scholarly journals The many states of STIM1

eLife ◽  
2021 ◽  
Vol 10 ◽  
Author(s):  
Marc Fahrner ◽  
Christoph Romanin

Harnessing single-molecule FRET illuminates the structural changes necessary for a protein to fine-tune the influx of calcium when reserves inside a cell run low.

2015 ◽  
Vol 112 (44) ◽  
pp. 13467-13472 ◽  
Author(s):  
Danya J. Martell ◽  
Chandra P. Joshi ◽  
Ahmed Gaballa ◽  
Ace George Santiago ◽  
Tai-Yen Chen ◽  
...  

Metalloregulators respond to metal ions to regulate transcription of metal homeostasis genes. MerR-family metalloregulators act on σ70-dependent suboptimal promoters and operate via a unique DNA distortion mechanism in which both the apo and holo forms of the regulators bind tightly to their operator sequence, distorting DNA structure and leading to transcription repression or activation, respectively. It remains unclear how these metalloregulator−DNA interactions are coupled dynamically to RNA polymerase (RNAP) interactions with DNA for transcription regulation. Using single-molecule FRET, we study how the copper efflux regulator (CueR)—a Cu+-responsive MerR-family metalloregulator—modulates RNAP interactions with CueR’s cognate suboptimal promoter PcopA, and how RNAP affects CueR−PcopAinteractions. We find that RNAP can form two noninterconverting complexes at PcopAin the absence of nucleotides: a dead-end complex and an open complex, constituting a branched interaction pathway that is distinct from the linear pathway prevalent for transcription initiation at optimal promoters. Capitalizing on this branched pathway, CueR operates via a “biased sampling” instead of “dynamic equilibrium shifting” mechanism in regulating transcription initiation; it modulates RNAP’s binding–unbinding kinetics, without allowing interconversions between the dead-end and open complexes. Instead, the apo-repressor form reinforces the dominance of the dead-end complex to repress transcription, and the holo-activator form shifts the interactions toward the open complex to activate transcription. RNAP, in turn, locks CueR binding at PcopAinto its specific binding mode, likely helping amplify the differences between apo- and holo-CueR in imposing DNA structural changes. Therefore, RNAP and CueR work synergistically in regulating transcription.


2014 ◽  
Vol 106 (2) ◽  
pp. 49a
Author(s):  
Mark S. Piraino ◽  
Michael T. Kelliher ◽  
Ramiah D. Jacks ◽  
Madeline E. Gemoules ◽  
Jihad Aburas ◽  
...  

2016 ◽  
Vol 113 (34) ◽  
pp. E4956-E4965 ◽  
Author(s):  
Namita Bisaria ◽  
Max Greenfeld ◽  
Charles Limouse ◽  
Dmitri S. Pavlichin ◽  
Hideo Mabuchi ◽  
...  

The past decade has seen a wealth of 3D structural information about complex structured RNAs and identification of functional intermediates. Nevertheless, developing a complete and predictive understanding of the folding and function of these RNAs in biology will require connection of individual rate and equilibrium constants to structural changes that occur in individual folding steps and further relating these steps to the properties and behavior of isolated, simplified systems. To accomplish these goals we used the considerable structural knowledge of the folded, unfolded, and intermediate states of P4-P6 RNA. We enumerated structural states and possible folding transitions and determined rate and equilibrium constants for the transitions between these states using single-molecule FRET with a series of mutant P4-P6 variants. Comparisons with simplified constructs containing an isolated tertiary contact suggest that a given tertiary interaction has a stereotyped rate for breaking that may help identify structural transitions within complex RNAs and simplify the prediction of folding kinetics and thermodynamics for structured RNAs from their parts. The preferred folding pathway involves initial formation of the proximal tertiary contact. However, this preference was only ∼10 fold and could be reversed by a single point mutation, indicating that a model akin to a protein-folding contact order model will not suffice to describe RNA folding. Instead, our results suggest a strong analogy with a modified RNA diffusion-collision model in which tertiary elements within preformed secondary structures collide, with the success of these collisions dependent on whether the tertiary elements are in their rare binding-competent conformations.


Nano Letters ◽  
2021 ◽  
Vol 21 (4) ◽  
pp. 1694-1701 ◽  
Author(s):  
Sung Hyun Kim ◽  
Hyunwoo Kim ◽  
Hawoong Jeong ◽  
Tae-Young Yoon

ACS Sensors ◽  
2021 ◽  
Author(s):  
Anoja Megalathan ◽  
Kalani M. Wijesinghe ◽  
Soma Dhakal

Entropy ◽  
2021 ◽  
Vol 23 (3) ◽  
pp. 290
Author(s):  
Maxim Pyzh ◽  
Kevin Keiler ◽  
Simeon I. Mistakidis ◽  
Peter Schmelcher

We address the interplay of few lattice trapped bosons interacting with an impurity atom in a box potential. For the ground state, a classification is performed based on the fidelity allowing to quantify the susceptibility of the composite system to structural changes due to the intercomponent coupling. We analyze the overall response at the many-body level and contrast it to the single-particle level. By inspecting different entropy measures we capture the degree of entanglement and intraspecies correlations for a wide range of intra- and intercomponent interactions and lattice depths. We also spatially resolve the imprint of the entanglement on the one- and two-body density distributions showcasing that it accelerates the phase separation process or acts against spatial localization for repulsive and attractive intercomponent interactions, respectively. The many-body effects on the tunneling dynamics of the individual components, resulting from their counterflow, are also discussed. The tunneling period of the impurity is very sensitive to the value of the impurity-medium coupling due to its effective dressing by the few-body medium. Our work provides implications for engineering localized structures in correlated impurity settings using species selective optical potentials.


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