Dynamics of voltage profile in enzymatic ion transporters, demonstrated in electrokinetics of proton pumping rhodopsin

H⁺-pumping rhodopsins mediate a primordial conversion of light to metabolic energy. Bacteriorhodopsin from Halobacterium salinarium is the first identified and (biochemically) best-studied H⁺-pumping rhodopsin. The electrical properties of H⁺-pumping rhodopsins, however, are known in more detail for the homolog Acetabularia rhodopsin, isolated from the eukaryotic green alga Acetabularia acetabulum. Based on data from Acetabularia rhodopsin we present a general reaction kinetic model of H⁺-pumping rhodopsins with only seven independent parameters, which fits the kinetic properties of photocurrents as functions of light, transmembrane voltage, internal and external pH, and time. The model describes fast photoisomerization of retinal with simultaneous H⁺ transfer to an H⁺ acceptor, reprotonation of retinal from the intracellular face via an H⁺ donor, and proton release to the extracellular space via an H⁺ release complex. The voltage sensitivities of the individual reaction steps and their temporal changes are treated here by a novel approach, whereby—as in an Ohmic voltage divider—the effective portions of the total transmembrane voltage decrease with the relative velocities of the individual reaction steps. This analysis quantitatively infers dynamic changes of the voltage profile and of the pK values of the H⁺-binding sites involved.     

The photophobic receptor from Natronobacterium pharaonis: temperature and pH dependencies of the photocycle of sensory rhodopsin II.

The photocycle of the photophobic receptor sensory rhodopsin II from N. pharaonis was analyzed by varying measuring wavelengths, temperature, and pH, and by exchanging H2O with D2O. The data can be satisfactorily modeled by eight exponents over the whole range of modified parameters. The kinetic data support a model similar to that of bacteriorhodopsin (BR) if a scheme of irreversible first-order reactions is assumed. Eight kinetically distinct protein states can then be identified. These states are formed from five spectrally distinct species. The chromophore states Si correspond in their spectral properties to those of the BR photocycle, namely pSRII510 (K), pSRII495 (L), pSRII400 (M), pSRII485 (N), and pSRII535 (O). In comparison to BR, pSRII400 is formed approximately 10 times faster than the M state; however, the back-reaction is almost 100 times slower. Comparison of the temperature dependence of the rate constants with those from the BR photocycle suggests that the differences are caused by changes of DeltaS. The rate constants of the pSRII photocycle are almost insensitive to the pH variation from 9.0 to 5.5, and show only a small H2O/D2O effect. This analysis supports the idea that the conformational dynamics of pSRII controls the kinetics of the photocycle of pSRII.     

Conformational changes in the archaerhodopsin-3 proton pump: detection of conserved strongly hydrogen bonded water networks

Archaerhodopsin-3 (AR3) is a light-driven proton pump from Halorubrum sodomense, but little is known about its photocycle. Recent interest has focused on AR3 because of its ability to serve both as a high-performance, genetically-targetable optical silencer of neuronal activity and as a membrane voltage sensor. We examined light-activated structural changes of the protein, retinal chromophore, and internal water molecules during the photocycle of AR3. Low-temperature and rapid-scan time-resolved FTIR-difference spectroscopy revealed that conformational changes during formation of the K, M, and N photocycle intermediates are similar, although not identical, to bacteriorhodopsin (BR). Positive/negative bands in the region above 3,600 cm^− 1, which have previously been assigned to structural changes of weakly hydrogen bonded internal water molecules, were substantially different between AR3 and BR. This included the absence of positive bands recently associated with a chain of proton transporting water molecules in the cytoplasmic channel and a weakly hydrogen bonded water (W401), which is part of a hydrogen-bonded pentagonal cluster located near the retinal Schiff base. However, many of the broad IR continuum absorption changes below 3,000 cm^− 1 assigned to networks of water molecules involved in proton transport through cytoplasmic and extracellular portions in BR were very similar in AR3. This work and subsequent studies comparing BR and AR3 structural changes will help identify conserved elements in BR-like proton pumps as well as bioengineer AR3 to optimize neural silencing and voltage sensing.     

