The rate of Qx→Qy relaxation in bacteriochlorophylls of reaction centers from Rhodobacter sphaeroides determined by kinetics of the ultrafast carotenoid bandshift

Transient absorption changes induced by excitation of isolated reaction centers (RCs) from Rhodobacter sphaeroides with 600 nm laser pulses of 20 fs (full width at half maximum) were monitored in the wavelength region of 420–560 nm. The spectral features of the spectrum obtained are characteristic for an electrochromic band shift of the single carotenoid (Car) molecule spheroidene, which is an integral constituent of these RCs. This effect is assigned to an electrochromic bandshift of Car due to the local electric field of the dipole moment formed by electronic excitation of bacteriochlorophyll (BChl) molecule(s) in the neighborhood of Car. Based on the known distances between the pigments, the monomeric BChl (B_B) in the inactive B-branch is inferred to dominate this effect. The excitation of B_B at 600 nm leads to a transition into the S₂ state (Q_x band), which is followed by rapid internal conversion to the S₁ state (Q_y band), thus leading to a change of strength and orientation of the dipole moment, i.e., of the electric field acting on the Car molecule. Therefore, the time course of the electrochromic bandshift reflects the rate of the internal conversion from S₂ to S₁ of B_B. The evaluation of the kinetics leads to a value of 30 fs for this relaxation process. This article is part of a Special Issue entitled: Photosynthesis Research for Sustainability: from Natural to Artificial.     

Fast structural changes (200–900 ns) may prepare the photosynthetic manganese complex for oxidation by the adjacent tyrosine radical

The Mn complex of photosystem II (PSII) cycles through 4 semi-stable states (S₀ to S₃). Laser-flash excitation of PSII in the S₂ or S₃ state induces processes with time constants around 350 ns, which have been assigned previously to energetic relaxation of the oxidized tyrosine (Y_Z^ox). Herein we report monitoring of these processes in the time domain of hundreds of nanoseconds by photoacoustic (or ‘optoacoustic’) experiments involving pressure-wave detection after excitation of PSII membrane particles by ns-laser flashes. We find that specifically for excitation of PSII in the S₂ state, nuclear rearrangements are induced which amount to a contraction of PSII by at least 30 Å³ (time constant of 350 ns at 25 °C; activation energy of 285 +/? 50 meV). In the S₃ state, the 350-ns-contraction is about 5 times smaller whereas in S₀ and S₁, no volume changes are detectable in this time domain. It is proposed that the classical S₂ = > S₃ transition of the Mn complex is a multi-step process. The first step after Y_Z^ox formation involves a fast nuclear rearrangement of the Mn complex and its protein–water environment (~ 350 ns), which may serve a dual role: (1) The Mn‐ complex entity is prepared for the subsequent proton removal and electron transfer by formation of an intermediate state of specific (but still unknown) atomic structure. (2) Formation of the structural intermediate is associated (necessarily) with energetic relaxation and thus stabilization of Y_Z^ox so that energy losses by charge recombination with the Q_A^? anion radical are minimized. The intermediate formed within about 350 ns after Y_Z^ox formation in the S₂-state is discussed in the context of two recent models of the S₂ = > S₃ transition of the water oxidation cycle. This article is part of a Special Issue entitled: Photosynthesis Research for Sustainability: From Natural to Artificial.     

Synthesis,spectroscopic and redox properties of some ruthenium(II) thiosemicarbazone complexes: Structural description of four of these complexes

Sixteen neutral mixed ligand thiosemicarbazone complexes of ruthenium having general formula [Ru(PPh₃)₂L₂], where LH = 1-(arylidine)4-aryl thiosemicarbazones, have been synthesized and characterized. All complexes are diamagnetic and hence ruthenium is in the +2 oxidation state (low-spin d⁶, S = 0). The complexes show several intense peaks in the visible region due to allowed metal to ligand charge transfer transitions. The structures of four of the complexes have been determined by single-crystal X-ray diffraction and they show that thiosemicarbazone ligands coordinate to the ruthenium center through the hydrazinic nitrogen and sulfur forming four-membered chelate rings with ruthenium in N₂S₂P₂ coordination environment. In dichloromethane solution, the complexes show two quasi-reversible oxidative responses corresponding to loss of electron from HOMO and HOMO − 1. The E⁰ values of the above two oxidations shows good linear relationship with Hammett substituents constant (σ) as well as with the HOMO energy of the molecules calculated by the EHMO method. A DFT calculation on one representative complex suggests that there is appreciable contribution of the sulfur p-orbitals to the HOMO and HOMO − 1. Thus, assignment of the oxidation state of the metal in such complexes must be made with caution.     

