共查询到20条相似文献,搜索用时 31 毫秒
1.
D. B. Gin V. G. Kiptily A. A. Pasternak I. N. Chugunov A. E. Shevelev G. Gorini M. Tardocchi M. Nocente JET-EFDA contributors 《Bulletin of the Russian Academy of Sciences: Physics》2011,75(7):931-936
A parametrization of the partial cross section of the 9Be(α, nγ)12C reaction in the α-particle energy range of 0.3–7.9 MeV is presented, along with the count rates of γ quanta. The need to
consider subbarrier (Eα < 1.9 MeV) α-particles in plasma for temperatures T
α < 0.2 MeV is substantiated. The shapes of the Doppler-broadened 4.44 MeV γ line and the count rates of γ quanta in the plasma
of the JET tokamak are measured for the first time and compared to the calculated values. An estimated T
α ≲ 160 keV is obtained. 相似文献
2.
O. G. Tchikilev S. A. Akimenko G. I. Britvich K. V. Datsko A. P. Filin A. V. Inyakin V. A. Khmelnikov A. S. Konstantinov I. Ya. Korolkov V. M. Leontiev V. P. Novikov V. F. Obraztsov V. A. Polyakov V. I. Romanovsky V. I. Shelikhov V. A. Uvarov O. P. Yushchenko V. N. Bolotov S. V. Laptev V. A. Duk A. Yu. Polyarush 《Physics of Atomic Nuclei》2007,70(1):29-34
Using data collected with the ISTRA+ spectrometer during the 2001 run of the U-70 proton synchrotron in Protvino, the first
observation of the radiative kaon decay K
− → μ−π0γν is reported. The ratio Br(K
μ3γ, 5 < E*γ < 30 MeV)/Br(K
μ3) is found to be [0.270 ± 0.029(stat.) ± 0.026(syst.)]% and the ratio Br(K
μ3γ, 30 < E*γ < 60 MeV)/Br(K
μ3) = [0.0448 ± 0.0068(stat.) ± 0.0099(syst.)]%. These ratios are consistent with the theoretical predictions 0.21 and 0.047%,
respectively. The measured angular distribution asymmetry for the region 5 < E*γ < 30 MeV, A(cos ϑ*μγ) = 0.093 ± 0.141, is two standard deviations away from the theoretical prediction of 0.354. The measured asymmetry in the
T-odd variable ξ = pγ · (pμ × pπ)/m
K
3
is −0.03 ± 0.13.
The text was submitted by the authors in English. 相似文献
3.
U. Siodlaczek P. Achenbach J. Ahrens H.-J. Arends R. Beck R. Bilger H. Clement V. Hejny J.D. Kellie M. Kotulla B. Krusche V. Kuhr R. Leukel J.C. McGeorge V. Metag R. Novotny V. Olmos de León F. Rambo M. Schepkin A. Schmidt H. Ströher G.J. Wagner Th. Walcher J. Weiß F. Wissmann M. Wolf 《The European Physical Journal A - Hadrons and Nuclei》2000,9(3):309-311
The reaction γd↦π0
X has been measured with TAPS at MAMI in the energy range E
γ = 140-300 MeV. Using the Glasgow tagging spectrometer a photon energy resolution of 0.8 MeV was achieved. The energy excitation
functions of integral and differential total cross-sections show no structures of statistical significance > 2σ. Upper limits
for the production of narrow isoscalar or isovector dibaryons with masses m? 2100 MeV/c2 were deduced. They are in the range 2-5 μb averaged over the 0.8 MeV energy resolution.
Received: 25 October 2000 / Accepted: 24 November 2000 相似文献
4.
