1,758,546 research outputs found
Observation of ? (3686)? ? (1530)- ? ? (1530)+ and ? (1530)- ? ? +
No full textUsing 448.1×106 ?(3686) events collected with the BESIII detector at BEPCII, we employ a single-baryon tagging technique to make the first observation of ?(3686)??(1530)-??(1530)+ and ?(1530)-??+ decays with a statistical significance of more than 10? and 5.0?, respectively. The branching fractions are measured to be B(?(3686)??(1530)-??(1530)+)=(11.45±0.40±0.59)×10-5 and B(?(3686)??(1530)-??+)=(0.70±0.11±0.04)×10-5. The angular distribution parameter for ?(3686)??(1530)-??(1530)+ is determined to be ?=0.40±0.24±0.06, which agrees with the theoretical predictions within 1?. The first uncertainties are statistical, and the second systematic
Анатомы - лечащие врачи папства (обзор литературы)
No full textСтаття присвячена анатомам, які були особистими лікарями Пап Римських у різний час:
М. Р. Коломбо (1515-1559), Г. Б. Канано (1515-1579), Г. C. Аранзі (1530-1589), К. Варолій (1543-
1575), А. Чезальпіно (1525-1603), М. Мальпігі (1628-1694), Дж. M. Ланцізі (1654-1720) та
Дж. Флайяні (1739-1808). Подається інформація про їх внесок у розвиток медицини та короткі
біографічні данні.
При цитуванні документа, використовуйте посилання http://essuir.sumdu.edu.ua/handle/123456789/31507Статья посвящена анатомам, которые были лечащими врачами Пап Римских в разные годы:
М. Р. Коломбо (1515-1559), Г. Б. Канано (1515-1579), Г. C. Аранзи (1530-1589), К. Варолий (1543-
1575), А. Чезальпино (1525-1603), М. Мальпиги (1628-1694), Дж. M. Ланцизи (1654-1720) и
Дж. Флайяни (1739-1808). Рассказывается об их вкладе в развитие медицины и короткие
биографические данные.
При цитировании документа, используйте ссылку http://essuir.sumdu.edu.ua/handle/123456789/31507Article is about anatomists, who were papal physicians: M.R. Colombo (c.1515-1559),
G.B. Canano (1515-1579), G.C. Aranzi (1530-1589), C. Varolio (1543-1575), A. Cesalpino (1525-
1603), M. Malpighi (1628-1694), G.M. Lancisi (1654-1720) and G. Flaiani (1739-1808). Their
contribution into anatomy and brief biographical information are given.
When you are citing the document, use the following link http://essuir.sumdu.edu.ua/handle/123456789/3150
Observation of and
No full textUsing events collected with the BESIII detector at BEPCII, we employ a single-baryon tagging technique to make the first observation of and decays with a statistical significance of more than 10 and 5.0, respectively. The branching fractions are measured to be and . The angular distribution parameter for is determined to be = 0.40 ± 0.24 ± 0.06, which agrees with the theoretical predictions within 1. The first uncertainties are statistical, and the second systematic
Observation of and
No full textUsing events collected with the BESIII detector at BEPCII, we employ a single-baryon tagging technique to make the first observation of and decays with a statistical significance of more than 10 and 5.0, respectively. The branching fractions are measured to be and . The angular distribution parameter for is determined to be = 0.40 ± 0.24 ± 0.06, which agrees with the theoretical predictions within 1. The first uncertainties are statistical, and the second systematic
Observation of psi(3886) -> Xi(1530)(-)(Xi)over-bar(1530)(+) and Xi(1530)(-)(Xi)over-bar(+)
No full textUsing 448.1 x 10(6) psi(3686) events collected with the BESIII detector at BEPCII, we employ a single-baryon tagging technique to make the first observation of psi(3686) -> Xi(1530)(-)(Xi) over bar (1530)(+) and Xi(1530)(-)(Xi) over bar (+) decays with a statistical significance of more than 10 sigma and 5.0 sigma, respectively. The branching fractions are measured to be B(psi(3686) -> Xi(1530)(-)(Xi) over bar (1530)(+)) = (11.45 +/- 0.40 +/- 0.59) x 10(-5) and B(psi(3686) -> Xi(1530)(-)(Xi) over bar (+)) = (0.70 +/- 0.11 +/- 0.04) x 10(-5). The angular distribution parameter for psi(3686) -> Xi(1530)(-)(Xi) over bar (1530)(+) is determined to be alpha = 0.40 +/- 0.24 +/- 0.06, which agrees with the theoretical predictions within 1 sigma. The first uncertainties are statistical, and the second systematic
Growing up in Hospitaller Malta (1530-1798) : sources and methodologies for the history of childhood and adoloscence
No full textThe study of young people in the past is fraught with methodological problems and
unearthing source material on children and adolescents can be problematic. It requires
the adoption of a different set of lenses through which textual primary material can be
viewed. This entails striving to recognise and release previously unheard voices. Furthermore,
the textual material can be complemented by an array of visual and material
objects that have preserved a certain image of children and adolescents in the past.
