1. |
K. Inaba, Y. Sasamoto, T. Kawabata, M. Fujiwara, Y. Funaki, K. Hatanaka, K. Itoh, M. Itoh, K. Kawase, H. Matsubara, Y. Maeda, K. Suda, S. Sakaguchi, Y. Shimizu, A. Tamii, Y. Tameshige, M. Uchida, T. Uesaka, T. Yamada, H. P. Yoshida, α condensed states in 13C using α inelastic scattering, *Progress of Theoretical and Experimental Physics*, Volume 2021, Issue 9, 093D01, 2021.08. |

2. |
M. Tsumura, T. Kawabata, Y. Takahashi, S. Adachi, H. Akimune, S. Ashikaga, T. Baba, Y. Fujikawa, H. Fujimura, H. Fujioka, T. Furuno, T. Hashimoto, T. Harada, M. Ichikawa, K. Inaba, Y. Ishii, N. Itagaki, M. Itoh, C. Iwamoto, N. Kobayashi, A. Koshikawa, S. Kubono, Y. Maeda, Y. Matsuda, S. Matsumoto, K. Miki, T. Morimoto, M. Murata, T. Nanamura, I. Ou, S. Sakaguchi, A. Sakaue, M. Sferrazza, K. N. Suzuki, T. Takeda, A. Tamii, K. Watanabe, Y. N. Watanabe, H. P. Yoshida and J. Zenihiro, First experimental determination of the radiative-decay probability of the 3-1 state in 12C for estimating the triple alpha reaction rate in high temperature environments, *Phys. Lett. B*, 817, 10 June 2021, 136283, 2021.06. |

3. |
K. Hagino and S. Sakaguchi, Subbarrier fusion reactions of an aligned deformed nucleus, *Physical Review C*, 10.1103/PhysRevC.100.064614, 100, 2019.12, We discuss heavy-ion fusion reactions of a well-deformed odd-mass nucleus at energies around the Coulomb barrier. To this end, we consider the 16O+165Ho reaction and take into account the effect of deformation of 165Ho using the orientation average formula. We show that fusion cross sections are sensitive to magnetic substates of the target nucleus, and cross sections for the side collision, which are relevant to a synthesis of superheavy elements, may be enhanced by a factor of around two by aligning the deformed target nuclei. We also discuss the effect of alignment on the fusion barrier distribution. We find that, for a particular choice of alignment, the shape of barrier distribution becomes similar to a typical shape of barrier distribution for a deformed nucleus with a negative hexadecapole deformation parameter, β4, even if the intrinsic β4 is positive in the target nucleus.. |

4. |
S. Chebotaryov, S. Sakaguchi, T. Uesaka, T. Akieda, Y. Ando, M. Assie, D. Beaumel, N. Chiga, M. Dozono, A. Galindo-Uribarri, B. Heffron, A. Hirayama, T. Isobe, K. Kaki, S. Kawase, W. Kim, T. Kobayashi, H. Kon, Y. Kondo, Y. Kubota, S. Leblond, H. Lee, T. Lokotko, Y. Maeda, Y. Matsuda, K. Miki, E. Milman, T. Motobayashi, T. Mukai, S. Nakai, T. Nakamura, A. Ni, T. Noro, S. Ota, H. Otsu, T. Ozaki, V. Panin, S. Park, A. Saito, H. Sakai, M. Sasano, H. Sato, K. Sekiguchi, Y. Shimizu, I. Stefan, L. Stuhl, M. Takaki, K. Taniue, K. Tateishi, S. Terashima, Y. Togano, T. Tomai, Y. Wada, T. Wakasa, T. Wakui, A. Watanabe, H. Yamada, Zh Yang, M. Yasuda, J. Yasuda, K. Yoneda, J. Zenihiro, Proton elastic scattering at 200 A MeV and high momentum transfers of 1.7-2.7 fm -1 as a probe of the nuclear matter density of 6 He, *Progress of Theoretical and Experimental Physics*, 10.1093/ptep/pty048, 2018, 5, 2018.05, Differential cross sections of p-6He elastic scattering were measured in inverse kinematics at an incident energy of 200 A MeV, covering the high momentum transfer region of 1.7-2.7 -1. The sensitivity of the elastic scattering at low and high momentum transfers to the density distribution was investigated quantitatively using relativistic impulse approximation calculations. In the high momentum transfer region, where the present data were taken, the differential cross section has an order of magnitude higher sensitivity to the inner part of the 6He density relative to the peripheral part (15:1). This feature makes the obtained data valuable for the deduction of the inner part of the 6He density. The data were compared to a set of calculations assuming different proton and neutron density profiles of 6He. The data are well reproduced by the calculation assuming almost the same profiles of proton and neutron densities around the center of 6He, and a proton profile reproducing the known point-proton radius of 1.94 fm. This finding is consistent with the assumption that the 6He nucleus consists of a rigid α-like core with a two-neutron halo.. |