Spectroscopic evidence for the formation of an N intermediate during the photocycle of sensory rhodopsin II (phoborhodopsin) from Natronobacterium pharaonis

Sensory rhodopsin II is a seven transmembrane helical retinal protein and functions as a photoreceptor protein in negative phototaxis of halophilic archaea. Sensory rhodopsin II from Natronomonas pharaonis (NpSRII) is stable under various conditions and can be expressed functionally in Escherichia coli cell membranes. Rhodopsins from microorganisms, known as microbial rhodopsins, exhibit a photocycle, and light irradiation of these molecules leads to a high-energy intermediate, which relaxes thermally to the original pigment after passing through several intermediates. For bacteriorhodopsin (BR), a light-driven proton pump, the photocycle is established as BR → K → L → M → N → O → BR. The photocycle of NpSRII is similar to that of BR except for N, i.e., M thermally decays into the O, and N has not been well characterized in the photocycle. Thus we here examined the second half of the photocycle in NpSRII, and in the present transient absorption study we found the formation of a new photointermediate whose absorption maximum is ～500 nm. This intermediate becomes pronounced in the presence of azide, which accelerates the decay of M. Transient resonance Raman spectroscopy was further applied to demonstrate that this intermediate contains a 13-cis retinal protonated Schiff base. However, detailed analysis of the transient absorption data indicated that M-decay does not directly produce N but rather produces O that is in equilibrium with N. These observations allowed us to propose a structural model for a photocycle that involves N.     

Aspartic acids 96 and 85 play a central role in the function of bacteriorhodopsin as a proton pump.

A spectroscopic and functional analysis of two point-mutated bacteriorhodopsins (BRs) from phototrophic negative halobacterial strains is reported. Bacteriorhodopsin from strain 384 contains a glutamic acid instead of an aspartic acid at position 85 and BR from strain 326 contains asparagine instead of aspartic acid at position 96. Compared to wild-type BR, the M formation in BR Asp85---Glu is accwelerated approximately 10-fold, whereas the M decay in BR Asp96---Asn is slowed down approximately 50-fold at pH6. Purple membrane sheets containing the mutated BRs were oriented and immobilized in polyacrylamide gels or adsorbed to planar lipid films. The measured kinetics of the photocurrents under various conditions agree with the observed photocycle kinetics. The ineffectivity of BR Asp85---Glu resides in the dominance of an inactive species absorbing maximally at approximately 610 nm, while BR Asp96---Asn is ineffective due to its slow photocycle. These experimental results suggest that aspartic acid 96 plays a crucial role for the reprotonation of the Schiff base. Both residues are essential for an effective proton pump.     

Proteorhodopsin is a light-driven proton pump with variable vectoriality

Proteorhodopsin, a homologue of archaeal bacteriorhodopsin (BR), belongs to a newly identified family of retinal proteins from marine bacteria, which could play an important role in the energy balance of the biosphere. We cloned the cDNA sequence of proteorhodopsin by chemical gene synthesis, expressed the protein in Escherichia coli cells, purified and reconstituted the protein in its functional active state. The photocycle characteristics were determined by time-resolved absorption and Fourier transform infrared (FT-IR) spectroscopy. The pH-dependence of the absorption spectrum indicates that the pK(a) of the primary acceptor of the Schiff base proton (Asp97) is 7.68. Generally, the photocycle of proteorhodopsin is similar to that of BR, although an L-like photocycle intermediate was not detectable. Whereas at pH>7 an M-like intermediate is formed upon illumination, at pH 5 no M-like intermediate could be detected. As the photocycle kinetics do not change between the acidic and alkaline state of proteorhodopsin, the only difference between these two forms is the protonation status of Asp97. This is corroborated by time-resolved FT-IR spectroscopy, which demonstrates that proton transfer from the retinal Schiff base to Asp97 is observed at alkaline pH, but the other vibrational changes are essentially pH-independent.After reconstitution into proteoliposomes, light-induced proton currents of proteorhodopsin were measured in a compound membrane system where proteoliposomes were adsorbed to planar lipid bilayers. Our results show that proteorhodopsin is a light-driven proton pump with characteristics similar to those of BR at alkaline pH. However, at acidic pH, the direction of proton pumping is inverted. Complementary experiments were carried out on proteorhodopsin expressed heterologously in Xenopus laevis oocytes under voltage clamp conditions.The following results were obtained. (1) At alkaline pH, proteorhodopsin mediates outwardly directed proton pumping like BR. (2) The direction of proton pumping can be inverted, when Asp97 is protonated. (3) The current can be inverted by changes of the polarity of the applied voltage. (4) The light intensity-dependence of the photocurrents leads to the conclusion that the alkaline form of proteorhodopsin shows efficient proton pumping after sequential excitation by two photons.     

