深度束缚（？）核态的研究
|
摘要
最近,深度束缚K核态是否存在成为大家争论的焦点。本文根据近年来的一些相关理论和实验,用Brueckner-Hartree-Fock方法来考察一些较轻的K核态,以寻求深度束缚态的存在。
在本文中,我们分两个阶段考察奇异核。在第一阶段(早期阶段)我们主要以早期实验发现深度束缚奇异核为依据,构造新的K N相互作用,特别是重点考虑以前理论所忽略的VπΣ,πΣ势。这个新的相互作用能产生一个共振态Λ(1405)即K介子和质子束缚态,以及与实验值相符的散射长度。结果[Li091]表明存在深度束缚K核态,但得到的结合能远远小于上面的实验值。更重要的是我们发现VπΣ,πΣ的作用对体系结合能影响非常大:它一方面降低体系的结合能,另一方面又增加了体系的宽度,因而不能轻易地将它舍弃。
在第二阶段(后期阶段)我们不再简单地把Λ(1405)看作是K介子和质子的束缚态而是两个共振的叠加态。首先建立两个I =0的K N相互作用模型,这两个模型一方面都能产生与实验值相符的散射长度,另一方面它们分别产生两个与实验观测相符的共振态:一个能量为1420MeV,宽度为40 MeV,主要以K N形式衰变;另一个能量为1392MeV,宽度较高达到135 MeV,主要以πΣ形式衰变。当调节这两个共振态的相对权重为7:5,就可以得到与实验相符的Λ(1405)。在此基础上,我们详细考察了一些奇异核(S=-1),发现了深度束缚的K核态。
Recently, many theoretical and experiment efforts have been devoted to investigation of deeply-bound kaonic nuclei. In order to seek possible narrow discrete nuclear bound states, Akaishi and Yamazaki have investigated theoretically several few-body systems and found deeply bound nuclear states with very small widths. They considered the Lamda(1405) state as the bound state of the kaon and proton and its width is caused by coupling to theπΣchannel. The binding energy of K ? ppn( K ? ppnn) they obtained is 108 (86) MeV and the width is 20 (34) MeV. A few years later, in search for quasi-bound states in the K ? ppsystem a three-body K ? NN?πΣNcoupled-channel Faddeev calculation by Shevchenko et al. yields a quasibound state with B K~55-70 MeV, andΓ~90-110 MeV. On the other hand, the strange tribaryons S 1(3140)with T =0 and S 0(3115) with T =1were observed by T. Suzuki and M.Iwasaki et al. in the interaction of stopped K ?mesons with 4 He. Another indication of K ? ppbound state was reported by the FINUDA Collaboration, the binding energy (width) is 115(67) MeV.
But the phenomenological K N interaction Akaishi and Yamazaki given is simple, It contains only one range parameter (0.66 fm) and VπΣ,πΣis set equal to zero. It is known that the latter is very important for the coupled channel consideration. To make phenomenological K N interaction more flexible, we (the first stage) have looked for a new phenomenological K N interaction ( VπΣ,πΣ≠0) with two range parameters. We considered the Lamda (1405) state as the bound state of the kaon and proton, too. The new I =0interaction produces a resonance stateΛ(1405) with EΛ=1406.5-i25 MeV, and gives a scattering length of a I=0=-1.76+i0.6fm which can be compared to Martin’s empirical value a I=0=-(1.70±0.07) + i(0.68±0.04)fm. The relative weight of g I=0with respect to g I=1is 1:5 for K ? pnn, 1:1 for K ? ppn, 3:1 for K ? pp, 1:3 for K ? pn. Within the framework of the Bruechner-Hartree-Fock we have studied these kaonic nuclear states, the binding energy of K ? ppn( K ? ppnn) we obtained is 124.1 MeV (94.1 MeV) and the width is 11.8 MeV (25.8 MeV). Our results show that these kaonic nuclear states are more bound and stable. On the other hand, in order to investigate the influence of VπΣ,πΣ, we have considered the interaction of model E with VπΣ,πΣ=0. We find Model E is similar to the model of Akaishi and Yamazaki, but B Kof Model E is bigger and the widthΓis narrow comparing other models’. So VπΣ,πΣis very important for the coupled channel consideration and can not discard easily!
However, the results of Akaishi and Yamazaki were criticized by Oset et al. , who agued that the model of Akaishi and Yamazaki is unrealistic. Within the SU(3) chiral unitary model, they found that there are not just one Lamda (1405) but two states, and the shape obtained in experiments comes from a superposition of the two resonances with different weights for different reactions. Recently, Magas et al. have provided firm evidence of the two poles structure of the Lamda(1405). Recently, M.Iwasaki et al. have performed a couple of experiments, KEK PS-E549/570, for the detailed study of the strange tribaryon S 0(3115)obtained in KEK PS-E471. In contrast to the previous proton spectrum, no narrow peak structure were found, the strange tribaryon S 0(3115) was an experimental artifact. CorrelatedΛdpairs emitted after the absorption of negative kaons at rest K ? A→ΛdA′in light nuclei 6Li and 12 C were performed with the FINUDA spectrometer at DAΦNE(LNF), and it was found that MΛd =3251±6 MeV from theΛdinvariant mass spectrum of 6Li. The corresponding binding energy is BKppn?=58±6 MeV, and K?ppnΓ=37 MeV. A similar experiment was performed by Suzuki et al. They found that MΛd≤3220 MeV.
So in second stage, we construct a quantitative K Ninteraction phenomenologic- ally using free K Nscattering data, the KpX data of kaonic hydrogen, and the binding energy and width of the two resonances. For I =0K N interaction, we construct two models which reproduce two resonances: one appears around 1420 MeV, which has a width of 40 MeV and couples mostly to K N; While the other one appears around 1392 MeV, has a width about 130 MeV and and couples mostly toπΣ. Furthermore, in the second resonance which is always seen from the invariant mass of its only strong decay channel, the strength of theπΣ→πΣis about 4/3 times larger than that of K N→KNwhich is in good agreement with the result provided by the chiral Lagrangians. The two models both gave a scattering length of a I=0=-1.90+ i0.88fm. If the relative weight of the first resonance with respect to the second one is 7:5, that is 7Λ(1420)/12+5Λ(1392)/12, we find that the superposition of the two resonances is in good agreement with the Lamda(1405) obtained in experiments with EΛ=1406.5-i25 MeV. We also investigate nuclear K ?bound states within the framework of Bruechner-Hartree-Fock theory. The binding energy of K ? ppn(T =0) is 93 MeV and the width is 13 MeV. The binding energy we obtained is smaller than Akaishi and Yamazaki’s about 15 Mev. A similar situation holds for K ? ppnn(T =1/2), the binding energy BKppnn ?=72 MeV and the width is about 25 MeV. Our results show that these nuclear K ?states are deeply bound. The binding energy (width) we obtained is 3 MeV (56 MeV) for K ? pnn(T =1), and 23 MeV (62 MeV) for K ? pp(T =1/2)。
On the other hand, instead of the resonance stateΛ(1405) the first resonance is considered as an isospin I =0bound state of K N. For example, A.Dote et al. have investigated the K ? pp system with chiral SU(3) effective interaction, they found that the system is weakly bound, with a binding energy BKpp =(19±3) MeV and a decay width K ?pp→ΣNΓπ~40-70 MeV. In order to investigate these strange systems in detail, we have also studied two models, only considering the first resonance or the second one as a bound K Nstate. For the former, the binding energy (width) we obtained is 80 MeV (33 MeV) for K ? ppn(T =0) and 22 MeV (56 MeV) for K ? pp. For the latter, the binding energy for K ? ppn(T =0) is 102 MeV and the width is 12 MeV. Thus, if we consider only one of the two resonances as a bound K Nstate, the results show that the strange tribaryons system is deeply bound, too.