5. |
S. Sakaguchi, T. Uesaka, N. Aoi, Y. Ichikawa, K. Itoh, M. Itoh, T. Kawabata, T. Kawahara, Y. Kondo, H. Kuboki, T. Nakamura, T. Nakao, Y. Nakayama, H. Sakai, Y. Sasamoto, K. Sekiguchi, T. Shimamura, Y. Shimizu, and T. Wakui, Shallow and diffuse spin-orbit potential for proton elastic scattering from neutron-rich helium isotopes at 71 MeV/nucleon, *Physical Review C*, 10.1103/PhysRevC.87.021601, 87, 021601-1-021601-5, 2013.02. |

6. |
S. Sakaguchi, Y. Iseri, T. Uesaka, M. Tanifuji, K. Amos, N. Aoi, Y. Hashimoto, E. Hiyama, M. Ichikawa, Y. Ichikawa, S. Ishikawa, K. Itoh, M. Itoh, H. Iwasaki, S. Karataglidis, T. Kawabata, T. Kawahara, H. Kuboki, Y. Maeda, R. Matsuo, T. Nakao, H. Okamura, H. Sakai, Y. Sasamoto, M. Sasano, Y. Satou, K. Sekiguchi, M. Shinohara, K. Suda, D. Suzuki, Y. Takahashi, A. Tamii, T. Wakui, K. Yako, M. Yamaguchi, and Y. Yamamoto
, Analyzing power in elastic scattering of 6He from a polarized proton target at 71 MeV/nucleon, *Physics Review C*, 10.1103/PhysRevC.84.024604, 84, 024604, 2011.08. |

7. |
T. Uesaka, S. Sakaguchi, Y. Iseri, K. Amos, N. Aoi, Y. Hashimoto, E. Hiyama, M. Ichikawa, Y. Ichikawa, S. Ishikawa, K. Itoh, M. Itoh, H. Iwasaki, S. Karataglidis, T. Kawabata, T. Kawahara, H. Kuboki, Y. Maeda, R. Matsuo, T. Nakao, H. Okamura, H. Sakai, Y. Sasamoto, M. Sasano, Y. Satou, K. Sekiguchi, M. Shinohara, K. Suda, D. Suzuki, Y. Takahashi, M. Tanifuji, A. Tamii, T. Wakui, K. Yako, Y. Yamamoto, and M. Yamaguchi, Analyzing power for proton elastic scattering from the neutron-rich 6He nucleus, *Physical Review C*, 10.1103/PhysRevC.82.021602, 82, 021602(R), 2010.08. |

8. |
Tomomi Kawahara, Satoshi Sakaguchi, Kenichiro Tateishi, Tsz Leung Tang, and Tomohiro Uesaka, Kinetic Parameters of Photo-Excited Triplet State of Pentacene Determined by Dynamic Nuclear Polarization, *JOURNAL OF THE PHYSICAL SOCIETY OF JAPAN*, 10.7566/JPSJ.84.044005, 84, 4, 044005-1-044005-７, 2015.03. |

9. |
M. Tsumura, T. Kawabata, T. Furuno, A. Koshikawa, M. Murata, T. Morimoto, S. Adachi, A. Tamii, K. Hatanaka, T. Ito, J. Zenihiro, S. Kubono, M. Itoh, Y. Matsuda, Y. Maeda, Satoshi Sakaguchi, H. Akimune, H. Fujimura, I. Ou, T. Hashimoto, C. Iwamoto, Search for the rare γ-decay mode in ^{12}C, *11th International Conference on Clustering Aspects of Nuclear Structure and Dynamics, CLUSTER 2016
Journal of Physics: Conference Series*, 10.1088/1742-6596/863/1/012075, 863, 1, 2017.07, Excited states in ^{12}C nuclei play a very important role in the nucleosynthesis in the universe. ^{12}C nuclei are synthesized by the triple α reaction. Normally the triple α process proceeds via the state (Hoyle states) at E_{x} = 7.65 MeV in ^{12}C. However, at high temperature T > 10^{9}, the highly excited 3α resonance states such as the state at E_{x} = 9.64 MeV might play a part of the triple α reaction. Unfortunately, the γ-decay probability of the state has not been determined, therefore we planned to measure ^{1}H(^{12}C, ^{12}Cp) reaction without measuring γ-rays. The test experiment using the solid hydrogen target and GAGG(Gd_{3}Al_{2}Ga_{3}O_{12}) was recently carried out at the cyclotron facility in RCNP. The results of the test experiment are reported in this paper.. |

