Uniformity calibration for large area XY strip parallel plate ionization chamber.

Demand for large area parallel plate ionization chamber (PPIC) or large area ionization chamber (LAIC) has risen in recent years due to several advantages of the large effective area in monitoring therapeutic radiation beams. PPICs are designed for the measurements of beam profile and dosimetry in radiation therapy quality assurance (QA) procedures.Objective. Heterogeneous responses over the large sensitive area pose an undeniable concern for the straightforward applications of PPICs in clinical dosimetry. Uniformity calibration for the detector response is thus essential for the accurate performance of each PPIC unit.Approach.A large area XY strip PPIC, characterized by a large effective area of 345.44 × 345.44 mm2and 256 readout channels, was investigated in this study. A new systematic uniformity calibration is developed to improve the lateral response of the PPIC over the measurements for both narrow beams and large square field beams. A 2D response map of the PPIC was obtained by a spot-scanning method using a compact x-ray tube (mini x-ray). The mini x-ray, providing stable radiation (uncertainty <0.1%), was moved with a step size of 20 mm in 2 dimensions across the entire PPIC surface to collect a complete spot scan. Different uniformity calibration methods were introduced for the measurement of the PPIC by adopting the information from the detector 2D response map.Main results.Deviation of the detector response, before calibration, was observed to reach about 7% for the testing PPIC unit which is much higher than the recommended uniformity response of 1% (IAEA TRS-398). The uniformity response of the PPIC improved significantly to less than 1% across the detector surface after calibration.Significance.The proposed methods enable the practical application of PPIC in routine clinical dosimetry and can be reliably adopted by any radiation facility to perform daily and monthly QA.

3D bioengineered tissues: From advancements in in vitro safety to new horizons in disease modeling.

Research aimed at more fully emulating human biology in vitro has rapidly progressed in recent years with advancements in 3D tissue engineering and microphysiological systems. The initial target of such systems has been directed towards drug and chemical safety assessment, with the goal of improving sensitivity and predictive capabilities. Here we discuss recent developments of in vitro organ culture systems, and their future applications in modeling human disease.

Anti-ribosomal and 'P-peptide'-specific autoantibodies bind to T lymphocytes.

Patients with systemic lupus erythematosus (SLE) frequently have anti-lymphocyte autoantibodies, some of which also bind to surfaces of neurons. Since anti-ribosomal P protein autoantibodies (anti-P) from SLE patients also bind to surfaces of neurons, we hypothesized that anti-P are anti-lymphocyte antibodies. A panel of human T lymphocytes was evaluated for anti-P binding by indirect immunofluorescence. Affinity-purified anti-ribosomal antibodies were used as a source of anti-P. These autoantibodies bound to the surfaces of all transformed T cell lines tested. This binding was not mediated by Fc receptors. It was inhibitable by ribosomes. Anti-P bound to circulating T lymphocytes from healthy adults and children. They also bound to thymocytes and cord blood T cells from normal neonates. Circulating T cells from SLE patients with anti-P bound less anti-P than cells from healthy controls. Two patients were studied on multiple occasions. The capacity of their T cells to bind anti-P correlated inversely with titres of anti-ribosomal antibodies. Anti-ribosomal antibodies, other than anti-P, also appear to bind to T cells. The surface of T cells contains a protein with the size and antigenicity of the ribosomal P protein, P0. We conclude that anti-ribosomal antibodies are a subset of anti-lymphocyte autoantibodies. Their possible role in the pathogenesis of lymphopenia or lymphocyte dysfunction in SLE has to be defined in further studies.

Charged-particle multiplicity near midrapidity in central Au+Au collisions at sqrt[SNN]=56 and 130 GeV.

We present the first measurement of pseudorapidity densities of primary charged particles near midrapidity in Au+Au collisions at sqrt[s(NN)] = 56 and 130 GeV. For the most central collisions, we find the charged-particle pseudorapidity density to be dN/deta|(|eta|<1) = 408+/-12(stat)+/-30(syst) at 56 GeV and 555+/-12(stat)+/-35(syst) at 130 GeV, values that are higher than any previously observed in nuclear collisions. Compared to proton-antiproton collisions, our data show an increase in the pseudorapidity density per participant by more than 40% at the higher energy.