Comparative Study of the Condensation of Chicken Erythrocyte and Calf Thymus Chromatins by Di- and Multivalent Cations

Abstract

The condensation of chicken erythrocyte (CE) and calf thymus (CT) chromatins upon addition of di- and multivalent cations has been studied using turbidityJulprecipitation and electric dichroism measurements. For all the cations investigated (Mg²⁺, Tb³⁺, Co(NH₃)₆ ³⁺, spermidine Spd²⁺ and spermine Sp⁴⁺) condensation of CE chromatin occurred before the onset of aggregation, while aggregation of CT chromatin started before condensation with all cations except Mg²⁺ and Tb³⁺. Precipitation of CE chromatin required lower di- and multivalent cations concentrations than CT chromatin. The electric dichroism data for both chromatins, at low ionic strength in the absence of di- or multivalent cations, indicated that the nucleoprotein molecules were not totally decondensed but that a “precondensed” state was already present. A positive electric dichroism was observed for the most condensed chromatin fibers, in agreement with the “cross-linker” models. Tb³⁺ led to less compact condensed particles as judged from the electric dichroism observations, but electron microscopy revealed that “30 nm fibers” were formed. Very little aggregation was produced by Tb³⁺. On the contrary, spermine produced very large networks of condensed molecules, but large spheroidal particles were also observed. The condensation of CE chromatin happened without changes of solution conductivity upon cation salt addition, regardless of the condensing cation, indicating a cooperative uptake of the ions during this process.     

Status of the intracellular gate in the activated-not-open state of shaker K+ channels

Voltage-dependent K⁺ channels like Shaker use an intracellular gate to control ion flow through the pore. When the membrane voltage becomes more positive, these channels traverse a series of closed conformations before the final opening transition. Does the intracellular gate undergo conformational changes before channel opening? To answer this question we introduced cysteines into the intracellular end of the pore and studied their chemical modification in conditions favoring each of three distinct states, the open state, the resting closed state, and the activated-not-open state (the closed state adjacent to the open state). We used two independent ways to isolate the channels in the activated-not-open state. First, we used mutations in S4 (ILT; Smith-Maxwell, C.J., J.L. Ledwell, and R.W. Aldrich. 1998. J. Gen. Physiol. 111:421–439; Ledwell, J.L., and R.W. Aldrich. 1999. J. Gen. Physiol. 113:389–414) that separate the final opening step from earlier charge-movement steps. Second, we used the open channel blocker 4-aminopyridine (4-AP), which has been proposed to promote closure of the intracellular gate and thus specifically to stabilize the activated-not-open state of the channels. Supporting this proposed mechanism, we found that 4-AP enters channels only after opening, remaining trapped in closed channels, and that in the open state it competes with tetraethylammonium for binding. Using these tools, we found that in the activated-not-open state, a cysteine located at a position considered to form part of the gate (Shaker 478) showed higher reactivity than in either the open or the resting closed states. Additionally, we have found that in this activated state the intracellular gate continued to prevent access to the pore by molecules as small as Cd²⁺ ions. Our results suggest that the intracellular opening to the pore undergoes some rearrangements in the transition from the resting closed state to the activated-not-open state, but throughout this process the intracellular gate remains an effective barrier to the movement of potassium ions through the pore.     

Ionic channels formed byStaphylococcus aureus alpha-toxin: Voltage-dependent inhibition by divalent and trivalent cations

Summary The interaction ofStaphylococcus aureus -toxin with planar lipid membranes results in the formation of ionic channels whose conductance can be directly measured in voltage-clamp experiments. Single-channel conductance depends linearly on the solution conductivity suggesting that the pores are filled with aqueous solution; a rough diameter of 11.4±0.4 Å can be estimated for the pore. The conductance depends asymmetrically on voltage and it is slightly anion selective at pH 7.0, which implies that the channels are asymmetrically oriented into the bilayer and that ion motion is restricted at least in a region of the pore. The pores are usually open in a KCl solution but undergo a dose- and voltage-dependent inactivation in the presence of diand trivalent cations, which is mediated by open-closed fluctuations at the single-channel level. Hill plots indicate that each channel can bind two to three inactivating cations. The inhibiting efficiency follows the sequence Zn²⁺>Tb³⁺>Ca²⁺>Mg²⁺>Ba²⁺. suggesting that carboxyl groups of the protein may be involved in the binding step. A voltage-gated inactivation mechanism is proposed which involves the binding of two polyvalent cations to the channel, one in the open and one in the closed configuration, and which can explain voltage, dose and time dependence of the inactivation.     

