Application of a noninvasive oral fluid test for detection of treponemal IgG in a predominantly HIV-infected population

The performance of a time-resolved fluorescence immunoassay (TRFIA) for detection of treponemal IgG from oral fluid specimens has been assessed in a predominantly HIV-infected population. Serological investigation is the method of choice for confirming clinical suspicion of syphilis; however, in the primary stage of disease, direct detection of treponemes in lesion fluid or Treponema pallidum DNA is recommended because of the reduced sensitivity of serological tests. There may be occasions when blood for serological investigation is difficult to obtain due to individual patient preference or logistical necessity to improve participation in screening initiatives, particularly in outreach situations. Collection of oral fluid for detection of treponemal antibody may prove an attractive alternative and, with this in mind, an oral fluid assay for detection of treponemal IgG was developed. Time-resolved fluorescence was used to detect treponemal IgG extracted from commercially available oral fluid collection devices. Paired serum and saliva samples were obtained from 210 individuals, 101 of whom were diagnosed with syphilis on the grounds of medical examination confirmed by serological testing. Oral fluid specimens from 14 subjects were rejected because they contained insufficient control antibody or were inhibitory. The population tested was predominantly men who have sex with men, many of whom were HIV infected. The overall sensitivity and specificity of the oral fluid assay was 95.8 and 86.1%, respectively, based on the 5th percentile of the positive results, and 93.7 and 91.1%, respectively, based on a cutoff derived by mixture model analysis. For individuals with primary syphilis, the optimum sensitivity of the oral fluid assay was 87.5%, whereas in those with disease classified as secondary syphilis and early latent syphilis, the sensitivity of the oral fluid assay was 100 and 94.7%, respectively. The oral fluid assay is a useful alternative to serological testing in certain situations, and further development of this technology to enable detection of treponemal IgM should increase its sensitivity for detecting cases of primary syphilis.     

National health expenditures, 1988. Office of National Cost Estimates

Every year, analysts in the Health Care Financing Administration present figures on what our Nation spends for health. As the result of a comprehensive re-examination of the definitions, concepts, methods, and data sources used to prepare those figures, this year's report contains new estimates of national health expenditures for calendar years 1960 through 1988. Significant changes have been made to estimates of spending for professional services and to estimates of what consumers pay out of pocket for health care. In the first article, trends in use of and expenditure for various types of goods and services are discussed, as well as trends in the sources of funds used to finance health care. In a companion article, the benchmark process is described in more detail, as are the data sources and methods used to prepare annual estimates of health expenditures.     

Isoelectronic perturbations to f-d-electron hybridization and the enhancement of hidden order in URu2Si2

Electrical resistivity measurements were performed on single crystals of URu_2–xOs_xSi₂ up to x = 0.28 under hydrostatic pressure up to P = 2 GPa. As the Os concentration, x, is increased, 1) the lattice expands, creating an effective negative chemical pressure P_ch(x); 2) the hidden-order (HO) phase is enhanced and the system is driven toward a large-moment antiferromagnetic (LMAFM) phase; and 3) less external pressure P_c is required to induce the HO→LMAFM phase transition. We compare the behavior of the T(x, P) phase boundary reported here for the URu_2-xOs_xSi₂ system with previous reports of enhanced HO in URu₂Si₂ upon tuning with P or similarly in URu_2–xFe_xSi₂ upon tuning with positive P_ch(x). It is noteworthy that pressure, Fe substitution, and Os substitution are the only known perturbations that enhance the HO phase and induce the first-order transition to the LMAFM phase in URu₂Si₂. We present a scenario in which the application of pressure or the isoelectronic substitution of Fe and Os ions for Ru results in an increase in the hybridization of the U-5f-electron and transition metal d-electron states which leads to electronic instability in the paramagnetic phase and the concurrent formation of HO (and LMAFM) in URu₂Si₂. Calculations in the tight-binding approximation are included to determine the strength of hybridization between the U-5f-electron states and the d-electron states of Ru and its isoelectronic Fe and Os substituents in URu₂Si₂.