Akaishi and Yamazaki have investigated theoretically several few-body systems and found the deeply bound K ?nuclear states with very small widths considering the Lamda(1405) state as the bound state of the kaon and proton. While E.Oset et al. found that there are not just one Lamda (1405) but two states, and they predicted that the binding energy of nuclear K states is smaller, but the width are larger. However, our results show that, contrary to Oset’s expectation, these nuclear K states are deeply bound.
在本文中,我们分两个阶段考察奇异核。在第一阶段(早期阶段)我们主要以早期实验发现深度束缚奇异核为依据,构造新的K N相互作用,特别是重点考虑以前理论所忽略的VπΣ,πΣ势。这个新的相互作用能产生一个共振态Λ(1405)即K介子和质子束缚态,以及与实验值相符的散射长度。结果[Li091]表明存在深度束缚K核态,但得到的结合能远远小于上面的实验值。更重要的是我们发现VπΣ,πΣ的作用对体系结合能影响非常大:它一方面降低体系的结合能,另一方面又增加了体系的宽度,因而不能轻易地将它舍弃。
在第二阶段(后期阶段)我们不再简单地把Λ(1405)看作是K介子和质子的束缚态而是两个共振的叠加态。首先建立两个I =0的K N相互作用模型,这两个模型一方面都能产生与实验值相符的散射长度,另一方面它们分别产生两个与实验观测相符的共振态:一个能量为1420MeV,宽度为40 MeV,主要以K N形式衰变;另一个能量为1392MeV,宽度较高达到135 MeV,主要以πΣ形式衰变。当调节这两个共振态的相对权重为7:5,就可以得到与实验相符的Λ(1405)。在此基础上,我们详细考察了一些奇异核(S=-1),发现了深度束缚的K核态。
Recently, many theoretical and experiment efforts have been devoted to investigation of deeply-bound kaonic nuclei. In order to seek possible narrow discrete nuclear bound states, Akaishi and Yamazaki have investigated theoretically several few-body systems and found deeply bound nuclear states with very small widths. They considered the Lamda(1405) state as the bound state of the kaon and proton and its width is caused by coupling to theπΣchannel. The binding energy of K ? ppn( K ? ppnn) they obtained is 108 (86) MeV and the width is 20 (34) MeV. A few years later, in search for quasi-bound states in the K ? ppsystem a three-body K ? NN?πΣNcoupled-channel Faddeev calculation by Shevchenko et al. yields a quasibound state with B K~55-70 MeV, andΓ~90-110 MeV. On the other hand, the strange tribaryons S 1(3140)with T =0 and S 0(3115) with T =1were observed by T. Suzuki and M.Iwasaki et al. in the interaction of stopped K ?mesons with 4 He. Another indication of K ? ppbound state was reported by the FINUDA Collaboration, the binding energy (width) is 115(67) MeV.
But the phenomenological K N interaction Akaishi and Yamazaki given is simple, It contains only one range parameter (0.66 fm) and VπΣ,πΣis set equal to zero. It is known that the latter is very important for the coupled channel consideration. To make phenomenological K N interaction more flexible, we (the first stage) have looked for a new phenomenological K N interaction ( VπΣ,πΣ≠0) with two range parameters. We considered the Lamda (1405) state as the bound state of the kaon and proton, too. The new I =0interaction produces a resonance stateΛ(1405) with EΛ=1406.5-i25 MeV, and gives a scattering length of a I=0=-1.76+i0.6fm which can be compared to Martin’s empirical value a I=0=-(1.70±0.07) + i(0.68±0.04)fm. The relative weight of g I=0with respect to g I=1is 1:5 for K ? pnn, 1:1 for K ? ppn, 3:1 for K ? pp, 1:3 for K ? pn. Within the framework of the Bruechner-Hartree-Fock we have studied these kaonic nuclear states, the binding energy of K ? ppn( K ? ppnn) we obtained is 124.1 MeV (94.1 MeV) and the width is 11.8 MeV (25.8 MeV). Our results show that these kaonic nuclear states are more bound and stable. On the other hand, in order to investigate the influence of VπΣ,πΣ, we have considered the interaction of model E with VπΣ,πΣ=0. We find Model E is similar to the model of Akaishi and Yamazaki, but B Kof Model E is bigger and the widthΓis narrow comparing other models’. So VπΣ,πΣis very important for the coupled channel consideration and can not discard easily!
However, the results of Akaishi and Yamazaki were criticized by Oset et al. , who agued that the model of Akaishi and Yamazaki is unrealistic. Within the SU(3) chiral unitary model, they found that there are not just one Lamda (1405) but two states, and the shape obtained in experiments comes from a superposition of the two resonances with different weights for different reactions. Recently, Magas et al. have provided firm evidence of the two poles structure of the Lamda(1405). Recently, M.Iwasaki et al. have performed a couple of experiments, KEK PS-E549/570, for the detailed study of the strange tribaryon S 0(3115)obtained in KEK PS-E471. In contrast to the previous proton spectrum, no narrow peak structure were found, the strange tribaryon S 0(3115) was an experimental artifact. CorrelatedΛdpairs emitted after the absorption of negative kaons at rest K ? A→ΛdA′in light nuclei 6Li and 12 C were performed with the FINUDA spectrometer at DAΦNE(LNF), and it was found that MΛd =3251±6 MeV from theΛdinvariant mass spectrum of 6Li. The corresponding binding energy is BKppn?=58±6 MeV, and K?ppnΓ=37 MeV. A similar experiment was performed by Suzuki et al. They found that MΛd≤3220 MeV.