Origin of magnetization tunneling in single-molecule magnets as determined by single-crystal high-frequency EPR

We review an extensive body of single-crystal high-frequency electron paramagnetic resonance (HFEPR) data in order to determine the transverse spin Hamiltonian parameters that control the tunneling of the direction of magnetization in a variety of integer and half-integer-spin single-molecule magnets (SMMs). The SMMs studied are members of the following families: S = 9/2 [Mn₄O₃Cl]⁶⁺; S = 5 [Mn₃NiO₄]⁶⁺; S = 6 [Mn₃ZnO₄]⁶⁺; and S = 4 [Ni₄(OR)₄]⁴⁺. HFEPR spectra for the half-integer S = 9/2 Mn₄ complexes that have C₃ symmetry do not provide measurable evidence for transverse spin Hamiltonian terms. This finding is consistent with the relatively large coercive field seen in the magnetization hysteresis loops for these complexes. On the other hand, a low symmetry S = 9/2 complex exhibits a much faster rate of ground-state magnetization tunneling, in agreement with HFEPR spectra for a powder sample that gives a rhombic zero-field splitting (ZFS) parameter of E = 0.140 cm^?1. The S = 5 Mn₃Ni systems exhibit magnetization tunneling that is much faster than seen for the high-symmetry S = 9/2 Mn₄ complexes. This can be attributed to their integer-spin ground states. Like the C₃ symmetry Mn₄ SMMs, the HFEPR spectra for high-symmetry Mn₃Ni complexes do not provide measurable evidence for transverse ZFS terms. However, the spectra exhibit broad peaks, suggesting distributions in the local molecular environments brought about by disordered solvate molecules. This disorder likely explains the fast tunneling in the high-symmetry S = 5 Mn₃Ni systems, though one cannot rule out fourth- (and higher-) order interactions that cannot be detected by HFEPR due to the broad resonances. The one S = 6 Mn₃Zn complex shows an even faster rate of tunneling compared to the isostructural S = 5 Mn₃Ni complex. Finally, the S = 4 [Ni(hmp)(dmb)Cl]₄ complex provides unique insights into the origin of fourth- (and higher-) order interactions found for many SMMs on the basis of analysis using a giant spin Hamiltonian (GSH) approximation. We conclude that the fourth-order anisotropy found for the S = 4 ground state of [Ni(hmp)(dmb)Cl]₄ originates from the second-order ZFS interactions associated with the individual Ni^II ions, but only as a result of higher-order processes that occur via S-mixing between the ground state and higher-lying (S < 4) spin-multiplets. The S-mixing is relatively strong in this system because of comparable exchange and anisotropy energy scales. The relatively fast tunneling is a direct consequence of this S-mixing, as opposed to any intrinsic fourth-order (spin–orbit) anisotropy associated with Ni^II.     

Design,synthesis, antiviral and cytostatic activity of ω-(1H-1,2,3-triazol-1-yl)(polyhydroxy)alkylphosphonates as acyclic nucleotide analogues

The efficient synthesis of a new series of polyhydroxylated dibenzyl ω-(1H-1,2,3-triazol-1-yl)alkylphosphonates as acyclic nucleotide analogues is described starting from dibenzyl ω-azido(polyhydroxy)alkylphosphonates and selected alkynes under microwave irradiation. Selected O,O-dibenzylphosphonate acyclonucleotides were transformed into the respective phosphonic acids. All compounds were evaluated in vitro for activity against a broad variety of DNA and RNA viruses and for cytostatic activity against murine leukemia L1210, human T-lymphocyte CEM and human cervix carcinoma HeLa cells. Compound (1S,2S)-16b exhibited antiviral activity against Influenza A H3N2 subtype (EC₅₀ = 20 μM—visual CPE score; EC₅₀ = 18 μM—MTS method; MCC >100 μM, CC₅₀ >100 μM) in Madin Darby canine kidney cell cultures (MDCK), and (1S,2S)-16k was active against vesicular stomatitis virus and respiratory syncytial virus in HeLa cells (EC₅₀ = 9 and 12 μM, respectively). Moreover, compound (1R,2S)-16l showed activity against both herpes simplex viruses (HSV-1, HSV-2) in HEL cell cultures (EC₅₀ = 2.9 and 4 μM, respectively) and feline herpes virus in CRFK cells (EC₅₀ = 4 μM) but at the same time it exhibited cytotoxicity toward uninfected cell (MCC ⩾ 4 μM). Several other compounds have been found to inhibit proliferation of L1210, CEM as well as HeLa cells with IC₅₀ in the 4–50 μM range. Among them compounds (1S,2S)- and (1R,2S)-16l were the most active (IC₅₀ in the 4–7 μM range).     

