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1.
The mean lifetime of the hypernucleus Λ3H has been measured in a helium bubble chamber with the result, τ(Λ3H)=(2.46?0.41+0.62)×10?10 sec, based on 16 examples of the decay mode Λ3H→π?+3He and 24 examples of the decay mode Λ3H→π?+p+d. The decay branching ratio R3 = Γ(Λ3H → π?+3He)/Γ(Λ3H → all π? modes) has been estimated to be 0.30 ± 0.07.  相似文献   

2.
A. Deloff 《Nuclear Physics A》1974,236(2):469-490
Angular distributions and energy spectra for the decay modes Λ4He→π?p3He, Λ4H → π?p3H, Λ4H → π?n3He are calculated and compared with experiment. Final state nuclear interactions have been adjusted to fit the corresponding scattering data. With S-, P- and D-wave interactions we were able to obtain reasonably good agreement with the experimental decay spectra. It is suggested that the Λ4H → π?n3He decay spectra may be decisive in selecting the right set of p3H complex phase shifts from several possible solutions.  相似文献   

3.
The exclusive reaction pp→Λ°K+p has been studied at 0.1<?tpp<0.6 GeV2 and energies √s=45 GeV and 53 GeV at the CERN ISR. Diffractive excitation p→Λ°K+ occurs predominantly in the mass range M(Λ°K+)≈2.1 GeV and peaks at 1.7 GeV. The cross section for pp→Λ°K+p is 10±3μb for M(Λ°K+)<2.5 GeV, and the tpp dependence is exp (bt) with b=7.0±0.5 GeV?2.  相似文献   

4.
Hidekatsu Nemura 《Few-Body Systems》2013,54(7-10):1223-1226
We present our recent study on ΛN and ΣN (isospin I = 3/2) interactions by measuring Nambu–Bethe–Salpeter wave functions on the Lattice QCD. The lattice QCD calculation is performed by using the N f  = 2 + 1 gauge configurations generated by PACS-CS collaboration together with employing an improved method to obtain potentials in lattice QCD simulations. For the 1 S 0 channel, the central ΣN (I = 3/2) potential and the central ΛN (1 S 0) potential are found to be very similar. For the spin triplet (3 S 1?3 D 1) channels, the central ΛN(3 S 1?3 D 1) potential is attractive while the central ΣN(I = 3/2, 3 S 1?3 D 1) potentials is repulsive. Tensor potentials, on the other hand, are rather weak in both ΛN and ΣN(I = 3/2) systems.  相似文献   

5.
X-band electron paramagnetic resonance (EPR) studies are carried out on Fe3+ ions doped in ammonium dihydrogen phosphate (ADP) single crystals at room temperature. The crystal field and spin Hamiltonian parameters are evaluated from the resonance lines obtained at different angular rotations. The obtained values of spin Hamiltonian and zero-field parameters of the Fe3+ ion in ADP are: g = 1.994 ± 0.002, |D| = (220 ± 5) × 10?4 cm?1 and a = (640 ± 5) × 10?4 cm?1. On the basis of EPR data, the site symmetry of the Fe3+ ion in the crystal is discussed. The Fe3+ ion enters the lattice substitutionally replacing the NH4 + sites. The optical absorption of the crystal is also studied at room temperature in the wavelength range of 195–925 nm. The energy values of different orbital levels are calculated. The observed bands are assigned as transitions from the 6 A 1g (S) ground state to various excited quartet levels of the Fe3+ ion in a cubic crystalline field. From the observed band positions, Racah interelectronic repulsion parameters (B and C), cubic crystal field splitting parameter (D q ) and Trees correction are calculated. There values are: B = 970, C = 1,923, D q  = 1,380 cm?1 and α = 90 cm?1, respectively. On the basis of EPR and optical data, the nature of bonding in the crystal is discussed. The zero-field splitting (ZFS) parameters are also determined theoretically using B kq parameters estimated from the superposition model. The values of ZFS parameters thus obtained are |D| = (213 ± 5) × 10?4 cm?1 and |E| = (21 ± 5) × 10?4 cm?1.  相似文献   