The heavy-fermion superconducting compound URu2Si2 is known for its second-order phase transition into the so-called “hidden-order” (HO) phase at a transition temperature T0 ≈17.5 K. Extensive investigation of the phase space in proximity to the HO phase transition has provided a detailed picture of the electronic and magnetic structure of this unique phase (1–42). However, more than three decades after the initial characterization of URu2Si2 (1–3), the order parameter for the HO phase is still unidentified.Most perturbations to the URu2Si2 compound have the effect of suppressing HO. The application of an external magnetic field (H) suppresses the HO phase (41, 43) and many of the chemical substitutions (x) at the U, Ru, or Si sites that have been explored significantly reduce T0, even at modest levels of substituent concentration (44–52). At present, only three perturbations are known to consistently enhance the HO phase in URu2Si2: 1) external pressure P, 2) isoelectronic substitution of Fe ions for Ru, and 3) isoelectronic substitution of Os ions for Ru. Upon applying pressure P, the HO phase in pure URu2Si2 is enhanced (6) and the system is driven toward a large-moment antiferromagnetic (LMAFM) phase (53). The HO→LMAFM phase transition is identified indirectly by a characteristic “kink” at a critical pressure Pc ≈1.5 GPa in the T0 (P) phase boundary (18, 53, 54) and also directly by neutron diffraction experiments, which reveal an increase in the magnetic moment from μ ∼ (0.03±0.02)μB/U in the HO phase to μ ∼ 0.4 μB/U in the LMAFM phase (13, 55, 56).Recent reports indicate that the isoelectronic substitution of Fe ions for Ru in URu2Si2 replicates the T0(P) behavior in URu2Si2 (57–59). An increase in x in URu2−xFexSi2 enhances the HO phase and drives the system toward the HO→LMAFM phase transition at a critical Fe concentration xc ≈0.15 (58, 60). The decrease in the volume of the unit cell due to substitution of smaller Fe ions for Ru may be interpreted as a chemical pressure, Pch, where the Fe concentration x can be converted to Pch (x) (57, 59). In addition, the induced HO→LMAFM phase transition in URu2−xFexSi2 occurs at combinations of x and P that consistently obey the additive relationship: Pch(x) + Pc ≈1.5 GPa (57, 59). These results have led to the suggestion that Pch is equivalent to P in affecting the HO and LMAFM phases (58, 59).Reports of the isoelectronic substitution of larger Os ions for Ru have shown that an increase in x in URu2−xOsxSi2 1) expands the volume of the unit cell, thus creating an effective negative chemical pressure (Pch ≤0); 2) enhances the HO phase; and 3) drives the system toward a similar HO→LMAFM phase transition at a critical Os concentration of xc ≈0.065 (60–62). These results are contrary to the expectation that a negative Pch would lead to a suppression of HO and complicate the view of chemical pressure as a mechanism affecting the evolution of phases in URu2Si2.In this paper, we report on the behavior of the T(x, P) boundary for the URu2−xOsxSi2 system based on ρ(T) measurements of single crystals of URu2−xOsxSi2 as a function of Os concentration x and applied pressure P. The T(x, P) phase boundary observed here for the URu2−xOsxSi2 system (57–59) is compared to that of the URu2−xFexSi2 system and also with the behavior of T(P) in pure URu2Si2. As an explanation for the enhancement of HO toward the HO→LMAFM phase transition, we suggest a scenario in which each of the perturbations of Os substitution, Fe substitution, and pressure P favors delocalization of the 5f electrons and increases the hybridization of the uranium 5f-electron and transition metal (Fe, Ru, Os) d-electron states. To avoid an ad hoc explanation of the effect of increasing the Os concentration x in URu2−xOsxSi2, compared to the effects of pressure P and Fe substitution, we explain how pressure P, Fe substitution, and Os substitution are three perturbative routes to enhancement of the U-5f- and d-electron hybridization. The importance of the 5f- and d-electron hybridization to the emergence of HO/LMAFM is presented in the context of the Fermi surface (FS) instability that leads to a reconstruction and partial gapping of the FS during the transition from the paramagnetic (PM) phase to the HO and LMAFM phases (2, 6, 20, 22, 24–26, 37, 38, 63).In an effort to further understand the effect of isoelectronic substitution on the 5f- and d-electron hybridization, calculations in the tight-binding approximation were made for compounds from the series UM2Si2 (M = Fe, Ru, and Os). The calculations indicate that the degree of hybridization is largely dependent on the magnitude of the difference between the binding energy of the localized U-5f electrons and that of the transition metal d electrons.     

Acute myocardial infarction: an unusual culmination of rheumatic pancarditis and antiphospholipid antibody syndrome

A 29-year-old man with history of antiphospholipid antibody syndrome (APS) and two prior episodes of acute rheumatic fever developed a third episode of acute rheumatic fever. This was complicated by acute myocardial infarction due to spontaneous arterial thrombosis of the left anterior descending and right coronary arteries. We postulate that rheumatic pancarditis created an inflammatory, thrombogenic environment that facilitated coronary artery thrombosis secondary to APS, a novel association. Our patient was left with significant left ventricular dysfunction at a young age, and cases such as this emphasize the need for early recognition and proper treatment of APS. Further, the pathogenesis of thrombosis in APS is incompletely understood, and the cellular and molecular basis for this, including the role of 'second hits', are areas needing further investigation.     

