The 2017 Xe run at CERN Linac3: Measurements and beam dynamics simulations.

At CERN, large hadron collider heavy ion and super proton synchrotron fixed target experiments are performed thanks to the Heavy-ion Facility, composed of different accelerators. The starting point is Linac3, which delivers 4.2 MeV/u ion beams to the low energy ion ring. In 2017, Linac3 accelerated Xe instead of the most usual Pb. This article summarizes the measurements performed during the machine development time allocated to characterize the line from the source to the filtering section. A parallel effort was devoted to matching those measurements to the beam dynamics simulations, and the second part of the article highlights the results achieved in this regard. Thanks to the improved understanding of the machine critical areas, a list of possible improvements is proposed at the end.

Upgrade of the beam extraction system of the GTS-LHC electron cyclotron resonance ion source at CERN.

Linac3 is the first accelerator in the heavy ion injector chain of the Large Hadron Collider (LHC), providing multiply charged heavy ion beams for the CERN experimental program. The ion beams are produced with GTS-LHC, a 14.5 GHz electron cyclotron resonance ion source, operated in afterglow mode. Improvement of the GTS-LHC beam formation and beam transport along Linac3 is part of the upgrade program of the injector chain in preparation for the future high luminosity LHC. A mismatch between the ion beam properties in the ion source extraction region and the acceptance of the following Low Energy Beam Transport (LEBT) section has been identified as one of the factors limiting the Linac3 performance. The installation of a new focusing element, an einzel lens, into the GTS-LHC extraction region is foreseen as a part of the Linac3 upgrade, as well as a redesign of the first section of the LEBT. Details of the upgrade and results of a beam dynamics study of the extraction region and LEBT modifications will be presented.

Linac4 low energy beam measurements with negative hydrogen ions.

Linac4, a 160 MeV normal-conducting H(-) linear accelerator, is the first step in the upgrade of the beam intensity available from the LHC proton injectors at CERN. The Linac4 Low Energy Beam Transport (LEBT) line from the pulsed 2 MHz RF driven ion source, to the 352 MHz RFQ (Radiofrequency Quadrupole) has been built and installed at a test stand, and has been used to transport and match to the RFQ a pulsed 14 mA H(-) beam at 45 keV. A temporary slit-and-grid emittance measurement system has been put in place to characterize the beam delivered to the RFQ. In this paper a description of the LEBT and its beam diagnostics is given, and the results of beam emittance measurements and beam transmission measurements through the RFQ are compared with the expectation from simulations.

Direct measurements of Ab and Ac using vertex and kaon charge tags at the SLAC detector.

Exploiting the manipulation of the SLAC Linear Collider electron-beam polarization, we present precise direct measurements of the parity-violation parameters A(c) and A(b) in the Z-boson-c-quark and Z-boson-b-quark coupling. Quark-antiquark discrimination is accomplished via a unique algorithm that takes advantage of the precise SLAC Large Detector charge coupled device vertex detector, employing the net charge of displaced vertices as well as the charge of kaons that emanate from those vertices. From the 1996-1998 sample of 400 000 Z decays, produced with an average beam polarization of 73.4%, we find A(c)=0.673+/-0.029(stat)+/-0.023(syst) and A(b)=0.919+/-0.018(stat)+/-0.017(syst).

Improved direct measurement of the parity-violation parameter Ab using a mass tag and momentum-weighted track charge.

We present an improved direct measurement of the parity-violation parameter A(b) in the Z boson-b-quark coupling using a self-calibrating track-charge technique applied to a sample enriched in Z-->bb events via the topological reconstruction of the B hadron mass. Manipulation of the Stanford Linear Collider electron-beam polarization permits the measurement of A(b) to be made independently of other Z-pole coupling parameters. From the 1996-1998 sample of 400,000 hadronic Z decays, produced with an average beam polarization of 73.4%, we find A(b)=0.906+/-0.022(stat)+/-0.023(syst).

Improved direct measurement of A(b) and A(c) at the Z(0) pole using a lepton tag.

The parity violation parameters A(b) and A(c) of the Zb(b) and Zc(c) couplings have been measured directly, using the polar angle dependence of the polarized cross sections at the Z(0) pole. Bottom and charmed hadrons were tagged via their semileptonic decays. Both the electron and muon analyses take advantage of new multivariate techniques to increase the analyzing power. Based on the 1993-1998 SLD sample of 550,000 Z(0) decays produced with highly polarized electron beams, we measure A(b) = 0.919+/-0.030(stat)+/-0.024(syst), and A(c) = 0.583+/-0.055(stat)+/-0.055(syst).

First symmetry tests in polarized Z0 decays to bbg.

We have made the first direct symmetry tests in the decays of polarized Z0 bosons into fully identified bbg states, collected in the SLD experiment at SLAC. We searched for evidence of parity violation at the bbg vertex by studying the asymmetries in the b-quark polar- and azimuthal-angle distributions, and for evidence of T-odd, CP-even or CP-odd, final-state interactions by measuring angular correlations between the three-jet plane and the Z0 polarization. We found results consistent with standard model expectations and set 95% C. limits on anomalous contributions.

Improved direct measurement of leptonic coupling asymmetries with polarized Z bosons.

We present final measurements of the Z boson-lepton coupling asymmetry parameters A(e), A(mu), and A(tau) with the complete sample of polarized Z bosons collected by the SLD detector at the SLAC Linear Collider. From the left-right production and decay polar angle asymmetries in leptonic Z decays we measure A(e) = 0.1544+/-0.0060, A(mu) = 0.142+/-0.015, and A(tau) = 0.136+/-0.015. Combined with our left-right asymmetry measured from hadronic decays, we find A(e) = 0.1516+/-0.0021. Assuming lepton universality, we obtain a combined effective weak mixing angle of sin (2)theta(eff)(W) = 0.230 98+/-0.000 26.