6.
X-band electron paramagnetic resonance (EPR) study of Cr3+-doped dipotassium tetrachloropalladate single crystal is done at liquid nitrogen temperature. EPR spectrum shows two sites. The spin-Hamiltonian parameters have been evaluated by employing hyperfine resonance lines observed in EPR spectra for different orientations of crystal in externally applied magnetic field. The values of spin-Hamiltonian and zero-field splitting (ZFS) parameters of Cr3+ ion-doped DTP for site I are: g x  = 2.096 ± 0.002, g y  = 2.167 ± 0.002, g z  = 2.220 ± 0.002, D = (89 ± 2) × 10?4 cm?1, E = (16 ± 2) × 10?4 cm?1. EPR study indicates that Cr3+ ion enters the host lattice substitutionally replacing K+ ion and local site symmetry reduces to orthorhombic. Optical absorption spectra are recorded at room temperature. From the optical absorption study, the Racah parameters (B = 521 cm?1, C = 2,861 cm?1), cubic crystal field splitting parameter (Dq = 1,851 cm?1) and nephelauxetic parameters (h = 2.06, k = 0.21) are determined. These parameters together with EPR data are used to discuss the nature of bonding in the crystal.  相似文献   

7.
From about 6×106 stoppingK ?-meson reactions in the Saclay 80 cm hydrogen bubble chamber 70Σ ?→Λe?¯ν and 11Σ+→Λe+ν decays have been identified. The ratio of the vector to axial vector coupling constant has been determined,f 1/g 1=?0.22±0.28, consistent with the predictionf 1=0 of the CVC-theory. The branching ratios for the two decay modes are,Γ(Σ ?→Λe?ν)/Γ(Σ?→ all modes)=(0.69±0.12). 10?4,Γ+→Λe+ν)/Γ(Σ+→ all modes)=(0.29±0.10). 10?4. The ratio, Γ(Σ+→Λe+)/Γ(Σ?→Λe?v)=0.69±0.18, agrees with the phase space ratio, 0.61, therefore a theory that includes no second class currents is consistent with the data.  相似文献   

8.
A Nd3+:Na2La4(WO4)7 crystal with dimensions of ? 17 × 30 mm3 was grown by the Czochralski method. The thermal expansion coefficients of Nd3+:Na2La4(WO4)7 crystal are 1.32 × 10?5 K?1 along c-axis and 1.23 × 10?5 K?1 along a-axis, respectively. The spectroscopic characteristics of Nd3+:Na2La4(WO4)7 crystal were investigated. The Judd–Ofelt theory was applied to calculate the spectral parameters. The absorption cross sections at 805 nm are 2.17 × 10?20 cm2 with a full width at half maximum (FWHM) of 15 nm for π-polarization, and 2.29 × 10?20 cm2 with a FWHM of 14 nm for σ-polarization. The emission cross sections are 3.19 × 10?20 cm2 for σ-polarization and 2.67 × 10?20 cm2 for π-polarization at 1,064 nm. The fluorescence quantum efficiency is 67 %. The quasi-cw laser of Nd3+:Na2La4(WO4)7 crystal was performed. The maximum output power is 80 mW. The slope efficiency is 7.12 %. The results suggest Nd3+:Na2La4(WO4)7 crystal as a promising laser crystal fit for laser diode pumping.  相似文献   

9.
J. K. Ahn 《Few-Body Systems》2013,54(7-10):1043-1046
While the results of partial-wave analyses agree on the properties of the S = ?1 hyperon resonances (S 01Λ(1670), D 03Λ(1690), and D 13Σ(1670)), there is some disagreement between production and formation experiments in this mass region. Formation experiments observe one Σ resonance in the 1,670 MeV mass region with J p = 3/2? and decaying primarily to ${N\overline{K}, \Lambda\pi}$ , and Σπ. On the other hand, production experiments have found evidence suggesting two Σ resonances in this mass region with comparable values of mass and width. Photoproduction of the hyperon resonances in the Σ(1670) region was measured from the proton in the energy from threshold to 3.0 GeV. Preliminary results from LEPS show some indication of possible different lineshapes and yields in π ? Σ+ and π + Σ? decay modes, which encourage further study in analogy of the Λ(1405).  相似文献   

10.
Electron paramagnetic resonance spectra of Cu2+ impurities in cytosine hydrochloride single crystals are observed at liquid nitrogen temperature. Two magnetically equivalent sites for Cu2+ have been observed. The parameters of 63Cu obtained with the fitting of spectra to rhombic symmetry spin Hamiltonian are: g x  = 2.047 ± 0.002, g y  = 2.187 ± 0.002, g z  = 2.390 ± 0.002, A x  = (86 ± 3) × 10?4 cm?1, A y  = (87 ± 3) × 10?4 cm?1, and A z  = (138 ± 3) × 10?4 cm?1. The observed bands in optical spectra of the single crystal recorded at room temperature are assigned to various d–d and charge-transfer transitions. Using both EPR and optical data, the nature of bonding of metal ion with different ligands is discussed.  相似文献   