Excited state properties of dinaphthyl ditelluride

Di-1-naphthyl ditelluride (Te₂naphthyl₂) is characterized by two low-energy excited states. The corresponding electronic transitions nTe → σ¹ Te–Te and nTe → π¹ naphthyl CT give rise to absorptions at λ_max = 403 and 311 nm, respectively. In solution nTe → σ¹ excitation leads to the cleavage of the Te–Te bond. In contrast to Te₂naphthyl₂ in the dissolved state the solid compound shows a luminescence (λ_max = 576 nm) which originates from nTe → π¹ naphthyl CT triplet.     

Single-electron photoreduction of the PM intermediate of cytochrome c oxidase

The P_M → F transition of the catalytic cycle of cytochrome c oxidase from bovine heart was investigated using single-electron photoreduction and monitoring the subsequent events using spectroscopic and electometric techniques. The P_M state of the oxidase was generated by exposing the oxidized enzyme to CO plus O₂. Photoreduction results in rapid electron transfer from heme a to oxoferryl heme a₃ with a time constant of about 0.3 ms, as indicated by transients at 605 nm and 580 nm. This rate is ∼ 5-fold more rapid than the rate of electron transfer from heme a to heme a₃ in the F → O transition, but is significantly slower than formation of the F state from the P_R intermediate in the reaction of the fully reduced enzyme with O₂ to form state F (70–90 μs). The ∼ 0.3 ms P_M → F transition is coincident with a rapid photonic phase of transmembrane voltage generation, but a significant part of the voltage associated with the P_M → F transition is generated much later, with a time constant of 1.3 ms. In addition, the P_M → F transition of the R. sphaeroides oxidase was also measured and also was shown to have two phases of electrogenic proton transfer, with τ values of 0.18 and 0.85 ms.     

Design and synthesis of novel chloramphenicol amine derivatives as potent aminopeptidase N (APN/CD13) inhibitors

Herein we report a series of novel chloramphenicol amine derivatives as aminopeptidase N (APN)/CD13 inhibitors. All compounds were synthesized starting from commercially available (1S,2S)-2-amino-1-(4-nitrophenyl) propane-1,3-diol. The preliminary biological screening showed that some compounds exhibited potent inhibitory activity against APN. It should be noted that one compound, 13b (IC₅₀ = 7.1 μM), possess similar APN inhibitory activity compared with Bestatin (IC₅₀ = 3.0 μM).     

Synthesis and antioxidant evaluation of (S,S)- and (R,R)-secoisolariciresinol diglucosides (SDGs)

