Light-driven Chloride Pump Research Articles

Light-driven chloride ion transport by halorhodopsin from Natronobacterium pharaonis. 1. The photochemical cycle.

The photochemical cycle of the light-driven chloride pump, halorhodopsin from N. pharaonis, is described by transient optical multichannel and single-wavelength spectroscopy in the visible, and in the infrared. Titration of a blue-shift of the absorption maximum upon addition of chloride describes a binding site with a KD of 1 mM. The reaction sequence after the all-trans to 13-cis photoisomerization of the retinal in this chloride binding form is itself dependent on chloride. At 2 M chloride it is described by the scheme: HR-->K<==>L<==>N-->HR that relaxes in a few milliseconds, and is very similar to the photocycle of bacteriorhodopsin under conditions where the retinal Schiff base cannot deprotonate. At lower chloride concentrations, e.g., 0.1 M, however, a red-shifted state termed O appears between N and HR, in equilibrium with N. The absorption spectra of K, L, N, and O are very similar to their counterparts in the bacteriorhodopsin photocycle. As in their equivalents in bacteriorhodopsin, in the N state the retinal is still 13-cis, but it is reisomerized in the O state to all-trans.

Light-driven chloride ion transport by halorhodopsin from Natronobacterium pharaonis. 2. Chloride release and uptake, protein conformation change, and thermodynamics.

The photocycle of the light-driven chloride pump, N. pharaonis halorhodopsin, is described by the scheme HR-->K--><==>L<==>N<==>O<==>HR'-->HR. From the chloride dependencies of the rate constants in this model we identify the N-->O and O-->HR' reactions as the steps where chloride release and uptake occur, respectively, during the transport. The dependencies of the rate constants on temperature describe a thermodynamic cycle in which enthalpy-entropy conversion occurs in the O-->HR' reaction. The dependencies of the rate constants on hydrostatic pressure indicate that a substantial volume decrease occurs at the L-->N reaction, a result of a large-scale conformational change. This is the opposite of the volume increase in the photocycle of the proton pump, bacteriorhodopsin, that is implicated in the access change of the active site during the transport and the passage of a proton from the cytoplasmic surface to the active site. The results together suggest a chloride transport mechanism, in which the equivalents of all the ion transfer steps in bacteriorhodopsin occur but in the reverse sense, so as to cause the extracellular-to-cytoplasmic translocation of a chloride ion instead of the cytoplasmic-to-extracellular transport of a proton.

The initial reaction dynamics of the light-driven chloride pump halorhodopsin

The light-induced dynamics of halorhodopsin has been studied by transient absorption spectroscopy with a time resolution better than 100 fs. Similar to the process known from bacteriorhodopsin a fast initial process with a time constant of 170 ± 70 fs occurs indicating motions of the retinal chromophore on the excited-state potential energy surface. The decay of the excited electronic state is biexponential with time constants of 1.5 ± 0.7 and 8.5 ± 1.5 ps. The formation of the first red-shifted ground-state photoproduct occurs on the same timescale. A qualitative model for the primary reactions is proposed, which explains the lower quantum yield Φ of about 0.3 in halorhodopsin compared to 0.6 in bacteriorhodopsin.

Photocycle of halorhodopsin from Halobacterium salinarium

The light-driven chloride pump, halorhodopsin, is a mixture containing all-trans and 13-cis retinal chromophores under both light and dark-adapted conditions and can exist in chloride-free and chloride-binding forms. To describe the photochemical cycle of the all-trans, chloride-binding state that is associated with the transport, and thereby initiate study of the chloride translocation mechanism, one must first dissect the contributions of these species to the measured spectral changes. We resolved the multiple photochemical reactions by determining flash-induced difference spectra and photocycle kinetics in halorhodopsin-containing membranes prepared from Halobacterium salinarium, with light- and dark-adapted samples at various chloride concentrations. The high expression of cloned halorhodopsin made it possible to do these measurements with unfractionated cell envelope membranes in which the chromophore is photostable not only in the presence of NaCl but also in the Na2SO4 solution used for reference. Careful examination of the flash-induced changes at selected wavelengths allowed separating the spectral changes into components and assigning them to the individual photocycles. According to the results, a substantial revision of the photocycle model for H. salinarium halorhodopsin, and its dependence on chloride, is required. The cycle of the all-trans chloride-binding form is described by the scheme, HR-hv-->K<==>L1<==>L2<==>N-->HR, where HR, K, L, and N designate halorhodopsin and its photointermediates. Unlike the earlier models, this is very similar to the photoreaction of bacteriorhodopsin when deprotonation of the Schiff base is prevented (e.g., at low pH or in the D85N mutant). Also unlike in the earlier models, no step in this photocycle was noticeably affected when the chloride concentration was varied between 20 mM and 2 M in an attempt to identify a chloride-binding reaction.