Basis for allosteric open-state stabilization of voltage-gated potassium channels by intracellular cations

The open state of voltage-gated potassium (Kv) channels is associated with an increased stability relative to the pre-open closed states and is reflected by a slowing of OFF gating currents after channel opening. The basis for this stabilization is usually assigned to intrinsic structural features of the open pore. We have studied the gating currents of Kv1.2 channels and found that the stabilization of the open state is instead conferred largely by the presence of cations occupying the inner cavity of the channel. Large impermeant intracellular cations such as N-methyl-d-glucamine (NMG⁺) and tetraethylammonium cause severe slowing of channel closure and gating currents, whereas the smaller cation, Cs⁺, displays a more moderate effect on voltage sensor return. A nonconducting mutant also displays significant open state stabilization in the presence of intracellular K⁺, suggesting that K⁺ ions in the intracellular cavity also slow pore closure. A mutation in the S6 segment used previously to enlarge the inner cavity (Kv1.2-I402C) relieves the slowing of OFF gating currents in the presence of the large NMG⁺ ion, suggesting that the interaction site for stabilizing ions resides within the inner cavity and creates an energetic barrier to pore closure. The physiological significance of ionic occupation of the inner cavity is underscored by the threefold slowing of ionic current deactivation in the wild-type channel compared with Kv1.2-I402C. The data suggest that internal ions, including physiological concentrations of K⁺, allosterically regulate the deactivation kinetics of the Kv1.2 channel by impairing pore closure and limiting the return of voltage sensors. This may represent a primary mechanism by which Kv channel deactivation kinetics is linked to ion permeation and reveals a novel role for channel inner cavity residues to indirectly regulate voltage sensor dynamics.     

Mechanism of luminal Ca<Superscript>2+</Superscript> and Mg<Superscript>2+</Superscript> action on the vacuolar slowly activating channels

The non-selective slow vacuolar (SV) channel can dominate tonoplast conductance, making it necessary to tightly control its activity. Applying the patch-clamp technique to vacuoles from sugar beet (Beta vulgaris L.) taproots we studied the effect of divalent cations on the vacuolar side of the SV channel. Our results show that the SV channel has two independent binding sites for vacuolar divalent cations, (i) a less selective one, inside the channel pore, binding to which impedes channel conductance, and (ii) a Ca²⁺-selective one outside the membrane-spanning part of the channel protein, binding to which stabilizes the channels closed conformations. Vacuolar Ca²⁺ and Mg²⁺ almost indiscriminately blocked ion fluxes through the open channel pore, decreasing measured single-channel current amplitudes. This low-affinity block displays marked voltage dependence, characteristic of a permeable blocker. Vacuolar Ca²⁺—with a much higher affinity than Mg²⁺—slows down SV channel activation and shifts the voltage dependence to more (cytosol) positive potentials. A quantitative analysis results in a model that exactly describes the Ca²⁺-specific effects on the SV channel activation kinetics and voltage gating. According to this model, multiple (approximately three) divalent cations bind with a high affinity at the luminal interface of the membrane to the channel protein, favoring the occupancy of one of the SV channels closed states (C2). Transition to another closed state (C1) diminishes the effective number of bound cations, probably due to mutual repulsion, and channel opening is accompanied by a decrease of binding affinity. Hence, the open state (O) is destabilized with respect to the two closed states, C1 and C2, in the presence of Ca²⁺ at the vacuolar side. The specificity for Ca²⁺ compared to Mg²⁺ is explained in terms of different binding affinities for these cations. In this study we demonstrate that vacuolar Ca²⁺ is a crucial regulator to restrict SV channel activity to a physiologically meaningful range, which is less than 0.1% of maximum SV channel activity.Abbreviation SV Slow vacuolar     

Hydrophobic interaction between contiguous residues in the S6 transmembrane segment acts as a stimuli integration node in the BK channel

