Playing around with how to represent volume in #Snouty light sheet data. Here is a dividing hiPSC with endogenously tagged histone in all three orthogonal projections. Bluer is further away. If anything, it distracts from politics.
08.10.2025 19:57 β π 32 π 9 π¬ 1 π 0
Yes, there's a nice trick to compensating for transferring possession to the table from the crane. But there's also certain steps you can take before giving possession to the crane that decrease tension, leading to less severe shifts during future transfers. I'd love to walk you through them!
23.09.2025 16:59 β π 1 π 0 π¬ 1 π 0
the anticipation is killing me
18.09.2025 22:45 β π 1 π 0 π¬ 1 π 0
18.09.2025 22:44 β π 0 π 0 π¬ 0 π 0
(I see nothing)
18.09.2025 22:42 β π 0 π 0 π¬ 1 π 0
@jsdaniel02.bsky.social can make it happen!
18.09.2025 03:39 β π 1 π 0 π¬ 1 π 0
@tanner-fadero.bsky.social told me there was a discussion about the unofficial name for #snouty V3. We have had Mr. Snouty and King Snouty, and there were people suggesting Emperor Snouty. I think it is time for a Lady or EMPRESS snouty. I have created Art to support this.
18.09.2025 03:02 β π 16 π 5 π¬ 3 π 0
What if we could use 'any' immersion objective and get good 3D imaging? Normally we can't as we must refractive index match the immersion to the sample (previous post).
-> However, I realized a few years ago that we can get good 3D imaging with any immersion using remote refocus optics!
01.09.2025 18:20 β π 7 π 1 π¬ 1 π 0
But yeah, a modest tilt angle between projections looks similar!
30.08.2025 23:25 β π 0 π 0 π¬ 1 π 0
Oh neat! You're looking at a projection from the "native" angle. Interestingly, the closer your sheet tilt angle is to 0Β°, the more similar the native projection is to the normal Z projection.
30.08.2025 23:09 β π 0 π 0 π¬ 1 π 0
If that projection is from the deskew plug-in, then it's a true max intensity Z projection (where Z is O1's optical axis).
The deskew plug-in deskews AND rotates your data.
30.08.2025 06:41 β π 0 π 0 π¬ 1 π 0
Some first raw (not deskewed) data of live human induced pluripotent stem cells from #Snouty now ready for some serious live imaging. Light sheet moving at a 38-degree angle through the cell layer; coverslip is on the bottom.
28.08.2025 23:40 β π 56 π 10 π¬ 7 π 1
Chroma said no, but thorlabs seems interested!
29.08.2025 11:05 β π 1 π 0 π¬ 0 π 0
Optics folks: does anyone know a manufacturer of a dichroic beamsplitter *cube*?
Essentially, a dichroic version of this (for fluorescence microscopy):
28.08.2025 00:15 β π 0 π 0 π¬ 1 π 0
Science hive mind!
Does anyone do hardware tech dev on MRI or CT? Or do you know someone who does? I'd love an introduction, if so. Let me know!
21.08.2025 16:43 β π 0 π 0 π¬ 1 π 0
It's playing, you've just learned how to tune it out after so many builds
21.08.2025 02:28 β π 0 π 0 π¬ 0 π 0
Also, this build doesn't actually take six months. I was mostly waiting on parts!
21.08.2025 02:24 β π 1 π 0 π¬ 0 π 0
Here's a six-month time-lapse of me building the single objective light sheet fluorescence microscope at the UCSF Center for Advanced Light Microscopy!
Also pictured is @nicostuurman.bsky.social and @kahsage.bsky.social.
#snouty
20.08.2025 18:57 β π 43 π 7 π¬ 3 π 0
You should get @jsdaniel02.bsky.social to help you add in a 808 laser!
20.08.2025 14:02 β π 1 π 0 π¬ 0 π 0
I noticed that too! StayGold seems to have a very short triplet lifetime, suggesting that it's already doing a similar triplet-quenching mechanism to what is happening with infrared. StayGold should definitely be a first target for directed evolution. Imagine StayGold with infrared depletion!
19.08.2025 21:24 β π 2 π 0 π¬ 0 π 0
Interesting! What's more interesting to me is not "what proteins does this work in?" and instead "can this be engineered with directed evolution?"
We got this effect in GFP by *accident*, and the primary sequence of the proteins seems to have huge influence over how strong this effect is.