T.T.-H. Yau I.J.D. MacGregor J. Ahrens J.R.M. Annand R. Beck D. Branford P. Grabmayr S.J. Hall P.D. Harty T. Hehl D.G. Ireland J.D. Kellie T. Lamparter K. Livingston M. Liang J.A. MacKenzie S. McAllister J.C. McGeorge R.O. Owens M. Sauer R. Schneider D.P. Watts 《The European Physical Journal A - Hadrons and Nuclei》1998,1(3):241-244
The angular distribution of nucleons emitted in the 12C(γ,pn) reaction has been measured using tagged photons at the Mainz microtron MAMI. The variation of the reaction strength
with the polar angles of the two emitted nucleons is reported for Eγ=120−150 MeV. The proton angular distribution peaks at more backward angles than the 2H(γ,p) differential cross section indicating a departure from the simple quasi-deuteron model of 2N photo-emission. The distribution
shape is in reasonable agreement with microscopic theoretical models which include both π- and ρ-exchange.
Received: 3 September 1997 / Revised version: 17 December 1997 相似文献
5.
We further discuss possible sgoldstino interpretation of the observation, reported by the HyperCP collaboration, of three
Σ+ → pμ+μ− decay events with the dimuon invariant mass 214.3 MeV within the detector resolution. With a sgoldstino mass equal to 214.3
MeV, this interpretation can be verified at existing and future B and ϕ factories. We find that the most natural values of the branching ratios of two-body B and D meson decays to sgoldstino P and vector meson V are about 10−6−10−7. The branching ratios of ϕ meson decay ϕ → Pγ are estimated to be in the range 1.8 × 10−13−1.6 × 10−7, depending on the hierarchy of supersymmetry-breaking soft terms. Similar branching ratios for ρ and ω mesons are in the
range 10−14−3.4 × 10−7.
The text was submitted by the authors in English. 相似文献
6.
A. P. Dubenskii E. A. Boykova 《Bulletin of the Russian Academy of Sciences: Physics》2011,75(7):946-948
The photoexcitation of isomer 157m
Gd (11/2-, 426 keV, T
1/2 = 18.5 μs) in reaction (γ, γ′) was studied on the pulsed nonferromagnetic betatron at St. Peterburg State University. Only
two strong intermediate structures (IntS) with E
1 = 4.0 ± 0.1 MeV, (σΓ)1iso = 5 eV b and E
2 = 5.3 ± 0.1 MeV, (σΓ)2iso = 40 eV b, respectively, were found. Comparison of the spectra IntS of isomers 157m
Gd and 181m
Ta demonstrates the weak correlation between isomer excitation probabilities and ground states deformation parameters. 相似文献
7.
Mixing angles of η and η′ mesons are obtained in the scheme of octet-singlet mixing θη = −15.4°, θ′η = −17.9°, and in the scheme connected with expansion in the quark basis $
\bar q
$
\bar q
q − $
\bar s
$
\bar s
s φ = 39.3°. The constants gV
ηγ, g
η′
V
γ of radiative decays η′ → V
γ and V → ηγ (V ≡ ρ, ω, φ) and the ratios of constants of weak decays of η and η′ mesons are calculated. The numerical values that were found
are in agreement with the experimental data. 相似文献
8.
J. Mrázek M. Honusek A. Špalek J. Bielčík J. Slívová J. Adam A.A. Pasternak 《The European Physical Journal A - Hadrons and Nuclei》1999,5(4):399-408
The results of in-beam investigations of excited states of 99Ru using the 98Mo(α,3n) reaction are presented. Angular distributions of γ–rays and γ–γ coincidences have been measured. Excited states have
been identified up to an energy of E = 5603 keV and spin of Iπ= 31/2−. Mean lifetimes τ have been determined using the DSA method for eleven levels. Aligned angular momenta are discussed and
the probable (νh
11/2) origin of a backbending at frequency about 0.5 MeV was confirmed. The possible role of (νd
5/2) alignment at frequencies above 0.5 MeV was pointed out.
Received: 13 January 1999 / Revised version: 26 March 1999 相似文献
9.