Large-conductance Ca²⁺- and voltage-activated K⁺ channel (BK) open probability is enhanced by depolarization, increasing Ca²⁺ concentration, or both. These stimuli activate modular voltage and Ca²⁺ sensors that are allosterically coupled to channel gating. Here, we report a point mutation of a phenylalanine (F380A) in the S6 transmembrane helix that, in the absence of internal Ca²⁺, profoundly hinders channel opening while showing only minor effects on the voltage sensor active–resting equilibrium. Interpretation of these results using an allosteric model suggests that the F380A mutation greatly increases the free energy difference between open and closed states and uncouples Ca²⁺ binding from voltage sensor activation and voltage sensor activation from channel opening. However, the presence of a bulky and more hydrophobic amino acid in the F380 position (F380W) increases the intrinsic open–closed equilibrium, weakening the coupling between both sensors with the pore domain. Based on these functional experiments and molecular dynamics simulations, we propose that F380 interacts with another S6 hydrophobic residue (L377) in contiguous subunits. This pair forms a hydrophobic ring important in determining the open–closed equilibrium and, like an integration node, participates in the communication between sensors and between the sensors and pore. Moreover, because of its effects on open probabilities, the F380A mutant can be used for detailed voltage sensor experiments in the presence of permeant cations.     

Modulation of P2X4 pore closure by magnesium,potassium, and ATP

The P2X4 receptor plays a prominent role in cellular responses to extracellular ATP. Through classical all-atom molecular dynamics (MD) simulations totaling 24 μs we have investigated how metal-complexed ATP stabilizes the channel's open state and prevents its closing. We have identified two metal-binding sites, Mg²⁺ and potassium K⁺, one at the intersection of the three subunits in the ectodomain (MBS1) and the second one near the ATP-binding site (MBS2), similar to those characterized in Gulf Coast P2X. Our data indicate that when Mg²⁺ and K⁺ ions are complexed with ATP, the channel is locked into an open state. Interestingly, irrespective of the number of bound ATP molecules, Mg²⁺ ions bound to the MBS2 impeded the collapse of the open-state protein to a closed state by stabilizing the ATP-protein interactions. However, when Mg²⁺ in the MBS2 was replaced with K⁺ ions, as might be expected when in equilibrium with an extracellular solution, the interactions between the subunits were weakened and the pore collapsed. This collapse was apparent when fewer than two ATPs were bound to MBS2 in the presence of K⁺. Therefore, the different capacities of common cations to stabilize the channel may underlie a mechanism governing P2X4 channel gating in physiological systems. This study therefore provides structural insights into the differential modulation of ATP activation of P2X4 by Mg²⁺ and K⁺.     

Interaction of ibogaine with human α3β4-nicotinic acetylcholine receptors in different conformational states

The interaction of ibogaine and phencyclidine (PCP) with human (h) α3β4-nicotinic acetylcholine receptors (AChRs) in different conformational states was determined by functional and structural approaches including, radioligand binding assays, Ca²⁺ influx detections, and thermodynamic and kinetics measurements. The results established that (a) ibogaine inhibits (±)-epibatidine-induced Ca²⁺ influx in hα3β4 AChRs with ～9-fold higher potency than that for PCP, (b) [³H]ibogaine binds to a single site in the hα3β4 AChR ion channel with relatively high affinity (K_d = 0.46 ± 0.06 μM), and ibogaine inhibits [³H]ibogaine binding to the desensitized hα3β4 AChR with slightly higher affinity compared to the resting AChR. This is explained by a slower dissociation rate from the desensitized ion channel compared to the resting ion channel, and (c) PCP inhibits [³H]ibogaine binding to the hα3β4 AChR, suggesting overlapping sites. The experimental results correlate with the docking simulations suggesting that ibogaine and PCP interact with a binding domain located between the serine (position 6′) and valine/phenylalanine (position 13′) rings. This interaction is mediated mainly by van der Waals contacts, which is in agreement with the observed enthalpic contribution determined by non-linear chromatography. However, the calculated entropic contribution also indicates local conformational changes. Collectively our data suggest that ibogaine and PCP bind to overlapping sites located between the serine and valine/phenylalanine rings, to finally block the AChR ion channel, and in the case of ibogaine, to probably maintain the AChR in the desensitized state for longer time.     