10. |
T. Wakasa, J. Yasuda, M. Dozono, T. Fukunaga, S. Gotanda, K. Hatanaka, K. Ishibashi, Y. Kanaya, S. Kimura, Y. Maeda, Y. Maeda, Y. Nishio, T. Noro, T. Nozoe, K. Ohnaka, S. Sakaguchi, Y. Sakemi, K. Sekiguchi, T. Taguchi, Y. Wada, Cross sections and analyzing powers for (p - ,np) reactions of H 2, Li 6, and C 12 at 296 MeV CROSS SECTIONS and ANALYZING POWERS for (... T. WAKASA et al., *Physical Review C*, 10.1103/PhysRevC.96.014604, 96, 1, 2017.07, We report measurements of cross sections and analyzing powers for nucleon-knockout (pnp) reactions of H2, Li6, and C12 at 296 MeV using the RCNP NPOL3 neutron detector and large acceptance spectrometer. The 1s and 1p knockout reactions were successfully separated with a separation-energy resolution of approximately 6 MeV. The resulting data were compared with plane-wave and distorted-wave impulse approximation calculations employing the nucleon-nucleon t matrix in free space. No significant differences were identified in the case of the present analyzing power data, in contrast to the significant reductions observed in (p2p) values. The conventional Pauli blocking and nuclear binding effects with the g matrix and the relativistic effect of nucleon mass reduction in the nuclei are also discussed.. |

11. |
Tomotsugu Wakasa, S. Goto, M. Matsuno, S. Mitsumoto, T. Okada, H. Oshiro, Satoshi Sakaguchi, Neutron production cross sections for (d, n) reactions at 55 MeV, *Progress of Theoretical and Experimental Physics*, 10.1093/ptep/ptx099, 2017, 8, 2017.08, The cross sections for (d, n) reactions on ^{nat} C- ^{197} Au have been measured at a bombarding energy of 55 MeV and a laboratory scattering angle of θ _{lab} = 9.5 ^{◦} . The angular distributions for the ^{nat} C(d, n) reaction have also been obtained at θ _{lab} = 0 ^{◦} -40 ^{◦} . The neutron energy spectra are dominated by deuteron breakup contributions and their peak positions can be reasonably reproduced by considering the Coulomb force effects. The data are compared with the TENDL-2015 nuclear data and Particle and Heavy Ion Transport code System (PHITS) calculations. Both calculations fail to reproduce the measured energy spectra and angular distributions.. |

12. |
K. Sekiguchi, H. Witała, T. Akieda, D. Eto, H. Kon, Y. Wada, A. Watanabe, S. Chebotaryov, M. Dozono, J. Golak, H. Kamada, S. Kawakami, Y. Kubota, Y. Maeda, K. Miki, E. Milman, A. Ohkura, H. Sakai, S. Sakaguchi, N. Sakamoto, M. Sasano, Y. Shindo, R. Skibiński, H. Suzuki, M. Tabata, T. Uesaka, T. Wakasa, K. Yako, T. Yamamoto, Y. Yanagisawa, J. Yasuda, Complete set of deuteron analyzing powers from d - p elastic scattering at 190 MeV/nucleon, *Physical Review C*, 10.1103/PhysRevC.96.064001, 96, 6, 2017.12, All deuteron analyzing powers for elastic deuteron-proton (dp) scattering have been measured with a polarized deuteron beam at 186.6 MeV/nucleon. They are compared with results of three-nucleon Faddeev calculations based on the standard, high-precision nucleon-nucleon (NN) potentials alone or combined with commonly used three-nucleon force (3NF) models such as the Tucson-Melbourne '99 or the Urbana IX. Predicted 3NF effects localized at backward angles are supported only partially by the data. The data are also compared to predictions based on locally regularized chiral NN potentials. An estimation of theoretical truncation uncertainties in the consecutive orders of chiral expansion suggests that the observed discrepancies between this modern theory and the data could probably be explained by including chiral 3NF's in future calculations. A systematic comparison to the deuteron analyzing power data previously taken at incident energies from 70 to 294 MeV/nucleon clearly shows that not only the cross section but also the analyzing powers reveal growing 3NF effects when the three-nucleon system energy is increased.. |

