wavefronts for astigmatism applied to DM, corrective wavefronts from PFAM-SIFT (top) and PFAM (bottom) from 1 μm, 2 μm, and 4 μm fluorescent beads, and 0.8 μm fluorescence films, respectively, at a camera frame rate of 50 Hz. Each method was iterated three times. RMSE: RMS errors between GT and measured wavefronts. ( g ) RMSEs for PFAM and PFAM-SIFT from different fluorescent structures.

Journal: bioRxiv

Article Title: Parallel frequency-multiplexed aberration measurement for widefield fluorescence microscopy

doi: 10.1101/2025.10.11.681535

Figure Lengend Snippet: ( a ) (Left) Schematic of structured illumination (SI); (Right) Simulated illumination pattern at the back pupil plane of the microscope objective and the periodic hexagonal SI pattern at the objective focal plane. Yellow dashed circle: cutoff frequency; ( b ) (Left) Example image of a fluorescence film of 0.8 μm thickness under SI; (Middle) Power spectrum (PS) of the Fourier Transform (FT) of the image in logarithmic scale; (Right) Profile along the dashed white line in PS image. Yellow dashed circle: 0.5k 0 ; k 0 : cutoff frequency; Red dashed lines: spatial frequency of SI. ( c ) Same as in ( b ) but for a 2-µm-diameter fluorescent bead. ( d ) PFAM-SIFT calculates the average PS values within regions containing modulated in-focus signals (red boxes) in each frame to obtain the PS trace, which is then Fourier transformed and Fourier magnitudes corresponding to the interference strength between each probe beamlet and the reference focus are extracted for phase gradient measurement. ( e ) Example tip/tilt interference maps obtained using PS values with two-group DM configuration. ( f ) (From left to right) Ground-truth (GT) corrective wavefronts for astigmatism applied to DM, corrective wavefronts from PFAM-SIFT (top) and PFAM (bottom) from 1 μm, 2 μm, and 4 μm fluorescent beads, and 0.8 μm fluorescence films, respectively, at a camera frame rate of 50 Hz. Each method was iterated three times. RMSE: RMS errors between GT and measured wavefronts. ( g ) RMSEs for PFAM and PFAM-SIFT from different fluorescent structures.

Article Snippet: Fluorescent beads with diameters of 0.2 μm, 0.5 μm, 1 μm, 2 μm (FluoSpheresTM Carboxylate-Modified Microspheres, yellow-green 505/515; ThermoFisher Scientific) or 4 μm (ThermoFisher Scientific TetraSpeck Microspheres, fluorescent blue/green/orange/dark red) were diluted 1:1000 to 1:3000 in deionized water and pipetted onto a microscope glass slide (12-550-12, Fisher Scientific).

Techniques: Microscopy, Fluorescence, Transformation Assay

Microinjection setup for needle and droplet calibration . A . The length of the pulled needle before cutting. B . Needle selection: cutting the tip of a pre-pulled needle with a sharp blade on a scale micrometer slide wrapped by parafilm under the microscope to produce a slant needle with similar opening. C . Injection with a slant needle backfilled with phenol red to produce a droplet. Volume determination by injecting into mineral oil placed on a micrometer. D . Fertilized embryos aligned into the ramps of pre-casted injection plate.

Journal: MethodsX

Article Title: Microinjection quality control in zebrafish model for genetic manipulations

doi: 10.1016/j.mex.2021.101418

Figure Lengend Snippet: Microinjection setup for needle and droplet calibration . A . The length of the pulled needle before cutting. B . Needle selection: cutting the tip of a pre-pulled needle with a sharp blade on a scale micrometer slide wrapped by parafilm under the microscope to produce a slant needle with similar opening. C . Injection with a slant needle backfilled with phenol red to produce a droplet. Volume determination by injecting into mineral oil placed on a micrometer. D . Fertilized embryos aligned into the ramps of pre-casted injection plate.

Article Snippet: Resource availability: , Materials and reagents • Phenol red (Sigma, cat#P0290, USA) • Petri dish • Phenyl Thio Urea (PTU) (P7629) • Egg water (E3): NaCl (Sigma, cat#S7653, USA), KCL (Sigma, cat#P9333, USA), MgSO4-7H2O (Sigma, cat#63138, USA), CaCl2-2H2o (Sigma, cat#C1016, USA) • Agarose (Sigma Aldrich, cat# A9539, USA) • Glass thin w/filament injection capillaries (World Precision Instrument, cat#TW100F-4, USA) • μTip Micropipette (World precision instruments cat#Tip05TW1F, USA) • Adhesive putty (tac patafix) • Mold (Eppendorf, Germany or Adaptive sciences tools, Cat # TU-1) • Micrometer - stage graticules S16 (VWR, cat#100499-308, USA) • Loading tips (Eppendorf, 20ul, cat#5242956.003, Germany) • Mineral oil (Sigma, cat#M5904, USA) • Blade • Parafilm • microscope slide • transfer pipette (VWR, cat#6124545) • DNA plasmid (Addgene, pCS2+8NmCherry, cat#34936, pSGEM-1 eGFP#44) • Subcloning efficiency chemi-competent cells: E.Coli (DH5α) (Thermofisher Scientific,18265017, USA) • Purelink Quick PCR purification kit (cat#K310002, Thermofisher Scientific, USA) • Mmessage Mmachine T7 transcription kit (Ambion, cat#Am1344, USA) • Mmessage Mmachine Sp6 transcription kit (Ambion, cat#Am1340, USA) • Restriction Enzymes: EcoRI (Thermofisher Scientific, cat#ER0271, USA), Nhel (cat#ER0971, Thermofisher Scientific, cat#ER0271, USA) • Rhodamine injection dye (Thermo Fisher Scientific, cat# D1816, USA) • Fluorescein injection dye (Thermo Fisher Scientific, cat# D1820, USA). Equipment's • Hood (Thermo scientific,1300 SERIES A2, USA) • Needle puller (Narishige, PC-10, Japan) • Picoliter injector (Harvard apparatus, Warner instrument, PLI-100A, USA) • Air source • Microscope (ZEISS, Stemi 2000-C, Lumar V.12, Germany) • Camera (ZEISS, Axiocam ERc 5s, USA) • ZEN blue Software (lite2.5, Germany).

Techniques: Microinjection, Selection, Microscopy, Injection