Tracking Dark Excitons with Exciton Polaritons in Semiconductor Microcavities.

Dark excitons are of fundamental importance for a wide variety of processes in semiconductors but are difficult to investigate using optical techniques due to their weak interaction with light fields. We reveal and characterize dark excitons nonresonantly injected into a semiconductor microcavity structure containing InGaAs/GaAs quantum wells by a gated train of eight 100 fs pulses separated by 13 ns by monitoring their interactions with the bright lower polariton mode. We find a surprisingly long dark exciton lifetime of more than 20 ns, which is longer than the time delay between two consecutive pulses. This creates a memory effect that we clearly observe through the variation of the time-resolved transmission signal. We propose a rate equation model that provides a quantitative agreement with the experimental data.

Reaction rate and collisional efficiency of the rhodopsin-transducin system in intact retinal rods.

A model of transducin activation is constructed from its partial reactions (formation of metarhodopsin II, association, and dissociation of the rhodopsin-transducin complex). The kinetic equations of the model are solved both numerically and, for small photoactivation, analytically. From data on the partial reactions in vitro, rate and activation energy profile of amplified transducin turnover are modeled and compared with measured light-scattering signals of transducin activation in intact retinal rods. The data leave one free parameter, the rate of association between transducin and rhodopsin. Best fit is achieved for an activation energy of 35 kJ/mol, indicating lateral membrane diffusion of the proteins as its main determinant. The absolute value of the association rate is discussed in terms of the success of collisions to form the catalytic complex. It is greater than 30% for the intact retina and 10 times lower after permeabilization with staphylococcus aureus alpha-toxin. Dissociation rates for micromolar guanosinetriphosphale (GTP) (Kohl, B., and K. P. Hofmann, 1987. Biophys. J. 52:271-277) must be extrapolated linearly up to the millimolar range to explain the rapid transducin turnover in situ. This is interpreted by an unstable rhodopsin-transducin-GTP transient state. At the time of maximal turnover after a flash, the rate of activation is determined as 30, 120, 800, 2,500, and 4,000 activated transducins per photoactivated rhodopsin and second at 5, 10, 20, 30, 37 degrees C, respectively.

Effect of bleached rhodopsin on signal amplification in rod visual receptors.

Bleaching of rhodopsin markedly desensitizes the vertebrate visual system during a subsequent period of dark adaptation. Previous studies have indicated an origin of bleaching desensitization in the visual pigment itself, but have not identified the mechanism of action. A candidate for the site at which densensitization is initially expressed is the activation of transducin (formation of T*) on the rod disk membranes; this reaction directly involves rhodopsin in its photoactivated (R*) form and mediates initial amplification of the visual signal (reviewed in refs 7-9). We have analysed the effect of bleaching on the sensitivity of a flash-induced light-scattering signal known to monitor the disk-based amplifier, and which has been established as specifically monitoring transducin activation. We have recorded this signal from functioning retinal rods in situ ('ATR' signal) and find that bleaches inducing a pronounced, sustained loss in rod electrophysiological sensitivity do not alter the sensitivity of the ATR response after correction for reduced quantum catch. Our results indicate that the biochemical gain of the R*----T* transduction stage remains unchanged in the presence of bleached pigment and implicate a subsequent reaction as the first to show a sustained, bleaching-dependent gain reduction.

Displacement of rhodopsin by GDP from three-loop interaction with transducin depends critically on the diphosphate beta-position.

We have studied the effect of GDP and its analog guanyl-5'-yl thiophosphate (GDP beta S) on the interaction between rhodopsin and transducin (Gt). Stabilization of the light-induced active intermediate, metarhodopsin II (MII), by bound Gt (extra-MII effect) monitored the catalytic interaction between the proteins. Extra-MII can be completely abolished by GDP, with a half-suppression at 10 microM under the conditions (4 degrees C, pH 8, 7.5 nM photoactivated rhodopsin). The effect of GDP did not depend on divalent cations, in contrast to GTP-induced dissociation of the complex. The GDP analog GDP beta S did not affect extra-MII although it binds to the MII-Gt complex with only three times lower affinity (reversal of the GDP effect by GDP beta S). However, GDP beta S enhanced considerably the efficiency of synthetic rhodopsin peptide competition against the formation of extra-MII. GDP and GDP beta S slow the Gt activation rate (monitored by kinetic light scattering), with the same relative efficiencies. We therefore assume that GDP, GDP beta S, and GTP bind at the same site. We discuss a generalized induced fit mechanism, where MII induces opening of the Gt nucleotide site and release of GDP which in turn is obligatory to establish the MII-stabilizing rhodopsin-Gt three-loop interaction (König, B., Arendt, A., McDowell, J.H., Kahlert, M., Hargrave, P.A., and Hofmann, K.P. (1989) Proc. Natl. Acad. Sci. U.S.A. 86, 6878-6882). The GDP beta S/GDP difference is discussed in terms of bound GDP disturbing the interaction with two and GDP beta S with only one of the rhodopsin binding sites. Mechanistically, our results indicate a critical role of the beta-phosphate interaction with the nucleotide binding site in the GDP-induced transformation of Gt.