13. |
S. Adachi, T. Kawabata, K. Minomo, T. Kadoya, N. Yokota, H. Akimune, T. Baba, H. Fujimura, M. Fujiwara, Y. Funaki, T. Furuno, T. Hashimoto, K. Hatanaka, K. Inaba, Y. Ishii, M. Itoh, C. Iwamoto, K. Kawase, Y. Maeda, H. Matsubara, Y. Matsuda, H. Matsuno, T. Morimoto, H. Morita, M. Murata, T. Nanamura, I. Ou, S. Sakaguchi, Y. Sasamoto, R. Sawada, Y. Shimizu, K. Suda, A. Tamii, Y. Tameshige, M. Tsumura, M. Uchida, T. Uesaka, H. P. Yoshida, S. Yoshida, Systematic analysis of inelastic α scattering off self-conjugate A=4n nuclei, *Physical Review C*, 10.1103/PhysRevC.97.014601, 97, 1, 2018.01, We systematically measured the differential cross sections of inelastic α scattering off self-conjugate A=4n nuclei at two incident energies Eα=130MeV and 386MeV at Research Center for Nuclear Physics, Osaka University. The measured cross sections were analyzed by the distorted-wave Born-approximation (DWBA) calculation using the single-folding potentials, which are obtained by folding macroscopic transition densities with the phenomenological αN interaction. The DWBA calculation with the density-dependent αN interaction systematically overestimates the cross sections for the ΔL=0 transitions. However, the DWBA calculation using the density-independent αN interaction reasonably well describes all the transitions with ΔL=0-4. We examined uncertainties in the present DWBA calculation stemming from the macroscopic transition densities, distorting potentials, phenomenological αN interaction, and coupled channel effects in C12. It was found that the DWBA calculation is not sensitive to details of the transition densities nor the distorting potentials, and the phenomenological density-independent αN interaction gives reasonable results. The coupled-channel effects are negligibly small for the 21+ and 31- states in C12, but not for the 02+ state. However, the DWBA calculation using the density-independent interaction at Eα=386MeV is still reasonable even for the 02+ state. We concluded that the macroscopic DWBA calculations using the density-independent interaction are reliably applicable to the analysis of inelastic α scattering at Eα∼100MeV/u.. |

14. |
Shoichiro Kawase, Tomohiro Uesaka, Tsz Leung Tang, Didier Beaumel, Masanori Dozono, Taku Fukunaga, Toshihiko Fujii, Naoki Fukuda, Alfredo Galindo-Uribarri, Sanghoon Hwang, Naoto Inabe, Takahiro Kawabata, Tomomi Kawahara, Wooyoung Kim, Keiichi Kisamori, Motoki Kobayashi, Toshiyuki Kubo, Yuki Kubota, Kensuke Kusaka, Cheongsoo Lee, Yukie Maeda, Hiroaki Matsubara, Shin Michimasa, Hiroyuki Miya, Tetsuo Noro, Yuki Nozawa, Alexandre Obertelli, Kazuyuki Ogata, Shinsuke Ota, Elizabeth Padilla-Rodal, Satoshi Sakaguchi, Hideyuki Sakai, Masaki Sasano, Susumu Shimoura, Samvel Stepanyan, Hiroshi Suzuki, Tomokazu Suzuki, Motonobu Takaki, Hiroyuki Takeda, Atsushi Tamii, Hiroshi Tokieda, Tomotsugu Wakasa, Takashi Wakui, Kentaro Yako, Jumpei Yasuda, Yoshiyuki Yanagisawa, Rin Yokoyama, Kazuki Yoshida, Koichi Yoshida, Juzo Zenihiro, Exclusive quasi-free proton knockout from oxygen isotopes at intermediate energies, *Progress of Theoretical and Experimental Physics*, 10.1093/ptep/pty011, 2018, 2, 2018.02, The dependence of the single-particle strength on the difference between proton and neutron separation energies is studied for oxygen isotopes in a wide range of isospins. The cross sections of the quasi-free (p, 2p) reaction on ^{14,16,18,22,24}O were measured at intermediate energies. The measured cross sections are compared to predictions based on the distorted wave impulse approximation and shell-model psd valence-space spectroscopic factors. The reduction factors, which are the ratio of the experimental cross sections to the theoretical predictions, show no apparent dependence on the proton–neutron separation energy difference. The result is compatible with the result of the (e, ep) reaction on stable targets and with the predictions of recent ab initio calculations.. |