Secoisolariciresinol diglucosides (SDGs) (S,S)-SDG-1 (major isomer in flaxseed) and (R,R)-SDG-2 (minor isomer in flaxseed) were synthesized from vanillin via secoisolariciresinol (6) and glucosyl donor 7 through a concise route that involved chromatographic separation of diastereomeric diglucoside derivatives (S,S)-8 and (R,R)-9. Synthetic (S,S)-SDG-1 and (R,R)-SDG-2 exhibited potent antioxidant properties (EC₅₀ = 292.17 ± 27.71 μM and 331.94 ± 21.21 μM, respectively), which compared well with that of natural (S,S)-SDG-1 (EC₅₀ = 275.24 ± 13.15 μM). These values are significantly lower than those of ascorbic acid (EC₅₀ = 1129.32 ± 88.79 μM) and α-tocopherol (EC₅₀ = 944.62 ± 148.00 μM). Compounds (S,S)-SDG-1 and (R,R)-SDG-2 also demonstrated powerful scavenging activities against hydroxyl [natural (S,S)-SDG-1: 3.68 ± 0.27; synthetic (S,S)-SDG-1: 2.09 ± 0.16; synthetic (R,R)-SDG-2: 1.96 ± 0.27], peroxyl [natural (S,S)-SDG-1: 2.55 ± 0.11; synthetic (S,S)-SDG-1: 2.20 ± 0.10; synthetic (R,R)-SDG-2: 3.03 ± 0.04] and DPPH [natural (S,S)-SDG-1: EC₅₀ = 83.94 ± 2.80 μM; synthetic (S,S)-SDG-1: EC₅₀ = 157.54 ± 21.30 μM; synthetic (R,R)-SDG-2: EC₅₀ = 123.63 ± 8.67 μM] radicals. These results confirm previous studies with naturally occurring (S,S)-SDG-1 and establish both (S,S)-SDG-1 and (R,R)-SDG-2 as potent antioxidants and free radical scavengers for potential in vivo use.     

Action spectra of photosystems II and I and quantum yield of photosynthesis in leaves in State 1

The spectral global quantum yield (Y_II, electrons/photons absorbed) of photosystem II (PSII) was measured in sunflower leaves in State 1 using monochromatic light. The global quantum yield of PSI (Y_I) was measured using low-intensity monochromatic light flashes and the associated transmittance change at 810 nm. The 810-nm signal change was calibrated based on the number of electrons generated by PSII during the flash (4 · O₂ evolution) which arrived at the PSI donor side after a delay of 2 ms. The intrinsic quantum yield of PSI (y_I, electrons per photon absorbed by PSI) was measured at 712 nm, where photon absorption by PSII was small. The results were used to resolve the individual spectra of the excitation partitioning coefficients between PSI (a_I) and PSII (a_II) in leaves. For comparison, pigment–protein complexes for PSII and PSI were isolated, separated by sucrose density ultracentrifugation, and their optical density was measured. A good correlation was obtained for the spectral excitation partitioning coefficients measured by these different methods. The intrinsic yield of PSI was high (y_I = 0.88), but it absorbed only about 1/3 of quanta; consequently, about 2/3 of quanta were absorbed by PSII, but processed with the low intrinsic yield y_II = 0.63. In PSII, the quantum yield of charge separation was 0.89 as detected by variable fluorescence F_v/F_m, but 29% of separated charges recombined (Laisk A, Eichelmann H and Oja V, Photosynth. Res. 113, 145–155). At wavelengths less than 580 nm about 30% of excitation is absorbed by pigments poorly connected to either photosystem, most likely carotenoids bound in pigment–protein complexes.     

Structure–cytotoxic activity relationship of sesquilignan,morinol A

The cytotoxic activities of sesquilignans, (7S,8S,7′R,8′R)- and (7R,8R,7′S,8′S)-morinol A and (7S,8S,7′S,8′S)- and (7R,8R,7′R,8′R)-morinol B were compared, showing no significant difference between stereoisomers (IC₅₀ = 24–35 μM). As a next stage, the effect of substituents at 7, 7′, and 7″-aromatic ring on the activity was evaluated to find out the higher activity of (7S,8S,7′R,8′R)-7,7′,7″-phenyl derivative 18 (IC₅₀ = 6–7 μM). In the research on the structure–activity relationship of 7″-position of (7S,8S,7′R,8′R)-7,7′,7″-phenyl derivative 18, the most potent compounds were 7,7′,7″-phenyl derivative 18 (IC₅₀ = 6 μM) against HeLa cells. Against HL-60 cells, 7″-(4-nitrophenyl)-7,7′-phenyl derivative 33 and 7″-hexyl-7,7′-phenyl derivative 37 (IC₅₀ = 5 μM) showed highest activity. We discovered the compounds showed four to sevenfold potent activity than that of natural (7S,8S,7′R,8′R)-morinol A. It was also confirmed that the 7′-benzylic hydroxy group have an important role for exhibiting activity, on the other hand, the resonance system of cinnamyl structure is not crucial for the potent activity.     

