Valentin Borshchevskiy

Crystal structure of a light-driven sodium pump

Recently, the first known light-driven sodium pumps, from the microbial rhodopsin family, were discovered. We have solved the structure of one of them, Krokinobacter eikastus rhodopsin 2 (KR2), in the monomeric blue state and in two pentameric red states, at resolutions of 1.45 Å and 2.2 and 2.8 Å, respectively. The structures reveal the ion-translocation pathway and show that the sodium ion is bound outside the protein at the oligomerization interface, that the ion-release cavity is capped by a unique N-terminal α-helix and that the ion-uptake cavity is unexpectedly large and open to the surface. Obstruction of the cavity with the mutation G263F imparts KR2 with the ability to pump potassium. These results pave the way for the understanding and rational design of cation pumps with new specific properties valuable for optogenetics.

Structural insights into the proton pumping by unusual proteorhodopsin from nonmarine bacteria

Light-driven proton pumps are present in many organisms. Here, we present a high-resolution structure of a proteorhodopsin from a permafrost bacterium, Exiguobacterium sibiricum rhodopsin (ESR). Contrary to the proton pumps of known structure, ESR possesses three unique features. First, ESRs proton donor is a lysine side chain that is situated very close to the bulk solvent. Second, the α-helical structure in the middle of the helix F is replaced by 310- and π-helix–like elements that are stabilized by the Trp-154 and Asn-224 side chains. This feature is characteristic for the proteorhodopsin family of proteins. Third, the proton release region is connected to the bulk solvent by a chain of water molecules already in the ground state. Despite these peculiarities, the positions of water molecule and amino acid side chains in the immediate Schiff base vicinity are very well conserved. These features make ESR a very unusual proton pump. The presented structure sheds light on the large family of proteorhodopsins, for which structural information was not available previously.

Active state of sensory rhodopsin II: structural determinants for signal transfer and proton pumping.

The molecular mechanism of transmembrane signal transduction is still a pertinent question in cellular biology. Generally, a receptor can transfer an external signal via its cytoplasmic surface, as found for G-protein-coupled receptors such as rhodopsin, or via the membrane domain, such as that in sensory rhodopsin II (SRII) in complex with its transducer, HtrII. In the absence of HtrII, SRII functions as a proton pump. Here, we report on the crystal structure of the active state of uncomplexed SRII from Natronomonas pharaonis, NpSRII. The problem with a dramatic loss of diffraction quality upon loading of the active state was overcome by growing better crystals and by reducing the occupancy of the state. The conformational changes in the region comprising helices F and G are similar to those observed for the NpSRII-transducer complex but are much more pronounced. The meaning of these differences for the understanding of proton pumping and signal transduction by NpSRII is discussed.

X-ray-radiation-induced changes in bacteriorhodopsin structure.

Bacteriorhodopsin (bR) provides light-driven vectorial proton transport across a cell membrane. Creation of electrochemical potential at the membrane is a universal step in energy transformation in a cell. Published atomic crystallographic models of early intermediate states of bR show a significant difference between them, and conclusions about pumping mechanisms have been contradictory. Here, we present a quantitative high-resolution crystallographic study of conformational changes in bR induced by X-ray absorption. It is shown that X-ray doses that are usually accumulated during data collection for intermediate-state studies are sufficient to significantly alter the structure of the protein. X-ray-induced changes occur primarily in the active site of bR. Structural modeling showed that X-ray absorption triggers retinal isomerization accompanied by the disappearance of electron densities corresponding to the water molecule W402 bound to the Schiff base. It is demonstrated that these and other X-ray-induced changes may mimic functional conformational changes of bR leading to misinterpretation of the earlier obtained X-ray crystallographic structures of photointermediates.