This chapter commences with a brief outline of the methodological developments that
have taken place in this field since Philippe Ariès’s seminal book appeared in 1960, and
traces the resulting changes and innovations that concern sources. In particular, it will
underline the importance to historians of taking into account recent developments in
the field of childhood archaeology. Furthermore, the fundamental role of religion in
people’s lives in early modern times necessarily influenced their upbringing. In turn,
most of the sources that are available from this era – court records, statutes, paintings
– were either produced by religious institutions, or were heavily influenced by religious
beliefs. Thus, this chapter will strive to demonstrate how approaches used in one place
can be adapted and used in different historiographical contexts, and how vital it is to
adopt an interdisciplinary approach.peer-reviewe
Observation of psi (3686) ->Xi (1530)(0) (Xi)over-bar (1530)(0) and Xi (1530)(0) (Xi)over-bar(0)
No full textUsing (448.1±2.9)×106 ψ(3686) events collected with the BESIII detector and a single-baryon tagging technique, we present the first observation of the decays ψ(3686)→Ξ(1530)0Ξ ̄(1530)0 and Ξ(1530)0Ξ ̄0. The branching fractions are measured to be B(ψ(3686)→Ξ(1530)0Ξ ̄(1530)0)=(6.77±0.14±0.39)×10-5 and B(ψ(3686)→Ξ(1530)0Ξ ̄0)=(0.53±0.04±0.03)×10-5. Here, the first and second uncertainties are statistical and systematic, respectively. In addition, the parameter associated with the angular distribution for the decay ψ(3686)→Ξ(1530)0Ξ ̄(1530)0 is determined to be α=0.32±0.19±0.07, in agreement with theoretical predictions within one standard deviation
Observation of ψ (3686)→ Ξ (1530)- Ξ ̄ (1530)+ and Ξ (1530)- Ξ ̄ + OBSERVATION of ... ABLIKIM M. et al
No full textUsing 448.1×106 ψ(3686) events collected with the BESIII detector at BEPCII, we employ a single-baryon tagging technique to make the first observation of ψ(3686)→Ξ(1530)-Ξ̄(1530)+ and Ξ(1530)-Ξ̄+ decays with a statistical significance of more than 10σ and 5.0σ, respectively. The branching fractions are measured to be B(ψ(3686)→Ξ(1530)-Ξ̄(1530)+)=(11.45±0.40±0.59)×10-5 and B(ψ(3686)→Ξ(1530)-Ξ̄+)=(0.70±0.11±0.04)×10-5. The angular distribution parameter for ψ(3686)→Ξ(1530)-Ξ̄(1530)+ is determined to be α=0.40±0.24±0.06, which agrees with the theoretical predictions within 1σ. The first uncertainties are statistical, and the second systematic
SB 1530
No full textSB 1530, Introduced version -- SB 1530-A, A-Engrossed version -- SB 1530-B, B-Engrossed version.Title from PDF caption (viewed on June 18, 2021).This archived document is maintained by the State Library of Oregon as part of the Oregon Documents Depository Program. It is for informational purposes and may not be suitable for legal purposes.Mode of access: Internet from the Oregon Government Publications Collection.Text in English
Observation of psi(3886) -> Xi(1530)(-)(Xi)over-bar(1530)(+) and Xi(1530)(-)(Xi)over-bar(+)
No full textUsing 448.1 x 10(6) psi(3686) events collected with the BESIII detector at BEPCII, we employ a single-baryon tagging technique to make the first observation of psi(3686) -> Xi(1530)(-)(Xi) over bar (1530)(+) and Xi(1530)(-)(Xi) over bar (+) decays with a statistical significance of more than 10 sigma and 5.0 sigma, respectively. The branching fractions are measured to be B(psi(3686) -> Xi(1530)(-)(Xi) over bar (1530)(+)) = (11.45 +/- 0.40 +/- 0.59) x 10(-5) and B(psi(3686) -> Xi(1530)(-)(Xi) over bar (+)) = (0.70 +/- 0.11 +/- 0.04) x 10(-5). The angular distribution parameter for psi(3686) -> Xi(1530)(-)(Xi) over bar (1530)(+) is determined to be alpha = 0.40 +/- 0.24 +/- 0.06, which agrees with the theoretical predictions within 1 sigma. The first uncertainties are statistical, and the second systematic.For complete list of authors see http://dx.doi.org/10.1103/PhysRevD.100.051101</p
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