15. |
S. Noji, H. Sakai, N. Aoi, H. Baba, G. P.A. Berg, P. Doornenbal, M. Dozono, N. Fukuda, N. Inabe, D. Kameda, T. Kawabata, S. Kawase, Y. Kikuchi, K. Kisamori, T. Kubo, Y. Maeda, H. Matsubara, S. Michimasa, K. Miki, H. Miya, H. Miyasako, S. Sakaguchi, Y. Sasamoto, S. Shimoura, M. Takaki, H. Takeda, S. Takeuchi, H. Tokieda, T. Ohnishi, S. Ota, T. Uesaka, H. Wang, K. Yako, Y. Yanagisawa, N. Yokota, K. Yoshida, R. G.T. Zegers, Excitation of the Isovector Spin Monopole Resonance via the Exothermic Zr 90 (N 12, C 12) Reaction at 175 MeV/u, *Physical Review Letters*, 10.1103/PhysRevLett.120.172501, 120, 17, 2018.04, The (N12, C12) charge-exchange reaction at 175 MeV/u was developed as a novel probe for studying the isovector spin giant monopole resonance (IVSMR), whose properties are important for better understanding the bulk properties of nuclei and asymmetric nuclear matter. This probe, now available through the production of N12 as a secondary rare-isotope beam, is exothermic, is strongly absorbed at the surface of the target nucleus, and provides selectivity for spin-transfer excitations. All three properties enhance the excitation of the IVSMR compared to other, primarily light-ion, probes, which have been used to study the IVSMR thus far. The Zr90(N12,C12) reaction was measured and the excitation energy spectra up to about 70 MeV for both the spin-transfer and non-spin-transfer channels were deduced separately by tagging the decay by γ emission from the C12 ejectile. Besides the well-known Gamow-Teller and isobaric analog transitions, a clear signature of the IVSMR was identified. By comparing with the results from light-ion reactions on the same target nucleus and theoretical predictions, the suitability of this new probe for studying the IVSMR was confirmed.. |

16. |
J. Yasuda, M. Sasano, R. G.T. Zegers, H. Baba, D. Bazin, W. Chao, M. Dozono, N. Fukuda, N. Inabe, T. Isobe, G. Jhang, D. Kameda, M. Kaneko, K. Kisamori, M. Kobayashi, N. Kobayashi, T. Kobayashi, S. Koyama, Y. Kondo, A. J. Krasznahorkay, T. Kubo, Y. Kubota, M. Kurata-Nishimura, C. S. Lee, J. W. Lee, Y. Matsuda, E. Milman, S. Michimasa, T. Motobayashi, D. Muecher, T. Murakami, T. Nakamura, N. Nakatsuka, S. Ota, H. Otsu, V. Panin, W. Powell, S. Reichert, S. Sakaguchi, H. Sakai, M. Sako, H. Sato, Y. Shimizu, M. Shikata, S. Shimoura, L. Stuhl, T. Sumikama, H. Suzuki, S. Tangwancharoen, M. Takaki, H. Takeda, T. Tako, Y. Togano, H. Tokieda, J. Tsubota, T. Uesaka, T. Wakasa, K. Yako, K. Yoneda, J. Zenihiro, Extraction of the Landau-Migdal Parameter from the Gamow-Teller Giant Resonance in Sn 132, *Physical Review Letters*, 10.1103/PhysRevLett.121.132501, 121, 13, 2018.09, The key parameter to discuss the possibility of the pion condensation in nuclear matter, i.e., the so-called Landau-Migdal parameter g′, was extracted by measuring the double-differential cross sections for the (p,n) reaction at 216 MeV/u on a neutron-rich doubly magic unstable nucleus, Sn132 with the quality comparable to data taken with stable nuclei. The extracted strengths for Gamow-Teller (GT) transitions from Sn132 leading to Sb132 exhibit the GT giant resonance (GTR) at the excitation energy of 16.3±0.4(stat)±0.4(syst) MeV with the width of Γ=4.7±0.8 MeV. The integrated GT strength up to Ex=25 MeV is SGT-=53±5(stat)-10+11(syst), corresponding to 56% of Ikeda's sum rule of 3(N-Z)=96. The present result accurately constrains the Landau-Migdal parameter as g′=0.68±0.07, thanks to the high sensitivity of the GTR energy to g′. In combination with previous studies on the GTR for Zr90 and Pb208, the result of this work shows the constancy of this parameter in the nuclear chart region with (N-Z)/A=0.11 to 0.24 and A=90 to 208.. |