Mechanism of transmembrane signaling by sensor histidine kinases

Bacterial sensing mechanism revealed Escherichia coli use a transmembrane sensor protein to sense nitrate in their external environment and initiate a biochemical response. Gushchin et al. compared crystal structures of portions of the NarQ receptor that included the transmembrane helices in ligand-bound or unbound states. The structures suggest a signaling mechanism by which piston- and lever-like movements are transmitted to response regulator proteins within the cell. Such two-component systems are very common in bacteria and, if better understood, might provide targets for antimicrobial therapies. Science, this issue p. eaah6345 Crystal structures show how sensing of nitrate occurs in bacteria. INTRODUCTION Microorganisms obtain most of the information about their environments through membrane-associated signaling systems. One of the most abundant classes of membrane receptors, present in all domains of life, is sensor histidine kinases, members of two-component signaling systems (TCSs). Tens of thousands of TCSs are known. Many of these systems are essential for cell growth, survival, or pathogenicity and consequently can be targeted to reduce virulence. Several large families of transmembrane (TM) TCS receptors are known: (i) sensor kinases, which generally possess a periplasmic, membrane, or intracellular sensor module; a transmembrane domain; often one or more intracellular signal transduction domains such as HAMP, PAS, or GAF; and an intracellular autokinase module (DHp and CA domains), which phosphorylates the response regulator protein; (ii) chemoreceptors, which also possess the sensor module and the TM domain but lack the kinase domain and control a separate kinase protein (CheA) via a kinase control module; and (iii) phototaxis systems, which are similar to chemotaxis systems except that the sensor module—a light receptor sensory rhodopsin—is a separate protein. RATIONALE Despite the wealth of biochemical data, the structural mechanisms of transmembrane signaling by TCS sensors are poorly understood at the atomic level. In particular, high-resolution structures of the TM segments connected to the adjacent domains are lacking. Deciphering of the signaling-associated conformational changes would shed light on the details of long-range transmembrane signal transduction and might help in the development of novel classes of antimicrobials targeting TCSs. RESULTS We used the in meso crystallization approach and single-wavelength anomalous dispersion to determine the crystal structures, at resolutions of up to 1.9 Å, of a fragment of Escherichia coli nitrate/nitrite sensor histidine kinase NarQ that contains the sensor, TM, and HAMP domains in a symmetric ligand-free apo state and in symmetric and asymmetric ligand-bound holo-S and holo-A states. In all of the structures, the TM domain is an antiparallel four-stranded coiled coil (CC) consisting of nine CC layers. The sensor domain is connected to the TM domain through continuous α-helical linkers that are partially disrupted in the holo state. The intracellular HAMP domain is connected to the TM helices via flexible proline junctions and robust hydrogen bonds conserved in all signaling states. The structures reveal the mechanism of transmembrane signal transduction in NarQ and show that binding of ligand induces displacement of the sensor domain helices by ~0.5 to 1 Å. This displacement translates into rearrangements and ~2.5 Å pistonlike shifts of transmembrane helices and is later converted, via leverlike motions of the HAMP domain protomers, into 7 Å shifts of the output helices and changes of the CC helical phase. The structures also demonstrate that the signaling-associated conformational changes in the TM domain do not need to be symmetric. CONCLUSION The determined structures of the transmembrane and membrane-proximal domains of the nitrate/nitrite receptor NarQ in ligand-free and ligand-bound forms present a template for studies of other TCS receptors, establish the importance of the pistonlike displacements of the TM helices for TM signal transduction, and highlight the role of the HAMP domain as an amplifier and converter of a piston-like displacement into helical rotation. Overall, the results show how a mechanistic signal is generated and amplified while being transduced through the protein over distances of 100 Å or more. Because membrane-associated TCSs are ubiquitous in microorganisms and are central for bacterial sensing, we believe that our results will help to elucidate a broad range of cellular processes such as basic metabolism, sporulation, quorum sensing, and virulence. They may also provide insights useful for the development of novel antimicrobial treatments targeting TCSs. The structures of histidine kinase NarQ in ligand-free and ligand-bound forms. The structures reveal rearrangement of transmembrane α helices during signal transduction and show that pistonlike shifts of the transmembrane helices result in leverlike motions of the HAMP domain protomers. One of the major and essential classes of transmembrane (TM) receptors, present in all domains of life, is sensor histidine kinases, parts of two-component signaling systems (TCSs). The structural mechanisms of TM signaling by these sensors are poorly understood. We present crystal structures of the periplasmic sensor domain, the TM domain, and the cytoplasmic HAMP domain of the Escherichia coli nitrate/nitrite sensor histidine kinase NarQ in the ligand-bound and mutated ligand-free states. The structures reveal that the ligand binding induces rearrangements and pistonlike shifts of TM helices. The HAMP domain protomers undergo leverlike motions and convert these pistonlike motions into helical rotations. Our findings provide the structural framework for complete understanding of TM TCS signaling and for development of antimicrobial treatments targeting TCSs.

Low-dose X-ray radiation induces structural alterations in proteins

X-ray-radiation-induced alterations to protein structures are still a severe problem in macromolecular crystallography. One way to avoid the influence of radiation damage is to reduce the X-ray dose absorbed by the crystal during data collection. However, here it is demonstrated using the example of the membrane protein bacteriorhodopsin (bR) that even a low dose of less than 0.06 MGy may induce structural alterations in proteins. This dose is about 500 times smaller than the experimental dose limit which should ideally not be exceeded per data set (i.e. 30 MGy) and 20 times smaller than previously detected specific radiation damage at the bR active site. To date, it is the lowest dose at which radiation modification of a protein structure has been described. Complementary use was made of high-resolution X-ray crystallography and online microspectrophotometry to quantitatively study low-dose X-ray-induced changes. It is shown that structural changes of the protein correlate with the spectroscopically observed formation of the so-called bR orange species. Evidence is provided for structural modifications taking place at the protein active site that should be taken into account in crystallographic studies which aim to elucidate the molecular mechanisms of bR function.