11.
L. N. Patro  K. Hariharan 《Ionics》2013,19(11):1611-1617
Investigation on the X-ray diffraction results of rare earth ions such as Eu3+ and Nd3+ doped BaSnF4 materials indicates that the doped materials show a similar pattern of BaSnF4 with the same tetragonal structure (P4/nmm). The transport properties of the materials have been investigated by impedance spectroscopy, and the results show that the conductivity values are closely related to both concentration and type of the dopant ion. All of these doped materials show an increase in conductivity over un-doped BaSnF4. The highest conductivity is observed in 3 mol% Nd3+ ion-doped BaSnF4 system (9.01?×?10?4 Scm?1), which is about one order higher in comparison to BaSnF4 conductivity (1.1?×?10?4 Scm?1). The room temperature emission spectrum of BaSnF4:Eu3+ and BaSnF4:Nd3+ shows the characteristic bands arising from 5D0?→?7F j (j?=?1, 2, 3, and 4) and 4F3/2 to 4I j (j?=?9/2 and 11/2) transitions of Eu3+ and Nd3+ ions, respectively.  相似文献   

12.
A soft chemical coprecipitation method has been proposed for synthesis of nano-sized multiferroic BiFeO3 (BFO) powders. The X-ray diffraction pattern confirms the perovskite structure of BFO and Rietveld refinement reveals the existence of rhombohedral R3c symmetry. Crystallite size and strain value are studied from Williamson–Hall (W–H) analysis. The transmission electron microscope (TEM) image shows that the particle size of BFO powders lies between 50–100 nm. 4A1 and 7E Raman modes have been observed in the range 100–650 cm?1 and a prominent band centered around 1150–1450 cm?1 have also been observed corresponding to the two-phonon scattering. Differential Thermal Analysis (DTA) shows the existence of two prominent peaks at 330 °C and 837 °C corresponding to the magnetic and ferroelectric ordering, respectively. From the temperature dependent dielectric studies, an anomaly in the dielectric constant is observed at the vicinity of Neel temperature (T N ) indicating a magnetic ordering. Also, BFO shows antiferromagnetic behavior measured from the magnetic studies.  相似文献   

13.
Experimental results concerning the decay modes Λ4H → π?p3H and Λ4He → π?p3He are presented. A sample of Λ4He → π?p3He decays almost free from a contamination of other hypernuclear decay modes was selected. Some experimental distributions are compared with theoretical predictions.  相似文献   

14.
The decay of charmed particles produced by high-energy neutrinos has been studied by an experiment using simultaneously emulsion, bubble chamber and counter techniques. Eight charmed particle candidates, 5 positively charged and 3 neutral, have been found in the emulsion, where their production and decay have been directly observed. One of these events is identified as a Λc+ baryon of mass 2.26±0.02 GeV/c2 which undergoes the decay Λc+→pK?π+ after a proper time of (7.3±0.1) · 10?13 s.A statistical analysis of the other observed decays leads to the mean-life values τ+=(2.5?1.1+2.2) · 10?13 s, τ0=(0.53?0.25+0.57) · 10?13 s, for the sample of charged particles enriched by a similar event found in a previous experiment, and for the sample of 3 neutral particles, respectively. The former value is only slightly affected by including in the sample the Λc+ event or excluding that of the previous experiment.  相似文献   

15.
Kinematic analysis of simple hypernuclear production reactions has produced a sample of hypernuclei of ΛB, ΛC and ΛN with negligible background, and a much smaller sample of ΛBe. The values of the non-mesonic to π? mesonic ratio Q? for the above samples are 5.5 ± 0.5 and 4.3 ± 1.1, respectively. A sub-sample of 11ΛB hypernuclei was separated on the basis of production via an excited state of Λ12C, giving Q? = 4.8 ± 1.1 for Λ11B. Assuming the Fermi gas model is applicable to nuclei of mass A ≈ 11, two independent means of analysis of the non-mesonic decays give values for the Λ-neutron stimulation fraction n of 0.41 ± 0.09 and 0.34 ± 0.07 for hypernuclei of charge 5 ≦ Z ≦ 7.  相似文献   

