Third-order implementation and convergence of the strong-property-fluctuation theory in electromagnetic homogenization.

The strong-property-fluctuation theory (SPFT) has been widely applied under the second-order approximation (also known as the bilocal approximation) to estimate the constitutive properties of effectively homogeneous composite mediums. A third-order mass operator approximation is developed here. The convergence of the long-wavelength, bilocally-approximated SPFT is demonstrated for isotropic chiral composite mediums, as well as for chiroferrite composite mediums.

Signalling properties of an HIV-encoded angiogenic peptide mimicking vascular endothelial growth factor activity.

HIV-1 expresses a multifunctional protein called TAT (trans-acting transcriptional activator), the function of which in vivo is tightly correlated with the incidence of Kaposi's sarcoma in AIDS patients. TAT is angiogenic and apparently binds to receptors specific for vascular endothelial growth factor (VEGF). Amino acids 46-60 of HIV-TAT, known as the basic peptide, have been shown to be responsible for its functional interaction with VEGF receptors. To characterize further the binding properties of this peptide, its coding sequence was fused to the reading frame of bacterial thioredoxin, allowing the production of large amounts of chimaeric polypeptides in bacteria in a biologically active form. Binding of chimaeric proteins to VEGF receptors was studied in vitro in endothelial cell cultures expressing either of the two receptors. Chimaeric thioredoxin proteins carrying the basic domain of TAT bound to both VEGF receptors with affinities similar to those of HIV-TAT or VEGF. Interestingly, these polypeptides competed only partially with VEGF for receptor binding, implying different binding sites for the TAT peptide and VEGF. This suggests that TAT binds VEGF receptors at new sites that might be useful targets for pharmacological intervention during pathological angiogenesis. The thioredoxin/basic-peptide chimaeras are functional agonists that mediate VEGF receptor signalling: (1) they stimulate the growth of endothelial cells; (2) together with basic fibroblast growth factor they cause tube formation of endothelial cells in collagen gels; (3) they induce blood vessel formation on the chicken chorioallantoic membrane; and (4) they activate VEGF receptor kinase and mitogen-activated protein kinase activity.

Comment on "Rigorous solution for transient propagation of electromagnetic waves through a medium: causality plus diffraction in time".

In a previous Letter [Opt. Lett. 25, 995 (2000)], Xiao claimed to have found a "rigorous solution for transient propagation of electromagnetic waves through a medium." We show that Xiao's results apply strictly only to vacuum, which serves as a reference medium in classical electromagnetics.

Vascular endothelial growth factor (VEGF) and its receptors in tumor-bearing dogs.

The molecular biology of the angiogenic growth factor, vascular endothelial growth factor (VEGF), has been studied in the dog. All major isoforms of VEGF are present in the dog. The amino acid sequences are identical between human and dog in the loop regions that are responsible for receptor binding. Accordingly, the VEGF receptors of dogs and humans are very similar and permit functional exchange of the growth factor. Here we show that canine VEGF activates human endothelial cells to the same extent as human VEGF. Similarly, the two proteins display identical cell binding properties. The VEGF receptor 1 (Flt-1) shows the same alternative splicing in humans and dogs and is overexpressed in the majority of tumors in both species. VEGF occurs also in canine tumors in similar relative quantities as in human malignancies. Based on the literature and our study we suggest that the molecular biology and the function of the VEGF signaling system are virtually identical in humans and canines and in healthy as well as in disease conditions.

Identification of the Bradyrhizobium japonicum degP gene as part of an operon containing small heat-shock protein genes.

A degP (htrA)-like gene of Bradyrhizobium japonicum was identified immediately downstream of two genes (hspB and hspC) coding for small heat-shock proteins. All three genes are oriented in the same direction and are separated by only 85 and 72 bp, and a heat-inducible transcript covering hspB, hspC, and degP was detected by RT-PCR. These results show that the genes are organized in an operon. Two mutants, a degP insertion mutant and a DeltahspBCdegP mutant, were constructed by marker replacement mutagenesis. Immunoblot analysis performed with a serum raised against the amino-terminal end of IbpA, an HspB homolog of Escherichia coli, identified three heat-inducible protein bands in B. japonicum extract, one of which was missing in the deletion mutant. None of the mutants showed an obvious defect during growth at different temperatures, after heat-shock treatment, or in the presence of solvents. Moreover, they were not affected in root-nodule symbiosis, indicating that the small heat-shock proteins HspB and HspC and the DegP homolog of B. japonicum are not required under a wide range of growth conditions.

The Bradyrhizobium japonicum rpoH1 gene encoding a sigma 32-like protein is part of a unique heat shock gene cluster together with groESL1 and three small heat shock genes.

The heat shock response of Bradyrhizobium japonicum is controlled by a complex network involving two known regulatory systems. While some heat shock genes are controlled by a highly conserved inverted-repeat structure (CIRCE), others depend on a sigma 32-type heat shock sigma factor. Using Western blot (immunoblot) analysis, we confirmed the presence of a sigma 32-like protein in B. japonicum and defined its induction pattern after heat shock. A B. japonicum rpoH-like gene (rpoH1) was cloned by complementation of an Escherichia coli strain lacking sigma 32. A knockout mutation in rpoH1 did not abolish sigma 32 production in B. japonicum, and the rpoH1 mutant showed the wild-type growth phenotype, suggesting the presence of multiple rpoH homologs in this bacterium. Further characterization of the rpoH1 gene region revealed that the rpoH1 gene is located in a heat shock gene cluster together with the previously characterized groESL1 operon and three genes encoding small heat shock proteins in the following arrangement: groES1, groEL1, hspA, rpoH1, hspB, and hspC. Three heat-inducible promoters are responsible for transcription of the six genes as three bicistronic operons. A sigma 32-dependent promoter has previously been described upstream of the groESL1 operon. Although the hspA-rpoH1 and hspBC operons were clearly heat inducible, they were preceded by sigma 70-like promoters. Interestingly, a stretch of about 100 bp between the transcription start site and the start codon of the first gene in each of these two operons was nearly identical, making it a candidate for a regulatory element potentially allowing heat shock induction of sigma 70-dependent promoters.

Dielectric polarizability of a sphere with arbitrary anisotropy: comment.

Sihvola's observation [Sihvola, Opt. Lett. 19, 430 (1994)] of an analogy between various elements of the polarizability dyadics for anisotropic spheres and the polarizabilities of chiral spheres is critically examined. It is argued that this analogy is both physically and mathematically misconceived.