So in second stage, we construct a quantitative K Ninteraction phenomenologic- ally using free K Nscattering data, the KpX data of kaonic hydrogen, and the binding energy and width of the two resonances. For I =0K N interaction, we construct two models which reproduce two resonances: one appears around 1420 MeV, which has a width of 40 MeV and couples mostly to K N; While the other one appears around 1392 MeV, has a width about 130 MeV and and couples mostly toπΣ. Furthermore, in the second resonance which is always seen from the invariant mass of its only strong decay channel, the strength of theπΣ→πΣis about 4/3 times larger than that of K N→KNwhich is in good agreement with the result provided by the chiral Lagrangians. The two models both gave a scattering length of a I=0=-1.90+ i0.88fm. If the relative weight of the first resonance with respect to the second one is 7:5, that is 7Λ(1420)/12+5Λ(1392)/12, we find that the superposition of the two resonances is in good agreement with the Lamda(1405) obtained in experiments with EΛ=1406.5-i25 MeV. We also investigate nuclear K ?bound states within the framework of Bruechner-Hartree-Fock theory. The binding energy of K ? ppn(T =0) is 93 MeV and the width is 13 MeV. The binding energy we obtained is smaller than Akaishi and Yamazaki’s about 15 Mev. A similar situation holds for K ? ppnn(T =1/2), the binding energy BKppnn ?=72 MeV and the width is about 25 MeV. Our results show that these nuclear K ?states are deeply bound. The binding energy (width) we obtained is 3 MeV (56 MeV) for K ? pnn(T =1), and 23 MeV (62 MeV) for K ? pp(T =1/2)。
On the other hand, instead of the resonance stateΛ(1405) the first resonance is considered as an isospin I =0bound state of K N. For example, A.Dote et al. have investigated the K ? pp system with chiral SU(3) effective interaction, they found that the system is weakly bound, with a binding energy BKpp =(19±3) MeV and a decay width K ?pp→ΣNΓπ~40-70 MeV. In order to investigate these strange systems in detail, we have also studied two models, only considering the first resonance or the second one as a bound K Nstate. For the former, the binding energy (width) we obtained is 80 MeV (33 MeV) for K ? ppn(T =0) and 22 MeV (56 MeV) for K ? pp. For the latter, the binding energy for K ? ppn(T =0) is 102 MeV and the width is 12 MeV. Thus, if we consider only one of the two resonances as a bound K Nstate, the results show that the strange tribaryons system is deeply bound, too.
Akaishi and Yamazaki have investigated theoretically several few-body systems and found the deeply bound K ?nuclear states with very small widths considering the Lamda(1405) state as the bound state of the kaon and proton. While E.Oset et al. found that there are not just one Lamda (1405) but two states, and they predicted that the binding energy of nuclear K states is smaller, but the width are larger. However, our results show that, contrary to Oset’s expectation, these nuclear K states are deeply bound.
引文
[Ag05] M.Agnello, et al. Evidence for a kaon-bound state K ? ppproduced in K ?absorption reactions at rest. Phys. Rev. Lett, 2005, 94: 212303
[Ag07] M.Agnello, et al. CorrelatedΛdpairs from the Ks?to p A→ΛdA' reaction. Phys. Lett. B , 2007, 654: 80
[Ak00] Y. Akaishi, T. Harada, S. Shinmura and Thin Swe Myint . CoherentΛ?Σcoupling in s-shell hypernuclei. Phys. Rev. Lett, 2000, 84: 3539
[Ak02] Yoshinori Akaishi and Toshimitsu Yamazaki. Nuclear K bound states in light nuclei. Phys. Rev. C , 2002, 65: 044005
[Ak05] Yoshinori Akaishi, Akinobu Dote and Toshimitsu Yamazaki. Strange tribaryons as K -mediated dense nuclear systems. Phys.Lett. B, 2005, 613: 140
[ Ak68] Yoshinori Akaishi, Hiroharu Bando, Atsushi Kuriyama, Sinobu Nagata. Binding energy of nuclear matter by the hole line expansion method. I. Prog. Theor. Phys , 1968, 40: 288
[Al61] M. H. Alston et al. Study of resonances of theΣ?πsystem. Phys. Rev. Lett , 1961, 6: 698
[Al76] M. Alberg, E. Henlfy and L. Wilets. Theory of kaonic atoms. Anna. Phys , 1976, 96: 43
[Ba63] P.L.Bastien and J. P. Berge. K ? p interactions near 760 Mev/c. Phys. Rev. Lett , 1963, 10: 188
[Ba71] B. R. Barrett, R. G.. L. Hewitt and R. J. Mccarthy. Simple and exact mothod for calculating the nuclear reaction Matrix. Phys. Rev. C, 1971, 3: 1137
[Ba97] C. J. Batty, E. Friedman and A. Gal. Strong interaction physics from hadronic atoms. Phys. Pep, 1997, 287: 385
[Be63] H. A. Bethe, B. H. Brandow and A. G. Petschek. Reference spectrummethod for nuclear matter. Phys. Rev , 1963, 129: 225
[Be95] V. Bernard, N. Kaiser and U. G. Meissner, Int. J. Mod. Phys. E,1995, 4: 193
[Br55] K. A. Brueckner and C. A. Levinson. Approximate reduction of the many-body problem for strangly interacting particles to a problem of self-consitent fields. Phys. Rev , 1955, 97: 1344
[Br58] K. A. Brueckner, J. L. Gamme and H. Weitzner. Properties of nucear matter. Phys. Rev , 1958, 109: 1023 K. A. Brueckner, J. L. Gamme and H. Weitzner. Theory of finite nuclei. Phys. Rev, 1958, 110: 431
[Br61] K. A. Brueckner, A. M. Lockett and M. Rotenberg. Properties of finite nuclei. Phys. Rev, 1961, 121: 255
[Br64] G. E. Brown, G. T. Shappert and C. W. Wong. Nucl. Phys, 1964, 56: 191
[Br78] R. Brockmann, W. Weise and L. Tauscher, Nucl. Phys. A, 1978, 308: 365
[Br94] G. E. Brown, C. H. Lee, M. Rho and V. Thorsson, Nucl. Phys. A , 1994, 567: 937
[Ci01] A. Cieply, E. Friedman, A.Gal and J. Mares. Study of chirally motivated low-energy K ?optical potentials. Nucl. Phys. A , 2001, 696: 173
