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961.
贾宝路 胡钧 何建军 许世伟 H.Yamaguchi D.Kahl 马朋 苏俊 王宏伟 T.Nakao Y.Wakabayashi T.Teranishi K.I.Hahn J.Y.Moon H.S.Jung T.Hashimoto A.A.Chen D.Irvine C.S.Lee S.Kubono 《原子核物理评论》2019,36(1):37-42
14O (α,p)17F是天体X射线暴中重要的突破反应。本工作通过厚靶方法测量其逆反应1H (17F,α)14O的反应截面来研究这一关键反应。本实验工作是在日本东京大学原子核科学研究中心(CNS)的低能次级束流线(CRIB)上完成的,后续的扣除本底实验是在兰州放射性束流线(RIBLL1)上完成的。CRIB实验是通过2H (16O,n)17F转移反应产生17F次级束,经过CRIB分离提纯之后,利用该次级束轰击氢气靶。在氢气靶后布置了三套望远镜探测器系统,用以探测不同实验角度的反冲α粒子,在数据处理的过程中经过动力学重构后得到了1H (17F,α)14O反应在质心系能区Ec.m.=2.7~3.4 MeV的反应截面。实验结果在3 MeV以上的高能区与前人的薄靶实验数据是一致的,在低能区本工作获得了新的实验数据,倾向于支持干涉相消的理论预言结果。The 14O(α, p)17F reaction is one of the important breakout reactions in type I X-ray burst. This work reported a new cross section measurement of its reverse reaction of 1H(17F,α)14O. The experiment was performed using the CNS radioactive ion beam separator (CRIB), located at the Center for Nuclear Study (CNS), the University of Tokyo. The sequent background measurement was carried out at Radioactive Beam Line in Lanzhou (RIBLL1). 17F beam was produced via the transfer reaction of 2H(16O, n)17F, subsequently separated and purified by CRIB and bombarded a thick hydrogen H2 gas target. The recoiling α particles were measured by three △E-E silicon telescopes at three different angles. The total cross sections of 1H(17F,α)14O have been derived at Ec.m.=2.7~3.4 MeV based on an isotropic angular distribution assumption. Our results are consistent with the previous ones in the energy region of Ec.m.>3 MeV, and we also obtained some new data in the low energy region, which partly support the destructive interference between the direct and resonant reaction mechanism predicted by the theory. 相似文献
962.
Mitsuhiro Okuda Masaki Takeguchi Motohiro Tagaya Toru Tonegawa Ayako Hashimoto Nobutaka Hanagata Toshiyuki Ikoma 《Micron (Oxford, England : 1993)》2009,40(5-6):665-668
Elemental distribution of calcium, phosphorus, oxygen, and carbon in a single collagen fibril obtained from tilapia fish scales was identified with an electron energy-loss spectroscopy and an energy-filtered transmission electron microscopy, for the first time. The carbon intensity profile of the single collagen fibril showed the specific D-periodic pattern at 67 nm of type I collagen fibrils. The calcium L2,3-edge and oxygen K-edge peak positions were detected at 347/350 eV and 137 eV, respectively, and these positions were identical to those of hydroxyapatite. Calcium, phosphorus, and oxygen were present in the hole zones as the amorphous phase, while carbon was present in the overlap zone. Our results indicated that the hole zones preferentially attract calcium and phosphate ions and thus serve as possible nucleation sites for mineralization. 相似文献
963.
HAN Yun-cheng N.Chiga Y.Fujii K.Futatsukawa O.Hashimoto K.Hirose T.Ishikawa H.Kanda M.Kaneta D.Kawama Konno MA Yue K.Maeda T.Maruta N.Maruyama A.Matsumura Y.Miyagi K.Miwa S.N.Nakamura A.Sasaki H.Shimizu K.Shirotori K.Suzuki T.Tamae H.Tamura K.Tsukada WANG Tie-shan H.Yarnazaki 《原子核物理评论》2009,26(Z1)
The reactions γd→π~- pp and γd→npπ~+π~- have been studied in an energy range from 0.8 to 1.1 GeV at the tagged photon facility of Laboratory of Nuclear Science,T ohoku University.Charged pions and protons in the final state were measured by using the Neutral Kaon Spectrometer (NKS2).The analysis of the γd→π~- pp was mainly used to check the acceptance of the NKS2 and to calibrate the tagged photon energy.The photoproduction of the Δ~(++)Δ~- was identified in the γd→npπ~+π~- reaction.Since the data analyses are still in progress,we issue an interim report and preliminary results. 相似文献
964.