Crystal structure of the eukaryotic light-driven proton-pumping rhodopsin, Acetabularia rhodopsin II, from marine alga

Acetabularia rhodopsin (AR) is a rhodopsin from the marine plant Acetabularia acetabulum. The opsin-encoding gene from A. acetabulum, ARII, was cloned and found to be novel but homologous to that reported previously. ARII is a light-driven proton pump, as demonstrated by the existence of a photo-induced current through Xenopus oocytes expressing ARII. The photochemical reaction of ARII prepared by cell-free protein synthesis was similar to that of bacteriorhodopsin (BR), except for the lack of light-dark adaptation and the different proton release and uptake sequence. The crystal structure determined at 3.2 Å resolution is the first structure of a eukaryotic member of the microbial rhodopsin family. The structure of ARII is similar to that of BR. From the cytoplasmic side to the extracellular side of the proton transfer pathway in ARII, Asp92, a Schiff base, Asp207, Asp81, Arg78, Glu199, and Ser189 are arranged in positions similar to those of the corresponding residues directly involved in proton transfer by BR. The side-chain carboxyl group of Asp92 appears to interact with the sulfhydryl group of Cys218, which is unique to ARII and corresponds to Leu223 of BR and to Asp217 of Anabaena sensory rhodopsin. The orientation of the Arg78 side chain is opposite to the corresponding Arg82 of BR. The putative absence of water molecules around Glu199 and Arg78 may disrupt the formation of the low-barrier hydrogen bond at Glu199, resulting in the “late proton release”.     

Voltage- and pH-Dependent Changes in Vectoriality of Photocurrents Mediated by Wild-type and Mutant Proteorhodopsins upon Expression in Xenopus Oocytes

Proteorhodopsin (PR), a light-driven proton pump from marine proteobacteria, exhibits photocycle characteristics similar to bacteriorhodopsin (BR) at neutral pH, including an M-like photointermediate. However, at acidic pH, spectroscopic evidence for an M-like species was absent, and the vectoriality of proton pumping was inverted. To gain further insight into this unusual property, we examined the voltage dependence of stationary and laser flash-induced photocurrents of PR under different pH conditions upon expression in Xenopus oocytes. The current-voltage curves were linear under all conditions tested, and photocurrent reversal potentials distinctly depended on the pH gradient. PR mutants D97N and D97T exhibited transient and stationary inward currents already at neutral pH, showing that neutralization of the proton acceptor abolishes forward pumping and permits only inward proton transport. Mutation E108G, which disrupts the donor site for Schiff base (SB) reprotonation, resulted in largely reduced photocurrents, which could be strongly stimulated by azide, similar to previous observations on BR mutant D96G. When PR and BR photocurrents in response to blue or green laser flashes during or after continuous illumination were compared, direct electrical evidence for the occurrence of an M-like intermediate at neutral pH could only be obtained when reprotonation of the SB was slowed down by PR mutation E108G. For PR at acidic pH, laser flashes only produced inwardly directed photocurrents, independent from background illumination, thus precluding electrical identification of an M-like species. However, when visible absorption spectroscopy was carried out at low temperatures, occurrence of an M-like species was robustly observed at low pH. This indicates that SB deprotonation and reprotonation occur during the PR photocycle also at low pH. Our results corroborate the conclusion that in PR, the direction of proton pumping can be switched by changes in pH and membrane potential, with the protonation state of Asp-97 being the key determinant for selecting between transport modes.     