Three-dimensional structure of halorhodopsin at 7 A resolution.

Two-dimensional crystalline patches containing the light-driven chloride pump, halorhodopsin, appear to form spontaneously in the cell membrane of an overproducing strain of Halobacterium. The three-dimensional structure (space group p42(1)2, a = 102 A) has been analysed by electron cryo-microscopy of tilted specimens. The map shows that halorhodopsin (HR) has an arrangement of seven transmembrane helices similar to that found in the related proton pump bacteriohodopsin (BR). The orientation of the polypeptide framework of HR in the membrane is rotated by 3 degrees relative to BR about an axis in the plane and the intramolecular space between the helices BC FG, which line the cytoplasmic half channel, appears slightly larger in HR than in BR, as would be expected for a chloride channel. The crystals of HR were too small for electron diffraction analysis of tilted specimens, so both the amplitudes and the phases of the Fourier components were obtained from images. This required anisotropic scaling of the image amplitudes in addition to correction for the defocus phase contrast transfer function. The procedure of rescaling the data (in this case roughly equivalent to sharpening with a temperature factor of-490) to compensate for a variety of image and crystal defects may also prove useful in the analysis of other structures for which no prior knowledge of a homologous structure exists and for which only small crystals can be obtained.

Three-dimensional structure of halorhodopsin at 7 Å resolution

Two-dimensional crystalline patches containing the light-driven chloride pump, halorhodopsin, appear to form spontaneously in the cell membrane of an overproducing strain of Halobacterium. The three-dimensional structure (space group p4212, a = 102 Å) has been analysed by electron cryo-microscopy of tilted specimens. The map shows that halorhodopsin (HR) has an arrangement of seven transmembrane helices similar to that found in the related proton pump bacteriohodopsin (BR). The orientation of the polypeptide framework of HR in the membrane is rotated by 3° relative to BR about an axis in the plane and the intramolecular space between the helices BC FG, which line the cytoplasmic half channel, appears slightly larger in HR than in BR, as would be expected for a chloride channel. The crystals of HR were too small for electron diffraction analysis of tilted specimens, so both the amplitudes and the phases of the Fourier components were obtained from images. This required anisotropic scaling of the image amplitudes in addition to correction for the defocus phase contrast transfer function. The procedure of rescaling the data (in this case roughly equivalent to sharpening with a temperature factor of −490) to compensate for a variety of image and crystal defects may also prove useful in the analysis of other structures for which no prior knowledge of a homologous structure exists and for which only small crystals can be obtained.

A new anion-sensitive biosensor using an ion-sensitive field effect transistor and a light-driven chloride pump, halorhodopsin

A new biosensor sensitive to chloride anion using a light-driven chloride pump protein, halorhodopsin (hR), and an ion-sensitive field effect transistor (ISFET) has been developed. Membrane vesicles of halophilic bacteria containing hR were immobilized in the matrix of polyvinylbutyral resin on the surface of the ISFET. The gate voltage of this device changed in the min time scale under yellow light illumination. The response for chloride anion increased according to the increase of chloride anion concentration in the bulk aqueous phase. In the dark, the gate potential did not change even in the presence of chloride anion. These chloride-dependent gate potential changes of the hR-ISFET indicate that the chloride pumping by hR is active on the ISFET and that ISFET detects the light-dependent chloride transport by hR.