The Link between Ion Permeation and Inactivation Gating of Kv4 Potassium Channels

Kv4 potassium channels undergo rapid inactivation but do not seem to exhibit the classical N-type and C-type mechanisms present in other Kv channels. We have previously hypothesized that Kv4 channels preferentially inactivate from the preopen closed state, which involves regions of the channel that contribute to the internal vestibule of the pore. To further test this hypothesis, we have examined the effects of permeant ions on gating of three Kv4 channels (Kv4.1, Kv4.2, and Kv4.3) expressed in Xenopus oocytes. Rb⁺ is an excellent tool for this purpose because its prolonged residency time in the pore delays K⁺ channel closing. The data showed that, only when Rb⁺ carried the current, both channel closing and the development of macroscopic inactivation are slowed (1.5- to 4-fold, relative to the K⁺ current). Furthermore, macroscopic Rb⁺ currents were larger than K⁺ currents (1.2- to 3-fold) as the result of a more stable open state, which increases the maximum open probability. These results demonstrate that pore occupancy can influence inactivation gating in a manner that depends on how channel closing impacts inactivation from the preopen closed state. By examining possible changes in ionic selectivity and the influence of elevating the external K⁺ concentration, additional experiments did not support the presence of C-type inactivation in Kv4 channels.     

Metal cations as synaptosomal calcium blockers in studies with Fura-2

Metal ions are often used to block calcium channels in various tissues, including synaptosomes. In the present study, Fura-2 was used to determine the effectiveness of various metal ions as calcium channel blockers in rat brain synaptosomes in vitro. In buffer solutions, La³⁺ and Cd²⁺ increased the Fura-2 fluorescence in a manner similar to Ca²⁺. Ni²⁺ and Mn²⁺ appeared to be fluorescence quenching cations, and Sr²⁺ and Co²⁺ had little effect on the fluorescence of Fura-2. In suspensions of synaptosomes under resting conditions, Cd²⁺, Ni²⁺ and Mn²⁺ were found to be not suitable for use in synaptosome studies. On the other hand, La³⁺ and Co²⁺ had little effect on the Fura-2 fluorescence of resting synaptosomes, and under depolarizing conditions, La³⁺ and Co²⁺ decreased the Fura-2 fluorescence. These resuls, therefore, suggest that La³⁺ and Co²⁺ may be suitable as calcium channel blockers in synaptosome studies.     

Terbium(III) fluorescence probe studies on metal ion-binding sites in anticoagulation factor I from Agkistrodon acutus venom

Anticoagulation factor I (ACF I) isolated from the venom of Agkistrodon acutus is an activated coagulation factor X-binding protein with marked anticoagulant activity. Present studies show that holo-ACF I assumes a compactly folded structure in the range of pH 5–6, in which the most interior Trp residues and quenchers are adjacent. Tb³⁺ ions can completely replace both Ca²⁺ ions in holo-ACF I, as determined by equilibrium dialysis. Although the two Tb³⁺ ions in Tb³⁺-ACF I have slightly different luminescence efficiencies, both have similar quenching effects on the intrinsic fluorescence, suggesting that probably there are same numbers of Trp residues close to both Tb³⁺-binding sites. Two Tb³⁺-binding sites with similar apparent Tb³⁺ association constant values, (1.69 ± 0.02) × 10⁷ M^–1 and (1.42 ± 0.01) × 10⁷ M^–1, respectively, were further identified through Tb³⁺ fluorescence titration. In addition, it has been confirmed from the titration of holo-ACF I and Tb³⁺-ACF I with NBS that only interior Trp residues are involved in the energy transfer to Tb³⁺ ions and that all accessible Trp residues located in the surface of holo-ACF I have similar affinity to NBS, while those located in the surface of Tb³⁺-ACF I have two different kinds of affinity to NBS, which strongly suggests a conformational change of holo-ACF I upon substitution of Tb³⁺ for Ca²⁺. The results show that although the Tb³⁺-altered conformation of ACF I cannot support the binding of Tb³⁺-ACF I with FXa, determined by nondenaturing PAGE, Tb³⁺ ions are effective and useful fluorescence probes to analyze the structures and properties of Ca²⁺-binding sites in ACF I.     