[Da59] R. H. Dalitz and S.F.Tuan. Possible resonant state in Pion-hyperon scattering. Phys. Rev. Lett , 1959, 2: 425
[Da67] B.D.Day. Elements of the Brueckner-Goldstone Theory of Nuclear matter. Rev. Mod. Phys, 1967, 39: 719
[Da91] R. H. Dalitz and A. Deloff. J. Phys. G, 1991, 17: 289
[Do04] A. Dote, H. Horiuchi, Y. Akaishi and T.Yamazaki . Kaonic nuclei studied based on a new framework of antisymmetrized molecular dynamics. Phys. Rev. C, 2004, 70: 044313 A. Dote, H. Horiuchi, Y. Akaishi and T.Yamazaki. High-densityK nuclear systems with isovector deformation. Phys. Lett. B, 2004, 590: 51
[De07] Deng Cheng-Rong and Ping Jia-Lun. Kaonic nuclear cluster K ? pp in quark Delocalization Screening Model. Chin. Phys. Lett , 2007, 590: 3381
[Do08] Akinobu Dote, Tetsuo Hyodo, Wolfram Weise. K ? ppsystem with chiral SU(3) effective interaction. Nucl. Phys. A, 2008, 804: 197
[Ec95] G. Ecker. Chiral perturbation theory. Prog. Part. Nucl. Phys, 1995, 35: 1
[Fe06] T. Femandez-Carames, A. Valcarce, H. Garcilazo and P. Ganzalez. Strange tribaryons. Phys. Rev. C , 2006, 73: 034004
[Fi93] E. Friedman, A. Gal and C. J. Batty, Phys. Lett. B, 1993, 308: 6
[Fi94] E. Friedman, A. Gal and C. J. Batty, Nucl. Phys. A , 1994, 579:
518
[Fr99] E. Friedman and A. Gal. Narrow deeply bound K ?atomic states. Phys. Lett. B, 1999, 459: 43
[Ga01] A. Gal. Phenomenology of K ?atoms and other strange hadronic atoms. Nucl. Phys. A, 2001, 691: 268(c)
[Ga02] C. Garcia-Recio, J. Nieves, T. Inonu and E. Oset.ηbound states in nuclei. Phys. Lett. B, 2002, 550: 47
[Ga03] C. Garcia-Recio, J. Nieves, E. Ruiz Arriola and M. J. Vicente Vacas. S=-1 meson-baryon unitarized coupled chiral perturbation theory and the S 01 resonancesΛ(1405)andΛ(1670). Phys. Rev. D, 2003, 67: 076009
[Gar04] C.Garcia-Recio, M.F.M.Lutz and J. Nieves. Quark mass dependence of s-wave baryon resonances. Phys. Lett. B, 2004, 582: 49
[Ga07] D.Gazda, E. Friedman, A.Gal and J. Mares. Dynamics of K ?and multi- K ? nuclei. Phys. Rev. C , 2007, 76: 055204
[Ga08] D.Gazda, E. Friedman, A.Gal and J. Mares. multi- K ? nuclei and kaon condensation. Phys. Rev. C , 2008, 77: 045206
[Ga85] J. Gasser and H. Leuteyler, Nucl. Phys. B, 1985, 250: 465 J. Gasser, M. E. Sainio and A. Svarc, Nucl. Phys. B, 1985, 307: 779
[Go57] J. Goldstone, Proc. Roy. Soc. A, 1957, 293: 267
[Ha71] A. Hasegawa and S. Nagata, Prog. Theor. Phys, 1971, 45: 1786
[Hi01] E. Hiyama, M. Kamimura, T. Motoba, T.Yamada and Y.Yamamoto.Λ?Σconversion inΛ4 He andΛ4 H based on a four-body calculation. Phys. Rev. C, 2001, 65: 011301(R)
[Hi91] S. Hirenzaki, H.Toki and T.Yamazaki. ( d , 3He) reactions for the formation of deeply bound pionic atoms. Phys. Rev. C, 1991, 44: 2472
[Hy03] T.Hyodo, S. I. Nam, D. Jido and A. Hosaka. Flavor SU(3) breaking effects in the chiral unitary model for meson-baryon scatterings. Phys. Rev. C, 2003, 68: 018201
[Hy08] Tetsuo Hyodo and Wolfram Weise. Effective K Ninteraction based on chiral SU(3) dynamics. Phys. Rev. C, 2008, 77: 035204
[Ik07] Y. Ikeda and T. Sato. Strange dibaryon resonance in the K NN?πYN system. Phys. Rev. C, 2007, 76: 035203
[It00] K.Itahashi, et al. Deeply boundπ?states in 207 Pbformed in the 208 Pb( d , 3He) deduced binding energies and widths and the pion-nucleus reaction. Phys. Rev. C, 2000, 62: 025202
[It98] T.M.Itoh, et al. Observation of kaonic hydrogen atom X rays. Phys. Rev. C, 1998, 58: 2366
[Iw04] M.Iwasaki, et al. Indication of a strange tribaryon S +from the 4 He(stopped K ? ,n) reaction. arXiv: nucl-ex/0310018
[Iw08] M.Iwasaki, et al. Kaonic nuclear state search via K ? reaction ar rest on 4 He target. Nucl. Phys. A, 2008, 804: 186
[Iw97] M.Iwasaki, et al. Observation of kaonic hydrogen KαXrays. Phys. Rev. Lett , 1997, 78: 3067
[Ji02] D.Jido, A. Hosaka, J. C. Nacher, E. Oset andA. Ramos. Magnetic moments of theΛ(1405)andΛ(1670) resonances. Phys.Rev.C, 2002, 66: 025203
[Ji03] D.Jido, J. A. Oller, E. Oset , A. Ramos and U. G. Meissner. Chiral dynamics of the twoΛ(1405) states. Nucl. Phys. A, 2003, 725: 181
[Ji94]井孝功,姚玉洁.多体理论与Green函数方法讲义[M].长春. 1994
[Ka95] N.Kaiser, P.B.Siegel and W. Weise. Chiral dynamics and the low - energy kaon-nucleon interaction. Nucl. Phys. A, 1995, 594: 325
[Ki06] Paul Kienle, Yoshinori Akaishi and Toshimitsu Yamazaki. Momentum correlation in the three-body decay of high-density K nuclear clusters: NNN K→N+N+Λ. Phys .Lett. B, 2006, 632: 187
[Ko07] Takahisa.Koike and Toru.Harada. Calculation of the 3 He (in-flight K ? ,n)reaction for searching the deeply-bound K ? pp state. Phys. Lett. B, 2007, 652: 262
[Ko94] V. Koch. Phys. Lett. B, 1994, 337: 7
[Kr90] A.Krause. Baryon Matrix elements of the vector cuttent in chiral perturbation theory. Helv. Phys. Act , 1990, 63: 1
[Ku66] T.T.Kuo and G.E.Brown. Structure of finite nuclei and the free nucleon -nucleon interaction. (An application to 18 Oand 18 F). Nucl. Phys, 1996, 85: 40
[ Ku71] T. T. Kuo, S.Y. Lee and K. F. Ratcliff. A folded-diagram expansion of the model-space effective Hamiltionian. Nucl. Phys A , 1971, 176:65
[Ku80] T. T. Kuo and E.M.Krenciglowa. An equation of motion method for deriving microscopic effective interactions in a correlated model space. Nucl. Phys. A, 1980, 342: 454
[Le75] Legrange. C H, JAERI-M-5984, 1975, 51
[Le94] C.H.Lee, H.Jung, D. P. Min and M. Rho, Phys. Lett. B, 1994, 326 14
[Li091] Yi-He. Li , Shi-Shu. Wu. Deeply bound kaonic states in nuclei. Chin. Phys. C (Suppl 1) , 2009, 33: 76
[Li092] Yi-He. Li, Shi-Shu Wu. Nuclear K bound states in 3 Heand 3 He. Chin. Phys. Lett , 2009, 26: 041203
[Li093] Yi-He. Li, Shi-Shu Wu. Strange K nuclear systems (S=-1). Chin. Phys. C已接收.