Photochemistry of Acetabularia rhodopsin II from a marine plant, Acetabularia acetabulum

Acetabularia rhodopsins are the first microbial rhodopsins discovered in a marine plant organism, Acetabularia acetabulum. Previously, we expressed Acetabularia rhodopsin II (ARII) by a cell-free system from one of two opsin genes in A. acetabulum cDNA and showed that ARII is a light-driven proton pump [Wada, T., et al. (2011) J. Mol. Biol. 411, 986-998]. In this study, the photochemistry of ARII was examined using the flash-photolysis technique, and data were analyzed using a sequential irreversible model. Five photochemically defined intermediates (P(i)) were sufficient to simulate the data. Noticeably, both P(3) and P(4) contain an equilibrium mixture of M, N, and O. Using a transparent indium tin oxide electrode, the photoinduced proton transfer was measured over a wide pH range. Analysis of the pH-dependent proton transfer allowed estimation of the pK(a) values of some amino acid residues. The estimated values were 2.6, 5.9 (or 6.3), 8.4, 9.3, 10.5, and 11.3. These values were assigned as the pK(a) of Asp81 (Asp85(BR)) in the dark, Asp92 (Asp96(BR)) at N, Glu199 (Glu204(BR)) at M, Glu199 in the dark, an undetermined proton-releasing residue at the release, and the pH to start denaturation, respectively. Following this analysis, the proton transfer of ARII is discussed.     

Purification of histidine tagged bacteriorhodopsin,pharaonis halorhodopsin and pharaonis sensory rhodopsin II functionally expressed in Escherichia coli

Bacteriorhodopsin (BR) from Halobacterium salinarum as well as halorhodopsin (pHR) and sensory rhodopsin II (pSRII) from Natronobacterium pharaonis were functionally expressed in E. coli using the method of Shimono et al. [FEBS Lett. (1997) 420, 54–56]. The histidine tagged proteins were purified with yields up to 1.0 mg/l cell culture and characterized by ESI mass spectrometry and their photocycle. The pSRII and pHR photocycles were indistinguishable from the wild type proteins. The BR photocycle was considerably prolonged. pSOII is located in the cytoplasmic membrane and the C-terminus is oriented towards the cytoplasm as determined by immunogold labelling.     

Two light-activated conductances in the eye of the green alga Volvox carteri

Photoreceptor currents of the multicellular green alga Volvox carteri were analyzed using a dissolver mutant. The photocurrents are restricted to the eyespot region of somatic cells. Photocurrents are detectable from intact cells and excised eyes. The rhodopsin action spectrum suggests that the currents are induced by Volvox rhodopsin. Flash-induced photocurrents are a composition of a fast Ca2+-carried current (PF) and a slower current (PS), which is carried by H+. PF is a high-intensity response that appears with a delay of less than 50 micros after flash. The stimulus-response curve of its initial rise is fit by a single exponential and parallels the rhodopsin bleaching. These two observations suggest that the responsible channel is closely connected to the rhodopsin, both forming a tight complex. At low flash energies PS is dominating. The current delay increases up to 10 ms, and the PS amplitude saturates when only a few percent of the rhodopsin is bleached. The data are in favor of a second signaling system, which includes a signal transducer mediating between rhodopsin and the channel. We present a model of how different modes of signal transduction are accomplished in this alga under different light conditions.     

两种状态细菌视紫红质光循环中间产物与pH的关系

本文主要用微机控制的毫秒级闪光动力学光谱仪研究含三体细菌视紫红质(Bacteriorhodopsin,简称BR)的紫膜碎片和含单体BR的DMPC(dimyristoyl-Phosphatidyl-choline)脂质囊泡在不同pH条件下光循环中间产物M_(412)和O_(640)的变化,研究结果表明:BR单体与其三体状态相比,BR单体的光循环中间产物M_(412)的产量受介质pH变化的影响较大,其慢衰减成份的衰减比三体BR慢3—10倍.说明单体BR的结构状态较易受PH影响,单体BR光循环中间产物O_(640)随pH变化的趋势与三体BR的有很大区别,可能是由于不同状态的BR受pH的影响,但其具有不同的构型,导致光循环途径的变化.     

FTIR analysis of the SII540 intermediate of sensory rhodopsin II: Asp73 is the Schiff base proton acceptor

