Sharing a recent, deep insight:
The concept of a membrane-less organelle is an interesting one, like calling something a house without walls
@lennarthilbert.bsky.social
Studying the cell nucleus in search of inspiration for future DNA computers. Systems Biology professor at Karlsruhe Institute of Technology, post opinions mine alone. hilbertlab.org
Sharing a recent, deep insight:
The concept of a membrane-less organelle is an interesting one, like calling something a house without walls
Happy 200th bday KIT π₯³
07.10.2025 07:44 β π 3 π 0 π¬ 0 π 0Sadly, yes, and applies also past junior level! Sorry to everyone affected by my unreal email and task overload in the form of non-responsiveness π£
04.10.2025 07:42 β π 8 π 0 π¬ 0 π 0This might explain a lot of emails I am getting. Using Mac Mailβ¦
28.09.2025 12:16 β π 2 π 0 π¬ 0 π 0Thought the same recently, glad we have an open and international discussion platform again! Still, engagement seems lower than on Twitter during the good days, despite the higher follower count here
28.09.2025 09:44 β π 3 π 0 π¬ 0 π 0I was about to ask :-)
26.09.2025 20:17 β π 1 π 0 π¬ 0 π 0Thanks, no need to defend, your points are clear & justified! We have data where gene and enhancer donβt come closer than ~200-300 nm, but do come into that distance systematically. Iβm trying to understand whether that distance is sufficient to mainly rule out itβs driven by your/a cohesion effect.
26.09.2025 18:14 β π 0 π 0 π¬ 0 π 0Warming up for October start of KIT teaching by guest lecturing for @unistra.fr Cell Physics Master βActive Dropletsβ. First of three lectures today. 3:00 h sharp, start to finish πͺ
Some travel impressions, including fancy and very white βLe Studiumβ on Strasbourg Central Campus π€
And, Gyoza π₯
Right, that makes sense, also and especially considering the question of your study. I was wondering how close a gene would have to cone to an enhancer to be βcaughtβ by a cohesion. It would help distinguish what type of event we see in our own data. Any idea?
26.09.2025 12:48 β π 0 π 0 π¬ 1 π 0One question, after reading your short overview:
How close, in terms of nm distance, would one locus have to come to a second locus for them to be caught into this type of cohesin-based long-lived engagement? Something below 100 nm? I hope my question makes senseβ¦
The goal of a PhD is not to learn some facts or read a few papers or learn a bunch of techniques. The goal of a PhD is to learn independence, problem solving, how to finish things you start, resilience, & gain the ability to adapt & think creatively. Learning these things is hard.
13.08.2025 17:28 β π 336 π 87 π¬ 4 π 5Very much on the case, also motivated as the project came back today during the defense in Erlangen π
23.09.2025 21:46 β π 1 π 0 π¬ 1 π 0βΊοΈ
23.09.2025 21:44 β π 0 π 0 π¬ 0 π 0Itβs moving for you! βΊοΈ
23.09.2025 21:27 β π 1 π 0 π¬ 1 π 0It was a pleasure and an honor to walk this part of the path together, and amazing to look back at the achievements today. Also, two very smart oral examiners, Alexandra Chambony & Helmut BrandstΓ€tter, quite insightful and sharp questions! Theyβre here, right after the grade was announced.
23.09.2025 21:18 β π 0 π 0 π¬ 0 π 0What a great doctoral defense by Tim Klingberg @fau.de
Based in the group of our collaborator @vasilyzaburdaev.bsky.social Tim decisively contributed to at least 3 of our own labβs foundational projects, which he showed today at βMax Planck Zentrum Physik und Medizinβ
Some impressions
Welcome on board, happy to see you joined!
19.09.2025 16:41 β π 0 π 0 π¬ 0 π 0Congratulations to the Fritz Lipmann Lecturer Michael Rosen (Dallas) by the GBM president Harald Kolmar.
18.09.2025 11:35 β π 11 π 4 π¬ 0 π 0GBM Compact Focus on Condensate Biology is opened by Edward Lemke. Looking forward to a great meeting!
18.09.2025 11:09 β π 15 π 6 π¬ 0 π 0If you are at GBM compact "Focus on Condensate Biology", we will be happy to talk to you at our lab's posters:
Mona WellhΓ€user, MC15 @mofrawe.bsky.social
Yuzhi Bao, CA03 @yuzhibao.bsky.social
Lennart Hilbert, MC06
Conference abstracts:
gbm-compact.org/abstracts.html
*sketch added as click bait
The label maker is the single most gratifying machine one can buy for a lab!
11.09.2025 05:41 β π 0 π 0 π¬ 1 π 0Um das Verhalten der DNS nachvollziehbar und vorhersagbar zu machen, kombinieren die Forschenden Laborexperimente mit Computersimulationen.
