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C(γ,η)X反应与N(1535)在核内的性质 总被引:15,自引:0,他引:15
在N*(1535)共振模型下,研究了γ在原子核上产生η的反应,通过N衰变的实验数据以及γp→ηp反应确定了模型参数,结果表明,MN*=1550MeV才较好地符合γp→ηp的实验,对12C上的η介子光生的总截面计算发现,N*(1535)在核内的宽度由于多体修正而增大,N*-核的相互作用具有排斥性质. 相似文献
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本文提出了π介子与核子作用产生η粒子的N*(1535)激发模型,计算了在阈能附近的πN→ηN反应截面以及S-波ηN散射长度,并与实验及其他理论作了比较. 相似文献
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利用N*(1535)共振道模型,在DWBA框架下分析计算了核上A(π,η)X单举产生反应,具体给出了12C(π,η)X单举反应的双重微分截面,得到与实验符合较好的结果,给出了N*-N之间是相互吸引作用的结论.计算还发现对于η产生过程,泡利原理的限制是不明显的. 相似文献
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在手征SU(3)夸克模型和扩展的手征SU(3)夸克模型的框架下, 用变分的方法系统地研究了同位旋为0、1, 自旋宇称为0+、1+和2+的udss四夸克系统6个低组态的能量. 模型的参数取自以前的工作, 它能很好地描述核子-核子散射相移以及核子-超子散射截面. S道相互作用的参数由拟合K介子和K*介子的质量定出, 并且考虑了具有相同量子数的态之间的态混合效应. 结果表明, 同位旋为0且自旋宇称为1+的udss能量低于相应的K*K*,的阈能, 且该组态中KK*的成分相当小, 因此该组态的宽度可能较小, 可视为一个可能的四夸克态的候选者. 相似文献
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DONGYu-Bing HEJun 《理论物理通讯》2003,40(3):345-348
Calculations of helicity amplitudes for the low-lying nucleon resonances are displayed based on a non-relativistic constituent quark model with a harmonic oscillator confinement. The explicit effect of quark confinement is shown. Our results show that the effect plays sizable role on some transition amplitudes of S11 (1535) and D13(1520) resonances. The effect on the △(1232) transition amplitudes is less than 10%. However, the effect on the Roper resonance is remarkable but is inconclusive. 相似文献
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Calculations of helicity amplitudes for the low-lying nucleon resonances are displayed based on a non-relativistic constituent quark model with a harmonic oscillator confinement. The explicit effect of quark confinement isshown. Our results show that the effect plays sizable role on some transition amplitudes of S11(1535) and D13(1520)resonances. The effect on the △(1232) transition amplitudes islessthan 10%. However, the effect on the Roper resonanceis remarkable but is inconclusive. 相似文献
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《Nuclear Physics B》1988,299(4):673-692
The dual representation, which gives a simple analytical form for purely gluonic amplitudes, is extended to amplitudes which include a quark-antiquark pair. To minimize the calculations, supersymmetry is used to relate the purely gluonic amplitudes to those including a gluino pair from which the quark-antiquark amplitudes are easily deduced. We explicitly give simple analytical forms for the full amplitudes for those multi-parton processes which involve a quark-antiquark pair plus two, three and four gluons. 相似文献
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G. S. Danilov 《Physics of Atomic Nuclei》2017,80(3):473-490
Multiloop superstring amplitudes are obtained upon integrating local amplitudes with respect to modular parameters of the Schottky supergroup and with respect to vertex coordinates in the nonsplit (1|1) complex supermanifold. Ambiguities in this integration are removed by the condition requiring that the local symmetries of the amplitudes under discussion be conserved. Local superstring amplitudes are calculated by summing local fermion-string amplitudes. The resulting superstring amplitudes are free from divergencies. The vacuum amplitude is zero, in just the same way as the one-, two-, and three-point massless-boson amplitudes are. The amplitudes in question vanish after integration of corresponding local amplitudes with respect to interaction-vertex coordinates and with respect to the limiting points of the Schottky supergroup, with the exception of those (3|2) points that are fixed by SL(2) symmetry. 相似文献
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The fragmentation functions and scattering amplitudes are investigated in the framework of light-front perturbation theory. It is demonstrated that, the factorization property of the fragmentation functions implies the recursion relations for the off-shell scattering amplitudes which are light-front analogs of the Berends–Giele relations. These recursion relations on the light-front can be solved exactly by induction and it is shown that the expressions for the off-shell light-front amplitudes are represented as a linear combinations of the on-shell amplitudes. By putting external particles on-shell we recover the scattering amplitudes previously derived in the literature. 相似文献
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A simple recursive expansion algorithm for the integrals of tree level superstring five point amplitudes in a flat background is given which reduces the expansion to simple symbol(ic) manipulations. This approach can be used for instance to prove the expansion is maximally transcendental to all orders and to verify several conjectures made in recent literature to high order. Closed string amplitudes follow from these open string results by the KLT relations. To obtain insight into these results in particular the maximal R-symmetry violating amplitudes (MRV) in type IIB superstring theory are studied. The obtained expansion of the open string amplitudes reduces the analysis for MRV amplitudes to the classification of completely symmetric polynomials of the external legs, up to momentum conservation. Using Molien?s theorem as a counting tool this problem is solved by constructing an explicit nine element basis for this class. This theorem may be of wider interest: as is illustrated at higher points it can be used to calculate dimensions of polynomials of external momenta invariant under any finite group for in principle any number of legs, up to momentum conservation. 相似文献
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N. Zovko 《Nuclear Physics B》1975,91(3):517-526
It is shown that, contrary to general belief, the uncertainties in the πN amplitudes are sufficient to account for the discrepancy between the Glauber model and the data for high-energy πd elastic scattering at large angles. The essential point is that the πd differential cross section in this kinematic region depends on the fourth power of the πN amplitudes and that, therefore, rather small changes in these amplitudes cause large effects in the πd cross section. Working with leading terms only it is found that more recent solutions for πN amplitudes (which are smaller in magnitude than those used in earlier analyses) may restore the agreement of theory and experiment at large angles. 相似文献
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B.H Kellett 《Annals of Physics》1974,83(1):169-185
The behavior of the invariant amplitudes for processes involving massive vector mesons is investigated in the limit as the mass goes to zero. The constraints of gauge invariance impose a definite structure on the amplitudes at k2 = 0, and the question of the uniqueness of this structure is examined. It is shown that if the limit is smooth, the consequent relations between the massive and massless helicity amplitudes are unique, provided only that any additional dynamical assumptions are made consistently. Some of the implications of this result are discussed, with particular reference to the unambiguous covariant formulation of vector meson dominance for scattering amplitudes. 相似文献
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J. Kwieciński 《Nuclear Physics B》1975,97(3):475-492
The analytic properties of the reggeon-reggeon amplitude in the missing-mass like variable are discussed. (This amplitude is defined through the suitable high-energy limit of the eight-point amplitude). It is shown on the basis of simple Feynman diagrams that it is possible to define reduced amplitudes which are free from kinematical singularities provided that the eight-point amplitude is expressed in a form explicitly consistent with Steinmann relations. In a simple model which is considered in this paper, the reduced amplitudes have the singularity structure of ordinary two-body scattering amplitudes. The finite energy sum rules and four reggeon vertices are also briefly discussed. 相似文献