Photic modulation of a highly sensitive, near-infrared light-scattering signal recorded from intact retinal photoreceptors.

On stimulation by green flashes, the isolated, aspartate-treated bovine retina exhibits transient changes in the scattering of near-infrared (880 nm) light. A single component, termed the "ATR" (a flash-induced scattering signal, where ATR designates amplified transient-retina), dominates the amplitude and rising-phase kinetics of the initial peak of the light-scattering response. Superfusion with physiological solution containing low Na+ concentration reversibly abolishes the photoreceptor electroretinographic response but preserves the ATR signal, indicating a receptoral origin for the ATR. The increase of ATR amplitude (A/Amax) with flash intensity (R*/R, where R indicates rhodopsin) is described by A/Amax = (1- e-kR*/R), with R*/R = k-1 occurring on generation of approximately two photoactivated rhodopsins (R*s) per disc surface in the rod outer segment. Weak background light and bright flashes reversibly depress the ATR. Kinetic and sensitivity data suggest a basis of the ATR in stochastic, unit activation events, each initiated by a single R*. They further suggest an essential invariance of the unit event under differing conditions of illumination. A delay, apparently governed by the lifetime of a light-activated substance regulating ATR generation, precedes ATR recovery after a bright flash. The flash dependence of the delay period indicates an upper limit of 3 s for the lifetime of R* in the ATR-generating process. The unit event appears to be an R*-catalyzed and disc-localized reaction of phototransduction.

Three cytoplasmic loops of rhodopsin interact with transducin.

Rhodopsin is a member of an ancient class of receptors that transduce signals through their interaction with guanine nucleotide-binding proteins (G proteins). We have mapped the sites of interaction of rhodopsin with its G protein, which by analogy suggests how other members of this class of receptors may interact with their G proteins. Three regions of rhodopsin's cytoplasmic surface interact with the rod cell G protein transducin (Gt). These are (i) the second cytoplasmic loop, which connects rhodopsin helices III and IV, (ii) the third cytoplasmic loop, which connects rhodopsin helices V and VI, and (iii) a putative fourth cytoplasmic loop formed by amino acids 310-321, as the carboxyl-terminal sequence emerges from helix VII and anchors to the lipid bilayer via palmitoylcysteines 322 and 323. Evidence for these regions of interaction of rhodopsin and Gt comes from the ability of synthetic peptides comprising these regions to compete with metarhodopsin II for binding to Gt. A spectroscopic assay that measures the "extra MII" caused by Gt binding was used to measure the extent of binding of Gt in the presence of competing peptides. The three peptides corresponding to the second, third, and fourth cytoplasmic loops competed effectively with metarhodopsin II, exhibiting Kd values in the 2 microM range; 11 additional peptides comprising all remaining surface regions of rhodopsin failed to compete even at 200 microM. Any two peptides that were effective competitors showed a synergistic effect, having 15 times higher effectiveness when mixed than when assayed separately. A mathematical model was developed to describe this behavior.

Light-dependent delay in the falling phase of the retinal rod photoresponse.

Using suction electrodes, photocurrent responses to 100-ms saturating flashes were recorded from isolated retinal rods of the larval-stage tiger salamander (Ambystoma tigrinum). The delay period (Tc) that preceded recovery of the dark current by a criterion amount (3 pA) was analyzed in relation to the flash intensity (If), and to the corresponding fractional bleach (R*0/Rtot) of the visual pigment; R*0/Rtot was compared with R*s/Rtot, the fractional bleach at which the peak level of activated transducin approaches saturation. Over an approximately 8 ln unit range of I(f) that included the predicted value of R*s/Rtot, Tc increased linearly with ln I(f). Within the linear range, the slope of the function yielded an apparent exponential time constant (tau c) of 1.7 +/- 0.2 s (mean +/- S.D.). Background light reduced the value of Tc measured at a given flash intensity but preserved a range over which Tc increased linearly with ln I(f); the linear-range slope was similar to that measured in the absence of background light. The intensity dependence of Tc resembles that of a delay (Td) seen in light-scattering experiments on bovine retinas, which describes the period of essentially complete activation of transducin following a bright flash; the slope of the function relating Td and ln flash intensity is thought to reflect the lifetime of photoactivated visual pigment (R*) (Pepperberg et al., 1988; Kahlert et al., 1990). The present data suggest that the electrophysiological delay has a similar basis in the deactivation kinetics of R*, and that tau c represents TR*, the lifetime of R* in the phototransduction process. The results furthermore suggest a preservation of the "dark-adapted" value of TR* within the investigated range of background intensity.