D.Kawama A.Acha I.Albayrak D.Androic O.Ates P.Baturin B.Beckford W.Boeglin A.Bruell C.Chen M.Christy R.Ent H.Fenker Y.Fujii M.Furic D.Gaskell S.Gogami O.Hashimoto T.Horn V.Hungerford Ed M.Jones H.Kanda C.Keppel M.Kohl L.Kramer Y.Li A.Liyanage P.Markowitz T.Maruta A.Matsumura S.N.Nakamura T.Petkovic B.Raue J.Reinhold T.Seva A.Shichijo G.Smith L.Tang N.Taniya W.Vulcan T.Walton S.A.Wood T.Yamamoto Z.Ye K.Yokota L.Yuan L.Zhu 《原子核物理评论》2009,26(Z1)
We are now preparing for the third generation (e,e′K~+) A hypernuclear spectroscopic experiment at Hall C,Jefferson Lab (USA).The goal of the experiment is the precise spectroscopy of hypernuclei in wide mass region.We have constructed a new high resolution electron spectrometer "HES" dedicated to (e,e′K~+) hypernuclear study in Japan and it was shipped to JLab in February,2008.We will discuss about the physics of the (e,e′K~+) hypernuclear study at JLab and report the current preparation status of the third generatrion experiment. 相似文献
965.
Takaaki Sakai Hiroshige Matsumoto Reiri Yamamoto Takao Kudo Sachio Okada Masato Watanabe Shin-ichi Hashimoto Hitoshi Takamura Tatsumi Ishihara 《Ionics》2009,15(6):665-670
An electrode design with no use of three-phase boundary was investigated using palladium electrode. The hydrogen evolution
rate of the palladium electrode cell using SrZr0.9Y0.1O3 − α
electrolyte followed Faraday’s law up to 180 mA cm−2, and the anode and cathode overpotentials were significantly lower than those of a platinum electrode cell, suggesting that
the palladium electrode is effective to improve the performance of the hydrogen-pumping cell using SrZrO3-based electrolyte. The rate-determining step (RDS) for electrode reaction was also investigated by changing the electrode
morphology and hydrogen partial pressure, and it was suggested that the RDS of the anode is a reaction at electrode/electrolyte
interface. 相似文献
966.
Noumi H Saha PK Abe D Ajimura S Aoki K Bhang HC Endo T Fujii Y Fukuda T Guo HC Imai K Hashimoto O Hotchi H Kim EH Kim JH Kishimoto T Krutenkova A Maeda K Nagae T Nakamura M Outa H Sekimoto M Saito T Sakaguchi A Sato Y Sawafta R Shimizu Y Takahashi T Tang L Tamura H Tanida K Watanabe T Xia HH Zhou SH Zhu LH Zhu XF 《Physical review letters》2002,89(7):072301
We have studied the (pi(-),K+) reaction on a silicon target to investigate the sigma-nucleus potential. The inclusive spectrum was measured at a beam momentum of 1.2 GeV/c with an energy resolution of 3.3 MeV (FWHM) by employing the superconducting kaon spectrometer system. The spectrum was compared with theoretical calculations within the framework of the distorted-wave impulse approximation, which demonstrates that a strongly repulsive sigma-nucleus potential with a nonzero size of the imaginary part reproduces the observed spectrum. 相似文献
967.
We have studied optical properties of near-infrared (NIR) spectra and birefringence of the manganese phthalocyanine (MnPc) thin films. The morphology of the MnPc thin film grown on KCl (0 0 1) substrates was observed by using an atomic force microscope. The NIR spectral range of 1.0-1.7 μm was studied in this study, because that of 1.3-1.5 μm is known as an optical communication wavelength. The birefringence was measured with changing the growth condition of a deposition rate and a substrate temperature. The birefringence of the film was most affected by the deposition rate. 相似文献
968.
