Günter K. Auernhammer

Dr. Günter K. Auernhammer

orcid

Research Focus & Metrics

Academic Career Length

27Years (2000-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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10 October 2016 in Nature Chemistry
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HZHongwei Zhou
Hongwei Zhou
CXChangguo Xue
Changguo Xue
PWPhilipp Weis
Philipp Weis
YSYasuhito Suzuki
Yasuhito Suzuki
SHShilin Huang
Shilin Huang
Si WuSi Wu
Si Wu

29 April 2021 in Nature Materials
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PPPatrick Thomas Probst
Patrick Thomas Probst
MMMartin Mayer
Martin Mayer
VGVaibhav Gupta
Vaibhav Gupta
ASAnja Maria Steiner
Anja Maria Steiner
ZZZiwei Zhou
Ziwei Zhou
AFAndreas Fery
Andreas Fery

27 January 2009 in Langmuir
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LZLijuan Zhang
Lijuan Zhang
MDMaria D’acunzi
Maria D’acunzi
MKMichael Kappl
Michael Kappl
GAGünter K. Auernhammer
Günter K. Auernhammer
DVDoris Vollmer
Doris Vollmer
ABAlfons van Blaaderen
Alfons van Blaaderen

30 July 2009 in Soft Matter
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RPRamon Pericet-Camara
Ramon Pericet-Camara
GAGünter K. Auernhammer
Günter K. Auernhammer
KKKaloian Koynov
Kaloian Koynov
SLSimone Lorenzoni
Simone Lorenzoni
Roberto RaiteriRoberto Raiteri
Roberto Raiteri
EBElmar Bonaccurso
Elmar Bonaccurso
A sessile droplet can deform the surface of a soft solid not only with its weight. The surface tension pulls up a ridge at the perimeter of the drop, and the capillary pressure embosses a quasi-spherical dimple underneath the drop. This holds for the case of a bulk solid. However, if the solid forms a film with thickness comparable to the deformation scale the shape and the depth of the dimple are strongly distorted. We investigated dimples on elastomer films with a Young's modulus of 25 kPa and thickness in the range 4–104 µm embossed by sessile ionic liquid droplets. The films are supported by an undeformable glass slide. Below a certain critical film thickness, the dimple is shallower and the ridge at the drop rim is less elevated than for the bulk elastomer. The deviations are more pronounced for thinner films. Further, troughs form at the two sides of the ridge. Their distance from the rim is equivalent to the layer thickness. The measurements are qualitatively reproduced by an analytical model and quantitatively by numerical simulations. A consistent physical picture of the deformation on the bulk elastomer and of the distortions on the thin films is given.

20 November 2009 in Langmuir
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MSMordechai Sokuler
Mordechai Sokuler
GAGünter K. Auernhammer
Günter K. Auernhammer
MRMarcel Roth
Marcel Roth
CLChuanjun Liu
Chuanjun Liu
EBElmar Bonaccurso
Elmar Bonaccurso
HBHans-Jürgen Butt
Hans-Jürgen Butt

7 August 2023 in Nature Nanotechnology
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YPYu-Hsuan Peng
Yu-Hsuan Peng
SHSyuan-Ku Hsiao
Syuan-Ku Hsiao
KGKrishna Gupta
Krishna Gupta
ARAndré Ruland
André Ruland
GAGünter K. Auernhammer
Günter K. Auernhammer
EKElisha Krieg
Elisha Krieg
Three-dimensional cell and organoid cultures rely on the mechanical support of viscoelastic matrices. However, commonly used matrix materials lack control over key cell-instructive properties. Here we report on fully synthetic hydrogels based on DNA libraries that self-assemble with ultrahigh-molecular-weight polymers, forming a dynamic DNA-crosslinked matrix (DyNAtrix). DyNAtrix enables computationally predictable and systematic control over its viscoelasticity, thermodynamic and kinetic parameters by changing DNA sequence information. Adjustable heat activation allows homogeneous embedding of mammalian cells. Intriguingly, stress-relaxation times can be tuned over four orders of magnitude, recapitulating mechanical characteristics of living tissues. DyNAtrix is self-healing, printable, exhibits high stability, cyto- and haemocompatibility, and controllable degradation. DyNAtrix-based cultures of human mesenchymal stromal cells, pluripotent stem cells, canine kidney cysts and human trophoblast organoids show high viability, proliferation and morphogenesis. DyNAtrix thus represents a programmable and versatile precision matrix for advanced approaches to biomechanics, biophysics and tissue engineering.