Molekulare #Bionik: Der Zellkern als Vorbild fΓΌr DNS-basierte #Computerchips. Forschende des #KITKarlsruhe (u. a. @lennarthilbert.bsky.social) nutzen zellulΓ€re Informationsverarbeitung als Inspiration fΓΌr die #Biotechnologie. www.kit.edu/kit/pi_2025_...
09.09.2025 11:02 β π 7 π 2 π¬ 0 π 0If you want actual evidence for cis and trans interactions, this might be one classic paper that has it:
www.nature.com/articles/ng....
We also have a full nucleus model (unpublished). Surprise: it seems to do both π€·πΌββοΈ
09.09.2025 07:03 β π 1 π 0 π¬ 1 π 0Our postdoc at the time aptly called this the Enhancer Shoe Box model. So, all that I can say for this model: the two chromosome segments are each attached to the opposing short sides of the shoe box ;-)
Simulation code is here, if anyone needs it:
github.com/lhilbert/Enh...
Simulation of the formation of a chromatin-attached condensate, which is visited by a gene undergoing transcriptional activation.
Read more about it here:
nyaspubs.onlinelibrary.wiley.com/doi/10.1111/...
The paper provides a broader discussion of the challenges of DNA computing and designing a chip architecture, and how methods from accelerated/virtual materials design can drive progress.
Thanks to all for contributions and input along the way! Co-author @mofrawe.bsky.social is also on BlueSky
Simulation of surface condensation in the presence of a model polymer chain. (A) Basic interaction rules in a system of diffusing particles result in liquidβliquid phase separation and surface condensation. 2D-projections of simulations show that for a low number of condensate-forming particles, droplets only form on interactive polymer sections. Only at higher numbers of condensate-forming particles can droplets form independently. (B) The association of particles into droplets is detected at lower particle concentrations in the presence of a condensation surface. (C) When increasing the bulk concentration of condensate-forming particles above the pre-wetting concentration, , a dense droplet phase appears in the presence of a condensation surface (top). Without a surface, a dense droplet phase forms only above the higher saturation concentration . Droplet phase concentration obtained using the convex hull around DBSCAN detected clusters. (D) Simulating the limited resolution of a microscope and implementing a quantification of condensate intensities similar to the analysis of microscopy images leads to a progressive increase of intensity above (in the presence of surface, top) or above (without surface, bottom). All values are mean SEM, independent simulations per condition.
A coarse-grained simulation reproduces, again, the behaviors seen in our synthetic DNA experiments, and explains some effects of finite microscope resolution, as well as complex interactions of condensates and surface DNA strands.
08.09.2025 13:50 β π 0 π 0 π¬ 1 π 0Use of synthetic DNA nanostructures to reconstruct the surface condensation process underlying transcription factory formation. (A) The condensed material of a transcription factory is mimicked using X-shaped nanomotifs made of short DNA oligomers. The nanomotifs have sequence-encoded binding sites for other nanomotifs (magenta) and for target areas located on DNA strands (green). These target areas enable the local formation of surface condensates, similar to the condensate formation at genomic control elements. (B) Two-color microscopy images showing nanomotifs (magenta), to which surfaces (green) were added or not added. Images are maximum intensity z-projections, intensity look-up tables were adjusted for each image individually to facilitate visual interpretation. For separate channel images, see Figure S1. (C) Number of condensates per volumetric stack, the nanomotif channel intensity within these condensates, and the nanomotif channel background intensity for increasing nanomotif concentration, in the presence or absence of added condensation surfaces. All values are mean with 95% confidence intervals, 500 bootstrap resamples, volumetric stacks per condition for condensate number and background intensity; for condensate intensity, is the total number of condensates pooled from 20 stacks per condition. For the middle and bottom intensity plots, the circle area is proportional to the number of detected condensates.
We took a short-cut, designed DNA-nanomotifs behaving similarly to the in vivo liquid phase, condensing in targeted fashion on long, repetitive DNA strands produced bz rolling circle amplification (RCA). Crucial behaviors of the surface condensate regime are reproduced! @xeniatschurikow.bsky.social
08.09.2025 13:50 β π 0 π 0 π¬ 1 π 0Delineation of the surface condensation regime in contrast to canonical liquidβliquid phase separation (LLPS). Reliable operation of a computing system that uses properties and functions afforded by surface condensation can be expected within the inner regions of the surface condensation regime, above the pre-wetting concentration () and below the saturation concentration (). Blue and red lines in the bottom diagram represent stable concentrations that can be obtained by demixing into condensates via surface condensation or LLPS, respectively. Dashed lines are theoretical expectations and solid lines are expected observations considering a finite microscope resolution. Sketch based on simulations in our previous work.
The surface condensation regime holds very specific implications for the behavior of liquid-phase condensates: they are growth-limited by amount of available surface, and localize to these surfaces. The regime occurs at sub-saturated (C<C_sat) concentrations, also relevant for the in vivo regime.
08.09.2025 13:50 β π 0 π 0 π¬ 1 π 0