Structural characterization of thermostable,solvent tolerant,cytosafe tannase from Bacillus subtilis PAB2

Tannase production by Bacillus subtilis PAB2, was investigated under solid state fermentation using tamarind seed as sole carbon source and it was found as the highest titer (73.44 U/gds). The enzyme was purified to homogeneity, which showed the molecular mass around 52 kDa (K_m = 0.445 mM, V_max = 125.8 mM/mg/min and K_cat = 2.88 min^–1). The enzyme was found stable in a range of pH (3.0–8.0) and temperature (30–70 °C) with an optimal activity at pH 5.0, pI of 4.4 and at 40 °C temperature. It exhibited half-life (t_1/2) of 4.5 h at 60 °C. The enzyme comprised a typical secondary structure containing α-helix (9.3%), β-pleated sheet (33.6%) and β-turn (17.2%). The native conformation of the enzyme was alike a 44 nm spherical nanoparticle upon aggregation. Thermodynamic parameters of tannase revealed that it was stable at 40 °C and showed Q₁₀, ΔG_d and ΔS_d values of 2.08, 99.37 KJ/mol and 252.38 J mol⁻¹ K⁻¹, respectively. Organic solvents were stimulatory with regard to enzyme activity. Moreover, the altered enzyme activity was determined to be correlated with the changes in structural conformation in presence of inducer and inhibitor. Tannase was explored to have no cytotoxicity on Vero cell line as well as rat model study.     

Structured near-infrared Magnetic Circular Dichroism spectra of the Mn4CaO5 cluster of PSII in T. vulcanus are dominated by Mn(IV) d-d ‘spin-flip’ transitions

Photosystem II passes through four metastable S-states in catalysing light-driven water oxidation. Variable temperature variable field (VTVH) Magnetic Circular Dichroism (MCD) spectra in PSII of Thermosynochococcus (T.) vulcanus for each S-state are reported. These spectra, along with assignments, provide a new window into the electronic and magnetic structure of Mn₄CaO₅. VTVH MCD spectra taken in the S₂ state provide a clear g = 2, S = 1/2 paramagnetic characteristic, which is entirely consistent with that known by EPR. The three features, seen as positive (+) at 749 nm, negative (?) at 773 nm and (+) at 808 nm are assigned as ⁴A → ²E spin-flips within the d³ configuration of the Mn(IV) centres present. This assignment is supported by comparison(s) to spin-flips seen in a range of Mn(IV) materials. S₃ exhibits a more intense (?) MCD peak at 764 nm and has a stronger MCD saturation characteristic. This S₃ MCD saturation behaviour can be accurately modelled using parameters taken directly from analyses of EPR spectra. We see no evidence for Mn(III) d-d absorption in the near-IR of any S-state. We suggest that Mn(IV)-based absorption may be responsible for the well-known near-IR induced changes induced in S₂ EPR spectra of T. vulcanus and not Mn(III)-based, as has been commonly assumed. Through an analysis of the nephelauxetic effect, the excitation energy of S-state dependent spin-flips seen may help identify coordination characteristics and changes at each Mn(IV). A prospectus as to what more detailed S-state dependent MCD studies promise to achieve is outlined.     

Hybrid fluorescent conjugates of COX-2 inhibitors: Search for a COX-2 isozyme imaging cancer biomarker

The observation that the cyclooxygenase-2 (COX-2) isozyme is over-expressed in multiple types of cancer, relative to that in adjacent non-cancerous tissue, prompted this investigation to prepare a group of hybrid fluorescent conjugates wherein the COX inhibitors ibuprofen, (S)-naproxen, acetyl salicylic acid, a chlororofecoxib analog and celecoxib were coupled via a linker group to an acridone, dansyl or rhodamine B fluorophore. Within this group of compounds, the ibuprofen-acridone conjugate (10) showed potent and selective COX-2 inhibition (COX-2 IC₅₀ = 0.67 μM; SI = 110.6), but its fluorescence emission (λ_em = 417, 440 nm) was not suitable for fluorescent imaging of cancer cells that over-express the COX-2 isozyme. In comparison, the celecoxib-dansyl conjugate (25) showed a slightly lower COX-2 potency and selectivity (COX-2 IC₅₀ = 1.1 μM; SI > 90) than the conjugate 10, and it possesses a better fluorescence emission (λ_em = 500 nm). Ultimately, a celecoxib-rhodamine B conjugate (28) that exhibited moderate COX-2 potency and selectivity (COX-2 IC₅₀ = 3.9 μM; SI > 25) having the best fluorescence emission (λ_em = 580 nm) emerged as the most promising biomarker for fluorescence imaging using a colon cancer cell line that over-expresses the COX-2 isozyme.     