Inflammatory bowel disease, peptic ulcer and diverticular disease as certified causes of death in an English population 1979-2003

BACKGROUND: When gastrointestinal diseases are certified as causes of death, they are often not selected as the underlying cause. Until recently, only one underlying cause of death has been coded and analysed in official national statistics in England and many other countries. AIMS: To report on the total 'burden of mortality' from some common gastrointestinal diseases, and whether it has changed over time, including all certified causes of death as well as underlying causes, (i) in the Oxford region from 1979 to 2003, (ii) in England from 1996 to 2003; and to quantify the under-ascertainment of cause-specific mortality when based on underlying cause alone. METHODS: We searched death certificate data from the Oxford Record Linkage Study database, and from English national data, for specified gastrointestinal diseases certified as underlying or contributory causes of death. RESULTS: For all the conditions studied, underlying-cause-coded mortality missed a substantial percentage of all certified deaths. The extent of underestimation varied according to the periods in which different criteria were used for the selection of the underlying cause. For example, in Oxford, in the latest period 1993-2003, underlying-cause-coded mortality identified only 37% of all death certificates with ulcerative colitis, 47% of Crohn's disease, between 62 and 68% for the different types of peptic ulcer and 66% of diverticular disease. CONCLUSIONS: Studies of mortality for these diseases should take account of all certified causes as well as underlying-cause mortality. This is particularly important for analyses that go across periods of change to the rules for selecting the underlying cause of death.     

Shifting towards an Opt-Out System in Greece: A General Practice Based Pilot Study

New legislation in Greece towards presumed consent for organ donation, effective as of June 2013, has come at a critical moment. This pilot study aims to explore awareness, specific concerns and intentions about the new organ donation framework among patients attending Greek general practices in a rural and urban setting. Only 2.6% of respondents had a donor card, a mere 9.6% was aware of new legislation, whereas only 3.8% considered that the public had been adequately informed. Higher income respondents were more likely to be aware that they would be considered organ donors upon death, unless declared differently. Urban practice respondents were less likely to have previously discussed with a significant other their intentions in regards to presumed consent. One quarter of all respondents (22.4%) intended to carry out their right to prohibit organ removal upon death. Survey results reveal that organ donation reform has yet to be disseminated by the Greek society, underscoring the urgency for targeted information campaigns.     

Defective DNA mismatch repair in long-term (> or =3 years) survivors with pancreatic cancer.

BACKGROUND/AIMS: Defective DNA mismatch repair (MMR) in pancreatic cancer, reported in up to 13% of sporadic pancreatic cancers, may predict a good prognosis. To determine if long-term survival in pancreatic cancer could be attributed to defective DNA MMR, we ascertained its prevalence in 35 pancreatic cancer patients who survived > or =3 years after surgery. METHODS: We performed immunohistochemistry (IHC) for MMR proteins hMLH1, hMSH2, and hMSH6 in all 35 tumors and microsatellite instability (MSI) studies in 34/35 tumors using 10 microsatellite markers in paired normal and tumor DNA. Defective DNA MMR was defined as absence of protein expression on IHC and/or MSI in > or =30% of markers studied. RESULTS: On IHC, 3/35 (8.6%) tumors had defective DNA MMR. All 3 had absent expression of a DNA MMR protein (hMLH1 in 2 and hMSH2) and 2/3 also had MSI; the third could not be tested. Definitely 2, and probably all 3 patients had hereditary nonpolyposis colon cancer as determined by clinical and genetic profiles. CONCLUSION: Defective DNA MMR is uncommon in long-term survivors of pancreatic cancer and does not account for the survival benefit in those with sporadic pancreatic cancer.     