[Ma05] V.K.Magas, E.Oset and A.Ramos. Evidence for the Two-Pole structure of theΛ(1405) resonance. Phys. Rev. Lett, 2005, 95: 052301
[Mar05] J.Mares, E.Ftiedman and A.Gal. Widths of K -nuclear deeply bound states in a dynamical model. Phys. Lett. B, 2005, 606: 295
[Ma06] V. K. Magas, E. Oset, A.Ramos and H.Toki. A critical view on the deeply bound K ? pp system. Phys. Rev. C , 2006, 74: 025206 V.K.Magas, E.Oset and A.Ramos. Critical review of K ? ppn bound states. Phys. Rev. C, 2008, 74: 065210
[Ma81] A.D. Martin. Nucl. Phys. B, 1981, 179: 33
[Mi93] U. G. Meissner. Rep. Prog. Phys, 1993, 56: 903
[Mi94] M. Mizoguchi, S. Hirenzaki and H. Toki, Nucl. Phys. A, 1994, 567: 834
[Na04] S. I. Nam, H. C. Kim, T. Hyodo, D. Jido and A. Hosaka. J. Korean. Phys. Soc, 2004, 45: 1446
[Na79] Sinobu Nagata, Hiroharu Bando and Yoshinori Akaishi. Nuclear reaction Matrix and nuclear forces. Suppl. Prog. Theor. Phys, 1979, 65: 10
[Ni93] J. Nieves, E. Oset and C. Garcia-Recio, Nucl. Phys. A , 1993, 554: 509
[Oh97] A.Ohnishi, Y.Nara and V. Koch. Branching ratio change in K ? absorption at rest and the nature of theΛ(1405). Phys. Rev. C, 1997, 56: 2767
[Ol01] J.A.Oller and Ulf-G. Meiβner. Chiral dynamics in the presence of bound states: kaon-nucleon interactions revisited. Phys. Lett. B, 2001, 500: 263
[Ol05] J.A.Oller, Joaquim Prade and Michela Verbeni. Surprises in threshold antikaon-nucleon physics. Phys. Rev. Lett , 2005, 95: 172502
[Os06] E.Oset and H.Toki. A critical analysis on deeply bound kaonic states in nuclei. Phys. Rev. C, 2006, 74: 015207
[Os98] E.Oset and A.Ramos. Non-perturbative chiral approach to s-wave K Ninteractions. Nucl. Phys. A, 1998, 635: 99
[Pi95] A. Pich. Rep. Prog. Phys, 1995, 58: 563
[Pf04] M. Pfeiffer et al. Photoproduction ofη?mesic 3 He. Phys.Rev. Lett, 2004, 92: 252001
[Ra00] A.Ramos and E.Oset. The properties of K in the nuclear medium. Nucl. Phys. A, 2000, 671: 481
[Ra96] S. A. Rakityansky, S. A. Sofianos, M. Braun, V. B. Belyaev and W. Sandhas, Phys. Rev. C, 1996, 53: 2043
[Sa08] M.Sato, H. Bhang, J. Chiba, et al. Search for strange tribaryon states in the inclusive 4 He (Ks?to pped,p) reaction. Phys.Lett B, 2008, 659:107
[Sc00] J.Schaffner-Bielich, V.Koch and M.Effenberger. Medium modifiedcross sections, temperature and finite momentum effects for antikaon production in heavy-ion collisions. Nucl. Phys. A, 2000, 669: 153
[Sh05]申庆彪.低能和中能核反应理论[M].北京:原子能出版社,2005
[Sh07] N.V.Shevchenk, A.Gal and J.Mares. Faddeev calculation of a K ? pp quasibound state. Phys. Rev. Lett, 2007, 98: 082301
[Si70] P. J. Siemens. Nuclear-matter reaction matrix. Nucl. Phys. A, 1970, 114: 1
[Su04] T.Suzuki, et al. Discovery of a strange tribaryon S 0(3115)in 4 He (stopped K ? ,p) reaction. Phys. Lett. B, 2004 , 597: 263
[Su05] T.Suzuki, et al. A search for deeply bound nuclear states. Nucl. Phys. A, 2005, 754: 375c
[Su07] T.Suzuki, et al.Λdcorrelations from the 4 He(stopped- K ?, d ) reaction. Phys. Rev. C , 2007, 76: 068202
[ Su71] S. H. Suck and W. R. Coker, Nucl. Phys. A , 1971, 176: 89
[To88] H. Toki and T.Yamazaki, Phys. Lett. B, 1988, 213: 129
[To89] H.Toki, S. Hirenzaki, T.Yamazaki and R. S. Hayano, Nucl. Phys. A, 1989, 501: 653
[To91] H.Toki, S. Hirenzaki and T.Yamazaki, Nucl. Phys. A, 1991, 530: 679
[Ts72] S. F. Tsai and T. T. Kuo. A new treatment for the projection operator in nuclear G-Matrix equation. Phys. Lett. B, 1972, 39: 427
[Ts98] K.Tsushima, D.H.Lu, A.W.Thomas and K. Saito. Areη- andω-nuclear states bound. Phys. Lett. B, 1998, 443: 26
[Wa96] T.Waas, N.Kaiser and W.Weise. Low energy K N interaction in nuclear matter. Phys. Lett. B, 1996, 365: 12
[We08] W. Weise and R. Hartle. Chiral SU(3) dynamics and antikao-nuclear quasibound states. Nucl. Phys. A, 2008, 530: 173
[Ya02] Toshimitsu Yamazaki and Yoshinori Akaishi. ( K ? ,π?)production of nuclear K bound states in proton-rich systems viaΛ? doorways. Phys. Lett. B, 2002, 535: 70
[Ya04] Toshimitsu Yamazaki, Akinobu Dote and Yoshinori Akaishi. Invariant -mass spectroscopy for condensed single- and double- K nuclear clusters to be formed as residues in relativistic heavy-ion collisions. Phys. Lett. B, 2004, 587: 167
[Ya05] Toshimitsu Yamazaki, Akinobu Dote and Yoshinori Akaishi. Strange tribaryons as K -mediated dense nuclear systems. Phys. Lett. B, 2005, 613: 140
