Correlation between plant cell wall stiffening and root extension arrest phenotype in combined abiotic stress of Fe and Al

The plasticity and growth of plant cell walls (CWs) is still not sufficiently understood on its molecular level. *

Atomic Force Microscopy (AFM) has been shown to be a powerful tool to measure the stiffness of plant tissues. *

In the article “Correlation between plant cell wall stiffening and root extension arrest phenotype in the combined abiotic stress of Fe and Al” Harinderbir Kaur, Jean-Marie Teulon, Christian Godon, Thierry Desnos, Shu-wen W. Chen and Jean-Luc Pellequer describe the use of atomic force microscopy (AFM) to observe elastic responses of the root transition zone of 4-day-old Arabidopsis thaliana wild-type and almt1-mutant seedlings grown under Fe or Al stresses. *

In order to evaluate the relationship between root extension and root cell wall elasticity, the authors used Atomic Force Microscopy to perform vertical indentations on surfaces of living plant roots. *

NanoWorld Pyrex-Nitride silicon-nitride PNP-TR AFM probes with triangular AFM cantilevers were used for the nanoindentation experiments with atomic force microscopy. (PNP-TR AFM cantilever beam 2 (CB2) with a typical force constant of 0.08 N/m and a typical resonant frequency of 17 kHz, typical AFM tip radius 10 nm, macroscopic half cone angles 35°). *

Force-distance (F-D) curves were measured using the Atomic Force Microscope and the PNP-TR AFM tips. *

Because of the heterogeneity of seedling CW surfaces, Harinderbir Kaur et al. used the recently developed trimechanics-3PCS framework for interpreting force-distance curves. The trimechanics-3PCS framework allows the extraction of both stiffness and elasticity along the depth of indentation and permits the investigation of the variation of stiffness with varied depth for biomaterials of heterogeneous elasticity responding to an external force. *

A glass slide with a glued seedling (see Figure 1 cited below) was positioned under the AFM cantilever with the help of an AFM optical camera. Due to the large motorized sample stage of the AFM, the glass slide was adjusted in such a way that the AFM cantilever could be positioned perpendicularly at the longitudinal middle of the glued root. The target working area, the transition zone, was 500 µm away from the root apex, almost twice the length of PNP-TR AFM cantilever. *

As shown in the article the presence of single metal species Fe2+ or Al3+ at 10 μM exerts no noticeable effect on the root growth compared with the control conditions. On the contrary, a mix of both the metal ions produced a strong root-extension arrest concomitant with significant increase of CW stiffness. *

Raising the concentration of either Fe2+or Al3+ to 20 μM, no root-extension arrest was observed; nevertheless, an increase in root stiffness occurred. In the presence of both the metal ions at 10 μM, root-extension arrest was not observed in the almt1 mutant, which substantially abolishes the ability to exude malate. The authors’ results indicate that the combination of Fe2+and Al3+ with exuded malate is crucial for both CW stiffening and root-extension arrest. *

It is shown that the elasticity of plant CW is sensitive and can be used to assess abiotic stresses on plant growth and stiffening. *

However, stiffness increase induced by single Fe2+ or Al3+ is not sufficient for arresting root growth in the described experimental conditions and unexpectedly, the stiffening and the phenotype of seedling roots such as REA are not directly correlated. *

Figure 1 from Harinderbir Kaur et al. 2024 “Correlation between plant cell wall stiffening and root extension arrest phenotype in the combined abiotic stress of Fe and Al”:Principle of nanomechanical measurement of seedling roots with atomic force microscopy. A seedling root (R) is deposited on a microscope slide using silicon glue (N, for Nusil). A fastening band of silicon is seen near the tip of the root (T). The thickness of the fastening band must be thin enough to avoid hindering the AFM support (S), but thick enough to withstand the bending of the root tip. The root is placed under the AFM cantilever (C) as observed by the AFM optical camera. The triangular shaped cantilever (200 µm long) was placed 500 µm away from the root tip in the transition zone where nanoindentation measurements proceeded (as shown). The seedling root and the AFM cantilever are placed within a liquid environment (growth solution, see Supplementary file of the cited article). AFM, atomic force microscopy. NanoWorld Pyrex-Nitride silicon-nitride PNP-TR AFM probes with triangular AFM cantilevers were used for the nanoindentation experiments with atomic force microscopy.
Figure 1 from Harinderbir Kaur et al. 2024 “Correlation between plant cell wall stiffening and root extension arrest phenotype in the combined abiotic stress of Fe and Al”:
Principle of nanomechanical measurement of seedling roots with atomic force microscopy.
A seedling root (R) is deposited on a microscope slide using silicon glue (N, for Nusil). A fastening band of silicon is seen near the tip of the root (T). The thickness of the fastening band must be thin enough to avoid hindering the AFM support (S), but thick enough to withstand the bending of the root tip. The root is placed under the AFM cantilever (C) as observed by the AFM optical camera. The triangular shaped cantilever (200 µm long) was placed 500 µm away from the root tip in the transition zone where nanoindentation measurements proceeded (as shown). The seedling root and the AFM cantilever are placed within a liquid environment (growth solution, see Supplementary file of the cited article). AFM, atomic force microscopy.