Sensory rhodopsin II (SRII), a repellent phototaxis receptor found in Halobacterium salinarum, has several homologous residues which have been found to be important for the proper functioning of bacteriorhodopsin (BR), a light-driven proton pump. These include Asp73, which in the case of bacteriorhodopsin (Asp85) functions as the Schiff base counterion and proton acceptor. We analyzed the photocycles of both wild-type SRII and the mutant D73E, both reconstituted in Halobacterium salinarum lipids, using FTIR difference spectroscopy under conditions that favor accumulation of the O-like, photocycle intermediate, SII540. At both room temperature and -20 degrees C, the difference spectrum of SRII is similar to the BR-->O640 difference spectrum of BR, especially in the configurationally sensitive retinal fingerprint region. This indicates that SII540 has an all-trans chromophore similar to the O640 intermediate in BR. A positive band at 1761 cm-1 downshifts 40 cm-1 in the mutant D73E, confirming that Asp73 undergoes a protonation reaction and functions in analogy to Asp85 in BR as a Schiff base proton acceptor. Several other bands in the C=O stretching regions are identified which reflect protonation or hydrogen bonding changes of additional Asp and/or Glu residues. Intense bands in the amide I region indicate that a protein conformational change occurs in the late SRII photocycle which may be similar to the conformational changes that occur in the late BR photocycle. However, unlike BR, this conformational change does not reverse during formation of the O-like intermediate, and the peptide groups giving rise to these bands are partially accessible for hydrogen/deuterium exchange. Implications of these findings for the mechanism of SRII signal transduction are discussed.     

Actinic light and pH effect on the proton pumping of bacteriorhodopsin

The actinic light effect on the bacteriorhodopsin (BR) photocycle kinetics led to the assumption of a cooperative interaction between the photocycling BR molecules. In this paper we report the results of the actinic light effect and pH on the proton release and uptake kinetics. An electrical method is applied to detect proton release and uptake during the photocycle [E. Papp, G. Fricsovszky, J. Photochem. Photobiol. B: Biol. 5 (1990) 321]. The BR photocycle kinetics was also studied by absorption kinetics measurements at 410 nm and the data were analyzed by the local analysis of the M state kinetics [E. Papp, V.H. Ha, Biophys. Chem. 57 (1996) 155]. While at high pH and ionic strength, we found a similar behavior as reported earlier, at low ionic strength the light effect proved to be more complex. The main conclusions are the following: Though the number of BR excited to the photocycle (fraction cycling, fc) goes to saturation with increasing laser pulse energy, the absorbed energy by BR increases linearly with pulse energy. From the local analysis we conclude that the light effect changes the kinetics much earlier, already at the L intermediate state decay. The transient electric signal, caused by proton release and uptake, can be decomposed into two components similarly to the absorption kinetic data of the M intermediate state. The actinic light energy affects mainly the ratio of the two components and the proton movements inside BR while pH has an effect on the kinetics of the proton release and uptake groups at the membrane surface.     

Pathways of the rise and decay of the M photointermediate(s) of bacteriorhodopsin

The photocycle of bacteriorhodopsin (BR) was studied at alkaline pH with a gated multichannel analyzer, in order to understand the origins of kinetic complexities in the rise and decay of the M intermediate. The results indicate that the biphasic rise and decay kinetics are unrelated to a photoreaction of the N intermediate of the BR photocycle, proposed earlier by others [Kouyama et al. (1988) Biochemistry 27, 5855-5863]. Rather, under conditions where N did not accumulate in appreciable amounts (high pH, low salt concentration), they were accounted for by conventional kinetic schemes. These contained reversible interconversions, either M in equilibrium with N in one of two parallel photocycles or L in equilibrium with as well as M in equilibrium with N in a single photocycle. Monomeric BR also showed these kinetic complications. Conditions were then created where N accumulated in a photo steady state (high pH, high salt concentration, background illumination). The apparent increase in the proportion of the slow M decay component by the background illumination could be quantitatively accounted for with the single photocycle model, by the mixing of the relaxation of the background light induced photo steady state with the inherent kinetics of the photocycle. Postulating a new M intermediate which is produced by the photoreaction of N was neither necessary nor warranted by the data. The difference spectra suggested instead that absorption of light by N generates only one intermediate, observable between 100 ns and 1 ms, which absorbs near 610 nm. Thus, the photoreaction of N resembles in some respects that of BR containing 13-cis-retinal.     

Bacteriorhodopsin in ice. Accelerated proton transfer from the purple membrane surface

The photocycle and the proton pumping kinetics of bacteriorhodopsin, as well as the transfer rate of protons from the membrane surface into the aqueous bulk phase were examined for purple membranes in water and ice. In water, the optical pH indicator pyranine residing in the aqueous bulk phase monitors the H(+)-release later than the pH indicator fluorescein covalently linked to the extracellular surface of BR. In the frozen state, however, pyranine responds to the ejected H+ as fast as fluorescein attached to BR, demonstrating that the surface/bulk transfer is in ice no longer rate limiting. The pumped H+ appears at the extracellular surface during the transition of the photocycle intermediate L550 to the intermediate M412. The Arrhenius plot of the M formation rate suggests that the proton is translocated through the protein via an ice-like structure.     