High-precision measurement of the left-right Z Boson cross-section asymmetry.

We present a measurement of the left-right cross-section asymmetry ( A(LR)) for Z boson production by e(+)e(-) collisions. The measurement includes the final data taken with the SLD detector at the SLAC Linear Collider during the period 1996-1998. Using a sample of 383 487 Z decays collected during the 1996-1998 runs we measure the pole value of the asymmetry, A(0)(LR), to be 0.150 56+/-0.002 39 which is equivalent to an effective weak mixing angle of sin (2)straight theta(eff)(W) = 0.231 07+/-0.000 30. Our result for the complete 1992-1998 data set comprising approximately 537 000 Z decays is sin (2)straight theta(eff)(W) = 0.230 97+/-0.000 27.

[Arterial hypertension in relation to life style and other cardiovascular risk factors. Epidemiologic study of a population of blood donors. Project AVIS]. / Ipertensione arteriosa in rapporto allo stile di vita e altri fattori di rischio cardiovascolare. Studio epidemiologico in una popolazione di donatori di sangue. Progetto AVIS.

The objectives of this research were to determine the prevalence of essential and borderline hypertension in a population of blood donors and their families and to determine if there is a correlation between blood pressure and lifestyle and/or other cardiovascular risk factors. The study was comprised of 1976 individuals, of whom 1290 were men and 686 were women, aged 18-65 years. The prevalence of essential hypertension was 15.1% for males and 12.5% for females: the prevalence of borderline hypertension was 22.3% for males and 15.7% for females. The population was divided into two groups: the first group included only subjects (1170 men, 543 women) who did not regularly use drugs that could modify the blood pressure and the heart rate, the second group included the entire population. In the first group, the multiple regression analysis indicated, in order of importance: age, BMI (body mass index), and heart rate. These variables were important in determining the systolic blood pressure in both sexes, uricemia for males and glycemia for females. The diastolic blood pressure was dependent on BMI, heart rate, and alcohol in both sexes, and glycemia, LDL cholesterol, and uricemia in the men. In the second group, primary and borderline hypertension are significantly correlated with age, BMI, and uricemia in both sexes and glycemia in females. A program of health and nutritional education could modify some factors related to blood pressure, such as obesity and alcohol consumption. The result would be a reduction of the prevalence not only of essential and borderline hypertension, but also of metabolic diseases such as dyslipidaemias, diabetes and hyperuricemia, with a global reduction of the cardiovascular risk.

Hyperglycemia and prognosis of acute myocardial infarction in patients without diabetes mellitus.

The present study assessed the prognostic value of hyperglycemia--a common feature in the early phase of acute myocardial infarction (AMI)--in 330 nondiabetic patients. Seventy-nine known diabetics and 10 (3%) unknown diabetics--diagnosed before discharge by stable glycosylated hemoglobin greater than 6.9% and by oral glucose tolerance testing--were excluded. Thirty-three (10%) patients died. The mortality rate was higher in women, in patients with anterior AMI, in older patients (greater than 65 years) and in the presence of heart failure. It was highest in patients with cardiogenic shock (24/36 vs 9/294; p less than 0.0001). Admission plasma glucose was significantly higher in nonsurvivors than in survivors (163 +/- 60 vs 114 +/- 36 mg/dl; p less than 0.0001). Mortality rate increased with increasing admission plasma glucose: 3% in normoglycemic patients (less than or equal to 120 mg/dl) versus 15% in patients with borderline plasma glucose (121 to 180 mg/dl) versus 43% in hyperglycemic patients (greater than 180 mg/dl) (p less than 0.0001). Multiple regression (stepwise) analysis identified cardiogenic shock, infarct site and age as the major determinants of mortality, while admission plasma glucose failed to reach full statistical significance (p = 0.067). Hyperglycemia was related to all 3 of these independent prognostic factors; when age and infarct site were accounted for, hyperglycemia was significantly associated with heart failure only and this association was characterized by a remarkable mortality rate. In nondiabetic patients with AMI, hyperglycemia is a correlate of heart failure and, therefore, an important factor of prognosis.

Evidence for an association of high blood pressure and hyperinsulinemia in obese man.

An association between hyperinsulinemia and hypertension has been suggested by epidemiological surveys. To assess whether this association is independent of the presence of other hyperinsulinemic states, such as obesity and glucose intolerance, we measured the insulin response to oral glucose in a group of middle-aged moderately obese [144 +/- 4% overweight (mean +/- SEM)] patients (n = 18) with essential hypertension (174 +/- 5/104 +/- 2 mm Hg) and normal glucose tolerance. Normotensive subjects (n = 17) with normal glucose tolerance, matched for age and degree of overweight, served as the control group. The mean insulin response to glucose was twice as high in the hypertensive patients (25.8 +/- 0.2 mU/ml X 2 h) as in the normotensive subjects (11.3 +/- 0.2; P less than 0.001), yet the glucose incremental area was 3-fold higher in the former (10.9 +/- 1.0 g/dl X 2 h) than in the latter (3.5 +/- 0.7; P less than 0.001), thus indicating more severe insulin resistance. In the hypertensive group, systolic blood pressure levels were directly correlated with the 2-h plasma insulin values (r = 0.75; P less than 0.001). Furthermore, the 2-h plasma insulin value and the degree of overweight accounted for 65% of the variation in the systolic blood pressure in a multiple regression model (r = 0.81; P less than 0.001). We conclude that in obesity, the occurrence of hypertension marks the presence of additional hyperinsulinemia and insulin resistance, independent of any impairment of glucose tolerance.