*Harinderbir Kaur, Jean‐Marie Teulon, Christian Godon, Thierry Desnos, Shu‐wen W. Chen and Jean‐Luc Pellequer
Correlation between plant cell wall stiffening and root extension arrest phenotype in the combined abiotic stress of Fe and Al
Plant, Cell & Environment 2024; 47:574–584
DOI: https://doi.org/10.1111/pce.14744

The article “Correlation between plant cell wall stiffening and root extension arrest phenotype in the combined abiotic stress of Fe and Al” by Harinderbir Kaur, Jean‐Marie Teulon, Christian Godon, Thierry Desnos, Shu‐wen W. Chen and Jean‐Luc Pellequer is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third-party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit https://creativecommons.org/licenses/by/4.0/.

Electrochemical detection of quinone reduced by Complex I Complex II and Complex III in full mitochondrial membranes

In the last decades enormous advances have been made in characterizing the atomic and molecular structure of respiratory chain supercomplexes. *

However, it still remains a challenge to stitch this refined spatial atomistic description with functional information provided by biochemical studies of isolated protein material. Development of functional assays that detect respiratory chain complexes in their native membrane environment contribute to address the open questions related to the role played by their association and interactions. *

In the article “Electrochemical detection of quinone reduced by Complex I Complex II and Complex III in full mitochondrial membranes” Daniel G. Cava, Julia Alvarez-Malmagro, Paolo Natale, Sandra López-Calcerrada, Iván López-Montero, Cristina Ugalde, Jose Maria Abad, Marcos Pita, Antonio L. De Lacey and Marisela Vélez present a characterization assay in which a functionalized gold electrode is modified with mitochondrial membrane fragments that allows monitoring electrochemically the activity of different respiratory chain complexes immersed in the mitochondrial membrane. *

Daniel G. Cava  et al. measure the intensity of the reducing current of the electron mediator CoQ1 at the electrode surface and its variation upon addition of the corresponding enzymatic substrates. The activities of Complex I, Complex II and Complex III were monitored by the way in which they reduce the current, reflecting the amount of quinone reduced by the complexes in the presence of their substrates. *

The authors detect that CoQ1H2 produced by Complex I remains partially trapped within the membrane and is more easily oxidized by Complex III or the electrode than the quinone reduced by Complex II. *

Atomic Force Microscopy (AFM) was used to image the topography of the membrane modified electrode. NanoWorld Pyrex-Nitride Silicon-Nitride AFM probes (PNP-DB, diving board shaped cantilevers, the short AFM cantilever with a typical force constant of 0.48 N/m and 67 kHz resonance frequency) were used. *

The surfaces analysed were the electrodes. The two surfaces imaged are the same previously polished electrodes used for electrochemical measurements. The microscope sample holder was adapted in-home to support the electrodes. Two surfaces were analysed: the polished gold functionalized with 4-aminothiophenol and the electrode after incubation with mitochondria subparticles prepared similarly to the electrodes used for the electrochemical measurements.*

Fig. 2 from Daniel G. Cava et al 2024 “Electrochemical detection of quinone reduced by Complex I Complex II and Complex III in full mitochondrial membranes” QCM and AFM characterization of modified gold. Panel A shows the frequency (left, black) and dissipation (right red) changes detected on a gold covered quartz crystal previously modified with a 4-ATP after injection in the chamber of the mitochondrial fragments at the time point indicated by the thick arrow. Panel B show AFM images of the surface topography of a modified gold electrode before (left) and after (right)incubation with the mitochondrial membrane. The inset below shows the height profile of the lines indicated in the images. NanoWorld Pyrex-Nitride Silicon-Nitride AFM probes (PNP-DB, the short AFM cantilever with a typical force constant of 0.48 N/m and 67 kHz resonance frequency) were used.
Fig. 2 from Daniel G. Cava et al 2024 “Electrochemical detection of quinone reduced by Complex I Complex II and Complex III in full mitochondrial membranes”
QCM and AFM characterization of modified gold. Panel A shows the frequency (left, black) and dissipation (right red) changes detected on a gold covered quartz crystal previously modified with a 4-ATP after injection in the chamber of the mitochondrial fragments at the time point indicated by the thick arrow. Panel B show AFM images of the surface topography of a modified gold electrode before (left) and after (right)incubation with the mitochondrial membrane. The inset below shows the height profile of the lines indicated in the images.

*Daniel G. Cava, Julia Alvarez-Malmagro, Paolo Natale, Sandra López-Calcerrada, Iván López-Montero, Cristina Ugalde, Jose Maria Abad, Marcos Pita, Antonio L. De Lacey and Marisela Vélez
Electrochemical detection of quinone reduced by Complex I Complex II and Complex III in full mitochondrial membranes
Electrochimica Acta, Volume 484, 20 April 2024, 144042
DOI: https://doi.org/10.1016/j.electacta.2024.144042

 

The article “Electrochemical detection of quinone reduced by Complex I Complex II and Complex III in full mitochondrial membranes” by Daniel G. Cava, Julia Alvarez-Malmagro, Paolo Natale, Sandra López-Calcerrada, Iván López-Montero, Cristina Ugalde, Jose Maria Abad, Marcos Pita, Antonio L. De Lacey and Marisela Vélez is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third-party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit https://creativecommons.org/licenses/by/4.0/.

