×
近期发现有不法分子冒充我刊与作者联系,借此进行欺诈等不法行为,请广大作者加以鉴别,如遇诈骗行为,请第一时间与我刊编辑部联系确认(《中国物理C》(英文)编辑部电话:010-88235947,010-88236950),并作报警处理。
本刊再次郑重声明:
(1)本刊官方网址为cpc.ihep.ac.cn和https://iopscience.iop.org/journal/1674-1137
(2)本刊采编系统作者中心是投稿的唯一路径,该系统为ScholarOne远程稿件采编系统,仅在本刊投稿网网址(https://mc03.manuscriptcentral.com/cpc)设有登录入口。本刊不接受其他方式的投稿,如打印稿投稿、E-mail信箱投稿等,若以此种方式接收投稿均为假冒。
(3)所有投稿均需经过严格的同行评议、编辑加工后方可发表,本刊不存在所谓的“编辑部内部征稿”。如果有人以“编辑部内部人员”名义帮助作者发稿,并收取发表费用,均为假冒。
                  
《中国物理C》(英文)编辑部
2024年10月30日

Medium effects in ΛK+ pair production by 2.83 GeV protons on nuclei

  • We study ΛK+ pair production in the interaction of protons of 2.83 GeV kinetic energy with C, Cu, Ag, and Au target nuclei in the framework of the nuclear spectral function approach for incoherent primary proton-nucleon and secondary pion-nucleon production processes, and processes associated with the creation of intermediate Σ0K+ pairs. The approach accounts for the initial proton and final Λ hyperon absorption, final K+ meson distortion in nuclei, target nucleon binding, and Fermi motion, as well as nuclear mean-field potential effects on these processes. We calculate the Λ momentum dependence of the absolute ΛK+ yield from the target nuclei considered, in the kinematical conditions of the ANKE experiment, performed at COSY, within the different scenarios for the Λ-nucleus effective scalar potential. We show that the above observable is appreciably sensitive to this potential in the low-momentum region. Therefore, direct comparison of the results of our calculations with the data from the ANKE-at-COSY experiment can help to determine the above potential at finite momenta. We also demonstrate that the two-step pion-nucleon production channels dominate in the low-momentum ΛK+ production in the chosen kinematics and, therefore, they have to be taken into account in the analysis of these data.
      PCAS:
  • 加载中
  • [1] A. Gal, E. V. Hungerford, and D. J. Millener, Rev. Mod. Phys., 88:035004(2016)
    [2] M. Nekipelov et al, Phys. Lett. B, 540:207(2002); G. Agakishiev et al, Phys. Rev. C, 82:044907(2010)
    [3] M. Lutz, Phys. Lett. B, 426:12(1998)
    [4] L. Tolos, A. Ramos, and E. Oset, Phys. Rev. C, 74:015203(2006)
    [5] L. Tolos, D. Cabrera, and A. Ramos, Phys. Rev. C, 78:045205(2008)
    [6] L. Tolos, A. Ramos, A. Polls, and T. T. S. Kuo, Nucl. Phys. A, 690:547(2001); L. Tolos, A. Ramos, and A. Polls, Phys. Rev. C, 65:054907(2002)
    [7] E. Friedman, A. Gal, J. Mares, and A. Cieply, Phys. Rev. C, 60:024314(1999)
    [8] A. Sibirtsev and W. Cassing, arXiv:nucl-th/9909053; W. Scheinast et al, Phys. Rev. Lett., 96:072301(2006); T. Kishimoto et al, Nucl. Phys. A, 827:321c (2009); H. W. Barz and L. Naumann, Phys. Rev. C, 68:041901(R) (2003)
    [9] Yu. T. Kiselev et al, Phys. Rev. C, 92:065201(2015)
    [10] V. K. Magas et al, Phys. Rev. C, 71:065202(2005); A. Polyanskiy et al, Phys. Lett. B, 695:74(2011); M. Hartmann et al, Phys. Rev. C, 85:035206(2012); T. Ishikawa et al, Phys. Lett. B, 608:215(2005); M. H. Wood et al, Phys. Rev. Lett., 105:112301(2010)
    [11] C. Fuchs, Prog. Part. Nucl. Phys., 56:1(2006); C. Hartnack et al, Phys. Rep., 510:119(2012); O. Buss et al, Phys. Rep., 512:1(2012)
    [12] Z. Q. Feng, Nucl. Phys. A, 919:32(2013); Z. Q. Feng, W. J. Xie, and G. M. Jin, Phys. Rev. C, 90:064604(2014)
    [13] G. Bunce et al, Phys. Rev. Lett., 36:1113(1976); K. Heller et al, Phys. Lett. B, 68:480(1977); K. Heller et al, Phys. Rev. Lett., 41:607(1978); F. Lomanno et al, Phys. Rev. Lett., 43:1905(1979); F. Abe et al, Phys. Rev. Lett., 50:1102(1983); A. M. Smith et al, Phys. Lett. B, 185:209(1987); B. E. Bonner et al, Phys. Rev. D, 38:729(1988); V. Fanti et al (NA48 Collaboration), Eur. Phys. J. C, 6:265(1999); B. Lundberg et al, Phys. Rev. D, 40:3557(1989)
    [14] G. Agakishiev et al, Eur. Phys. J. A, 50:81(2014)
    [15] O. Hashimoto and H. Tamura, Prog. Part. Nucl. Phys., 57:279(2010); A. Feliciello and T. Nagae, Rep. Prog. Phys., 78:096301(2015)
    [16] M. Kaskulov and E. Oset, Phys. Rev. C, 73:045213(2006)
    [17] M. Kaskulov, L. Roca, and E. Oset, Eur. Phys. J. A, 28:139(2006); E. Ya. Paryev, Yad. Fiz., 75:1602(2012)
