Higher Risk of Incident HCV-Coinfections in MSM with a Wide HIV Transmission Bottleneck

BACKGROUND  High-risk sexual behaviors have been suggested as drivers of the recent dramatic increase of sexually-transmitted HCV among HIV-infected men who have sex with men(MSM). METHODS  We assessed the association between the HIV-transmission-bottleneck and the prevalence and incidence of HCV-coinfections in HIV-infected MSM from the Swiss-HIV-Cohort-Study(SHCS). As a proxy for the width of the transmission bottleneck we used the fraction of ambiguous nucleotides in Genotypic-Resistance-Tests(GRTs) from recent HIV-infections. We defined a broad bottleneck as a fraction of ambiguous nucleotides exceeding a previously-established threshold(0.5%). RESULTS  From the SHCS, we identified 671 MSMs with available HCV-serologies and with a HIV-GRT sampled during recent infection. Of those, 161(24.0%) exhibited a broad HIV-transmission-bottleneck, 38(5.7%) had at least one positive HCV test, and 26(3.9%) had an incident HCV infection. Individuals with broad HIV-transmission bottlenecks exhibited a twofold-higher odds of having ever experienced an HCV coinfection(OR[95%CI]=2.2[1.1, 4.3]) and a threefold-higher hazard of an incident HCV infection(HR[95%CI]= 3.0[1.4, 6.6]) than individuals with narrow HIV-transmission-bottlenecks. CONCLUSIONS  Our results indicate that the currently occurring sexual spread of HCV is focused on those MSMs that are prone to exhibit broad HIV-transmission-bottlenecks. This is consistent with an important role of high-risk behavior and mucosal-barrier-impairment in the transmission of HCV among MSM.

Loop formulation of supersymmetric Yang-Mills quantum mechanics

We derive the fermion loop formulation of N=4 supersymmetric SU(N) Yang-Mills quantum mechanics on the lattice. The loop formulation naturally separates the contributions to the partition function into its bosonic and fermionic parts with fixed fermion number and provides a way to control potential fermion sign problems arising in numerical simulations of the theory. Furthermore, we present a reduced fermion matrix determinant which allows the projection into the canonical sectors of the theory and hence constitutes an alternative approach to simulate the theory on the lattice.

Compactified N = 1 supersymmetric Yang-Mills theory on the lattice: continuity and the disappearance of the deconfinement transition

Fermion boundary conditions play a relevant role in revealing the confinement mechanism of N=1 supersymmetric Yang-Mills theory with one compactified space-time dimension. A deconfinement phase transition occurs for a sufficiently small compactification radius, equivalent to a high temperature in the thermal theory where antiperiodic fermion boundary conditions are applied. Periodic fermion boundary conditions, on the other hand, are related to the Witten index and confinement is expected to persist independently of the length of the compactified dimension. We study this aspect with lattice Monte Carlo simulations for different values of the fermion mass parameter that breaks supersymmetry softly. We find a deconfined region that shrinks when the fermion mass is lowered. Deconfinement takes place between two confined regions at large and small compactification radii, that would correspond to low and high temperatures in the thermal theory. At the smallest fermion masses we find no indication of a deconfinement transition. These results are a first signal for the predicted continuity in the compactification of supersymmetric Yang-Mills theory.

Yang-Baxter deformations of Minkowski spacetime

We study Yang-Baxter deformations of 4D Minkowski spacetime. The Yang-Baxter sigma model description was originally developed for principal chiral models based on a modified classical Yang-Baxter equation. It has been extended to coset curved spaces and models based on the usual classical Yang-Baxter equation. On the other hand, for flat space, there is the obvious problem that the standard bilinear form degenerates if we employ the familiar coset Poincaré group/Lorentz group. Instead we consider a slice of AdS5 by embedding the 4D Poincaré group into the 4D conformal group SO(2, 4) . With this procedure we obtain metrics and B-fields as Yang-Baxter deformations which correspond to well-known configurations such as T-duals of Melvin backgrounds, Hashimoto-Sethi and Spradlin-Takayanagi-Volovich backgrounds, the T-dual of Grant space, pp-waves, and T-duals of dS4 and AdS4. Finally we consider a deformation with a classical r-matrix of Drinfeld-Jimbo type and explicitly derive the associated metric and B-field which we conjecture to correspond to a new integrable system.

Numerical corrections to the strong coupling effective Polyakov-line action for finite T Yang-Mills theory

We consider a three-dimensional effective theory of Polyakov lines derived previously from lattice Yang-Mills theory and QCD by means of a resummed strong coupling expansion. The effective theory is useful for investigations of the phase structure, with a sign problem mild enough to allow simulations also at finite density. In this work we present a numerical method to determine improved values for the effective couplings directly from correlators of 4d Yang-Mills theory. For values of the gauge coupling up to the vicinity of the phase transition, the dominant short range effective coupling are well described by their corresponding strong coupling series. We provide numerical results also for the longer range interactions, Polyakov lines in higher representations as well as four-point interactions, and discuss the growing significance of non-local contributions as the lattice gets finer. Within this approach the critical Yang-Mills coupling β c is reproduced to better than one percent from a one-coupling effective theory on N τ = 4 lattices while up to five couplings are needed on N τ = 8 for the same accuracy.