17. |
A. Corsi, Y. Kubota, J. Casal, M. Gómez-Ramos, A. M. Moro, G. Authelet, H. Baba, C. Caesar, D. Calvet, A. Delbart, M. Dozono, J. Feng, F. Flavigny, J. M. Gheller, J. Gibelin, A. Giganon, A. Gillibert, K. Hasegawa, T. Isobe, Y. Kanaya, S. Kawakami, D. Kim, Y. Kiyokawa, M. Kobayashi, N. Kobayashi, T. Kobayashi, Y. Kondo, Z. Korkulu, S. Koyama, V. Lapoux, Y. Maeda, F. M. Marqués, T. Motobayashi, T. Miyazaki, T. Nakamura, N. Nakatsuka, Y. Nishio, A. Obertelli, A. Ohkura, N. A. Orr, S. Ota, H. Otsu, T. Ozaki, V. Panin, S. Paschalis, E. C. Pollacco, S. Reichert, J. Y. Rousse, A. T. Saito, S. Sakaguchi, M. Sako, C. Santamaria, M. Sasano, H. Sato, M. Shikata, Y. Shimizu, Y. Shindo, L. Stuhl, T. Sumikama, Y. L. Sun, M. Tabata, Y. Togano, J. Tsubota, T. Uesaka, Z. H. Yang, J. Yasuda, K. Yoneda, J. Zenihiro, Structure of ^{13}Be probed via quasi-free scattering, *Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics*, 10.1016/j.physletb.2019.134843, 797, 2019.10, We present an investigation of the structure of ^{13}Be obtained via a kinematically complete measurement of the (p,pn) reaction in inverse kinematics at 265 MeV/nucleon. The relative energy spectrum of ^{13}Be is compared to Transfer-to-the-Continuum calculations which use as structure inputs the overlaps of the ^{14}Be ground-state wave function, computed in a three-body model, with the unbound states of the ^{13}Be residual nucleus. The key role of neutron p-wave orbital in the interpretation of the low-relative-energy part of the spectrum is discussed.. |

18. |
S. Noji, H. Sakai, N. Aoi, H. Baba, G. P. A. Berg, P. Doornenbal, M. Dozono, N. Fukuda, N. Inabe, D. Kameda, T. Kawabata, S. Kawase, Y. Kikuchi, K. Kisamori, T. Kubo, Y. Maeda, H. Matsubara, S. Michimasa, K. Miki, H. Miya, H. Miyasako, S. Sakaguchi, Y. Sasamoto, S. Shimoura, M. Takaki, H. Takeda, S. Takeuchi, H. Tokieda, T. Ohnishi, S. Ota, T. Uesaka, H. Wang, K. Yako, Y. Yanagisawa, N. Yokota, K. Yoshida, and R. G. T. Zegers, Excitation of the Isovector Spin Monopole Resonance via the Exothermic 90Zr(12N,12C) Reaction at 175 MeV/u, *Phys. Rev. Lett. 120, 172501 (2018)*, https://doi.org/10.1103/PhysRevLett.120.172501, 2019.06. |

19. |
Satoshi Sakaguchi, Enlargement of solid polarized proton target for RI-beam experiment, *RIKEN Accelerator Progress Report *, 46, 163, 2014.01. |

20. |
Satoshi Sakaguchi, Analyzing Power in Elastic Scattering of Polarized Protons from Neutron-rich Helium Isotopes, *FEW-BODY SYSTEMS*, 10.1007/s00601-013-0617-1, 54, 7-10, 1393-1398, 2013.08. |