    [18] M. F. M. Lutz, C. L. Copra, and M. Moeller, Nucl. Phys. A, 808:124(2008)
    [19] D. Cabrera et al, Phys. Rev. C, 90:055207(2014)
    [20] S. Petschauer et al, Eur. Phys. J. A, 52:15(2016); Ulf-G. Meissner and J. Haidenbauer, arXiv:1603.06429[nucl-th]
    [21] V. Flaminio et al Compilation of cross-sections. Ⅲ-p and bar p} induced reactions. CERN-HERA 79-03 (1979)
    [22] J. Balewski et al (COSY-11 Collaboration), Nucl. Phys. A, 626:85c (1997)
    [23] J. T. Balewski et al (COSY-11 Collaboration), Phys. Lett. B, 420:211(1998)
    [24] S. Sewerin et al (COSY-11 Collaboration), Phys. Rev. Lett., 83:682(1999)
    [25] P. Kowina et al (COSY-11 Collaboration), Eur. Phys. J. A, 22:293(2004)
    [26] R. Bilger et al (COSY-TOF Collaboration), Phys. Lett. B, 420:217(1998)
    [27] S. Abd El-Samad et al (COSY-TOF Collaboration), Phys. Lett. B, 632:27(2006); S. Abd El-Samad et al (COSY-TOF Collaboration), Phys. Lett. B, 688:142(2010)
    [28] M. Abdel-Bary et al (COSY-TOF Collaboration), Eur. Phys. J. A, 46:27(2010)
    [29] Yu. Valdau et al (ANKE Collaboration), Phys. Lett. B, 652:245(2007); Yu. Valdau et al (ANKE Collaboration), Phys. Rev. C, 81:045208(2010)
    [30] J. Adamczewski-Musch et al (HADES Colaboration), Phys. Rev. C, 95:015207(2017); arXiv:1611.01040[nucl-ex]
    [31] E. Ya. Paryev, Eur. Phys. J. A, 5:307(1999)
    [32] G. Fldt and C. Wilkin, Z. Phys. A, 357:241(1997)
    [33] M. Nekipelov et al, J. Phys. G:Nucl. Part. Phys., 34:627(2007)
    [34] G. Agakishiev et al, Phys. Rev. C, 90:015202(2014); arXiv:1403.6662[nucl-ex]
    [35] G. Q. Li, C.-H. Lee, G. E. Brown, Nucl. Phys. A, 625:372(1997)
    [36] G. Agakishiev et al, Phys. Rev. C, 90:054906(2014); arXiv:1404.7011[nucl-ex]
    [37] Yu. Valdau et al (ANKE Collaboration), Phys. Rev. C, 84:055207(2011)
    [38] M. Bscher et al, Eur. Phys. J. A, 22:301(2004)
    [39] K. Tsushima et al, Phys. Rev. C, 59:369(1999)
    [40] A. N. Ivanov et al, arXiv:nucl-th/0509055
    [41] G. Fldt and C. Wilkin, Eur. Phys. J. A, 24:431(2005)
    [42] E. Ya. Paryev, J. Phys. G:Nucl. Part. Phys., 40:025201(2013)
    [43] H. Nagahiro, M. Takizawa, and S. Hirenzaki, Phys. Rev. C, 74:045203(2006)
    [44] E. Ya. Paryev, Eur. Phys. J. A, 9:521(2000)
    [45] K. Tsushima et al, Phys. Lett. B, 429:239(1998)
    [46] C.-H. Lee et al, Phys. Lett. B, 412:235(1997)
    [47] C. B. Dover and G. E. Walker, Phys. Rep., 89:1(1982); D. J. Millener, C. B. Dover and A. Gal, Phys. Rev. C, 38:2700(1988); Y. Yamamoto, H. Bando, and J. Zofka, Prog. Theor. Phys., 80:757(1988)
    [48] M. Rufa et al, Phys. Rev. C, 42:2469(1990)
    [49] N. K. Glendenning et al, Phys. Rev. C, 48:889(1993)
    [50] Y. Yamamoto and H. Bando, Phys. Lett. B, 214:173(1988)
    [51] J. Hu, E. Hiyama, and H. Toki, Phys. Rev. C, 90:014309(2014)
    [52] M. Kohno and Y. Fujiwara, Phys. Rev. C, 79:054318(2009); M. Kohno, Phys. Rev. C, 81:014003(2010)
    [53] T. Inoue et al, arXiv:1612.08399[hep-lat]
    [54] G. Q. Li and C. M. Ko, Phys. Rev. C, 54:1897(1996)
    [55] E. Ya. Paryev, Yad. Fiz., 71:1985(2008)
    [56] E. Ya. Paryev, J. Phys. G:Nucl. Part. Phys., 43:015106(2016)
    [57] E. Ya. Paryev, J. Phys. G:Nucl. Part. Phys., 37:105101(2010)
    [58] E. Ya. Paryev, M. Hartmann, and Yu. T. Kiselev, J. Phys. G:Nucl. Part. Phys., 42:075107(2015)
    [59] E. Ya. Paryev, J. Phys. G:Nucl. Part. Phys., 36:015103(2009)
    [60] S. V. Efremov and E. Ya. Paryev, Eur. Phys. J. A, 1:99(1998)
    [61] E. Ya. Paryev, Eur. Phys. J. A, 7:127(2000)
    [62] S. K. Singh and M. J. Vicente Vacas, Phys. Rev. D, 74:053009(2006)
    [63] J. Haidenbauer and Ulf-G. Meissner, Nucl. Phys. A, 936:29(2015)
    [64] E. Friedman and A. Gal, Phys. Rep., 452:89(2007)
    [65] J. Cugnon and R. M. Lombard, Nucl. Phys. A, 422:635(1984)
    [66] A. Baldini et al, Landolt-Brnstein, New Series, I/12a (1988)
    [67] I. Zychor et al, Phys. Lett. B, 660:167(2008)
    [68] E. Ya. Paryev, Phys. Atom. Nucl., 69:721(2006)
    [69] A. V. Akindinov et al, J. Phys. G:Nucl. Part. Phys., 37:015107(2010)
    [70] S. Friedrich et al, Phys. Lett. B, 736:26(2014)
  • 加载中