M. Wolf J. Ahrens R. Beck V. Hejny J.D. Kellie M. Kotulla B. Krusche V. Kuhr R. Leukel V. Metag J.C. Nacher R. Novotny V. Olmos de León R.O. Owens F. Rambo A. Schmidt M. Schumacher U. Siodlaczek H. Ströher J. Weiß F. Wissmann 《The European Physical Journal A - Hadrons and Nuclei》2000,9(1):5-8
Double neutral pion photoproduction from the proton has been measured at MAMI for photon energies between threshold and 820
MeV. The reaction was identified by an invariant mass and missing mass analysis. From threshold up to 370 MeV the total cross-section
does not exceed 30 nb. For higher energies it shows a smooth rise until it reaches a maximum of about 10 μb at E
γ = 740 MeV. Dalitz plots of m
2(π0π0) versus
m
2(p,π0) for seven bins of incident photon energy have been analysed. For E
γ > 610 MeV, a strong contribution of a sequential decay is observed with the Δ(1232)-resonance as intermediate state. A comparison
to model calculations shows that these sequential decays presumably originate from the D
13(1520) and also the P
11(1440)-resonance.
Received: 6 June 2000 / Accepted: 18 August 2000 相似文献
10.
B. M. Forster J. M. Bailey G. A. Beer J. L. Beveridge J. H. Brewer W. N. Hardy T. M. Huber K. R. Kendall A. R. Kunselman J. A. Macdonald G. M. Marshall G. R. Mason A. Olin M. Senba J. B. Warren 《Hyperfine Interactions》1991,65(1-4):1007-1013
Muonic hydrogen isotopes (μ− p, μ− d, and μ−t) are simple quantum mechanical systems ideally suited for studies of numerous fundamental phenomena in electroweak and strong
interactions as well as in applied areas such as muon chemistry or muon catalyzed fusion.
Emission of muonic hydrogen isotopes into vacuum helps to overcome the limitations which are normally imposed on conventional
investigations with gaseous and liquid targets. A proof of principle experiment for this new technique was performed at TRIUMF
last year. Negative muons with 30 MeV/c momentum were stopped in a thin film of solid hydrogen and produced very low energy μ−d in vacuum. The distribution center of the normal velocity components of emitted μ−d atoms was measured to be ∼1 cm/μs. The yield of μ−d in vacuum is an increasing function of H2 film thickness δ up to a value of δ≥1 mm. 相似文献
11.
L. I. Galanina N. S. Zelenskaya I. A. Konyukhova 《Bulletin of the Russian Academy of Sciences: Physics》2011,75(4):561-565
The differential cross sections of the 28Si(α, αγ)28Si reaction at E
α = 30.3 MeV, calculated according to the coupled channel method (CCM) with the FRESCO program, are presented for a wide α-particle
scattering region with the excitation of the lower 28Si states (0+, ground; 2+, 1.78 MeV; 4+, 4.62 MeV; 0+, 4.96 MeV; 3− + 4+, 6.88 MeV + 6.89 MeV). The coupling factors are calculated in the Nilsson model. 相似文献
12.
B. Cameron Reed 《Central European Journal of Physics》2005,3(1):1-7
The ground-state energy of neutral helium is estimated variationally with a trial wavefunction of the form ϕ≈e
−γ(rA/a
o)ne−γ(rB/a
o)n. This model represents a modification of traditional textbook examinations of this problem via inclusion of the power “n”
as a second nonlinear variational parameter in addition to the usual effective nuclear charge γ and leads to an upper-limit
on the ground state energy of −2.86107 E
h
(E
h
=1 hartree) in comparison with the traditional (n=1) result of −2.84766 E
h
. This result represents a reduction of the percentage overestimate from the true ground-state energy (−2.90373 E
h
) of from 1.93 to 1.47. In comparison with the maximum accuracy obtainable from an uncorrelated trial wavefunction, −2.86168
E
h
, the present trial wavefunction reduces the percentage overestimate from 0.49 (n=1) to 0.021. The optimum values of (n, γ)
are determined to be ≈(0.897, 1.825). 相似文献
13.
