681 research outputs found

    Synthesis of Phosphorothioate Oligonucleotides with Stereodefined Phosphorothioate Linkages

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    A method for solid‐phase synthesis of stereodefined PS‐oligos via an oxathiaphospholane approach using pure P‐diastereomers of nucleoside oxathiaphospholane monomers is described. The oxathiaphospholane monomers are synthesized by phosphitylation of 5′‐O‐DMTr‐N‐protected deoxyribonucleosides with 2‐chloro‐spiro‐4,4‐pentamethylene‐1,3,2‐oxathiaphospholane followed by sulfurization. The procedure is general and may be applied to other analogs, depending on the aldehyde (or mercaptoalcohol) used. Starting from an 18O‐labeled mercaptoalcohol, the corresponding 18O‐labeled phosphitylating reagent and nucleoside monomers can be obtained and used for synthesis of labeled stereodefined PS‐oligos, which are useful for studying mechanisms of enzymatic reactions. Details are provided for chromatographic separation of the 5′‐O‐DMTr‐N‐protected‐deoxyribonucleoside‐3′‐O‐(2‐thio‐spiro‐4,4‐pentamethylene‐1,3,2‐oxathiaphospholane)s into their P‐diastereomers, and for manual solid‐phase synthesis of PS‐oligos. Oxidation of 5′‐O‐DMTr‐N‐protected‐deoxyribonucleoside‐3′‐O‐(2‐thio‐spiro‐4,4‐pentamethylene‐1,3,2‐oxathiaphospholane)s with selenium dioxide yields their 2‐oxo‐analogs, which are suitable either for elongation of stereodefined PS‐oligos with segments consisting of unmodified nucleotide units possessing phosphate internucleotide linkages, or for generating isotopomeric 18O‐labeled PO‐oligos of predetermined P‐chirality.Peer Reviewedhttps://deepblue.lib.umich.edu/bitstream/2027.42/143684/1/cpnc0417.pd

    Blinatumomab compared with standard of care for the treatment of adult patients with relapsed/refractory Philadelphia chromosome–positive B-precursor acute lymphoblastic leukemia

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    Background: A single-arm, phase 2 trial demonstrated the efficacy and safety of blinatumomab, a bispecific T-cell\u2013engaging antibody construct, in patients with relapsed/refractory (r/r) Philadelphia chromosome\u2013positive (Ph+) acute lymphoblastic leukemia (ALL), a rare hematologic malignancy with limited treatment options. This study compared outcomes with blinatumomab with those of a historical control treated with the standard of care (SOC). Methods: The blinatumomab trial enrolled adult patients with Ph+ ALL who were r/r to at least 1 second-generation tyrosine kinase inhibitor (n = 45). Propensity score analysis (PSA) was used to compare outcomes with blinatumomab with those of an external cohort of similar patients receiving SOC chemotherapy (n = 55). The PSA mitigated confounding variables between studies by adjusting for imbalances in the age at diagnosis and start of treatment, sex, duration from diagnosis to most recent treatment, prior allogeneic hematopoietic stem cell transplantation, prior salvage therapy, and number of salvage therapies. Bayesian data augmentation was applied to improve power to 80% with data from a phase 3 blinatumomab study in r/r Philadelphia chromosome\u2013negative ALL. Results: In the PSA, the rate of complete remission or complete remission with partial hematologic recovery was 36% for blinatumomab and 25% for SOC, and this resulted in an odds ratio of 1.54 (95% confidence interval [CI], 0.61-3.89) or 1.70 (95% credible interval [CrI], 0.94-2.94) with Bayesian data augmentation. Overall survival favored blinatumomab over SOC, with a hazard ratio of 0.81 (95% CI, 0.57-1.14) or 0.77 (95% CrI, 0.61-0.96) with Bayesian data augmentation. Conclusions: These results further support blinatumomab as a treatment option for patients with r/r Ph+ ALL

    Presupernova Structure of Massive Stars

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    Issues concerning the structure and evolution of core collapse progenitor stars are discussed with an emphasis on interior evolution. We describe a program designed to investigate the transport and mixing processes associated with stellar turbulence, arguably the greatest source of uncertainty in progenitor structure, besides mass loss, at the time of core collapse. An effort to use precision observations of stellar parameters to constrain theoretical modeling is also described.Comment: Proceedings for invited talk at High Energy Density Laboratory Astrophysics conference, Caltech, March 2010. Special issue of Astrophysics and Space Science, submitted for peer review: 7 pages, 3 figure