Terbium replacement of calcium in parvalbumin

Carp muscle calcium binding parvalbumin, crystallized in 2.9 m-ammonium sulfate, can bind two Tb³⁺ ions, which displace the two Ca²⁺ ions normally present. The Ca²⁺ co-ordinated in the loop between the E and the F α-helices is displaced at low Tb³⁺ concentrations; whereas the Ca²⁺ at the CD site is replaced only at higher Tb³⁺ concentration. There is not a third Tb³⁺ site as had been suggested in interpretations of Tb³⁺ fluorescence experiments performed without ammonium sulfate. A third electron density peak in the difference Fourier maps is tentatively assigned to a sulfate ion co-ordinating the EF site Tb³⁺ ion.     

Ion binding properties and structure stability of the NaK channel

Ion distribution in the selectivity filter and ion-water and ion-protein interactions of NaK channel are systematically investigated by all-atom molecular dynamics simulations, with the tetramer channel protein being embedded in a solvated phospholipid bilayer. Analysis of the simulation results indicates that K⁺ ions prefer to bind within the sites formed by two adjacent planes of oxygen atoms from the selectivity filter, while Na⁺ ions are inclined to bind to a single plane of four oxygen atoms. At the same time, both K⁺ and Na⁺ ions can diffuse in the vestibule, accompanying with movements of the water molecules confined in a complex formed by the vestibule together with four small grottos connecting to it. As a result, K⁺ ions show a wide range of coordination numbers (6-8), while Na⁺ ions display a constant coordination number of ∼ 6 in the selectivity filter, which may result in the loss of selectivity of NaK. It is also found that a Ca²⁺ can bind at the extracellular site as reported in the crystal structure in a partially hydrated state, or at a higher site in a full hydration state. Furthermore, the carbonyl group of Asp66 can reorient to point towards the center pore when an ion exists in the vestibule, while that of Gly65 always aligns tangentially to the channel axis, as in the crystallographic structures.     

Molecular dynamics simulation of TMEM16A channel: Linking structure with gating

TMEM16A, the calcium-activated chloride channel, is broadly expressed and plays pivotal roles in diverse physiological processes. To understand the structural and functional relationships of TMEM16A, it is necessary to fully clarify the structural basis of the gating of the TMEM16A channel. Herein, we performed the protein electrostatic analysis and molecular dynamics simulation on the TMEM16A in the presence and absence of Ca²⁺. Data showed that the separation of TM4 and TM6 causes pore expansion, and Q646 may be a key residue for the formation of π-helix in the middle segment of TM6. Moreover, E705 was found to form a group of H-bond interactions with D554/K588/K645 below the hydrophobic gate to stabilize the closed conformation of the pore in the Ca²⁺-free state. Interestingly, in the Ca²⁺ bound state, the E705 side chain swings 100^o to serve as Ca²⁺-binding coordination and released K645. K645 is closer to the hydrophobic gate in the calcium-bound state, which facilitates the provision of electrostatic forces for chloride ions as the ions pass through the hydrophobic gate. Our findings provide the structural-based insights to understanding the mechanisms of gating of TMEM16A.     

In yeast, Ca and octylguanidine interact with porin (VDAC) preventing the mitochondrial permeability transition

In yeast, Ca²⁺ and long chain alkylguanidines interact with mitochondria modulating the opening of the yeast mitochondrial unspecific channel. Mammalians possess a similar structure, the mitochondrial permeability transition pore. The composition of these pores is under debate. Among other components, the voltage-dependent anion channel has been proposed as a component of either pore. In yeast from an industrial strain, octylguanidine and calcium closed the yeast mitochondrial unspecific channel. Here, the effects of the cations Ca²⁺ or octylguanidine and the voltage-dependent anion channel effector decavanadate were evaluated in yeast mitochondria from either a wild type or a voltage-dependent anion channel deletion laboratory strain. It was observed that in the absence of voltage-dependent anion channel, the yeast mitochondrial unspecific channel was desensitized to Ca²⁺, octylguanidine or decavanadate but remained sensitive to phosphate. It is thus suggested that in yeast mitochondria, the voltage-dependent anion channel has a cation binding site where Ca²⁺ and octylguanidine interact, conferring cation sensitivity to the yeast mitochondrial unspecific channel.     