Anion-protein interactions during halorhodopsin pumping: halide binding at the protonated Schiff base.

Halorhodopsin (hR), the light-driven chloride pump of Halobacterium halobium, has been studied by Fourier transform infrared (FTIR) spectroscopy. Direct hydrogen bonding of halide ions with the protonated Schiff base (PSB) group was detected by means of halide-dependent perturbations on this group's vibrational frequencies. FTIR difference spectra were obtained of the hR-->hL photoreaction in reconstituted membrane vesicles. Nearly identical results were obtained using either low-temperature static difference spectroscopy at 1-cm-1 resolution or a stroboscopic time-resolved technique with 5-ms temporal and 2-cm-1 spectral resolution. The frequency of the negative difference band due to the PSB C = N stretch mode in the hR state shows a dependence on the type of halide counteranion that is present, 1632 cm-1 in the presence of Cl-, 1631 cm-1 in Br-, and 1629 cm-1 in I-. The C = NH+ stretch frequency thus correlates with the strength of the hydrogen bond formed by the halide. Analogous halide-dependent shifts of the C = NH+ frequency were observed in IR spectra of model compound retinylidene PSB salts. We also observed a significant halide dependence of the visible absorption maximum of hR solubilized in lauryl maltoside detergent. From such halide perturbation effects, we conclude that there is a direct hydrogen-bonded interaction between the Schiff base group and an externally supplied halide ion in the hR state. Halide perturbation effects are also observed for PSB-group vibrations in the hL state. Thus, despite an apparent overall weakening of hydrogen-bonding interactions of the PSB with its environment after chromophore photoisomerization to form hL, the PSB remains hydrogen-bonded to the halide. The results are best explained in terms of a "one-site, two-state" model for anion binding near the chromophore in the hR state, as opposed to a previously proposed two-site model.

Homologous overexpression of a light-driven anion pump in an archaebacterium.

The retinal protein halorhodopsin (HR), a light-driven chloride pump from Halobacterium halobium, was homologously overexpressed in this archaebacterium. Two DNA expression systems differing in their promoter region were investigated. The halopsin, hop, promoter coupled to the hop gene gave an increased level of HR synthesis. However, the extent of expression was driven by the copy number of the shuttle vector and did not reach the magnitude of the bacterio-opsin, bop, promoter system. Employing a gene fusion approach, the promoter for the bop gene was used to drive expression of the hop gene. A shuttle vector containing a bop-hop-cartridge was transformed into a HR-deficient strain and blueish-coloured transformants were obtained. The bop promoter expressed HR to an extent where a specific membrane fraction resembled the crystalline purple membrane of BR in terms of the lipid to protein ratio. HR could, therefore, be easily isolated in a natural membrane-bound state. This allows for direct use in biophysical studies without the application of detergents. This was the first successful overexpression of a 7-helical transmembrane protein and may be extended to other proteins of this family.

Light-driven proton or chloride pumping by halorhodopsin.

Halorhodopsin from Halobacterium halobium was purified and reconstituted with lipids from purple membranes. The resulting protein-containing membrane sheets were adsorbed to a planar lipid membrane and photoelectric properties were analyzed. Depending on light conditions, halorhodopsin acted either as a light-driven chloride pump or as a proton pump: green light caused chloride transport and additional blue light induced proton pumping. In the living cell, both to these vectorial processes would be directed toward the cytoplasm and, compared to ion transport by bacteriorhodopsin, this is an inversed proton flow. Azide, a catalyst for reversible deprotonation of halorhodopsin, enhanced proton transport, and the deprotonated Schiff base in the 13-cis configuration (H410) was identified as the key intermediate of this alternative catalytic cycle in halorhodopsin. While chloride transport in halorhodopsin is mediated by a one-photon process, proton transport requires the absorption of two photons: one photon for formation of H410 and release of a proton, and one photon for photoisomerization of H410 and re-formation of H578 with concomitant uptake of a proton by the Schiff base.