H. Yazawa T. Shioyama H. Hashimoto F. Kannari R. Itakura K. Yamanouchi 《Applied physics. B, Lasers and optics》2010,98(2-3):275-282
We experimentally investigate how parameters of ultrashort laser pulses such as the pulse width and wavelength could induce changes in the dynamics of vibrational wave packets on the light-dressed-potential energy surface (LD-PES) of C2H5OH+ using a pump-and-probe pulse excitation scheme. The probability of non-adiabatic transition at 800 nm from the singly ionized ground state to the repulsive excited state leading to C–O bond breaking is enhanced when a probe laser pulse is delayed by ~180 fs. At this pulse delay, on the other hand, C–C bond breaking is significantly suppressed. Therefore, the deformation of LD-PES is considered to change the direction of the wave packet traveling originally along the C–C stretching into the direction along the C–O stretching. This non-adiabatic transition leading to the redirection of the dissociating wave packet is found to occur more efficiently at the probe laser wavelengths at 400 nm than at 800 nm. The critical pulse delay is still ~180 fs even at 400 nm. 相似文献
969.
Ogura M. Minamisono K. Sumikama T. Nagatomo T. Iwakoshi T. Miyake T. Hashimoto K. Kudo S. Arimura K. Ota M. Akutsu K. Sato K. Mihara M. Fukuda M. Matsuta K. Akai H. Minamisono T. 《Hyperfine Interactions》2001,136(3-8):195-199
It was confirmed by detecting the β-NMR of 12B (I
π=1+, T
1/2=20.2 ms) in a TiO2 (rutile) crystal that the nuclear spin polarization of 12B was totally maintained in the crystal as produced through a nuclear reaction before implantation. Two locations, site 1
and site 2, were found with the relative populations 9 and 1, respectively, and the electric field gradients (EFGs) at those
sites were obtained to be q(site 1)=+(37.1±0.5)1015 V/cm2, η(site 1)<0.03, q(site 2)=+(185±5)1015 V/cm2 and η(site 2)=0.62±0.02. We also found that about 30% of the initial polarization of 8Li (I
π=2+, T
1/2=838 ms) was maintained in the crystal. Since the polarizations of other β emitting nuclei, 12,16N, 13,19O, and 41Sc were also totally maintained in the crystal, the crystal can be a “Spin Dewar” in which many short-lived nuclides can be
implanted with their polarizations totally maintained during their lifetimes for the studies not only on the electronic structure
of impurities in it but also on the nuclear properties.
This revised version was published online in September 2006 with corrections to the Cover Date. 相似文献
970.
Tanida K Tamura H Abe D Akikawa H Araki K Bhang H Endo T Fujii Y Fukuda T Hashimoto O Imai K Hotchi H Kakiguchi Y Kim JH Kim YD Miyoshi T Murakami T Nagae T Noumi H Outa H Ozawa K Saito T Sasao J Sato Y Satoh S Sawafta RI Sekimoto M Takahashi T Tang L Xia HH Zhou SH Zhu LH 《Physical review letters》2001,86(10):1982-1985
We report on the first measurement of a hypernuclear gamma-transition probability. gamma rays emitted in the E2(5/2(+)-->1/2(+)) transition of (7)(Lambda)Li were detected by a large-acceptance germanium detector array (Hyperball), and the lifetime of the parent state ( 5/2(+)) was determined by the Doppler shift attenuation method. The obtained result, 5.8(+0.9)(-0.7)+/-0.7 ps, was then converted into the reduced transition probability [ B(E2)] to be B(E2;5/2(+)-->1/2(+)) = 3.6+/-0.5(+0.5)(-0.4) e(2) fm(4). Compared with the B(E2) of the corresponding E2(3(+)-->1(+)) transition in the 6Li nucleus, our result gives evidence that the size of the 6Li core in (7)(Lambda)Li is smaller than the 6Li nucleus in the free space. 相似文献