Simulations of calcium channel block by trivalent cations: Gd competes with permeant ions for the selectivity filter

Current through L-type calcium channels (Ca_V1.2 or dihydropyridine receptor) can be blocked by micromolar concentrations of trivalent cations like the lanthanide gadolinium (Gd³⁺). It has been proposed that trivalent block is due to ions competing for a binding site in both the open and closed configuration, but possibly with different trivalent affinities. Here, we corroborate this general view of trivalent block by computing conductance of a model L-type calcium channel. The model qualitatively reproduces the Gd³⁺ concentration dependence and the effect that substantially more Gd³⁺ is required to produce similar block in the presence of Sr²⁺ (compared to Ba²⁺) and even more in the presence of Ca²⁺. Trivalent block is explained in this model by cations binding in the selectivity filter with the charge/space competition mechanism. This is the same mechanism that in the model channel governs other selectivity properties. Specifically, selectivity is determined by the combination of ions that most effectively screen the negative glutamates of the protein while finding space in the midst of the closely packed carboxylate groups of the glutamate residues.     

Resting potential of the mouse neuroblastoma cells: II. Significant contribution of the surface potential to the resting potential of the cells under physiological conditions

In the previous paper, we showed that the K⁺ channels of the mouse neuroblastoma cell (clone N-18) are closed at low concentration of external K⁺ ([K⁺]₀) including the physiological concentration for the cells. In the present study, the origin of the resting membrane potential of N-18 cells has been examined. (1) The resting membrane potential of N-18 cells was depolarized by increasing concentration of the polyvalent cations (La³⁺, Fe³⁺, Co²⁺, Ca²⁺, Sr²⁺, Mg²⁺) and by decreasing the pH of the medium. The input membrane resistance was slightly increased during the depolarization. The depolarization was not explained in terms of the diffusion of the cations across the membrane, since the trivalent cations of greater ionic size were effective at much lower concentrations than the divalent cations. The results obtained from the measurements of ⁸⁶Rb efflux suggested that the depolarization cannot be explained in terms of blocking of the K⁺ channels by the cations. (2) An increase in Ca²⁺ concentration from 0.3 to 1.8 mM induced depolarization of about 10 mV at low [K⁺]₀ where the K⁺ channels are closed, but did not induce any depolarization at high [K⁺]₀ where the channels are open. (3) In order to estimate the changes in the zeta-potential, the electrophoretic mobility of N-18 cells was measured under various conditions. There was a close correlation between the changes in the zeta-potential and those in the membrane potential in response to the polyvalent cations and proton. On the other hand, an increase in K⁺-concentration in the medium, which induced a large depolarization in the cells, did not affect the zeta-potential. (4) The results obtained were explained by an electrical circuit model for the membranes of N-18 cells. In this model, an electrical circuit for the membrane part carrying no selective ionic channels, in which changes in the surface potential directly affect the transmembrane potential, is connected in parallel to the usual circuit model representing selective ionic channel systems. It was concluded that the surface potential contributes significantly to the resting membrane potential of N-18 cells at low [K⁺]₀ where the K⁺ channels are closed.     

Luminescence and energy‐transfer properties of color‐tunable Ca2Mg0.25Al1.5Si1.25O7:Ce3+/Eu2+/Tb3+ phosphors for ultraviolet light‐emitting diodes

