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Nucleon Form Factor 作田 理論センター 1. Axial vector mass のまとめ 2. Quasi-elastic scattering の現状 3. Nucleon Form Factor の復習 4. まとめ= Axial vector form.

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Presentation on theme: "Nucleon Form Factor 作田 理論センター 1. Axial vector mass のまとめ 2. Quasi-elastic scattering の現状 3. Nucleon Form Factor の復習 4. まとめ= Axial vector form."— Presentation transcript:

1 Nucleon Form Factor 作田 誠(岡大理) @JPARC 理論センター 1. Axial vector mass のまとめ 2. Quasi-elastic scattering の現状 3. Nucleon Form Factor の復習 4. まとめ= Axial vector form factor はこれか ら

2 21 September 2004 M.Sakuda Neutrino - Nucleus Interactions Nucleon Form Factors p P q ee

3 1. 前回の検討会での早戸氏のまとめ 21 September 2004 M.Sakuda Neutrino - Nucleus Interactions

4 CC Quasi-elastic interaction -Hayato

5 K2K の MA 解析 21 September 2004 M.Sakuda Neutrino - Nucleus Interactions

6 K2K Q 2 distribution (QE=Shadow) 21 September 2004 M.Sakuda Neutrino - Nucleus Interactions

7 MiniBooNE QE 21 September 2004 M.Sakuda Neutrino - Nucleus Interactions

8 問題点 Q 2 <0.2 GeV 2 で不定性。 断面積をどう補正するかで不定性残る。 形のみの解析。 Dipole?? で良いのか。 Energy scale が Shape fit に効く。 バックグランドのない実験で T2K 、 SciBooNE できちんと出るか? 21 September 2004 M.Sakuda Neutrino - Nucleus Interactions

9 2 . Quasi-elastic の現状 21 September 2004 M.Sakuda Neutrino - Nucleus Interactions

10 MiniBooNE QE Anomaly (PRD81,092005,’09) Is theory (IA calculation) underestimates quasi-elastic cross section data C(,  ), while it agrees with C(e,e’) data?? M A :M A =1.0-1.2GeV  1.6GeV?? 2p-2h/MEC large?? Benhar-Meloni, PRL105,132301,2010 C(,  ) C(e,e’)

11 2p-2h/MEC or Contribution from the high energy tail Martini, Nieves, Donnelly …estimates 2p-2h/MEC contribution (~20%) and proposes a solution to MiniBooNE QE anomaly. Nieves et al., PRC83,045501,2011;Meucci et al., PRL107,172501,2011;Amaro et al.,PRD84,033004,2011 Benhar (hep-th/1110.1835) points out a big difference between A(e,e’) and A(,  ), where E spead is large.

12 MiniBooNE anomaly quasi-elastic 10 Feb, 2012 Makoto Sakuda @ JPARC

13 3 . Form Factor の復習 21 September 2004 M.Sakuda Neutrino - Nucleus Interactions

14 21 September 2004 M.Sakuda Neutrino - Nucleus Interactions

15 電子ー陽子散乱断面積の復習 Rutherford 散乱(古典電磁気学) 電子= Dirac 粒子、 陽子は古典的点電荷 電子、陽子 =Dirac 粒子、反跳

16 陽子の電荷・磁気構造の考慮 21 September 2004 M.Sakuda Neutrino - Nucleus Interactions

17 Rothenbluth の公式(電荷・磁気構造の考慮) 21 September 2004 M.Sakuda Neutrino - Nucleus Interactions

18 核子構造の発見 21 September 2004 M.Sakuda Neutrino - Nucleus Interactions

19 G E, G M の実験測定法 21 September 2004 M.Sakuda Neutrino - Nucleus Interactions

20 Yennie, Levy,Ravenhall,Rev.Mod.Phys.29(1957)144 21 September 2004 M.Sakuda Neutrino - Nucleus Interactions

21 21 September 2004 M.Sakuda Neutrino - Nucleus Interactions Progress in Electron Scattering experiments -Nucleon Vector Form Factors- In the past, the nucleon electromagnetic form factors have been measured from unpolarized electron beam scattering experiments using the Rosenbluth separation technique. The accuracy at high Q 2 (>1 (GeV/c) 2 ) was limited with this method. Nucleaon form factors were studied using a simple dipole parametrizations. Since 1993, new accurate measurements of the nucleon form factors were made possible with a new method using polarized electron beams and polarized targets. Clear deviation from a simple dipole parametrization is seen for the form factors and the better parametrizations for vector form factors were proposed. Recoil polarization P x  G E N, P x /P z  G E N / G M N The effect of those new form factors on the neutrino quasi-elastic cross sections was shown to be a few %.

22 BBBA0 5 Dipole 型 形状因子による断面積の 違い エネルギー移行量 Q 2 1 1 0.4 BBBA05 と Dipole 型の比 (G/D) 1 0.4 1 陽子:電荷形状因子 中性子:電荷分 布 陽子:磁気分布 中性子:磁気分布 陽子・中性子の最新の電荷、磁気形状因子 R.Bradford et al., Nucl. Phys. Proc. Suppl.159:127-132 (2006).  一般的な電荷、磁気形状因子 (Dipole 型 ) 電子原子核散乱で測定された最 新の形状因子 (BBBA05) を用い る  核子の電気的、磁気的な広がりを表すも の

23 Kelly 2004 21 September 2004 M.Sakuda Neutrino - Nucleus Interactions

24 21 September 2004 M.Sakuda Neutrino - Nucleus Interactions GEp  GMpGEp  GMp Polarized electron beam experiments Q2Q2 All dataPolarization

25 Gen : Riodan et al.,PRL105,262302,2010 21 September 2004 M.Sakuda Neutrino - Nucleus Interactions

26 4. まとめ : Axial vector Form Factor についての復習をした。 QE については、 2p-2h (MEC) の解決と MA の 2 つの独立の問題がある。 核子= Deutron (neutron) で精度の良い QE 実験がほしい。 (橋本氏の講演): Lattice QCD の形状因 子計算がこれほど進んでいるとは知らなか った。今後の進展に大変興味ある。 21 September 2004 M.Sakuda Neutrino - Nucleus Interactions


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