One-dimensional spatial patterning along mitotic chromosomes: A mechanical basis for macroscopic morphogenesis.

Spatial patterns are ubiquitous in both physical and biological systems. We have recently discovered that mitotic chromosomes sequentially acquire two interesting morphological patterns along their structural axes [L. Chu et al.

The 3D Topography of Mitotic Chromosomes.

A long-standing conundrum is how mitotic chromosomes can compact, as required for clean separation to daughter cells, while maintaining close parallel alignment of sister chromatids. Pursuit of this question, by high resolution 3D fluorescence imaging of living and fixed mammalian cells, has led to three discoveries. First, we show that the structural axes of separated sister chromatids are linked by evenly spaced "mini-axis" bridges.

The Expression of Calprotectin and Factors in TLR4/NF-κB/MyD88 Pathway in Patients with Idiopathic Acute Anterior Uveitis.

: The purpose of the article is to investigate the contribution of calprotectin and factors in toll-like receptor 4/nuclear factor-κB/myeloid differentiation factor 88 (TLR4/NF-κB/MyD88) pathway in patients with idiopathic acute anterior uveitis (IAAU). : In total, 72 patients with IAAU and 56 healthy individuals were enrolled. Serum calprotectin, TLR-4, and MyD88 were determined.

Chromosomes Progress to Metaphase in Multiple Discrete Steps via Global Compaction/Expansion Cycles.

Mammalian mitotic chromosome morphogenesis was analyzed by 4D live-cell and snapshot deconvolution fluorescence imaging. Prophase chromosomes, whose organization was previously unknown, are revealed to comprise co-oriented sister linear loop arrays displayed along a single, peripheral, regularly kinked topoisomerase II/cohesin/condensin II axis. Thereafter, rather than smooth, progressive compaction as generally envisioned, progression to metaphase is a discontinuous process involving chromosome expansion as well as compaction.

Crossover patterning by the beam-film model: analysis and implications.

Crossing-over is a central feature of meiosis. Meiotic crossover (CO) sites are spatially patterned along chromosomes. CO-designation at one position disfavors subsequent CO-designation(s) nearby, as described by the classical phenomenon of CO interference.

α1A-adrenergic receptor induces activation of extracellular signal-regulated kinase 1/2 through endocytic pathway.

G protein-coupled receptors (GPCRs) activate mitogen-activated protein kinases through a number of distinct pathways in cells. Increasing evidence has suggested that endosomal signaling has an important role in receptor signal transduction. Here we investigated the involvement of endocytosis in α(1A)-adrenergic receptor (α(1A)-AR)-induced activation of extracellular signal-regulated kinase 1/2 (ERK1/2).

Two-state displacement by the kinesin-14 Ncd stalk.

The nonprocessive kinesin-14 Ncd motor binds to microtubules and hydrolyzes ATP, undergoing a single displacement before releasing the microtubule. A lever-like rotation of the coiled-coil stalk is thought to drive Ncd displacements or steps along microtubules. Crystal structures and cryoelectron microscopy reconstructions imply that stalk rotation is correlated with ADP release and microtubule binding by the motor.

Mature Drosophila meiosis I spindles comprise microtubules of mixed polarity.

New information has been obtained recently regarding microtubule organization in Xenopus extract spindles. These spindles assemble in vitro by chromatin-mediated microtubule nucleation and consist of randomly interspersed long and short microtubules with minus ends distributed throughout the spindle. Fluorescence speckle microscopy has led to the proposal that the Xenopus steady-state spindles contain two overlapping arrays of parallel or antiparallel microtubules with differing poleward-flux velocities.

Ncd motor binding and transport in the spindle.

The Ncd kinesin-14 motor is required for meiotic spindle assembly in Drosophila oocytes and produces force in mitotic spindles that opposes other motors. Despite extensive studies, the way the motor binds to the spindle to perform its functions is not well understood. By analyzing Ncd deleted for the conserved head or the positively charged tail, we found that the tail is essential for binding to spindles and centrosomes, but both the head and tail are needed for normal spindle assembly and function.

Real-time detection of alpha1A-AR movement stimulated by phenylephrine in single living cells.

Aim: To investigate the movement of alpha(1A)-adrenergic receptors(alpha(1A)-AR) stimulated by agonist, phenylephrine (PE), and the dynamics of receptor movement in real time in single living cells with millisecond resolution.

Methods: We labeled alpha(1A)-AR using the monoclonal, anti-FLAG (a kind of tag) antibody and Cy3-conjugated goat anti-mouse IgG and recorded the trajectory of their transport process in living HEK293A cells stimulated by agonist, PE, and then analyzed their dynamic properties.

Results: The specific detection of alpha(1A)-AR on the surface of living HEK293A-alpha(1A) cells was achieved.

Heterogeneous transportation of alpha1B-adrenoceptor in living cells.

The heterogeneous motion of alpha(1B)-adrenoceptor (alpha(1B)-AR) was visualized in living cells with BODIPY-labeled antagonist of AR by single molecule fluorescence microscopy at high spatial resolution. The moving trajectory was reconstructed by precise localization (better than 20 nm) with a least-square fit of a two-dimensional Gaussian point spread function to each single spot. Trajectory analysis revealed two apparent groups of movements: directed motion and hindered motion.

The transport of alpha(1A)-adrenergic receptor with 33-nm step size in live cells.

We used the technique of single particle tracking (SPT) with high tempo-spatial resolution to efficiently explore the route and mechanism for the transport of alpha(1A)-adrenergic receptor (alpha(1A)-AR) in real time in living cells. We found that the initial transport of alpha(1A)-AR in cells depended on actin filaments with the velocity of 0.2 microm/s and exhibited discrete 33-nm steps.