[Ya07] Toshimitsu Yamazaki and Yoshinori Akaishi. Emission spectra and invariant masses ofΛand p in the stopped- K ? NNabsorption process in 4 He and 6 Li. Nucl. Phys. A, 2007, 792: 229 Toshimitsu Yamazaki and Yoshinori Akaishi. Basic K nuclear cluster, K ? pp, and its enhanced formation in the p + p→K+ +X reaction. Phys. Rev. C , 2007, 76: 045201
[Ya54] Yoshio Yamaguchi. Two-nucleon problem when the potential is nonlocal but separable.I. Phys. Rev, 1954, 95: 1628
[Ya96] Toshimitsu Yamazaki, et al. Z. Phys. A , 1996, 355: 219
[Ya80]杨泽森,高能物理与核物理, 1980, Vol.4: 374
[Ze97]曾谨言.量子力学[M].北京:科学出版社,1997
[Zy08] I.Zychor, M. Buscher and M. Hartmann. Lineshape of theΛ(1405) hyperon measured through itsΣ0π0 decay. Phys. Lett. B, 2008, 660: 167
[Ag07] M.Agnello, et al. CorrelatedΛdpairs from the Ks?to p A→ΛdA' reaction. Phys. Lett. B , 2007, 654: 80
[Ak00] Y. Akaishi, T. Harada, S. Shinmura and Thin Swe Myint . CoherentΛ?Σcoupling in s-shell hypernuclei. Phys. Rev. Lett, 2000, 84: 3539
[Ak02] Yoshinori Akaishi and Toshimitsu Yamazaki. Nuclear K bound states in light nuclei. Phys. Rev. C , 2002, 65: 044005
[Ak05] Yoshinori Akaishi, Akinobu Dote and Toshimitsu Yamazaki. Strange tribaryons as K -mediated dense nuclear systems. Phys.Lett. B, 2005, 613: 140
[ Ak68] Yoshinori Akaishi, Hiroharu Bando, Atsushi Kuriyama, Sinobu Nagata. Binding energy of nuclear matter by the hole line expansion method. I. Prog. Theor. Phys , 1968, 40: 288
[Al61] M. H. Alston et al. Study of resonances of theΣ?πsystem. Phys. Rev. Lett , 1961, 6: 698
[Al76] M. Alberg, E. Henlfy and L. Wilets. Theory of kaonic atoms. Anna. Phys , 1976, 96: 43
[Ba63] P.L.Bastien and J. P. Berge. K ? p interactions near 760 Mev/c. Phys. Rev. Lett , 1963, 10: 188
[Ba71] B. R. Barrett, R. G.. L. Hewitt and R. J. Mccarthy. Simple and exact mothod for calculating the nuclear reaction Matrix. Phys. Rev. C, 1971, 3: 1137
[Ba97] C. J. Batty, E. Friedman and A. Gal. Strong interaction physics from hadronic atoms. Phys. Pep, 1997, 287: 385
[Be63] H. A. Bethe, B. H. Brandow and A. G. Petschek. Reference spectrummethod for nuclear matter. Phys. Rev , 1963, 129: 225
[Be95] V. Bernard, N. Kaiser and U. G. Meissner, Int. J. Mod. Phys. E,1995, 4: 193
[Br55] K. A. Brueckner and C. A. Levinson. Approximate reduction of the many-body problem for strangly interacting particles to a problem of self-consitent fields. Phys. Rev , 1955, 97: 1344
[Br58] K. A. Brueckner, J. L. Gamme and H. Weitzner. Properties of nucear matter. Phys. Rev , 1958, 109: 1023 K. A. Brueckner, J. L. Gamme and H. Weitzner. Theory of finite nuclei. Phys. Rev, 1958, 110: 431
[Br61] K. A. Brueckner, A. M. Lockett and M. Rotenberg. Properties of finite nuclei. Phys. Rev, 1961, 121: 255
[Br64] G. E. Brown, G. T. Shappert and C. W. Wong. Nucl. Phys, 1964, 56: 191
[Br78] R. Brockmann, W. Weise and L. Tauscher, Nucl. Phys. A, 1978, 308: 365
[Br94] G. E. Brown, C. H. Lee, M. Rho and V. Thorsson, Nucl. Phys. A , 1994, 567: 937
[Ci01] A. Cieply, E. Friedman, A.Gal and J. Mares. Study of chirally motivated low-energy K ?optical potentials. Nucl. Phys. A , 2001, 696: 173
[Da59] R. H. Dalitz and S.F.Tuan. Possible resonant state in Pion-hyperon scattering. Phys. Rev. Lett , 1959, 2: 425
[Da67] B.D.Day. Elements of the Brueckner-Goldstone Theory of Nuclear matter. Rev. Mod. Phys, 1967, 39: 719
[Da91] R. H. Dalitz and A. Deloff. J. Phys. G, 1991, 17: 289
[Do04] A. Dote, H. Horiuchi, Y. Akaishi and T.Yamazaki . Kaonic nuclei studied based on a new framework of antisymmetrized molecular dynamics. Phys. Rev. C, 2004, 70: 044313 A. Dote, H. Horiuchi, Y. Akaishi and T.Yamazaki. High-densityK nuclear systems with isovector deformation. Phys. Lett. B, 2004, 590: 51
[De07] Deng Cheng-Rong and Ping Jia-Lun. Kaonic nuclear cluster K ? pp in quark Delocalization Screening Model. Chin. Phys. Lett , 2007, 590: 3381
[Do08] Akinobu Dote, Tetsuo Hyodo, Wolfram Weise. K ? ppsystem with chiral SU(3) effective interaction. Nucl. Phys. A, 2008, 804: 197
[Ec95] G. Ecker. Chiral perturbation theory. Prog. Part. Nucl. Phys, 1995, 35: 1
[Fe06] T. Femandez-Carames, A. Valcarce, H. Garcilazo and P. Ganzalez. Strange tribaryons. Phys. Rev. C , 2006, 73: 034004
[Fi93] E. Friedman, A. Gal and C. J. Batty, Phys. Lett. B, 1993, 308: 6
[Fi94] E. Friedman, A. Gal and C. J. Batty, Nucl. Phys. A , 1994, 579:
518