Synthesis and characterization of a fluorescent probe for α-tocopherol suitable for fluorescence microscopy

Previously prepared fluorescent derivatives of α-tocopherol have shown tremendous utility in both in vitro exploration of the mechanism of ligand transfer by the α-tocopherol transfer protein (α-TTP) and the intracellular transport of α-tocopherol in cells and tissues. We report here the synthesis of a 4,4-difluoro-4-bora-3a,4a-diaza-s-indacene (BODIPY) containing α-tocopherol analog having extended conjugation with an alkenyl thiophene group that extends the absorption and emission maxima to longer wavelengths (λ_ex = 571 nm and λ_em = 583 nm). The final fluorophore thienyl-ene-BODIPY-α-tocopherol, 2, binds to recombinant human α-TTP with a K_d = 8.7 ± 1.1 nM and is a suitable probe for monitoring the secretion of α-tocopherol from cultured Mcf7#189 cells.     

Hyptenolide,a new α-pyrone with spasmolytic activity from Hyptis macrostachys

A new α-pyrone was isolated from aerial parts of Hyptis macrostachys Benth. Its structure was determined as 6R-[(5′S,6′S-diacetoxy)-1′Z,3′E-heptenyl]-5,6-dihydro-2H-pyran-2-one, named hyptenolide based on a combination of 1D and 2D NMR techniques and CD data. Hyptenolide inhibited the contractions induced by CCh (IC₅₀ = 1.7 ± 0.3 × 10⁻⁴ M) or histamine (IC₅₀ = 0.9 ± 0.05 × 10⁻⁴ M) in guinea pig ileum, demonstrating for the first time a pharmacological activity for the pyrone.     

Trispyrazolylmethane piano stool complexes of iron(II) and cobalt(II)

A series of cationic trispyrazolylmethane complexes of the general form [Tm^RM(CH₃CN)₃]²⁺ (Tm = tris(pyrazolyl)methane, 1, R = 3,5-Me₂, M = Fe(II); 2, R = 3-Ph, M = Fe(II); 3, R = 3,5-Me₂, M = Co(II); 4, R = 3-Ph, M = Co(II)) with ‘piano-stool’ structures was prepared by the reaction of the N₃tripodal ligands (Tm^R)with [(CH₃CN)₆M](BF₄)₂ in a 1:1 stoichiometric ratio. Magnetic susceptibility measurements indicate that all four complexes with BF₄⁻ counter anions are paramagnetic, high-spin systems in the solid state with μ_eff at high temperatures of 5.2 (1, S = 2), 5.4 (2, S = 2), 4.9 (3, S = 3/2) and 4.6 (4, S = 3/2) BM, respectively. Comparisons of bond lengths from the metal centre to the Tm^R nitrogen donors, and from the metal centre to the acetonitrile nitrogen donors indicate that the neutral tripodal ligands appear to be more weakly coordinated to the metal centre than are the acetonitrile ligands. Reactions of these tripodal complexes with bidentate phosphine ligands, such as 1,2-diphosphinoethane or 1,2-bis(diallylphosphino)ethane leads to displacement of the tripodal ligand, or to the formation of more thermally stable bis-ligand complexes M(Tm^R)₂ (R = 3,5-dimethyl).     

Diverse magnetic and electrical properties of molecular solids containing the thiazyl radical BDTA