Manipulating hyperbolic transient plasmons in a layered semiconductor

Anisotropic materials with oppositely signed dielectric tensors support hyperbolic polaritons, displaying enhanced electromagnetic localization and directional energy flow. *

However, the most reported hyperbolic phonon polaritons are difficult to apply for active electro-optical modulations and optoelectronic devices. *

In the nature communications letter “Manipulating hyperbolic transient plasmons in a layered semiconductor”, Rao Fu, Yusong Qu, Mengfei Xue, Xinghui Liu, Shengyao Chen, Yongqian Zhao, Runkun Chen, Boxuan Li, Hongming Weng, Qian Liu, Qing Dai and Jianing Chen report a dynamic topological plasmonic dispersion transition in black phosphorus (BP) via photo-induced carrier injection, i.e., transforming the iso-frequency contour from a pristine ellipsoid to a non-equilibrium hyperboloid. *

They introduce a promising approach to optically manipulate robust transient hyperbolic plasmons in the layered semiconductor black phosphorus using a dedicated ultrafast nanoscopy scheme. Optical pumping allows the BP’s IFCs to topologically transit from the pristine ellipsoid to the non-equilibrium hyperboloid, exhibiting exotic non-equilibrium hyperbolic plasmon properties, such as the optically tunable plasmonic dispersion and the coexistence of different transient plasmonic modes. *

Their work also demonstrates the peculiar transient plasmonic properties of the studied layered semiconductor, such as the ultrafast transition, low propagation losses, efficient optical emission from the black phosphorus’s edges, and the characterization of different transient plasmon modes. *

The results that Rao Fu et al. present may be relevant for the development of future optoelectronic applications. *

NanoWorld® ARROW-NCPt AFM probes with a Pt/Ir coating were used for the characterization with ultrafast nanoscopy. The pump and probe pulses were spatially overlapped on the Platinum/Iridium coated Arrow probe through a parabolic mirror of a commercial scattering-type scanning near-field optical microscope. *

Fig. 4 from Rao Fu et al. “Manipulating hyperbolic transient plasmons in a layered semiconductor”:Dynamic analysis of the transient plasmons. a Normalized near-field amplitude s3/s3,Si of a 280-nm-thick BP slab for twelve delay times τ. Scale bar, 1 µm. b Near-field amplitude curves for the corresponding twelve different delay times τ in a. c Dynamics of the relative near-field intensity of the first (∆S1) and the second bright strip (∆S2) in b. Opened circles are the experimental data, and solid lines are bi-exponential fitting for ∆S1 and exponential fitting for ∆S2, respectively. d Dynamics of the near-field amplitude s3 from the black circle in a. The inset displays the s3 at τ = −2 to 6 ps, and the dashed line marks the s3 level of the pristine state. NanoWorld® ARROW-NCPt AFM probes with a Pt/Ir coating were used for the characterization with ultrafast nanoscopy. The pump and probe pulses were spatially overlapped on the Pt/Ir coated Arrow probe through a parabolic mirror of a commercial scattering-type scanning near-field optical microscope.
Fig. 4 from Rao Fu et al. “Manipulating hyperbolic transient plasmons in a layered semiconductor”:
Dynamic analysis of the transient plasmons.
a Normalized near-field amplitude s3/s3,Si of a 280-nm-thick BP slab for twelve delay times τ. Scale bar, 1 µm. b Near-field amplitude curves for the corresponding twelve different delay times τ in a. c Dynamics of the relative near-field intensity of the first (∆S1) and the second bright strip (∆S2) in b. Opened circles are the experimental data, and solid lines are bi-exponential fitting for ∆S1 and exponential fitting for ∆S2, respectively. d Dynamics of the near-field amplitude s3 from the black circle in a. The inset displays the s3 at τ = −2 to 6 ps, and the dashed line marks the s3 level of the pristine state.

*Rao Fu, Yusong Qu, Mengfei Xue, Xinghui Liu, Shengyao Chen, Yongqian Zhao, Runkun Chen, Boxuan Li, Hongming Weng, Qian Liu, Qing Dai and Jianing Chen
Manipulating hyperbolic transient plasmons in a layered semiconductor

Nature Communications volume 15, Article number: 709 (2024)
DOI: https://doi.org/10.1038/s41467-024-44971-3

Please follow this external link to read the full article: https://rdcu.be/dBD85

The article “Manipulating hyperbolic transient plasmons in a layered semiconductor” by Rao Fu, Yusong Qu, Mengfei Xue, Xinghui Liu, Shengyao Chen, Yongqian Zhao, Runkun Chen, Boxuan Li, Hongming Weng, Qian Liu, Qing Dai and Jianing Chen is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third-party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit https://creativecommons.org/licenses/by/4.0/.