Anion binding to the chloride pump, halorhodopsin, and its implications for the transport mechanism

The light-driven chloride pump, halorhodopsin, binds and transports chloride across the membrane, and to a lesser extent nitrate. Binding and transport kinetics, and resonance Raman spectra of the retinal Schiff base, with these anions suggest the existence of two mutually exclusive binding sites. One of these may be the uptake site, and the other the release site during the transport. Plausible locations can be suggested for these sites, because halorhodopsin is a small protein with few buried positively charged residues, and the primary structure of a second pigment with similar function has recently become available for comparison.

The orientation of halorhodopsin in the cell membrane of halobacteria.

The orientation of the light-driven chloride pump, halorhodopsin, in the membrane was determined using antibodies directed against a synthetic peptide which represents the C-terminal segment of the protein. Antibodies against this decapeptide did not bind to right-side-out cell vesicles. Partial inversion by sonication or lysis under low salt conditions exposed this COOH-terminal antigenic site. Antibody binding was removed by preincubation with the decapeptide. The COOH terminus of the molecule is therefore located on the cytoplasmic surface of the membrane.

Fourier transform infrared study of the halorhodopsin chloride pump.

Halorhodopsin (hR) is a light-driven chloride pump located in the cell membrane of Halobacterium halobium. Fourier transform infrared difference spectroscopy has been used to study structural alterations occurring during the hR photocycle. The frequencies of peaks attributed to the retinylidene chromophore are similar to those observed in the spectra of the related protein bacteriorhodopsin (bR), indicating that in hR as in bR an all-trans----13-cis isomerization occurs during formation of the early bathoproduct. Spectral features due to protein structural alterations are also similar for the bR and hR photocycles. For example, formation of the red-shifted primary photoproducts of both hR and bR results in similar carboxyl peaks in the 1730-1745-cm-1 region. However, in contrast to bR, no further changes are observed in the carboxyl region during subsequent steps in the hR photocycle, indicating that additional carboxyl groups are not directly involved in chloride translocation. Overall, the close similarity of vibrations in hR and bR photoproduct difference spectra supports the existence of some common elements in the molecular mechanisms of energy transduction and active transport by these two proteins.

Structure and orientation of halorhodopsin in the membrane: a proteolytic fragmentation study.

Halorhodopsin (HR), the light-driven chloride pump in halobacteria, was digested with various proteolytic enzymes. As expected, carboxypeptidase A removed 14 amino acids from the C-terminal tail of detergent-solubilized HR, producing a fragment of 25.2 kd in size. Membrane-associated HR could be digested as well, but not in right-side-out sealed cell envelope vesicles. We conclude, therefore, that the orientation of HR in the cytoplasmic membrane is such that the C-terminal tail faces the cytoplasmic side. Tryptic digestion of detergent-solubilized HR resulted in the removal of the same C-terminal segment, but also in the production of two more cleavage products (molecular masses of 20.9 and 16.8 kd respectively). These cleavage sites were determined by amino acid sequencing of the newly produced N termini, and they turned out to be within interhelical loops in an earlier proposed structural model for HR. Incubation with chymotrypsin and thermolysin yielded different sites of cleavage, but also in regions which were proposed to be accessible on the surface of the protein. Since the results show that three of six proposed interhelical loop segments contain proteolytic digestion sites, they support the proposed structural model for HR.

The halo-opsin gene. I. Identification and isolation

Halorhodopsin (HR), the light-driven chloride pump in halobacteria, was purified in the denatured as well as in the native state and chemically cleaved into peptide fragments. Isolation of peptide and liquid phase sequencing yielded approximately 20% of the halo-opsin (HO) structure in non-overlapping peptides. Chemically synthesized oligodeoxynucleotides corresponding to a peptide sequence obtained from both HR preparations were used to screen a cosmid gene bank of Halobacterium halobium strain L-33. A positive clone contained cosmid pAB H47 which by subcloning and nucleotide sequencing was shown to encode at least part of the HO gene.