We have examined the crystal structures and the electrical and magnetic properties of the molecular compounds of a thiazyl radical, 1,3,2-benzodithiazolyl (abbreviated as BDTA). BDTA was found to be a useful building block for molecular conductors and magnets because it can operate as a counter cation, a donor or a ligand, depending on its charge. (i) A charge-transfer complex, [BDTA][TCNQ], crystallizes into a uniform segregated stacking structure with a short contact between the donor and acceptor columns. In spite of the partial charge transfer between the two components, this complex exhibits semiconductive behaviour, probably due to a large electron correlation on BDTA. (ii) The crystal structure of [BDTA][Ni(mnt)₂] (mnt = maleonitriledithiolate) consists of alternating stacking columns of S = 0 [BDTA]⁺ and S = 1/2 [Ni(mnt)₂]^?, in which a ferromagnetic coupling operates between the [Ni(mnt)₂]^? anions through the [BDTA] ⁺ cation. (iii) [BDTA]₂[Cu(mnt)₂] consists of an alternating stack of a head-to-head [BDTA]⁺ dimer and a planar [Cu(mnt)₂]^2? dianion. Short intermolecular S?S contacts between the stacks give rise to an ideal 1D Heisenberg antiferromagnetic chain of [Cu(mnt)₂]^2? with a coupling constant of J/k_B = 16–17 K. (iv) The crystal structure of [BDTA]₂[Co(mnt)₂] is similar to that of [BDTA]₂[Cu(mnt)₂] at 253 K, but this salt undergoes a phase transition at 190 K, below which a partial electron transfer occurs from [Co(mnt)₂]^2? to one of the [BDTA]⁺ cations along with formation of a coordination bond. (v) [BDTA][Ni(dmit)₂]₂ (dmit = 1,3-dithiol-2-thione-4,5-dithiolate) exhibits room-temperature conductivity of 0.1 S cm^?1 and semiconductive behaviour over the range 80–200 K, which can be interpreted in terms of multi-conducting bands.     

The influence of starvation on fast-start performance of Spinibarbus sinensis

Juvenile Spinibarbus sinensis (n = 48, body length, 5.86 ± 0.10 cm, 25 °C) were fasted for 0, 0.5, 1, 2, 4 and 6 weeks. The fast-start performances of the experimental fish were assessed using high-speed video photography and the locomotive kinematics analysis. The morphological parameters including tail height (H₂), tail length (L₂), lateral body area (S₁), median fin area (S₂), dorsal cross section area (S₃) and tail cross section area (S₄) were also measured using TpsDig and the Photoshop. The results showed that 6 week starvation resulted in significant decreases in the escape distance (d), maximum linear velocity (V_max) and maximum linear acceleration (a_max) of center of mass in Stage 1 and Stage 2 of fast-start process (P < 0.05), however there were two relatively sTable phases in the V_max and d, during the week 1–2 (V_max = 0.67 ± 0.06 mm/ms; d = 8.86 ± 0.73 mm) and week 4–6 (V_max = 0.31 ± 0.04 mm/ms; d = 3.70 ± 0.56 mm). When compared with the control group (0 week starvation group), only the 6 week starvation group showed the significantly different response time (t) with average t = 9.20 ± 0.37 ms in week 1–4. There were no significant difference in mass center turning angles at first stage (T_a1) , second stage (T_a2) and the sum of two stages (T_a(1+2)) was also not different (P > 0.05). The fish did not show any directional preference for left or right during escape turning, and all of the related parameters also remained unchanged among treatment group (P > 0.05). The areas of dorsal body cross-section decreased more acutely (P < 0.05) than caudal body cross-section (45.4% vs 38.0%) during the entire starvation period while no significant differences were observed in both the tail height and tail length among all treatment groups (P > 0.05). The results indicated that fast-start performance of juvenile S. sinensis is affected by the starvation; metabolic energy related traits such as the maximum linear velocity and the maximum linear acceleration decreased significantly after starvation; whereas traits with no direct link to metabolic energy such as the response time and turning angle remained unchanged during starvation. The lack of starvation induced change in the maneuverability of the fish suggests that fast-start ability related to escape strategy is relatively well conservative in juvenile S. sinensis.     

Spirostanols from the roots and rhizomes of Trillium tschonoskii

Two novel spirostanols, (23S,24R,25S)-18-norspirost-1,4,13-triene-21,23,24-triol-3,15-dione (1) and (23S,24S,25S)-spirost-5-ene-1β,3β,21,23,24-pentaol (2), a new natural product (3), and two known analogues (4 and 5) were isolated from the ethyl acetate-soluble portion of the ethanolic extract of Trillium tschonoskii Maxim. Their structures were elucidated by extensive spectroscopic analyses, and their cytotoxic activities on four kinds of human tumor cells were studied in vitro. Compound 4 showed significant cytotoxic activity against MCF-7 and A549 with IC₅₀ values of 6.16 ± 2.21 and 28.5 ± 11.5 μM, respectively, while 5 exhibited selective cytotoxicity against A549 with an IC₅₀ value of 13.0 ± 4.51 μM.