Conformational changes in the photocycle of Anabaena sensory rhodopsin: absence of the Schiff base counterion protonation signal

Anabaena sensory rhodopsin (ASR) is a novel microbial rhodopsin recently discovered in the freshwater cyanobacterium Anabaena sp. PCC7120. This protein most likely functions as a photosensory receptor as do the related haloarchaeal sensory rhodopsins. However, unlike the archaeal pigments, which are tightly bound to their cognate membrane-embedded transducers, ASR interacts with a soluble cytoplasmic protein analogous to transducers of animal vertebrate rhodopsins. In this study, infrared spectroscopy was used to examine the molecular mechanism of photoactivation in ASR. Light adaptation of the pigment leads to a phototransformation of an all-trans/15-anti to 13-cis/15-syn retinylidene-containing species very similar in chromophore structural changes to those caused by dark adaptation in bacteriorhodopsin. Following 532 nm laser-pulsed excitation, the protein exhibits predominantly an all-trans retinylidene photocycle containing a deprotonated Schiff base species similar to those of other microbial rhodopsins such as bacteriorhodopsin, sensory rhodopsin II, and Neurospora rhodopsin. However, no changes are observed in the Schiff base counterion Asp-75, which remains unprotonated throughout the photocycle. This result along with other evidence indicates that the Schiff base proton release mechanism differs significantly from that of other known microbial rhodopsins, possibly because of the absence of a second carboxylate group at the ASR photoactive site. Several conformational changes are detected during the ASR photocycle including in the transmembrane helices E and G as indicated by hydrogen-bonding alterations of their native cysteine residues. In addition, similarly to animal vertebrate rhodopsin, perturbations of the polar head groups of lipid molecules are detected.     

Thermal motions in bacteriorhodopsin at different hydration levels studied by neutron scattering: correlation with kinetics and light-induced conformational changes.

Bacteriorhodopsin (BR) is a transmembrane protein in the purple membrane (PM) of Halobacterium salinarum. Its function as a light-driven proton pump is associated with a cycle of photointermediates which is strongly hydration-dependent. Using energy-resolved neutron scattering, we analyzed the thermal motions (in the nanosecond-to-picosecond time range) in PM at different hydration levels. Two main populations of motions were found that responded differently to water binding. Striking correlations appeared between these "fast" motions and the "slower" kinetic constants (in the millisecond time range) of relaxations and conformational changes occurring during the photocycle.     

pH dependence of light-driven proton pumping by an archaerhodopsin from Tibet: comparison with bacteriorhodopsin

The pH-dependence of photocycle of archaerhodopsin 4 (AR4) was examined, and the underlying proton pumping mechanism investigated. AR4 is a retinal-containing membrane protein isolated from a strain of halobacteria from a Tibetan salt lake. It acts as a light-driven proton pump like bacteriorhodopsin (BR). However, AR4 exhibits an "abnormal" feature--the time sequence of proton release and uptake is reversed at neutral pH. We show here that the temporal sequence of AR4 reversed to "normal"--proton release preceding proton uptake--when the pH is increased above 8.6. We estimated the pK(a) of the proton release complex (PRC) in the M-intermediate to be approximately 8.4, much higher than 5.7 of wide-type BR. The pH-dependence of the rate constant of M-formation shows that the pK(a) of PRC in the initial state of AR4 is approximately 10.4, whereas it is 9.7 in BR. Thus in AR4, the chromophore photoisomerization and subsequent proton transport from the Schiff base to Asp-85 is coupled to a decrease in the pK(a) of PRC from 10.4 to 8.4, which is 2 pK units less than in BR (4 units). This weakened coupling accounts for the lack of early proton release at neutral pH and the reversed time sequence of proton release and uptake in AR4. Nevertheless the PRC in AR4 effectively facilitates deprotonation of primary proton acceptor and recovery of initial state at neutral pH. We found also that all pK(a)s of the key amino acid residues in AR4 were elevated compared to those of BR.