A series of layered CeO1−xFxFeAs compounds with x=0 to 0.20 are synthesized by solid state reaction method. Similar to the LaOFeAs, the pure CeOFeAs shows a strong resistivity anomaly near 145 K, which was ascribed to the spin-density-wave instability. F-doping suppresses this instability and leads to the superconducting ground state. Most surprisingly, the superconducting transition temperature could reach as high as 41 K. The very high superconducting transition temperature strongly challenges the classic BCS theory based on the electron-phonon interaction. The very closeness of the superconducting phase to the spin-density-wave instability suggests that the magnetic fluctuations play a key role in the superconducting paring mechanism. The study also reveals that the Ce 4f electrons form local moments and ordered antiferromagnetically below 4 K, which could coexist with superconductivity.PACS numbers: 74.62.Bf, 74.25.Gz The recent discovery of superconductivity with transition temperature of 26 K in LaO 1−x F x FeAs system[1] has generated tremendous interest in the scientific community. Except for a relatively high transition temperature, the system displays many interesting properties. Among others, the presence of competing ordered ground states is one of the most interesting phenomena [2]. The pure LaOFeAs itself is not superconducting but shows an anomaly near 150 K in both resistivity and dc magnetic susceptibility.[1] This anomaly was shown to be caused by the spin-density-wave (SDW) instability.[2] Electrondoping by F suppresses the SDW instability and recovers the superconductivity. Here we show that similar competing orders exist in another rear-earth transition metal oxypnictide Ce(O 1−x F x )FeAs. Most surprisingly, the superconducting transition temperature in this system could reach as high as 41 K. Except for cuprate superconductors, T c in such iron-based compounds has already become the highest.The very high superconducting transition temperature has several important implications. First, the T c value has already reached the well-accepted limit value of classic BCS theory [3,4]. Considering the small carrier density and rather week electron-phonon coupling estimated from first-principle calculations [5,6], the observation result strongly challenges the BCS theory based on the electron-phonon interaction. Second, the rare-earth Cebased compounds usually show hybridization between localized f-electrons and itinerant electrons. This often leads to a strong enhancement of carrier effective mass at low temperature. Even for 4d transition metal oxypnictide with the same type of structure, a recent report indicates that the electronic specific heat coefficient of Ce-based CeORuP (γ=77 mJ/mol K 2 ) is 20 times higher than the value of La-based LaORuP (γ=3.9 mJ/mol K 2 ) [7]. The hybridization also tends to cause various ordered states at low temperature, like ferromagnetic (FM) or antiferromagnetic (AFM) ordering. Although superconducting state could occur in Ce-based materials, the superconducti...

The interplay between different ordered phases, such as superconducting, charge or spin ordered phases, is of central interest in condensed-matter physics. The very recent discovery of superconductivity with a remarkable Tc = 26 K in Fe-based oxypnictide La(O1−xFx)FeAs (see Kamihara Y. et al., J. Am. Chem. Soc., 130 (2008) 3296) is a surprise to the scientific community and has generated tremendous interest. The pure LaOFeAs itself is not superconducting but shows an anomaly near 150 K in both resistivity and dc magnetic susceptibility. Here we provide combined experimental and theoretical evidences showing that a spin-density-wave (SDW) state develops at low temperature, in association with electron Nematic order. The electron-doping by F suppresses the SDW instability and induces the superconductivity. Therefore, the La(O1−xFx)FeAs offers an exciting new system showing competing orders in layered compounds.

Nonlinear optical excitation of infrared active lattice vibrations has been shown to melt magnetic or orbital orders and to transform insulators into metals. In cuprates, this technique has been used to remove charge stripes and promote superconductivity, acting in a way opposite to static magnetic fields. Here, we show that excitation of large-amplitude apical oxygen distortions in the cuprate superconductor YBa2Cu3O6.5 promotes highly unconventional electronic properties. Below the superconducting transition temperature (Tc = 50 K) inter-bilayer coherence is transiently enhanced at the expense of intra-bilayer coupling. Strikingly, even above Tc a qualitatively similar effect is observed up to room temperature, with transient inter-bilayer coherence emerging from the incoherent ground state and similar transfer of spectral weight from high to low frequency. These observations are compatible with previous reports of an inhomogeneous normal state that retains important properties of a superconductor, in which light may be melting competing orders or dynamically synchronizing the interlayer phase. The transient redistribution of coherence discussed here could lead to new strategies to enhance superconductivity in steady state.

