Singularities in the optical response of cuprates

We argue that the detailed analysis of the optical response in cuprate superconductors allows one to verify the magnetic scenario of superconductivity in cuprates, as for strong coupling charge carriers to antiferromagnetic spin fluctuations, the second derivative of optical conductivity should contain detectable singularities at $2\Delta +\Delta_{\rm spin}$, $4\Delta$, and $2\Delta+2\Delta_{\rm spin}$, where $\Delta$ is the amplitude of the superconducting gap, and $\Delta_{s}$ is the resonance energy of spin fluctuations measured in neutron scattering. We argue that there is a good chance that these singularities have already been detected in the experiments on optimally doped $YBCO$.Comment: 6 pages, 4 figure

Rapid selection of BRCA1-proficient tumor cells during neoadjuvant therapy for ovarian cancer in BRCA1 mutation carriers

Ovarian carcinomas (OC) often demonstrate rapid tumor shrinkage upon neoadjuvant chemotherapy (NACT). However, complete pathologic responses are very rare and the mechanisms underlying the emergence of residual tumor disease remain elusive. We hypothesized that the change of somatic BRCA1 status may contribute to this process. The loss-of-heterozygosity (LOH) at the BRCA1 locus was determined for 23 paired tumor samples obtained from BRCA1 germ-line mutation carriers before and after NACT. We observed a somatic loss of the wild-type BRCAI allele in 74% (17/23) of OCs before NACT. However, a retention of the wild-type BRCA1 copy resulting in a reversion of LOH status was detected in 65% (11/17) of those patients after NACT. Furthermore, we tested 3 of these reversion samples for LOH at intragenic BRCA1single nucleotide polymorphisms (SNPs) and confirmed a complete restoration of the SNP heterozygosity in all instances. The neoadjuvant chemotherapy for BRCA1-associated OC is accompanied by a rapid expansion of pre-existing BRCA1-proficient tumor clones suggesting that continuation of the same therapy after NACT and surgery may not be justified even in patients initially experiencing a rapid tumor regression. (C) 2017 Elsevier B.V. All rights reserved.Peer reviewe

The YABBY Genes of Leaf and Leaf-Like Organ Polarity in Leafless Plant Monotropa hypopitys

Monotropa hypopitys is a mycoheterotrophic, nonphotosynthetic plant acquiring nutrients from the roots of autotrophic trees through mycorrhizal symbiosis, and, similar to other extant plants, forming asymmetrical lateral organs during development. The members of the YABBY family of transcription factors are important players in the establishment of leaf and leaf-like organ polarity in plants. This is the first report on the identification of YABBY genes in a mycoheterotrophic plant devoid of aboveground vegetative organs. Seven M. hypopitys YABBY members were identified and classified into four clades. By structural analysis of putative encoded proteins, we confirmed the presence of YABBY-defining conserved domains and identified novel clade-specific motifs. Transcriptomic and qRT-PCR analyses of different tissues revealed MhyYABBY transcriptional patterns, which were similar to those of orthologous YABBY genes from other angiosperms. These data should contribute to the understanding of the role of the YABBY genes in the regulation of developmental and physiological processes in achlorophyllous leafless plants

Effects of Mutations in The Calcium-binding Sites of Recoverin on Its Calcium Affinity: Evidence for Successive Filling of The Calcium Binding Sites