T. Sasanuma A. Taniguchi M. Tanigaki Y. Ohkubo Y. Kawase 《Hyperfine Interactions》2004,159(1-4):251-255
The g-factor of the first excited state of 93Sr (E = 213 keV, T
1/2 = 4.6 ns) was measured by an on-line TDPAC technique with use of the strong hyperfine field in Fe metal. The Larmor frequency
ω
L = (2.60 ± 0.15) × 108 rad/s was obtained. The g-factor is derived as g = −0.227 ± 0.013 from g = −ℏω
L/B
hf
μ
N. If the spin of the first excited state of 93Sr is assumed to be 3/2, the g-factor is predicted by a simple core-excitation model as g = −0.22, which is in good agreement with the present experimental result. 相似文献
14.
Preliminary data on the reactions e
+
e
−→φ→γ f
0(980)→γπ0π0 together with data on ππ scattering and the reactions J/ψ→φπ+π− and K
−
p→π +π−(Λ,Σ) are analyzed. The analysis shows that the mass of the f
0(980) meson is
= 950 MeV, and BR(φ→γf
0→γπ0π0)≃ 1× 10−4, indicating that the f
0(980) resonance is of a four-quark nature.
Pis’ma Zh. éksp. Teor. Fiz. 67, No. 7, 445–449 (10 April 1998) 相似文献
15.
We calculate the contribution of semi-hadronic states with the pseudoscalar P = π0, η and scalar (σ(550)) meson accompanied with a real photon as an intermediate state of a heavy photon to the anomalous magnetic
moment of the muon. We consider the intermediate states with π0 and σ as hadrons in the frame-work of the Nambu-Jona-Lasinio (NJL) model. The contribution of the π0γ state is in agreement with results obtained in previous theoretical considerations as well as with the experimental data
$
a_\mu ^{\pi _0 \gamma } \approx 4.5 \times 10^{ - 10}
$
a_\mu ^{\pi _0 \gamma } \approx 4.5 \times 10^{ - 10}
, besides we estimate a
μηγ = 0.7 × 10−10, a
μσγ ∼ 1.5 × 10−11, $
a_\mu ^{\pi ^ + \pi ^ - \gamma } \sim 3.2 \times 10^{ - 10}
$
a_\mu ^{\pi ^ + \pi ^ - \gamma } \sim 3.2 \times 10^{ - 10}
. We also discuss the light-by-light (LbL) mechanism with a
μ
lbl
= 10.5 × 10−10. 相似文献
16.
Silviu Olariu Agata Olariu Diana Martin Anastase Niculescu 《Hyperfine Interactions》2001,135(1-4):71-81
In this paper we study the nuclear transitions induced by incident electrons having an energy of several MeV's. We measured
the cross sections for the excitation of isomeric nuclear states by 7.7 MeV electrons. The cross sections were 1.2 μb for
111m
Cd, 5.5 μb for 113m
In and 7.0 μb for 115m
In. The peak activation rates were 1.8×10−12 s−1 for 111m
Cd, 8.1×10−12 s−1 for 113m
In and 1.0×10−11 s−1 for 115m
In, for a peak power of the electron beam of 1.8×106 W cm−2. Then we describe for the first time the results of a series of experiments in which samples containing the isomeric nuclei
166m
Ho and 186m
Re have been irradiated with MeV electron beams. An upper limit of 17 mb has been determined for the cross section of electron-induced
γ-emission from 166m
Ho and an upper limit of 2.2 mb has been determined for the cross section of electron-induced γ-emission from 186m
Re.
This revised version was published online in July 2006 with corrections to the Cover Date. 相似文献
17.
S. Wolf V. Lisin R. Kondratiev A.M. Massone G. Galler J. Ahrens H.-J. Arends R. Beck M. Camen G.P. Capitani P. Grabmayr F. Härter T. Hehl P. Jennewein K. Kossert A.I. L'vov C. Molinari P. Ottonello R.O. Owens J. Peise I. Preobrajenskij S. Proff A. Robbiano M. Sanzone M. Schumacher M. Schmitz F. Wissmann 《The European Physical Journal A - Hadrons and Nuclei》2001,12(2):231-252
18.