X-ray structure of a CDP-alcohol phosphatidyltransferase membrane enzyme and insights into its catalytic mechanism

Phospholipids have major roles in the structure and function of all cell membranes. Most integral membrane proteins from the large CDP-alcohol phosphatidyltransferase family are involved in phospholipid biosynthesis across the three domains of life. They share a conserved sequence pattern and catalyse the displacement of CMP from a CDP-alcohol by a second alcohol. Here we report the crystal structure of a bifunctional enzyme comprising a cytoplasmic nucleotidyltransferase domain (IPCT) fused with a membrane CDP-alcohol phosphotransferase domain (DIPPS) at 2.65 Å resolution. The bifunctional protein dimerizes through the DIPPS domains, each comprising six transmembrane α-helices. The active site cavity is hydrophilic and widely open to the cytoplasm with a magnesium ion surrounded by four highly conserved aspartate residues from helices TM2 and TM3. We show that magnesium is essential for the enzymatic activity and is involved in catalysis. Substrates docking is validated by mutagenesis studies, and a structure-based catalytic mechanism is proposed.

Structural insights into ion conduction by channelrhodopsin 2.

The inner workings of an optogenetic tool Channelrhodopsins are membrane channel proteins whose gating is controlled by light. In their native setting, they allow green algae to move in response to light. Their expression in neurons allows precise control of neural activity, an approach known as optogenetics. Volkov et al. describe the high-resolution structure of channelrhodopsin 2, the most widely used optogenetics tool, as well as the structure of a mutant with a longer open-state lifetime (see the Perspective by Gerwert). Light activation perturbs an intricate hydrogen-bonding network to open the channel. The structures provide a basis for designing better optogenetic tools. Science, this issue p. 10.1126/science.eaan8862; see also p. 1000 Channelrhodopsin has an intricate hydrogen-bonding network that is perturbed by light activation, resulting in channel opening. INTRODUCTION Ion channels are integral membrane proteins that upon stimulation modulate the flow of ions across the cell or organelle membrane. The resulting electrical signals are involved in biological functions such as electrochemical transmission and information processing in neurons. Channelrhodopsins (ChRs) appear to be unusual channels. They belong to the large family of microbial rhodopsins, seven-helical transmembrane proteins containing retinal as chromophore. Photon absorption initiates retinal isomerization resulting in a photocycle, with different spectroscopically distinguishable intermediates, thereby controlling the opening and closing of the channel. In 2003, it was demonstrated that light-induced currents by heterologously expressed ChR2 can be used to change a host’s membrane potential. The concept was further applied to precisely control muscle and neural activity by using light-induced depolarization to trigger an action potential in neurons expressing ChR2. This optogenetic approach with ChR2 and other ChRs has been widely used for remote control of neural cells in culture and in living animals with high spatiotemporal resolution. It is also used in biomedical studies aimed to cure severe diseases. RATIONALE Despite the wealth of biochemical and biophysical data, a high-resolution structure and structural mechanisms of a native ChR2 (and other ChRs) have not yet been known. A step forward was the structure of a chimera (C1C2). However, recent electrophysiological and Fourier transform infrared data showed that C1C2 exhibits light-induced responses that are functionally and mechanistically different from ChR2. Given that ChR2 is the most frequently used tool in optogenetics, a high-resolution structure of ChR2 is of high importance. Deciphering the structure of the native channel would shed light on how the light-induced changes at the retinal Schiff base (RSB) are linked to the channel operation and may make engineering of enhanced optogenetic tools more efficient. RESULTS We expressed ChR2 in LEXSY and used in the meso crystallization approach to determine the crystal structure of the wild-type ChR2 and C128T slow mutant at 2.4 and 2.7 Å, respectively (C, cysteine; T, threonine). Two different dark-state conformations of ChR2 in the two protomers in the asymmetric unit were resolved. The overall structure alignment of the protomers does not show a visible difference in backbone conformation. However, the conformation of some amino acids and the position of water molecules are not the same. The dimerization is strong and provided mainly through the interaction of helices 3 and 4 and the N termini. In addition, the protomers are connected with a disulfide bond, C34/C36′. In both protomers, we identified ion conduction pathway comprising four cavities [extracellular cavity 1 (EC1), EC2, intracellular cavity 1 (IC1), and IC2] that are separated by three gates [extracellular gate (ECG), central gate (CG), and intracellular gate (ICG)] (figure, panel A). Arginines R120 and R268 are the cores of ECG and ICG, respectively, in all ChRs. The Schiff base is hydrogen-bond–connected to E123 and D253 amino acids (E, glutamic acid; D, aspartic acid) and is a key part of the CG that is further connected with two other gates through an extended H-bond network mediated by numerous water molecules (figure, panel B). The DC gate is separate from the gates in the channel pathway and is bridged by hydrogen bonds through the water molecule w5. Hydrogen bonding of the DC pair (C128 and D156) has two important consequences. It stabilizes helices 3 and 4 and provides connection from D156, a possible proton donor, to the RSB. The presence of the hydrogen bonds provides structural insights into how the DC gate controls ChR2 gating lifetime. CONCLUSION The determined structures of ChR2 and its C128T mutant present the molecular basis for the understanding of ChR functioning. They provide insights into mechanisms of channel opening and closing. A plausible scenario is that the disruption of the H-bonds between E123 and D253 and the Schiff base and the protonation of D253 upon retinal isomerization trigger rearrangements in the extended hydrogen-bonded networks, stabilizing the ECG and CG and also rearranging the H-bonding network in the cavities. Upon retinal isomerization, these two gates are opened and the network is broken. This leads to the reorientation of helix 2. Additional changes in helices 6 and 7 induced by the isomerization could help with opening the ICG and channel pore formation. General structure presentation of ChR2. (A) Four cavities and three gates forming the channel pore. (B) Extended hydrogen-bond network. The DC gate is shown in the red ellipse. The black arrows and gray horizontal lines show the putative ion pathway and position of hydrophobic/hydrophilic boundaries, respectively. The light-gated ion channel channelrhodopsin 2 (ChR2) from Chlamydomonas reinhardtii is a major optogenetic tool. Photon absorption starts a well-characterized photocycle, but the structural basis for the regulation of channel opening remains unclear. We present high-resolution structures of ChR2 and the C128T mutant, which has a markedly increased open-state lifetime. The structure reveals two cavities on the intracellular side and two cavities on the extracellular side. They are connected by extended hydrogen-bonding networks involving water molecules and side-chain residues. Central is the retinal Schiff base that controls and synchronizes three gates that separate the cavities. Separate from this network is the DC gate that comprises a water-mediated bond between C128 and D156 and interacts directly with the retinal Schiff base. Comparison with the C128T structure reveals a direct connection of the DC gate to the central gate and suggests how the gating mechanism is affected by subtle tuning of the Schiff base’s interactions.