[Fr99] E. Friedman and A. Gal. Narrow deeply bound K ?atomic states. Phys. Lett. B, 1999, 459: 43
[Ga01] A. Gal. Phenomenology of K ?atoms and other strange hadronic atoms. Nucl. Phys. A, 2001, 691: 268(c)
[Ga02] C. Garcia-Recio, J. Nieves, T. Inonu and E. Oset.ηbound states in nuclei. Phys. Lett. B, 2002, 550: 47
[Ga03] C. Garcia-Recio, J. Nieves, E. Ruiz Arriola and M. J. Vicente Vacas. S=-1 meson-baryon unitarized coupled chiral perturbation theory and the S 01 resonancesΛ(1405)andΛ(1670). Phys. Rev. D, 2003, 67: 076009
[Gar04] C.Garcia-Recio, M.F.M.Lutz and J. Nieves. Quark mass dependence of s-wave baryon resonances. Phys. Lett. B, 2004, 582: 49
[Ga07] D.Gazda, E. Friedman, A.Gal and J. Mares. Dynamics of K ?and multi- K ? nuclei. Phys. Rev. C , 2007, 76: 055204
[Ga08] D.Gazda, E. Friedman, A.Gal and J. Mares. multi- K ? nuclei and kaon condensation. Phys. Rev. C , 2008, 77: 045206
[Ga85] J. Gasser and H. Leuteyler, Nucl. Phys. B, 1985, 250: 465 J. Gasser, M. E. Sainio and A. Svarc, Nucl. Phys. B, 1985, 307: 779
[Go57] J. Goldstone, Proc. Roy. Soc. A, 1957, 293: 267
[Ha71] A. Hasegawa and S. Nagata, Prog. Theor. Phys, 1971, 45: 1786
[Hi01] E. Hiyama, M. Kamimura, T. Motoba, T.Yamada and Y.Yamamoto.Λ?Σconversion inΛ4 He andΛ4 H based on a four-body calculation. Phys. Rev. C, 2001, 65: 011301(R)
[Hi91] S. Hirenzaki, H.Toki and T.Yamazaki. ( d , 3He) reactions for the formation of deeply bound pionic atoms. Phys. Rev. C, 1991, 44: 2472
[Hy03] T.Hyodo, S. I. Nam, D. Jido and A. Hosaka. Flavor SU(3) breaking effects in the chiral unitary model for meson-baryon scatterings. Phys. Rev. C, 2003, 68: 018201
[Hy08] Tetsuo Hyodo and Wolfram Weise. Effective K Ninteraction based on chiral SU(3) dynamics. Phys. Rev. C, 2008, 77: 035204
[Ik07] Y. Ikeda and T. Sato. Strange dibaryon resonance in the K NN?πYN system. Phys. Rev. C, 2007, 76: 035203
[It00] K.Itahashi, et al. Deeply boundπ?states in 207 Pbformed in the 208 Pb( d , 3He) deduced binding energies and widths and the pion-nucleus reaction. Phys. Rev. C, 2000, 62: 025202
[It98] T.M.Itoh, et al. Observation of kaonic hydrogen atom X rays. Phys. Rev. C, 1998, 58: 2366
[Iw04] M.Iwasaki, et al. Indication of a strange tribaryon S +from the 4 He(stopped K ? ,n) reaction. arXiv: nucl-ex/0310018
[Iw08] M.Iwasaki, et al. Kaonic nuclear state search via K ? reaction ar rest on 4 He target. Nucl. Phys. A, 2008, 804: 186
[Iw97] M.Iwasaki, et al. Observation of kaonic hydrogen KαXrays. Phys. Rev. Lett , 1997, 78: 3067
[Ji02] D.Jido, A. Hosaka, J. C. Nacher, E. Oset andA. Ramos. Magnetic moments of theΛ(1405)andΛ(1670) resonances. Phys.Rev.C, 2002, 66: 025203
[Ji03] D.Jido, J. A. Oller, E. Oset , A. Ramos and U. G. Meissner. Chiral dynamics of the twoΛ(1405) states. Nucl. Phys. A, 2003, 725: 181
[Ji94]井孝功,姚玉洁.多体理论与Green函数方法讲义[M].长春. 1994
[Ka95] N.Kaiser, P.B.Siegel and W. Weise. Chiral dynamics and the low - energy kaon-nucleon interaction. Nucl. Phys. A, 1995, 594: 325
[Ki06] Paul Kienle, Yoshinori Akaishi and Toshimitsu Yamazaki. Momentum correlation in the three-body decay of high-density K nuclear clusters: NNN K→N+N+Λ. Phys .Lett. B, 2006, 632: 187
[Ko07] Takahisa.Koike and Toru.Harada. Calculation of the 3 He (in-flight K ? ,n)reaction for searching the deeply-bound K ? pp state. Phys. Lett. B, 2007, 652: 262
[Ko94] V. Koch. Phys. Lett. B, 1994, 337: 7
[Kr90] A.Krause. Baryon Matrix elements of the vector cuttent in chiral perturbation theory. Helv. Phys. Act , 1990, 63: 1
[Ku66] T.T.Kuo and G.E.Brown. Structure of finite nuclei and the free nucleon -nucleon interaction. (An application to 18 Oand 18 F). Nucl. Phys, 1996, 85: 40
[ Ku71] T. T. Kuo, S.Y. Lee and K. F. Ratcliff. A folded-diagram expansion of the model-space effective Hamiltionian. Nucl. Phys A , 1971, 176:65
[Ku80] T. T. Kuo and E.M.Krenciglowa. An equation of motion method for deriving microscopic effective interactions in a correlated model space. Nucl. Phys. A, 1980, 342: 454
[Le75] Legrange. C H, JAERI-M-5984, 1975, 51
[Le94] C.H.Lee, H.Jung, D. P. Min and M. Rho, Phys. Lett. B, 1994, 326 14
[Li091] Yi-He. Li , Shi-Shu. Wu. Deeply bound kaonic states in nuclei. Chin. Phys. C (Suppl 1) , 2009, 33: 76
[Li092] Yi-He. Li, Shi-Shu Wu. Nuclear K bound states in 3 Heand 3 He. Chin. Phys. Lett , 2009, 26: 041203
[Li093] Yi-He. Li, Shi-Shu Wu. Strange K nuclear systems (S=-1). Chin. Phys. C已接收.