A molecule of the photoreceptor Ca2+-binding protein recoverin contains four potential EF-hand Ca2+-binding sites, of which only two, the second and the third, are capable of binding calcium ions. We have studied the effects of substitutions in the second, third and fourth EF-hand sites of recoverin on its Ca2+-binding properties and some other characteristics, using intrinsic fluorescence, circular dichroism spectroscopy and differential scanning microcalorimetry. The interaction of the two operating binding sites of wild-type recoverin with calcium increases the protein\u27s thermal stability, but makes the environment around the tryptophan residues more flexible. The amino acid substitution in the EF-hand 3 (E121Q) totally abolishes the high calcium affinity of recoverin, while the mutation in the EF-hand 2 (E85Q) causes only a moderate decrease in calcium binding. Based on this evidence, we suggest that the binding of calcium ions to recoverin is a sequential process with the EF-hand 3 being filled first. Estimation of Ca2+-binding constants according to the sequential binding scheme gave the values 3.7 × 106 and 3.1 × 105 M–1 for third and second EF-hands, respectively. The substitutions in the EF-hand 2 or 3 (or in both the sites simultaneously) do not disturb significantly either tertiary or secondary structure of the apo-protein. Amino acid substitutions, which have been designed to restore the calcium affinity of the EF-hand 4 (G160D, K161E, K162N, D165G and K166Q), increase the calcium capacity and affinity of recoverin but also perturb the protein structure and decrease the thermostability of its apo-form

Point Amino Acid Substitutions in The Ca\u3csup\u3e2+\u3c/sup\u3e-binding Sites of Recoverin: III. A Mutant with The Fourth Reconstructed Ca\u3csup\u3e2+\u3c/sup\u3e-binding Site

Unlike wild type recoverin with only two (the second and the third) functioning Ca+2-binding sites out of four potential ones, the +EF4 mutant contains a third active Ca+2-binding site. This site was reconstructed from the fourth potential Ca+2-binding domain by the introduction of several amino acid substitutions in it by site-directed mutagenesis. The effect of these mutations in the fourth potential Ca+2-binding site of myristoylated recoverin on the structural features and conformational stability of the protein was studied by fluorimetry and circular dichroism. The apoform of the resulting mutant (free of Ca2+ ions) was shown to have a higher calcium capacity, significantly lower thermal stability, and noticeably different secondary and tertiary structures as compared with the apoform of wild-type recoverin

ILC Reference Design Report Volume 1 - Executive Summary

The International Linear Collider (ILC) is a 200-500 GeV center-of-mass high-luminosity linear electron-positron collider, based on 1.3 GHz superconducting radio-frequency (SCRF) accelerating cavities. The ILC has a total footprint of about 31 km and is designed for a peak luminosity of 2x10^34 cm^-2s^-1. This report is the Executive Summary (Volume I) of the four volume Reference Design Report. It gives an overview of the physics at the ILC, the accelerator design and value estimate, the detector concepts, and the next steps towards project realization.The International Linear Collider (ILC) is a 200-500 GeV center-of-mass high-luminosity linear electron-positron collider, based on 1.3 GHz superconducting radio-frequency (SCRF) accelerating cavities. The ILC has a total footprint of about 31 km and is designed for a peak luminosity of 2x10^34 cm^-2s^-1. This report is the Executive Summary (Volume I) of the four volume Reference Design Report. It gives an overview of the physics at the ILC, the accelerator design and value estimate, the detector concepts, and the next steps towards project realization

ILC Reference Design Report Volume 4 - Detectors

This report, Volume IV of the International Linear Collider Reference Design Report, describes the detectors which will record and measure the charged and neutral particles produced in the ILC's high energy e+e- collisions. The physics of the ILC, and the environment of the machine-detector interface, pose new challenges for detector design. Several conceptual designs for the detector promise the needed performance, and ongoing detector R&D is addressing the outstanding technological issues. Two such detectors, operating in push-pull mode, perfectly instrument the ILC interaction region, and access the full potential of ILC physics.This report, Volume IV of the International Linear Collider Reference Design Report, describes the detectors which will record and measure the charged and neutral particles produced in the ILC's high energy e+e- collisions. The physics of the ILC, and the environment of the machine-detector interface, pose new challenges for detector design. Several conceptual designs for the detector promise the needed performance, and ongoing detector R&D is addressing the outstanding technological issues. Two such detectors, operating in push-pull mode, perfectly instrument the ILC interaction region, and access the full potential of ILC physics