Overcoming merohedral twinning in crystals of bacteriorhodopsin grown in lipidic mesophase

Twinning is one of the most common crystal-growth defects in protein crystallography. There are neither efficient rational approaches for the growth of nontwinned protein crystals nor are there examples of systematic studies of the dependence of the twinning-ratio distribution on crystallization conditions. The description of the twinning phenomenon has been covered even less for membrane-protein crystals and is non-existent for crystals grown using lipidic phases (in meso). In the present work, possibilities for overcoming merohedral twinning are investigated for crystals of the membrane protein bacteriorhodopsin (bR) grown in meso. It is shown that traditional crystallization additives are not effective in the case of the in meso crystallization of bR. The twinning ratio was determined for 310 crystals grown under different crystallization conditions. A correlation of the twinning ratio with the growth rate of the crystals was observed. Slow growth indicated that crystals had a noticeable chance of avoiding twinning. Model calculations were performed in order to rationalize this observation. The calculations confirmed the experimental observation that most crystals consist of two twin domains and showed that under this condition small changes in the probability of twin-domain formation lead to dramatic changes in the number of nontwinned crystals, which explains why slow crystal growth results in a considerable number of nontwinned crystals.

Ground state structure of D75N mutant of sensory rhodopsin II in complex with its cognate transducer

The complex of sensory rhodopsin II (NpSRII) with its cognate transducer (NpHtrII) mediates negative phototaxis in halobacteria Natronomonas pharaonis. Upon light activation NpSRII triggers, by means of NpHtrII, a signal transduction chain homologous to the two component system in eubacterial chemotaxis. Here we report on the crystal structure of the ground state of the mutant NpSRII-D75N/NpHtrII complex in the space group I212121. Mutations of this aspartic acid in light-driven proton pumps dramatically modify or/and inhibit protein functions. However, in vivo studies show that the similar D75N mutation retains functionality of the NpSRII/NpHtrII complex. The structure provides the molecular basis for the explanation of the unexpected observation that the wild and the mutant complexes display identical physiological response on light excitation.