265,938 research outputs found
J.B. McNamara from Rose Baron, August 9, 1937-November 29, 1937
No full textLetters to J.B. McNamara from Rose Baron dated August 9, 1937 to November 29, 1937
J.B. McNamara from Rose Baron, June 7, 1937-July 19, 1937
No full textLetters to J.B. McNamara from Rose Baron dated June 7, 1937 to July 19, 1937
J.B. McNamara from Rose Baron, head of International Labor Defense Prison Relief, December 18, 1934-November 10, 1936
No full textLetters to J.B. McNamara from Rose Baron, head of International Labor Defense Prison Relief, dated December 18, 1934 to November 10, 1936
Matthews, J B (John Baron), QX11387
No full textThis record was harvested from a previous catalogue system and will be withdrawn in 2025. Information in this record may be superseded or incomplete. Visit this record in UMA's new catalogue at: https://archives.library.unimelb.edu.au/nodes/view/402157Surname: MATTHEWS. Given Name(s) or Initials: J B (JOHN BARON). Military Service Number or Last Known Location: QX11387. Missing, Wounded and Prisoner of War Enquiry Card Index Number: 41914.221803
Item: [2016.0049.34450] "Matthews, J B (John Baron), QX11387
Evidence for the decay B0→J/ψω and measurement of the relative branching fractions of meson decays to J/ψη and J/ψη′
No full textFirst evidence of the B 0 → J / ψ ω decay is found and the B s 0 → J / ψ η and B s 0 → J / ψ η ′ decays are studied using a dataset corresponding to an integrated luminosity of 1.0 fb -1 collected by the LHCb experiment in proton-proton collisions at a centre-of-mass energy of sqrt(s) = 7 TeV. The branching fractions of these decays are measured relative to that of the B 0 → J / ψ ρ 0 decay:frac(B (B 0 → J / ψ ω), B (B 0 → J / ψ ρ 0)) = 0.89 ± 0.19 (stat) - 0.13 + 0.07 (syst),frac(B (B s 0 → J / ψ η), B (B 0 → J / ψ ρ 0)) = 14.0 ± 1.2 (stat) - 1.5 + 1.1 (syst) - 1.0 + 1.1 (frac(f d, f s)),frac(B (B s 0 → J / ψ η ′), B (B 0 → J / ψ ρ 0)) = 12.7 ± 1.1 (stat) - 1.3 + 0.5 (syst) - 0.9 + 1.0 (frac(f d, f s)), where the last uncertainty is due to the knowledge of f d / f s, the ratio of b-quark hadronization factors that accounts for the different production rate of B 0 and B s 0 mesons. The ratio of the branching fractions of B s 0 → J / ψ η ′ and B s 0 → J / ψ η decays is measured to befrac(B (B s 0 → J / ψ η ′), B (B s 0 → J / ψ η)) = 0.90 ± 0.09 (stat) - 0.02 + 0.06 (syst)
The Baron, his niece and friends : Friedrich von Hügel as a spiritual director, 1915-1925
No full textWhile the practice of spiritual direction is widespread and increasingly popular, there has been relatively little research on the practices of those perceived to be exemplary spiritual directors. The primary focus of this dissertation is Baron Friedrich von Hügel's spiritual direction of Gwendolen Greene, during the final decade of his life (1915-1925). It also analyses his direction of nine other individuals during this same period, enabling one to recognise and evaluate recurring trends in von Hügel's approach to spiritual nurture.
The key to the interpretation of von Hügel's approach is his conception of the 'Three Elements of Religion,' the Mystical, Intellectual and Institutional Elements. The thesis illustrates through analysis of von Hügel's correspondence and diaries the extent to which these shape his whole approach to spiritual direction.
The research is archival, focusing on von Hügel's letters of spiritual direction and his personal diaries. The methodology is critical historical research, based on a close reading and assessment of the materials available. To this end, a great deal of original material is unearthed and discussed for the purposes of articulating and evaluating the nature of von Hügel's role as a spiritual director.
The findings of this investigation indicate strengths and weaknesses in von Hügel's approach to spiritual direction. His primary contribution is his articulation and utilisation of the 'Three Elements of Religion.' These provide a balanced and holistic approach to spiritual direction. The primary weaknesses in his approach to spiritual direction are evident when he succumbs to values more indicative of the age in which he lived, than of the essence of the Christian tradition
Observations of Bºs→ψ(2S)η and Bº(s)→ψ(2S)π+π- decays
No full textFirst observations of the B0s
→ψ(2S)η, B0 →ψ(2S)π
+
π
− and B0s
→ψ(2S)π
+
π
− decays are made
using a dataset corresponding to an integrated luminosity of 1.0 fb−1 collected by the LHCb experiment in
proton–proton collisions at a centre-of-mass energy of
√
s = 7 TeV. The ratios of the branching fractions
of each of the ψ(2S) modes with respect to the corresponding J/ψ decays are
B(B0s
→ψ(2S)η)
÷
B(B0s
→J/ψη)
= 0.83± 0.14 (stat)±0.12 (syst) ±0.02 (B),
;
B(B0→ψ(2S)π
+
π
−
)
÷
B(B0→J/ψπ
+
π
−
)
= 0.56± 0.07 (stat)±0.05 (syst)± 0.01 (B),
;
B(B0s
→ψ(2S)π
+
π
−
)
÷
B(B0s
→J/ψπ
+
π
−
)
= 0.34± 0.04 (stat)±0.03 (syst)± 0.01 (B),
where the third uncertainty corresponds to the uncertainties of the dilepton branching fractions of the J/ψ
and ψ(2S) meson decays
Étude de l'activité tonique posturale et son enregistrement
No full textBaron J.-B. Étude de l'activité tonique posturale et son enregistrement. In: Bulletin de psychologie, tome 24 n°291, 1971. Thèmes et travaux de recherche du laboratoire de psychophysiologie de l'Université de paris VI. pp. 471-472
Measurement of the branching fraction
No full textThe B
0
s
→ J/ψK
0
S
branching fraction is measured in a data sample corresponding to 0.41 fb−1
of integrated luminosity collected with the LHCb detector at the LHC. This channel is sensitive to
the penguin contributions affecting the sin 2β measurement from B
0
→ J/ψK
0
S
. The time-integrated
branching fraction is measured to be B(B
0
s
→ J/ψK
0
S
) = (1.83±0.28)×10−5
. This is the most precise
measurement to date
Measurement of the B0–B0 oscillation frequency Δmd with the decays B0→D−π+ and B0→ J/ψK∗0
No full textThe B
0
–B
0
oscillation frequency Δmd is measured by the LHCb experiment using a dataset corresponding
to an integrated luminosity of 1.0 fb−1
of proton–proton collisions at √
s = 7 TeV, and is found to be
Δmd
=0.5156±0.0051 (stat.)±0.0033 (syst.) ps−1
. The measurement is based on results from analyses
of the decays B
0
→ D
−π
+ (D
−
→ K
+π
−π
−) and B
0
→ J/ψK
∗0
(J/ψ →μ
+μ
−,K
∗0
→ K
+π
−) and
their charge conjugated modes
- …