[Ma05] V.K.Magas, E.Oset and A.Ramos. Evidence for the Two-Pole structure of theΛ(1405) resonance. Phys. Rev. Lett, 2005, 95: 052301
[Mar05] J.Mares, E.Ftiedman and A.Gal. Widths of K -nuclear deeply bound states in a dynamical model. Phys. Lett. B, 2005, 606: 295
[Ma06] V. K. Magas, E. Oset, A.Ramos and H.Toki. A critical view on the deeply bound K ? pp system. Phys. Rev. C , 2006, 74: 025206 V.K.Magas, E.Oset and A.Ramos. Critical review of K ? ppn bound states. Phys. Rev. C, 2008, 74: 065210
[Ma81] A.D. Martin. Nucl. Phys. B, 1981, 179: 33
[Mi93] U. G. Meissner. Rep. Prog. Phys, 1993, 56: 903
[Mi94] M. Mizoguchi, S. Hirenzaki and H. Toki, Nucl. Phys. A, 1994, 567: 834
[Na04] S. I. Nam, H. C. Kim, T. Hyodo, D. Jido and A. Hosaka. J. Korean. Phys. Soc, 2004, 45: 1446
[Na79] Sinobu Nagata, Hiroharu Bando and Yoshinori Akaishi. Nuclear reaction Matrix and nuclear forces. Suppl. Prog. Theor. Phys, 1979, 65: 10
[Ni93] J. Nieves, E. Oset and C. Garcia-Recio, Nucl. Phys. A , 1993, 554: 509
[Oh97] A.Ohnishi, Y.Nara and V. Koch. Branching ratio change in K ? absorption at rest and the nature of theΛ(1405). Phys. Rev. C, 1997, 56: 2767
[Ol01] J.A.Oller and Ulf-G. Meiβner. Chiral dynamics in the presence of bound states: kaon-nucleon interactions revisited. Phys. Lett. B, 2001, 500: 263
[Ol05] J.A.Oller, Joaquim Prade and Michela Verbeni. Surprises in threshold antikaon-nucleon physics. Phys. Rev. Lett , 2005, 95: 172502
[Os06] E.Oset and H.Toki. A critical analysis on deeply bound kaonic states in nuclei. Phys. Rev. C, 2006, 74: 015207
[Os98] E.Oset and A.Ramos. Non-perturbative chiral approach to s-wave K Ninteractions. Nucl. Phys. A, 1998, 635: 99
[Pi95] A. Pich. Rep. Prog. Phys, 1995, 58: 563
[Pf04] M. Pfeiffer et al. Photoproduction ofη?mesic 3 He. Phys.Rev. Lett, 2004, 92: 252001
[Ra00] A.Ramos and E.Oset. The properties of K in the nuclear medium. Nucl. Phys. A, 2000, 671: 481
[Ra96] S. A. Rakityansky, S. A. Sofianos, M. Braun, V. B. Belyaev and W. Sandhas, Phys. Rev. C, 1996, 53: 2043
[Sa08] M.Sato, H. Bhang, J. Chiba, et al. Search for strange tribaryon states in the inclusive 4 He (Ks?to pped,p) reaction. Phys.Lett B, 2008, 659:107
[Sc00] J.Schaffner-Bielich, V.Koch and M.Effenberger. Medium modifiedcross sections, temperature and finite momentum effects for antikaon production in heavy-ion collisions. Nucl. Phys. A, 2000, 669: 153
[Sh05]申庆彪.低能和中能核反应理论[M].北京:原子能出版社,2005
[Sh07] N.V.Shevchenk, A.Gal and J.Mares. Faddeev calculation of a K ? pp quasibound state. Phys. Rev. Lett, 2007, 98: 082301
[Si70] P. J. Siemens. Nuclear-matter reaction matrix. Nucl. Phys. A, 1970, 114: 1
[Su04] T.Suzuki, et al. Discovery of a strange tribaryon S 0(3115)in 4 He (stopped K ? ,p) reaction. Phys. Lett. B, 2004 , 597: 263
[Su05] T.Suzuki, et al. A search for deeply bound nuclear states. Nucl. Phys. A, 2005, 754: 375c
[Su07] T.Suzuki, et al.Λdcorrelations from the 4 He(stopped- K ?, d ) reaction. Phys. Rev. C , 2007, 76: 068202
[ Su71] S. H. Suck and W. R. Coker, Nucl. Phys. A , 1971, 176: 89
[To88] H. Toki and T.Yamazaki, Phys. Lett. B, 1988, 213: 129
[To89] H.Toki, S. Hirenzaki, T.Yamazaki and R. S. Hayano, Nucl. Phys. A, 1989, 501: 653
[To91] H.Toki, S. Hirenzaki and T.Yamazaki, Nucl. Phys. A, 1991, 530: 679
[Ts72] S. F. Tsai and T. T. Kuo. A new treatment for the projection operator in nuclear G-Matrix equation. Phys. Lett. B, 1972, 39: 427
[Ts98] K.Tsushima, D.H.Lu, A.W.Thomas and K. Saito. Areη- andω-nuclear states bound. Phys. Lett. B, 1998, 443: 26
[Wa96] T.Waas, N.Kaiser and W.Weise. Low energy K N interaction in nuclear matter. Phys. Lett. B, 1996, 365: 12
[We08] W. Weise and R. Hartle. Chiral SU(3) dynamics and antikao-nuclear quasibound states. Nucl. Phys. A, 2008, 530: 173
[Ya02] Toshimitsu Yamazaki and Yoshinori Akaishi. ( K ? ,π?)production of nuclear K bound states in proton-rich systems viaΛ? doorways. Phys. Lett. B, 2002, 535: 70
[Ya04] Toshimitsu Yamazaki, Akinobu Dote and Yoshinori Akaishi. Invariant -mass spectroscopy for condensed single- and double- K nuclear clusters to be formed as residues in relativistic heavy-ion collisions. Phys. Lett. B, 2004, 587: 167
[Ya05] Toshimitsu Yamazaki, Akinobu Dote and Yoshinori Akaishi. Strange tribaryons as K -mediated dense nuclear systems. Phys. Lett. B, 2005, 613: 140
[Ya07] Toshimitsu Yamazaki and Yoshinori Akaishi. Emission spectra and invariant masses ofΛand p in the stopped- K ? NNabsorption process in 4 He and 6 Li. Nucl. Phys. A, 2007, 792: 229 Toshimitsu Yamazaki and Yoshinori Akaishi. Basic K nuclear cluster, K ? pp, and its enhanced formation in the p + p→K+ +X reaction. Phys. Rev. C , 2007, 76: 045201
[Ya54] Yoshio Yamaguchi. Two-nucleon problem when the potential is nonlocal but separable.I. Phys. Rev, 1954, 95: 1628
[Ya96] Toshimitsu Yamazaki, et al. Z. Phys. A , 1996, 355: 219
[Ya80]杨泽森,高能物理与核物理, 1980, Vol.4: 374
[Ze97]曾谨言.量子力学[M].北京:科学出版社,1997
[Zy08] I.Zychor, M. Buscher and M. Hartmann. Lineshape of theΛ(1405) hyperon measured through itsΣ0π0 decay. Phys. Lett. B, 2008, 660: 167