Phytoremediation of multiple persistent pollutants co-contaminated soil by HhSSB transformed plant

The high toxicity of persistent pollutants limits the phytoremediation of pollutants-contaminated soil. In this study, heterologous expressing Halorhodospira halophila single-stranded DNA binding protein gene (HhSSB) improves tolerance to 2,4,6-trinitrotoluene (TNT), 2,4,6-trichlorophenol (2,4,6-TCP), and thiocyanate (SCN^-) in A. thaliana and tall fescue (Festuca arundinacea). The HhSSB transformed Arabidopsis, and tall fescue also exhibited enhanced phytoremediation of TNT, 2,4,6-TCP, and SCN^- separately contaminated soil and co-contaminated soil compared to control plants. TNT assay was selected to explore the mechanism of how HhSSB enhances the phytoremediation of persistent pollutants. Our result indicates that HhSSB enhances the phytoremediation of TNT by enhancing the transformation of TNT in Arabidopsis. Moreover, transcriptomics and comet analysis revealed that HhSSB improves TNT tolerance through three pathways: strengthening the defense system, enhancing the ROS scavenging system, and reducing DNA damage. These results presented here would be particularly useful for further studies in the remediation of soil contaminated by organic and inorganic pollutants.

Noncanonical Photocycle Initiation Dynamics of the Photoactive Yellow Protein (PYP) Domain of the PYP-Phytochrome-Related (Ppr) Photoreceptor

The photoactive yellow protein (PYP) from Halorhodospira halophila (Hhal) is a bacterial photoreceptor and model system for exploring functional protein dynamics. We report ultrafast spectroscopy experiments that probe photocycle initiation dynamics in the PYP domain from the multidomain PYP-phytochrome-related photoreceptor from Rhodospirillum centenum (Rcen). As with Hhal PYP, Rcen PYP exhibits similar excited-state dynamics; in contrast, Rcen PYP exhibits altered photoproduct ground-state dynamics in which the primary I₀ intermediate as observed in Hhal PYP is absent. This property is attributed to a tighter, more sterically constrained binding pocket around the p-coumaric acid chromophore due to a change in the Rcen PYP protein structure that places Phe98 instead of Met100 in contact with the chromophore. Hence, the I₀ state is not a necessary step for the initiation of productive PYP photocycles and the ubiquitously studied Hhal PYP may not be representative of the broader PYP family of photodynamics.

(1)H, (13)C, and (15)N resonance assignment of photoactive yellow protein

Photoactive yellow protein (PYP) is involved in the negative phototactic response towards blue light of the bacterium Halorhodospira halophila. Here, we report nearly complete backbone and side chain (1)H, (13)C and (15)N resonance assignments at pH 5.8 and 20 °C of PYP in its electronic ground state.

Vibrational assignment of the 4-hydroxycinnamyl chromophore in photoactive yellow protein

Photoactive yellow protein (PYP) is a bacterial photoreceptor containing a 4-hydroxycinnamyl chromophore. We report the Raman spectra for the dark state of PYP whose chromophore is isotopically labeled with 13C at the carbonyl carbon atom or at the ring carbon atoms. Spectra have been also measured with PYP in D2O where the exchangeable protons are deuterated. Most of the observed Raman bands are assigned on the basis of the observed isotope shifts and normal mode calculations using a density functional theory. We discuss the implication for the analysis of the infrared spectra of PYP. The comprehensive assignment provides a satisfactory framework for future investigations of the photocycle mechanism in PYP by vibrational spectroscopy.

Photoreversal kinetics of the I1 and I2 intermediates in the photocycle of photoactive yellow protein by double flash experiments with variable time delay