21. |
Satoshi Sakaguchi, Proton polarization in photo-excited aromatic molecule at room temperature enhanced by intense optical source and temperature control, *Nuclear Instruments and Methods in Physics Research B *, 317 , 679-684, 2013.12. |

22. |
S. Sakaguchi, T. Uesaka, T. Kawabata, T. Wakui, N. Aoi, Y. Hashimoto, Y. Ichikawa, K. Itoh, M. Itoh, H. Iwasaki, T. Kawahara, Y. Kondo, H. Kuboki, Y. Maeda, T. Nakamura, T. Nakao, Y. Nakayama, H. Okamura, H. Sakai, Y. Sasamoto, M. Sasano, Y. Satou, K. Sekiguchi, T. Shimamura, Y. Shimizu, M. Shinohara, K. Suda, D. Suzuki, Y. Takahashi, A. Tamii, K. Yako and M. Yamaguchi, Elastic Scattering of Neutron-Rich Helium Isotopes from Polarized Protons at 71 MeV/A, *Journal of Physics: Conf. Ser.*, 10.1088/1742-6596/312/8/082037, 312, 082037 , 2011.09. |

23. |
S. Sakaguchi, T. Uesaka, T. Wakui, T. Kawabata, N. Aoi, Y. Hashimoto, M. Ichikawa, Y. Itoh, M. Itoh, H. Iwasaki, T. Kawahara, H. Kuboki, Y. Maeda, R. Matsuo, T. Nakao, H. Okamura, H. Sakai, N. Sakamoto, Y. Sasamoto, M. Sasano, Y. Satou, K. Sekiguchi, M. Shinohara, K. Suda, D. Suzuki, Y. Takahashi, A. Tamii, K. Yako, M. Yamaguchi, Spin–orbit potential in 6He studied with polarized proton target, *Nuclear Physics A*, 805, 467, 2008.06. |

24. |
T. Uesaka and S. Sakaguchi, Spin observable in proton elastic scattering of 6He and its relevance to cluster structure, *Journal of Physics: Conf. Ser.*, 321, 012011 , 2011.09. |

25. |
J. L. Lou, Y. L. Ye, D. Y. Pang, Z. X. Cao, D. X. Jiang, T. Zheng, H. Hua, Z. H. Li, X. Q. Li, Y. C. Ge, L. H. Lv, J. Xiao, Q. T. Li, R. Qiao, H. B. You, R. J. Chen, H. Sakurai, H. Otsu, M. Nishimura, S. Sakaguchi, H. Baba, Y. Togano, K. Yoneda, C. Li, S. Wang, H. Wang, K. A. Li, T. Nakamura, Y. Nakayama, Y. Kondo, S. Deguchi, Y. Satou and K. Tshoo, Quasielastic scattering of 6He from 12C at 82.3 MeV/nucleon, *Phys. Rev. C*, 83, 034612 , 2011.03. |

26. |
Z.X. Cao, Y.L. Ye, J. Xiao, L.H. Lv, D.X. Jian, T. Zheng, H. Hua, Z.H. Li, X.Q. Li, Y.C. Ge, J.L. Lou, R. Qiao, Q.T. Li, H.B. You, R.J. Chen, D.Y. Pang, H. Sakurai, H. Otsu, M. Nishimura, S. Sakaguchi, H. Baba, Y. Togano, K. Yoneda, C. Li, S. Wang, H. Wang, K.A. Lib, T. Nakamura, Y. Nakayama, Y. Kondo, S. Deguchi, Y. Satou, and K. Tshoo, Recoil proton tagged knockout reaction for 8He, *Phys. Lett. B*, 707, 46, 2012.01. |

27. |
P.K. Kurilkin, V.P. Ladygin, T. Uesaka, K. Suda, Yu.V. Gurchin, A.Yu. Isupov, K. Itoh, M. Janeka, J.-T. Karachuk, T. Kawabata, A.N. Khrenov, A.S. Kiselev, V.A. Kizka, V.A. Krasnova, N.B. Ladygin, A.N. Livanova, Y. Maeda, A.I. Malakhov, S.M. Piyadin, S.G. Reznikov, S. Sakaguchi, H. Sakai, Y. Sasamoto, K. Sekiguchi, M.A. Shikhalev, T.A. Vasiliev, H. Witala, Measurement of the vector and tensor analyzing powers for dp-elastic scattering at 880 MeV, *Physics Letters B*, 715 , 61, 2012.06. |

28. |
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