High-statistics data on the γγ → π0η reaction will make it possible to conclude whether the K
+
K
−-loop rescattering mechanism, γγ → K
+
K
− → a
0(980) → π0η, is the main mechanism of the production of a
0(980) isovector resonance. This mechanism provides a reasonable value of 20–30 nb at the maximum for the manifestation of
a
0(980) in the γγ → π0η cross section. It also gives rise to a noticeable narrowing of the a
0(980) peak to its effective (observed) width ≈20–30 MeV in the γγ → π0η channel. The decay width averaged over the resonance mass distribution is 〈Γα
0 → K
+
K
− → γγ〉πη ≈ 0.13 keV. The experimental confirmation of this scenario would be important evidence in favor of the q
2
$
\bar q
$
\bar q
2 nature of light scalar mesons. 相似文献
19.
O. Bartalini V. Bellini J. P. Bocquet P. Calvat A. D’Angelo J. -P. Didelez R. Di Salvo A. Fantini F. Ghio B. Girolami M. Guidal A. Giusa E. Hourany A. S. Ignatov R. Kunne A. M. Lapik P. Levi Sandri A. Lleres D. Moricciani A. N. Mushkarenkov V. G. Nedorezov C. Perrin D. Rebreyend F. Renard N. V. Rudnev T. Russew G. Russo C. Schaerf M. -L. Sperduto M. -C. Sutera A. A. Turinge 《Physics of Atomic Nuclei》2008,71(1):75-82
The total photoabsorption cross section on a free proton was measured at the GRAAL facility in the energy range E
γ = 600−1500 MeV. The large-aperture LAGRANγE detector and a liquid hydrogen target were used in the experiment performed with
a back-scattered Compton gamma beam. To improve the accuracy, two alternative methods were employed. First, a subtraction
method of using empty-target measurements allowed the cross section σ
tot to be evaluated directly because of a low level of the electromagnetic background. Second, an algorithm for evaluating σ
tot on the basis of summing the dominating partial cross sections was developed. Experimental results obtained for σ
tot by the two methods are compared with existing data.
The article was translated by the authors.
Published in Russian in Yadernaya Fizika, 2008, Vol. 71, No. 1, pp. 76–83. 相似文献
20.
W. J. Kossler X. H. Yu A. Greer H. E. Schone C. E. Stronach M. Davis R. S. Cary J. E. Crow W. F. Lankford J. Oostens 《Hyperfine Interactions》1991,63(1-4):81-86
Transverse and zero-field μSR measurements were made on YBa2(Cu1−xNix)3O7−y withx=0.1 and 0.2, and YBa2(Cu1−x
Zn
x
)3O7−y
withx=0.03, 0.06, 0.1, and 0.16, wherey≈0.1. Since doping may lead to magnetic ordering this was searched for with both zero and transverse field μSR, but no evidence
was found over the temperature range studied: 10–100 K. However, depolarization rates as functions of temperature were obtained,
and the low temperature values of these are σ=3.2 μs−1.1.6μs−1, and 1 μs−1 forx=0.01, and 0.2 Ni, respectively, and σ=0.8 μs−1, 0.75 μs−1, 0.65 μs−1, and 0.4 μs−1 forx=0.03, 0.06, 0.1, and 0.16 Zn, respectively. Estimates for the effect of decreasing electron concentration for Zn are made,
but these alone do not account for the drop in σ. Estimates for the effect of scattering on λ and hence σ are made. The reduction
in σ for Ni dopant is in surprisingly good agreement with these estimates. For Zn the order of magnitude is correct, but the
relative lack of further change in σ after the effect of the first 0.03 addition seems to imply a saturation of the effect
of scattering. 相似文献