    The convective Urca process

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    One possible fate of an accreting white dwarf is explosion in a type Ia supernova. However, the route to the thermonuclear runaway has always been uncertain owing to the lack of a convective model consistent with the Urca process. We derive a formalism for convective motions involving two radial flows. This formalism provides a framework for convective models that guarantees self-consistency for chemistry and energy budget, allows time-dependence and describes the interaction of convective motions with the global contraction or expansion of the star. In the one-stream limit, we reproduce several already existing convective models and allow them to treat chemistry. We also suggest as a model easy to implement in a stellar evolution code. We apply this formalism to convective Urca cores in Chandrasekhar mass white dwarfs. We stress that in degenerate matter, nuclear reactions that change the number of electrons strongly influence the convective velocities. We point out the sensitivity of the energy budget on the mixing. We illustrate our model by computing {\it stationary} convective cores with Urca nuclei. We show that even a very small mass fraction of Urca nuclei (10−810^{-8}) strongly influences the convective velocities. Finally, we present preliminary computations of the late evolution of a close to Chandrasekhar mass C+O white dwarf including the convective Urca process.Comment: 4 pages, 1 figure, to appear in the 8th Nuclei In Cosmos conference proceeding

    The formation and evolution of bright spots on Ceres

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    The otherwise homogeneous surface of Ceres is dotted with hundreds of anomalously bright, predominantly carbonate-bearing areas, termed "faculae," with Bond albedos ranging from ∼0.02 to >0.5. Here, we classify and map faculae globally to characterize their geological setting, assess potential mechanisms for their formation and destruction, and gain insight into the processes affecting the Ceres surface and near-surface. Faculae were found to occur in four distinct geological settings, associated predominantly with impact craters: (1) crater pits, peaks, or floor fractures (floor faculae), (2) crater rims or walls (rim/wall faculae), (3) bright ejecta blankets, and (4) the mountain Ahuna Mons. Floor faculae were identified in eight large, deep, and geologically young (asteroid-derived model (ADM) ages of <420 ± 60 Ma) craters: Occator, Haulani, Dantu, Ikapati, Urvara, Gaue, Ernutet, and Azacca. The geometry and geomorphic features of the eight craters with floor faculae are consistent with facula formation via impact-induced heating and upwelling of volatile-rich materials, upwelling/excavation of heterogeneously distributed subsurface brines or their precipitation products, or a combination of both processes. Rim/wall faculae and bright ejecta occur in and around hundreds of relatively young craters of all sizes, and the geometry of exposures is consistent with facula formation via the excavation of subsurface bright material, possibly from floor faculae that were previously emplaced and buried. A negative correlation between rim/wall facula albedo and crater age indicates that faculae darken over time. Models using the Ceres crater production function suggest initial production or exposure of faculae by large impacts, subsequent dissemination of facula materials to form additional small faculae, and then burial by impact-induced lateral mixing, which destroys faculae over timescales of less than 1.25 Gyr. Cumulatively, these models and the observation of faculae limited to geologically young craters indicate relatively modern formation or exposure of faculae, indicating that Ceres' surface remains active and that the near surface may support brines in the present day

    A Centre-Stable Manifold for the Focussing Cubic NLS in R1+3R^{1+3}

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    Consider the focussing cubic nonlinear Schr\"odinger equation in R3R^3: iψt+Δψ=−∣ψ∣2ψ. i\psi_t+\Delta\psi = -|\psi|^2 \psi. It admits special solutions of the form eitαϕe^{it\alpha}\phi, where ϕ\phi is a Schwartz function and a positive (ϕ>0\phi>0) solution of −Δϕ+αϕ=ϕ3. -\Delta \phi + \alpha\phi = \phi^3. The space of all such solutions, together with those obtained from them by rescaling and applying phase and Galilean coordinate changes, called standing waves, is the eight-dimensional manifold that consists of functions of the form ei(v⋅+Γ)ϕ(⋅−y,α)e^{i(v \cdot + \Gamma)} \phi(\cdot - y, \alpha). We prove that any solution starting sufficiently close to a standing wave in the Σ=W1,2(R3)∩∣x∣−1L2(R3)\Sigma = W^{1, 2}(R^3) \cap |x|^{-1}L^2(R^3) norm and situated on a certain codimension-one local Lipschitz manifold exists globally in time and converges to a point on the manifold of standing waves. Furthermore, we show that \mc N is invariant under the Hamiltonian flow, locally in time, and is a centre-stable manifold in the sense of Bates, Jones. The proof is based on the modulation method introduced by Soffer and Weinstein for the L2L^2-subcritical case and adapted by Schlag to the L2L^2-supercritical case. An important part of the proof is the Keel-Tao endpoint Strichartz estimate in R3R^3 for the nonselfadjoint Schr\"odinger operator obtained by linearizing around a standing wave solution.Comment: 56 page

    Sharp Trace Hardy-Sobolev-Maz'ya Inequalities and the Fractional Laplacian

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    In this work we establish trace Hardy and trace Hardy-Sobolev-Maz'ya inequalities with best Hardy constants, for domains satisfying suitable geometric assumptions such as mean convexity or convexity. We then use them to produce fractional Hardy-Sobolev-Maz'ya inequalities with best Hardy constants for various fractional Laplacians. In the case where the domain is the half space our results cover the full range of the exponent s∈(0,1)s \in (0,1) of the fractional Laplacians. We answer in particular an open problem raised by Frank and Seiringer \cite{FS}.Comment: 42 page
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