The halo-opsin gene. II. Sequence, primary structure of halorhodopsin and comparison with bacteriorhodopsin

The gene for the protein moiety of the light-driven chloride pump halorhodopsin (HR), hop gene, was sequenced and the primary structure of the protein derived thereof. The gene has a GC content of 67% and codes for 274 amino acids. A promoter structure, resembling that of the halobacterial 16S rRNA genes, is present and both a terminating stem and a loop sequence is found downstream of the TGA stop codon. A ribosomal binding site is located within the translated region. The HR protein moiety is processed at the amino terminus, as well as the carboxy terminus, yielding a dominant species of calculated Mr 26 961.

Trans-cis isomerization of retinal and a mechanism for ion translocation in halorhodopsin

The chromophore in halorhodopsin (HR) which acts as a light-driven chloride pump in halobacteria shares many properties with its counterpart in bacteriorhodopsin (BR): (i) a similar retinal protein interaction, (ii) trans to cis isomerization and (iii) similar intermediates of its photocycle. One major difference between the two chromoproteins is that the HR chromophore does not become deprotonated during its photocycle. A mechanism for the photocycle of HR is presented, which, in close analogy to an earlier proposed mechanism for BR, involves the sequence of all-trans → 13-cis, 14s-cis → 13-cis → all-trans isomerizations of the chromophore, a Schiff base of retinal. In contrast to the situation in BR the 13-cis, 14s-cis→13-cis isomerization is induced not by deprotonation of the retinal Schiff base chromophore but rather by the movement of an anion (Cl-) towards the protonated nitrogen of the Schiff's base. The suggested mechanism involves the Schiff base directly in the chloride translocation in halorhodopsin.

Primary and secondary chloride transport in Halobacterium halobium.

Chloride uptake in intact cells of Halobacterium halobium was characterized by rates of influx and efflux of 36Cl- under conditions of light, respiration, or both. Halobacterial mutant strains with and without retinal transport proteins allowed study of the effects of halorhodopsin and bacteriorhodopsin under illumination. Two structurally independent chloride transport systems could be distinguished: halorhodopsin, the already known light-driven chloride pump, and a newly described secondary uptake system, which was energized by respiration or by light via bacteriorhodopsin.

Photoactive retinal pigments in haloalkaliphilic bacteria.

Light-induced fast transient absorbance changes were detected by time-resolved spectroscopy in 38 of 51 haloalkaliphilic isolates from alkaline salt lakes in Kenya and the Wadi Natrun in Egypt. They indicate the presence of two retinal pigments, Pf and Ps, which undergo cyclic photoreactions with half-times of 2 ms and 500 ms respectively. Pf absorbs maximally near 580 nm and Ps near 500 nm. The pigments differ in their sensitivity to hydroxylamine and detergent bleaching and the photoreactions of Pf are strongly dependent on chloride concentration. Of the 38 pigment-containing strains, 29 possess both Pf and Ps, 9 possess only Ps. Inhibition of retinal synthesis with nicotine blocks pigment formation and addition of retinal restores it. Hydroxylamine-bleached pigments can be reconstituted with retinal or retinal analogues. Their similarity to the retinal pigments of Halobacterium halobium strongly suggests that they are also rhodopsin-like retinyledene proteins. Pf in all properties tested is almost identical to halorhodopsin, the light-driven chloride pump of H. halobium, and may serve the same function in the haloalkaliphiles. Ps has photocycle kinetics similar to sensory rhodopsin and a far-blue-shifted long-lived photocycle intermediate, but its ground state absorption maximum is near 500 nm instead of 587 nm. We have not found a bacteriorhodopsin-like pigment in the haloalkaliphiles.

Secondary structure of halorhodopsin.

Ultraviolet circular dichroism (CD) spectroscopy in the interval from 190 to 240 nm has been used to estimate the secondary structural content of halorhodopsin (hR), a light-driven chloride pump isolated from the membranes of Halobacterium halobium. Least-squares curve fitting of the CD spectrum for hR solubilized with octyl glucoside yields an alpha-helical content of approximately 50% and a beta-structure content of approximately 30%. The CD spectrum of hR is unaffected by the absence or presence of chloride ions or by the ionic strength of the medium. The CD spectrum of halorhodopsin is very similar to that of bacteriorhodopsin, indicating that these light-driven pumps possess nearly identical fractions of alpha- and beta-secondary structures.