19.08.2025 19:53 β π 2 π 0 π¬ 1 π 0
In summary, for < $10,000 USD and less than a day's work, you can more than double the efficiency of your light sheet fluorescence microscope!
19.08.2025 19:40 β π 5 π 0 π¬ 0 π 0
Unlike confocal, light sheet also doesn't need to deplete triplets outside of the focal plane, because light sheet doesn't *generate* out-of-plane triplets.
19.08.2025 19:40 β π 3 π 0 π¬ 2 π 0
That brings us to light sheet fluorescence microscopy. Unlike widefield, it's easy to achieve the infrared intensity needed to reduce photobleaching in light sheet because the infrared laser is focused into a line. Here, we're getting a 2.5-fold reduction using a 200-mW 808-nm laser from Vortran.
19.08.2025 19:37 β π 2 π 0 π¬ 1 π 0
So the total volumetric bleaching reduction in confocal microscopy will be far less than the two- to ten-fold that Ludvikova et al. demonstrated.
19.08.2025 19:37 β π 3 π 0 π¬ 1 π 0
Infrared co-illumination in a confocal microscope will only remove triplets quickly enough from the in-focus plane. But confocal microscopy generates the same number of triplets at every plane!
19.08.2025 19:37 β π 3 π 0 π¬ 1 π 0
The less time that green proteins spend in the triplet state, the less likely they are to bleach (and poison your organism)!
19.08.2025 19:36 β π 3 π 0 π¬ 1 π 0
Infrared co-illumination works by selectively exciting green proteins in the triplet state, which converts them back to the singlet state more quickly. Triplets interact with dissolved oxygen and can donate their energy to create reactive oxygen species.
19.08.2025 19:36 β π 2 π 0 π¬ 1 π 0
Fundamental Cell Biology and Neuroscience at UCSF. Formerly Microbial Evolution at UBC. https://jcforward.github.io/
Playing with #singlemolecules, bending light, and algorithms to see really small things. Led by Matthew Lew, Associate Professor @WashUESE @WashUengineers @WashU #superresolution #microscopy #SMLM #computationalimaging
zookeeper to two tiny humans, professor, cell herder, bioelectrician, 'professional' storyteller, and waterbears just because. see us at:
cohenlab.princeton.edu
Light microscopy facility of #CEITEC_Brno #muni_cz. Part of #CzechBioimaging and #EuroBioimaging research infrastructures.
PhD student at Karolinska Institutet and Scilifelab | Cell physics
https://www.csi-nano.org/
Assistant professor, Shenzhen Bay Laboratory https://houlab.szbl.ac.cn/
Incoming Assistant Professor, Columbia University | @DamonRunyon.org Postdoc, UC Berkeley | PhD Princeton University | Mobile elements, Structural biology and Genome engineering | http://thawanilab.org
Assistant Professor at Aarhus University, Denmark | biophysical chemistry PhD | into chembio, synbio, protein design, photochem, microscopy | 2018-2022 at Stanford Bio-X | westberglab.com
Physicist, opinions my own, repost might not be endorsements.
www.afisakovic.com
Posts in English and Bosnian
Postdoc | Melbourne, Australia | cell & dev bio, signalling, mechanobio, transcription, microscopy | he/him
Assistant Professor at University of Warwick
Leading FMD Lab: https://fmd-lab.org/
Postdoc in Fraser Lab (USC)
Postdoc Fritzsche Lab (Oxford)
PhD in Eggeling Lab (Oxford)
Into all things Biophysics, Fluorescence, and Membranes
https://faldalf.github.io
scientist at UC Berkeley inventing advanced genomic technologies
lover of molecules, user of computers
https://scholar.google.com/citations?user=63ZRebIAAAAJ&hl=en
#OpenScience supporter, I work @Addgene.bsky.social curating DNA and web content. Previously worked at ASCB, publishing, Yale Biophysics PhD. He/him
Light microscopy at Bruker Fluorescence Microscopy division.
#lightsheet #multiphoton #superresolution #screening
Cell biologist in my previous life. Alumnus @mpicbg.bsky.social
@turkubioscience.bsky.socialβ¬
PhD student @MPI Science of Light
Currently post-doc at Harvard with David Weitz | PhD at MPIB with Petra Schwille
Interested in the cytoskeleton and membranes