Department of Physics, Tohoku University

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Department of Physics, Tohoku University Complete Set of Deuteron Analyzing Powers for dp Elastic Scattering at Intermediate Energies and Three Nucleon Force Kimiko Sekiguchi Department of Physics, Tohoku University

a good probe to study the dynamical aspects of 3NFs. Nucleon-Deuteron Scattering a good probe to study the dynamical aspects of 3NFs. Momentum & Spin dependence Iso-spin dependence : only T=1/2 Direct Comparison between Theory and Experiment Theory : Faddeev Calculations Rigorous Numerical Calculations of 3N System Experiment : Precise Data dσ/dΩ, Spin Observables (Aij, Kij, Cij) 2NF Input CDBonn Argonne V18 (AV18) Nijmegen I, II, 93 3NF Input Tucson-Melbourne Urbana IX etc.. 2NF & 3NF Input Chiral Effective Field Theory Extract information of Three Nucleon Forces.

Where is the Hot Spot for 3NF Effects in Three Nucleon Scattering? Predictions by H. Witala et al. (1998) Cross Section minimum for Nd Scattering at 100-200 MeV/A Nd scattering Low Energy Higher Energy NN direct term 3NF exchange term NN Forward Backward 3NF 3NF q =0 ~ 4 fm-1

@ RIKEN Accelerator Research Facility (RARF) How to attack 3NF – 1st Step - d-p Elastic Scattering at 135 MeV/nucleon @ RIKEN Accelerator Research Facility (RARF) Cross Section : Good description by 2p-3NF First Clear Signature of 3NFs in 3N scattering Spin Observables : Insufficient descriptions by 2p-3NF Defects of 3NF in Spin parts ?? K. S. et al., Phys. Rev. C 65, 034003 (2002). K. S. et al., Phys. Rev. Lett. 95, 162301 (2005). NN( CDBonn, AV18, Nijmegen I,II) NN( CDBonn, AV18, Nijmegen I,II) + TM’99 3NF NN( AV18 ) + Urbana IX 3NF NN( CDBonn ) + Delta-isobar NN( CDBonn ) + Delta-isobar + Coulomb

@ RIKEN RI Beam Factory (RIBF) How to attack 3NF – Next Step - Few Nucleon Scattering with pol.d beams @ RIKEN RI Beam Factory (RIBF) RARF : AVF+RRC Incident energy of deuteron : 65 – 135 MeV/nucleon RIBF : AVF+RRC + SRC 170 - 400MeV/nucleon First Experiment at RIBF dp Elastic Scattering at 250 &300 MeV/nucleon All deuteron analyzing powers Wide Angular Range High accuracy Go to higher energies - Effects of 3NFs are relatively enhanced. - Theory : harder Polarized Deuterons - rich set of spin observables

RIKEN RI Beam Factory (RIBF) Polarized d beam was accelerated by the AVF+RRC+ the new cyclotron SRC up to 250 & 300 MeV/nucleon. Spin axis of deuteron beam was rotated prior to acceleration. Single turn extraction of beam was successfully obtained for all the cyclotrons. Polarization amplitudes were maintained during acceleration. Beam Polarization : 80% of theoretical maximum values Spin axis of polarized d beams is freely controlled ! Polarized Ion Source SRC SMART ( - 2005) Polarimeter BigDpol

Differential Cross Section at 70 - 400 MeV/nucleon NN only - Large discrepancy in the backward region With 2π-3NF ? - improve the agreement - not enough at very backward angles at higher energies

Differential Cross Section at 70 - 400 MeV/nucleon Relativistic Faddeev Calculations with TM’99 3NF H. Witala et al, private communications pd/nd @ 250 MeV Relativistic effects are visible at backward angles, but small.

iT11 T20 T21 T22 Deuteron Analyzing Powers at 70 - 300 MeV/nucleon 135 MeV/A

iT11 T22 Deuteron Analyzing Powers at 70 - 300 MeV/nucleon NN only - Large discrepancy in the backward region + 2π3NF at 〜 100 MeV/A - results are NOT always similar to the cross section. + 2π3NF at 〜 250 MeV/A - improve the agreement - not enough at very backward angles →similar to the cross section K.S. et al., Phys. Rev. C 83,061001 (2011)

iT11 T22 dp @ 250 MeV Deuteron Analyzing Powers Relativistic Faddeev Calculations with TM’99 3NF H. Witala et al, private communications dp @ 250 MeV iT11 T22 Small relativistic effects

iT11 T22 dp @ 250 MeV Deuteron Analyzing Powers Relativistic Faddeev Calculations with TM’99 3NF H. Witala et al, private communications dp @ 250 MeV iT11 T22 Small relativistic effects

How does Chiral EFT pot. describe the Nd elastic scattering ? Various types of 3NFs, including 2π3NF, appear in N2LO, N3LO. Theory in Progress : up to N3LO (NN + NNN) for higher energies So far calc. based on χEFT pot. is available below 100 MeV/nucleon. 3NFs in N2LO d-p at 70 MeV/nucleon Calc. with χEFT Pot. (N2LO) by E. Epelbaum et al. In view of studying properties of 3NFs it is interesting to see how cEFT pot describe ...

Summary & Outlook Next Step Nucleon-Deuteron Scattering is a good probe to investigate the dynamics of 3NFs. - Momentum & Spin dependence - . For iso-spin, T=1/2 only. Precise data of dσ/dΩ and many spin observables at 65 - 300 MeV/nucleon Cross Sections : 3NFs are clearly needed in Elastic Scattering. Spin Observables : not always described by adding 2π-exchange 3NFs New Data from RIBF at 250 & 300 MeV : serious discrepancy in backward angles New Challenge to be solved Next Step Energy Dependence for Pol. Transfer and /or Spin Correlation Coefficients for Elastic Nd Scattering : Natural extension of 3NF study in Elastic scatt. Nd Breakup Experiments : Study of Relativistic Effects Four Nucleon Scattering : from Few to Many & Iso-spin dependence

RIBF pol.d beam experiment Gr. (2009〜) Collaboration Tohoku University K. Sekiguchi, J. Miyazaki, Y. Wada, T. Taguchi, U. Gebauer, K. Takahashi, T. Mashiko RIKEN Nishina Center N. Sakamoto, H. Sakai, T. Uesaka, M. Sasano, M. Dozono, Y. Shimizu CNS, University of Tokyo K. Yako, R. Tang, S. Kawase, Y. Kubota, C.S. Lee, RCNP, Osaka University H. Okamura, K. Miki Kyushu University T. Wakasa, S. Sakaguchi Miyazaki University Y. Maeda, T. Saito