Get Citation
E. Ya. Paryev, M. Hartmann and Yu. T. Kiselev. Medium effects in ΛK+ pair production by 2.83 GeV protons on nuclei[J]. Chinese Physics C, 2017, 41(12): 124108. doi: 10.1088/1674-1137/41/12/124108
E. Ya. Paryev, M. Hartmann and Yu. T. Kiselev. Medium effects in ΛK+ pair production by 2.83 GeV protons on nuclei[J]. Chinese Physics C, 2017, 41(12): 124108.  doi: 10.1088/1674-1137/41/12/124108 shu
Milestone
Received: 2017-07-28
Revised: 2017-10-05
Fund

    Supported by the Ministry of Education and Science of the Russian Federation

Article Metric

Article Views(1516)
PDF Downloads(22)
Cited by(0)
Policy on re-use
To reuse of subscription content published by CPC, the users need to request permission from CPC, unless the content was published under an Open Access license which automatically permits that type of reuse.
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Email This Article

Title:
Email:

Medium effects in ΛK+ pair production by 2.83 GeV protons on nuclei

  • 1. Institute for Nuclear Research, Russian Academy of Sciences, Moscow 117312, Russia
  • 2. Institute for Theoretical and Experimental Physics, Moscow 117218, Russia
  • 3.  Institut fmü
  • 4.  Institute for Theoretical and Experimental Physics, Moscow 117218, Russia
Fund Project:  Supported by the Ministry of Education and Science of the Russian Federation

Abstract: We study ΛK+ pair production in the interaction of protons of 2.83 GeV kinetic energy with C, Cu, Ag, and Au target nuclei in the framework of the nuclear spectral function approach for incoherent primary proton-nucleon and secondary pion-nucleon production processes, and processes associated with the creation of intermediate Σ0K+ pairs. The approach accounts for the initial proton and final Λ hyperon absorption, final K+ meson distortion in nuclei, target nucleon binding, and Fermi motion, as well as nuclear mean-field potential effects on these processes. We calculate the Λ momentum dependence of the absolute ΛK+ yield from the target nuclei considered, in the kinematical conditions of the ANKE experiment, performed at COSY, within the different scenarios for the Λ-nucleus effective scalar potential. We show that the above observable is appreciably sensitive to this potential in the low-momentum region. Therefore, direct comparison of the results of our calculations with the data from the ANKE-at-COSY experiment can help to determine the above potential at finite momenta. We also demonstrate that the two-step pion-nucleon production channels dominate in the low-momentum ΛK+ production in the chosen kinematics and, therefore, they have to be taken into account in the analysis of these data.

    HTML

Reference (70)

目录

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return