16.
Aluminum oxide, a promising material for high temperature applications, is synthesized by combustion route and characterized by X-ray diffraction technique. Photoluminescence of aluminum oxide bombarded with 120 MeV swift Au9+ ions have been studied at room temperature. The observed PL emission with peak at ~420 nm is attributed to F-center while the two more weak emissions with peaks at ~482 and ~525 nm are attributed to aggregates of F-centers. It is found that PL intensity increases with increase in Au9+ ion fluence up to ~1×1013 ions cm?2 and thereafter it reaches saturation. The Fourier transform Infrared spectroscopy results show the destruction of Al?O?H bonds whereas the XRD results indicate the surface amorphization of Al2O3.  相似文献   

17.
The γ-spectra induced by stopped K? mesons in 6Li and 7Li targets in coincidence with the accompanying charged pions and π0 mesons. The γ-line at (1.04 ± 0.04) MeV observed with charged pions was identified as a γ-transition in Λ4H, whereas the γ-line at (1.15 ± 0.04)_MeV observed with π0 mesons was ascribed to a γ-transition in Λ4He. Using these new values for the excitation energies of the 1+ levels of Λ4H and Λ4He hypernuclei, the phenomenological ΛN potential for the s-state interaction was recalculated.  相似文献   

18.
Let ?1, ?2, ?3, ?4 be irreducible representations of a compact connected semisimple Lie group G with highest weights Λ1, Λ2, Λ3, Λ4, respectively. Let ?1?2 (resp. ?3?4) be irreducible representations of G with highest weights Λ1·Λ2 (resp. Λ3·Λ4). It is assumed that one knows the Clebsch-Gordan series of ?1??3 and ?2??4 (resp. of S2?1, S2?2, A2?1 and A2?2). Then we formulate a result (Theorem 2) which gives information on the decomposition of ?1?2??3?4 (resp. of S2(?1?2) and A2(?1?2)). Though this result is not complete, it is useful because it delivers the information very quickly and in a very simple manner.  相似文献   

19.
Two siloxane-based di-urethanesil frameworks incorporating poly(oxyethylene) (POE) chains have been synthesized by the sol–gel process and doped with magnesium triflate (Mg(CF3SO3)2) with the goal of developing electrolytes for the fabrication of solid-state rechargeable magnesium batteries. In these matrices, short POE chains are covalently bonded to the siloxane network via urethane linkages. The xerogels have been represented by the notation d-Ut(Y) n Mg(CF3SO3)2, where Y?=?300 and 600 represents the average molecular weight of the POE chains and n stands for salt composition (molar ratio of OCH2CH2 units per Mg2+). Xerogels with compositions ranging from 2?≤?n?<?∞ were prepared. A crystalline POE/Mg(CF3SO3)2 complex of unknown stoichiometry is formed in the d-Ut(300) n Mg(CF3SO3)2 materials with n?≤?6 and in the d-Ut(600) n Mg(CF3SO3)2 materials with n?≤?5. The organically modified silicate electrolytes with the highest conductivity of the d-Ut(300) n Mg(CF3SO3)2 and d-Ut(600) n Mg(CF3SO3)2 series are the samples with n?=?6 (3.9?×?10?8 S cm?1 at 26 °C and 8.7?×?10?5 S cm?1 at 97 °C) and n?=?100 (2.63?×?10?7 S cm?1 at 20 °C and 1.4?×?10?5 S cm?1 at 85 °C), respectively. Since the electrolytes for Mg batteries that have been proposed up to now have many intrinsic problems and although the room temperature conductivity values exhibited by the systems developed in the present study are still low in view of practical application, this work opens new directions for the development of solid-state Mg ion electrolytes.  相似文献   

20.
5032 proton-emulsion interactions at 400 GeV/c momentum have been carefully scrutinized for production and decay of charged charm particles. In order to detect these decays, shower tracks from 3056 stars have been followed to a maximum length of 1 mm and those from 1976 stars up to 2 mm. A total of 23 three-prong charm-like candidates have been recorded in the forward cone. The background due to γ-overlap on a shower track, trident/pseudo-trident production and secondary interactions is estimated to be 15. Attributing the signal of 8 events to Λc+ and assuming the branching ratio of Λc+ → 3 prong to be 0.6 and τΛc to be 10?13 sec we obtain the production cross section to be 106±39μb/nucleon. Out of these 8 events one example of semileptonic decay of Λc+ is seen.  相似文献   

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