We report on a photoinduced transient state of YBa 2 Cu 2 O 6+δ in which transport perpendicular to the Cu-O planes becomes highly coherent. This effect is achieved by excitation with mid-infrared optical pulses, tuned to the resonant frequency of apical oxygen vibrations, which modulate both lattice and electronic properties. Below the superconducting transition temperature T c , the equilibrium signatures of superconducting interlayer coupling are enhanced. Most strikingly, the optical excitation induces a new reflectivity edge at higher frequency than the equilibrium Josephson plasma resonance, with a concomitant enhancement of the low-frequency imaginary conductivity σ 2 (ω). Above T c , the incoherent equilibrium conductivity becomes highly coherent, with the appearance of a reflectivity edge and a positive σ 2 (ω) that increases with decreasing frequency. These features are observed up to room temperature in YBa 2 Cu 2 O 6.45 and YBa 2 Cu 2 O 6.5. The data above T c can be fitted by hypothesizing that the light establishes a transient superconducting state over only a fraction of the solid, with a lifetime of a few picoseconds. Non-superconducting transport could also explain these observations, although one would have to assume transient carrier mobilities near 10 4 cm 2 /V sec at 100 K, with a density of charge carriers similar to the below-T c superfluid density. Our results are indicative of highly unconventional nonequilibrium physics and open new prospects for optical control of complex solids.

Plants of Artemisia annua produce artemisinin, a sesquiterpene lactone widely used in malaria treatment. Amorpha-4,11-diene synthase (ADS), a sesquiterpene synthase, and CYP71AV1, a P450 monooxygenase, are two key enzymes of the artemisinin biosynthesis pathway. Accumulation of artemisinin can be induced by the phytohormone jasmonate (JA). Here, we report the characterization of two JA-responsive AP2 family transcription factors--AaERF1 and AaERF2--from A. annua L. Both genes were highly expressed in inflorescences and strongly induced by JA. Yeast one-hybrid and electrophoretic mobility shift assay (EMSA) showed that they were able to bind to the CRTDREHVCBF2 (CBF2) and RAV1AAT (RAA) motifs present in both ADS and CYP71AV1 promoters. Transient expression of either AaERF1 or AaERF2 in tobacco induced the promoter activities of ADS or CYP71AV1, and the transgenic A. annua plants overexpressing either transcription factor showed elevated transcript levels of both ADS and CYP71AV1, resulting in increased accumulation of artemisinin and artemisinic acid. By contrast, the contents of these two metabolites were reduced in the RNAi transgenic lines in which expression of AaERF1 or AaERF2 was suppressed. These results demonstrate that AaERF1 and AaERF2 are two positive regulators of artemisinin biosynthesis and are of great value in genetic engineering of artemisinin production.

Cotton fibers elongate rapidly after initiation of elongation, eventually leading to the deposit of a large amount of cellulose. To reveal features of cotton fiber cells at the fast elongation and the secondary cell wall synthesis stages, we compared the respective transcriptomes and metabolite profiles. Comparative analysis of transcriptomes by cDNA array identified 633 genes that were differentially regulated during fiber development. Principal component analysis (PCA) using expressed genes as variables divided fiber samples into four groups, which are diagnostic of developmental stages. Similar grouping results are also found if we use non-polar or polar metabolites as variables for PCA of developing fibers. Auxin signaling, wall-loosening and lipid metabolism are highly active during fiber elongation, whereas cellulose biosynthesis is predominant and many other metabolic pathways are downregulated at the secondary cell wall synthesis stage. Transcript and metabolite profiles and enzyme activities are consistent in demonstrating a specialization process of cotton fiber development toward cellulose synthesis. These data demonstrate that cotton fiber cell at a certain stage has its own unique feature, and developmental stages of cotton fiber cells can be distinguished by their transcript and metabolite profiles. During the secondary cell wall synthesis stage, metabolic pathways are streamed into cellulose synthesis.

We performed optical spectroscopy measurement on single crystals of BaFe2As2 and SrFe2As2, the parent compounds of FeAs-based superconductors. Both are found to be quite metallic with fairly large plasma frequencies at high temperature. Upon entering the spin-density-wave state, the formation of partial energy gaps was clearly observed with the surprising presence of two different energy scales. A large part of the Drude component was removed by the gapping of Fermi surfaces. Meanwhile, the carrier scattering rate was even more dramatically reduced. We elaborate that the spin-density-wave instability is more likely to be driven by the Fermi surface nesting of itinerant electrons than a local-exchange mechanism.

Cuticle, including wax and cutin, is the barrier covering plant aerial organs and protecting the inner tissues. The Arabidopsis thaliana ATP-binding cassette (ABC) transporter CER5 (AtWBC12) has been identified as a wax exporter. In agreement with the latest report of another wax exporter, AtWBC11, here we show that atwbc11 mutants displayed organ fusions and stunted growth, and became vulnerable to chlorophyll leaching and toluidine blue staining. Chemical analysis showed that wax and cutin monomers were both reduced in the atwbc11 mutant. AtWBC11 was widely expressed in aerial organs. Interestingly, we found that the expression was light dependent, and the phytohormone ABA up-regulated AtWBC11 expression. We also found that while the AtWBC11 promoter had a broad pattern of activity, the expression was converted to epidermis specific when the reporter gene was fused to AtWBC11 cDNA. Furthermore, RNA blot analysis supported epidermis-specific expression of AtWBC11. Our results support that AtWBC11 is involved in cuticle development.