Hierarchical self-assembly of a striped gyroid formed by threaded chiral mesoscale networks

Numerical simulations reveal a family of hierarchical and chiral multicontinuous network structures self-assembled from a melt blend of Y-shaped ABC and ABD three-miktoarm star terpolymers, constrained to have equal-sized A/B and C/D chains, respectively. The C and D majority domains within these patterns form a pair of chiral enantiomeric gyroid labyrinths (srs nets) over a broad range of compositions. The minority A and B components together define a hyperbolic film whose midsurface follows the gyroid minimal surface. A second level of assembly is found within the film, with the minority components also forming labyrinthine domains whose geometry and topology changes systematically as a function of composition. These smaller labyrinths are well described by a family of patterns that tile the hyperbolic plane by regular degree-three trees mapped onto the gyroid. The labyrinths within the gyroid film are densely packed and contain either graphitic hcb nets (chicken wire) or srs nets, forming convoluted intergrowths of multiple nets. Furthermore, each net is ideally a single chiral enantiomer, induced by the gyroid architecture. However, the numerical simulations result in defect-ridden achiral patterns, containing domains of either hand, due to the achiral terpolymeric starting molecules. These mesostructures are among the most topologically complex morphologies identified to date and represent an example of hierarchical ordering within a hyperbolic pattern, a unique mode of soft-matter self-assembly.Liquid crystals formed by molecular self-assembly provide fascinating examples of complicated space partitions in soft-material science. Relatively complex examples are the bicontinuous mesostructures found ubiquitously in both natural and synthetic soft matter, including lipid–water systems and block copolymer melts, namely the double diamond (symmetry ), the primitive , and, particularly, the gyroid mesophases. The structure of these mesophases can be described by a molecular membrane folded onto one of the three simplest triply periodic minimal surfaces (TPMS), namely the D, P, and G(yroid) surfaces, named by Schoen in the 1960s (1). From a 3D perspective, these structures are characterized by the nets describing the pair of mutually threaded labyrinths carved out of space by the convoluted hyperbolic architecture of the TPMS. For the gyroid, this is a racemic mixture of two chiral srs nets, one left- and the other right-handed [the three-letter nomenclature follows the Reticular Chemistry Structure Resource naming convention for 3D nets (2)]. This leads to an overall achiral structure when the two nets are chemically identical, which is the case in most experimentally identified gyroid liquid-crystal structures. One such structure recently reported is a gyroid assembly found in an ABC three-miktoarm star terpolymer melt (3). In this structure, the majority C component constitutes the two labyrinth nets while the A and B minority components together form the dividing membrane. Because of the connectivity of the star molecular architecture and because all components microphase separate, the A and B components segregate on the dividing hyperbolic interface. This structure is an experimental indication of a unique mode of self-assembly, namely “hierarchical assembly of a hyperbolic pattern.” Complementing this finding and further motivating our work reported here, a recent simulation study by one of us (J.J.K.K.) explored self-assembly of blends of equal amounts of two distinct three-miktoarm stars, namely ABC and ABD three-miktoarm star terpolymers (Fig. 1). Both molecules were assigned equal molecular weights, and the proportions of the equal volume C (green) and D (yellow) chains relative to the equal A (red) and B (blue) chains were varied (4). Despite these severe compositional constraints, a number of unique four-colored mesophases were revealed. The most striking feature of the predicted phase behavior in this system was the presence of interesting patterns whose general features are reminiscent of the gyroid, albeit far more complex in both geometric and topological aspects. In the system reported here, two ordering regimes form. At the larger length scale, ordering induces a gyroid-like membrane, which is itself also spontaneously ordered at a smaller length scale, giving unique microdomain patterning due to the membrane confinement to a hyperbolic curved interface. Each of these patterns contain distinct numbers and types of interwoven 2D and 3D A and B domains forming nets of equal hand, immersed within the hyperbolic interface between an enantiomeric pair of C and D srs nets. These structures are spectacularly convoluted in 3D space and correspond to special members of a sequence of chiral cubic patterns that emerge by local striping of the gyroid membrane. We demonstrate how this is performed systematically by mapping a particular family of tilings in the hyperbolic plane onto the gyroid in 3D euclidean space. Careful analysis of the morphologies formed in the simulations, described below, reveals the presence of up to three distinct chiral cubic mesophases within this striped gyroid region of the phase diagram. We explore the geometric and topological variety of these self-assemblies in detail and discuss how they emerge as a response to a hierarchy of frustrations imposed by the three-arm star molecular architecture, acting in both two and three dimensions.Open in a separate windowFig. 1.(A) Model ABC and ABD three-miktoarm star terpolymer molecules. All molecules contain equal-sized A (red) and B (blue) arms, and longer C (green) and D (yellow) arms, also of equal size. The parameter x (equal to in this image), corresponds to the number ratio of C to A beads. (B) C and D domain geometry, a pair of intertwined srs nets. (C–G) Single-unit cell snapshots illustrating the curved striped pattern formed by the minority components A and B for varying x. (C) x = 2, (D) x = 3.33, (E) x = 3.67, (F) x = 5, and (G) x = 6. Note the threefold branching of the stripes for all values of x.