We investigated the kinetics of photoreversal from the I(1) and I(2) intermediates of photoactive yellow protein (PYP) by time-resolved optical absorption spectroscopy with double flash excitation. A first flash, at 430 nm, initiated the photocycle. After a variable time delay, the I(1) intermediate was photoreversed by a second flash, at 500 nm, or a mixture of I(2) and I(2)' intermediates was photoreversed by a second flash, at 355 nm. By varying the delay from 1 micros to 3 s, we were able to selectively excite the intermediates I(1), I(2), and I(2)'. The photoreversal kinetics of I(2) and I(2)' at 21 different delays and two wavelengths (340 and 450 nm) required two exponentials for a global fit with time constants of tau(1) = 57 +/- 5 micros and tau(2) = 380 +/- 40 micros (pH 6, 20 degrees C). These were assigned to photoreversal from sequential I(2) and I(2)' intermediates, respectively. The good agreement of the delay dependence of the two amplitudes, A(1) and A(2), with the time dependence of the I(2) and I(2)' populations provided strong evidence for the sequential model. The persistence of A(1) beyond delay times of 5 ms and its decay, together with A(2) around 500 ms, suggest moreover that I(2) and I(2)' are in thermal equilibrium. The wavelength dependence of the photoreversal kinetics was measured at 26 wavelengths from 510 to 330 nm at the two fixed delays of 1 and 10 ms. These data also required two exponentials for a global fit with tau(1) = 59 +/- 5 micros and tau(2) = 400 +/- 40 micros, in good agreement with the delay results. Photoreversal from I(2)' is slower than from I(2), since, in addition to chromophore protonation, the global conformational change has to be reversed. Our data thus provide a first estimate of about 59 micros for deprotonation and 400 micros for the structural change, which also occurs in the thermal decay of the signaling state but is obscured there since reisomerization is rate-limiting. The first step in photoreversal is rapid cis-trans isomerization of the chromophore, which we could not resolve, but which was detected by the instantaneous increase in absorbance between 330 and 380 nm. In agreement with this observation, the spectrum of the I(2)'(trans) intermediate, derived from the A(2) amplitude spectrum, has a much larger extinction coefficient than the spectrum of the I(2)'(cis) intermediate. With a first flash, at 430 nm, and a second flash, at 500 nm, we observed efficient photoreversal of the I(1) intermediate at a delay of 20 micros when most molecules in the cycle are in I(1). We conclude that each of the three intermediates studied can be reversed by a laser flash. Depending on the progression of the photocycle, reversal becomes slower with the time delay, thus mirroring the individual steps of the forward photocycle.

Low-temperature Fourier transform infrared spectroscopy of photoactive yellow protein

The photocycle intermediates of photoactive yellow protein (PYP) were characterized by low-temperature Fourier transform infrared spectroscopy. The difference FTIR spectra of PYP(B), PYP(H), PYP(L), and PYP(M) minus PYP were measured under the irradiation condition determined by UV-visible spectroscopy. Although the chromophore bands of PYP(B) were weak, intense sharp bands complementary to the 1163-cm(-1) band of PYP, which show the chromophore is deprotonated, were observed at 1168-1169 cm(-1) for PYP(H) and PYP(L), indicating that the proton at Glu46 is not transferred before formation of PYP(M). Free trans-p-coumaric acid had a 1294-cm(-1) band, which was shifted to 1288 cm(-1) in the cis form. All the difference FTIR spectra obtained had the pair of bands corresponding to them, indicating that all the intermediates have the chromophore in the cis configuration. The characteristic vibrational modes at 1020-960 cm(-1) distinguished the intermediates. Because these modes were shifted by deuterium-labeling at the ethylene bond of the chromophore while labeling at the phenol part had no effect, they were attributed to the ethylene bond region. Hence, structural differences among the intermediates are present in this region. Bands at about 1730 cm(-1), which show that Glu46 is protonated, were observed for all intermediates except for PYP(M). Because the frequency of this mode was constant in PYP(B), PYP(H), and PYP(L), the environment of Glu46 is conserved in these intermediates. The photocycle of PYP would therefore proceed by changing the structure of the twisted ethylene bond of the chromophore.

The role of the N-terminal domain of photoactive yellow protein in the transient partial unfolding during signalling state formation

It is shown that the N-terminal domain of photoactive yellow protein (PYP), which appears relatively independently folded in the ground state of the protein, plays a key role in the transient unfolding during signalling state formation: genetic truncation of the N-terminal domain of PYP significantly decreases the extent of cooperativity of the titration curve that describes chromophore protonation in the ground state of PYP, which is in agreement with the notion that the N-terminal domain is linked through a hydrogen-bonding network with the chromophore-containing domain of the protein. Furthermore, deletion of the N-terminal domain completely abolishes the non-linearity of the Arrhenius plot of the rate of ground state recovery.

Probing the nature of the blue-shifted intermediate of photoactive yellow protein in solution by NMR: hydrogen-deuterium exchange data and pH studies

The nature of the pB intermediate of photoactive yellow protein (PYP) from Ectothiorhodospira halophila has been probed by NMR. pH-dependent changes in the NMR spectrum of the dark state of PYP are shown to closely mimic exchange broadening effects observed previously in the NMR spectrum of the pB intermediate in solution. Amide H-D exchange data show that while pB retains a solid protected core, two regions become significantly less protected than the dark state. The amide exchange data help to rationalize why the conformational exchange process affects the N-terminal 28-residue segment of the protein, which is not close to the site of chromophore rearrangement. At very low pH (pH 1.7), the dark state NMR spectrum displays approximately 30 very sharp signals, which are characteristic of a portion of the molecule becoming unfolded. Similarities between the dark state spectra at pH approximately 3.2 and the spectra of pB suggest a model for pB in solution where the protein exists in an equilibrium between a well-ordered state and a state in which a region is unfolded. Such a two-state model accounts for the exchange phenomena observed in the NMR spectra of pB, and the hydrophobic exposure and lability inferred from thermodynamic data. It is likely that in the crystalline environment the ordered form of pB is strongly favored.