A series of Ca₂Mg_0.25Al_1.5Si_1.25O₇:Ce³⁺/Eu²⁺/Tb³⁺ phosphors was been prepared via a conventional high temperature solid‐state reaction and their luminescence properties were studied. The emission spectra of Ca₂Mg_0.25Al_1.5Si_1.25O₇:Ce³⁺,Eu²⁺ and Ca₂Mg_0.25Al_1.5Si_1.25O₇:Ce³⁺,Tb³⁺ phosphors show not only a band due to Ce³⁺ ions (409 nm) but also as a band due to Eu²⁺ (520 nm) and Tb³⁺ (542 nm) ions. More importantly, the effective energy transfer from Ce³⁺ to Eu²⁺ and Tb³⁺ ions was confirmed and investigated by emission/excitation spectra and luminescent decay behaviors. Furthermore, the energy level scheme and energy transfer mechanism were investigated and were demonstrated to be of resonant type via dipole–dipole (Ce³⁺ to Eu²⁺) and dipole–quadrupole (Ce³⁺ to Tb³⁺) reactions, respectively. Under excitation at 350 nm, the emitting color could be changed from blue to green by adjusting the relative doping concentration of Ce³⁺ and Eu²⁺ ions as well as Ce³⁺ and Tb³⁺ ions. The above results indicate that Ca₂Mg_0.25Al_1.5Si_1.25O₇:Ce³⁺,Eu²⁺/Tb³⁺ are promising single‐phase blue‐to‐green phosphors for application in phosphor conversion white‐light‐emitting diodes. Copyright © 2015 John Wiley & Sons, Ltd.     

Tunable emission,energy transfer and charge compensation in SrMoO4:Sm3+,Tb3+,Na+ phosphor

A series of SrMoO₄:Sm³⁺,Tb³⁺,Na⁺ phosphors was synthesized using a high‐temperature solid‐state reaction method in air. On excitation at 290 nm, SrMoO₄:Sm³⁺,Tb³⁺ phosphor emitted light that varied systematically from green to reddish‐orange on changing the Sm³⁺ and Tb³⁺ ion concentrations. The emission intensities of SrMoO₄:Sm³⁺ and SrMoO₄:Sm³⁺,Tb³⁺ phosphors were increased two to four times due to charge compensation when Na⁺ was added as a charge compensator. The luminescence mechanism and energy transfer could be explained using energy‐level diagrams of the MoO₄^2– group, Sm³⁺ and Tb³⁺ ions. SrMoO₄:Sm³⁺,Tb³⁺,Na⁺ could be used as reddish‐orange phosphor in white light‐emitting diodes (LEDs) based on an ~ 405 nm near‐UV LED chip. This research is helpful in adjusting and improving the luminescence properties of other phosphors. Copyright © 2015 John Wiley & Sons, Ltd.     

Probing Pore Constriction in a Ligand-gated Ion Channel by Trapping a Metal Ion in the Pore upon Agonist Dissociation

Eukaryotic pentameric ligand-gated ion channels (pLGICs) are receptors activated by neurotransmitters to rapidly transport ions across cell membranes, down their electrochemical gradients. Recent crystal structures of two prokaryotic pLGICs were interpreted to imply that the extracellular side of the transmembrane pore constricts to close the channel (Hilf, R. J., and Dutzler, R. (2009) Nature 457, 115–118; Bocquet, N., Nury, H., Baaden, M., Le Poupon, C., Changeux, J. P., Delarue, M., and Corringer, P. J. (2009) Nature 457, 111–114). Here, we utilized a eukaryotic acetylcholine (ACh)-serotonin chimeric pLGIC that was engineered with histidines to coordinate a metal ion within the channel pore, at its cytoplasmic side. In a previous study, the access of Zn²⁺ ions to the engineered histidines had been explored when the channel was either at rest (closed) or active (open) (Paas, Y., Gibor, G., Grailhe, R., Savatier-Duclert, N., Dufresne, V., Sunesen, M., de Carvalho, L. P., Changeux, J. P., and Attali, B. (2005) Proc. Natl. Acad. Sci. U.S.A. 102, 15877–15882). In this study, the interactions of Zn²⁺ with the pore were probed upon agonist (ACh) dissociation that triggers the transition of the receptor from the active conformation to the resting conformation (i.e. during deactivation). Application of Zn²⁺ onto ACh-bound open receptors obstructed their pore and prevented ionic flow. Removing ACh from its extracellular binding sites to trigger deactivation while Zn²⁺ is still bound led to tight trapping of Zn²⁺ within the pore. Together with single-channel recordings, made to explore single pore-blocking events, we show that dissociation of ACh causes the gate to shut on a Zn²⁺ ion that effectively acts as a “foot in the door.” We infer that, upon deactivation, the cytoplasmic side of the pore of the ACh-serotonin receptor chimera constricts to close the channel.