Shoichi Sakata

From Wikipedia, the free encyclopedia
Jump to navigation Jump to search
Shoichi Sakata
Sakata Shoichi.JPG
Sakata in 1949
Born(1911-01-18)January 18, 1911
DiedOctober 16, 1970(1970-10-16) (aged 59)
Known forTwo meson theory
Sakata model
Maki–Nakagawa–Sakata matrix
Scientific career
InstitutionsNagoya University
Osaka University
Kyoto University
Notable studentsMakoto Kobayashi
Toshihide Maskawa

Shoichi Sakata (坂田 昌一, Sakata Shōichi, 18 January 1911 – 16 October 1970) was a Japanese physicist who was internationally known for theoretical work on the subatomic particles.[1] He proposed the two meson theory, the Sakata model (an early precursor to the quark model), and the Pontecorvo–Maki–Nakagawa–Sakata neutrino mixing matrix.

After the end of World War II, he joined other physicists in campaigning for the peaceful uses of nuclear power.[1]


Sakata got in to the Kyoto Imperial University in 1930. When he was a second year student, Yoshio Nishina, a granduncle-in-law of Sakata, gave a lecture on quantum mechanics at the Kyoto Imperial University. Sakata became acquainted with Hideki Yukawa and Shin'ichirō Tomonaga, the first and the second Japanese Nobel laureates, through the lecture. After the graduation from the University, Sakata worked with Tomonaga and Nishina at Rikagaku Kenkyusho (RIKEN) in 1933 and moved to Osaka Imperial University in 1934 to work with Yukawa. Yukawa published his first paper on the meson theory in 1935 and Sakata closely collaborated with him for the developments of the meson theory. Possible existence of the neutral nuclear force carrier particle
was postulated by them.[2] Accompanied by Yukawa, Sakata moved to Kyoto Imperial University as a lecturer in 1939.

Sakata and Inoue proposed their two-meson theory in 1942.[3] At the time, a charged particle discovered in the hard component cosmic rays was misidentified as the Yukawa’s meson (
, nuclear force career particle). The misinterpretation led to puzzles in the discovered cosmic ray particle. Sakata and Inoue solved these puzzles by identifying the cosmic ray particle as a daughter charged fermion produced in the
decay. A new neutral fermion was also introduced to allow
decay into fermions.

We now know that these charged and neutral fermions correspond to the second generation leptons μ and
in the modern language. They then discussed the decay of the Yukawa particle,



Sakata and Inoue predicted correct spin assignment for the muon, and they also introduced the second neutrino. They treated it as a distinct particle from the beta decay neutrino, and anticipated correctly the three body decay of the muon. The English printing of Sakata-Inoue’s two-meson theory paper was delayed until 1946,[4] one year before the experimental discovery of π → μν decay.

Sakata moved to Nagoya Imperial University as a professor in October 1942 and remained there until his death. The name of the university was changed to Nagoya University in October 1947 after the end of the Pacific War (1945). Sakata reorganized his research group in Nagoya to be administrated under the democracy principle after the War.

Sakata stayed at the Niels Bohr Institute from May to October 1954 at the invitation of N. Bohr and C. Møller. During his stay, Sakata gave a talk introducing works of young Japanese particle physics researchers, especially emphasizing an empirical relation found by Nakano and Nishijima,[5][6] which is now known as the Nakano-Nishijima-Gell-Mann (NNG) rule[5][6][7] among the strongly interacting particles (hadrons).

After Sakata returned to Nagoya, Sakata and his Nagoya group started researches trying to uncover the physics behind the NNG rule. Sakata then proposed his Sakata Model[8] in 1956, which explains the NNG rule by postulating the fundamental building blocks of all strongly interacting particles are the proton, the neutron and the lambda baryon. The positively charged pion is made out of a proton and an antineutron, in a manner similar to the Fermi-Yang composite Yukawa meson model,[9] while the positively charged kaon is composed of a proton and an anti-lambda, succeeding to explain the NNG rule in the Sakata model. Aside from the integer charges, the proton, neutron, and lambda have similar properties as the up quark, down quark, and strange quark respectively.

In 1959, Ikeda, Ogawa and Ohnuki[10][11] and, independently, Yamaguchi[12][13] found out the U(3) symmetry in the Sakata model. The U(3) symmetry provides a mathematical descriptions of hadrons in the eightfold way[14] idea (1961) of Murray Gell-Mann. Sakata's model was superseded by the quark model, proposed by Gell-Mann and George Zweig in 1964, which keeps the U(3) symmetry, but made the constituents fractionally charged and rejected the idea that they could be identified with observed particles. Still, within Japan, integer charged quark models parallel to Sakata's were used until the 1970s, and are still used as effective descriptions in certain domains.

Sakata's model was used in Harry J. Lipkin's book "Lie Groups for Pedestrians" (1965).[15] The Sakata model and its SU(3) symmetry were also explained in the textbook "Weak Interaction of Elementary Particles", L.B.Okun (1965).[16]

In 1959, Gamba, Marshak and Okubo[17] found Sakata’s baryon triplet (proton, neutron and lambda baryon) bears striking similarity to the lepton triplet (neutrino, electron and muon) in the weak interaction aspects. In order to explain the physics behind this similarity in the composite model framework, in 1960, Sakata expanded his composite model to include leptons with his Nagoya University associates Maki, Nakagawa, and Ohnuki.[18] The expanded model was termed “Nagoya Model”. Shortly thereafter the existence of two kinds of neutrinos was experimentally confirmed. In 1962, Maki, Nakagawa and Sakata,[19] and also Katayama, Matumoto, Tanaka and Yamada[20] accommodated the two distinct types of neutrino into the composite model framework.

In his 1962 paper with Maki and Nakagawa, they used the Gell-Mann-Levy proposal of modified universality to define the weak mixing angle that later became known as Cabibbo angle; and extended it to the leptons, clearly distinguishing neutrino weak and mass eigenstates, thus defining the neutrino flavor mixing angle as well as predicting neutrino flavor oscillations. The neutrino flavor mixing matrix is now named Maki–Nakagawa–Sakata matrix. The nontrivial neutrino mixing as introduced in the Maki–Nakagawa–Sakata paper is now experimentally confirmed through the neutrino oscillation experiments.


The U(3) symmetry found first in the Sakata model gave a guiding principle to construct the quark model of Gell-Mann and Zweig. The two-meson theory of Sakata and Inoue became well-recognized in the world around 1950.

The 2008 physics Nobel laureates Yoichiro Nambu, Toshihide Maskawa and Makoto Kobayashi, who received their awards for work on symmetry breaking, all came under his tutelage and influence.[21] The baryonic mixing in the weak current in the Nagoya Model was the inspiration for the later Cabibbo–Kobayashi–Maskawa matrix of 1973, which specifies the mismatch of quantum states of quarks, when they propagate freely and when they take part in weak interactions. Physicists however, generally attribute the introduction of a third generation of quarks (the "top" and "bottom" quarks) into the Standard Model of the elementary particles to that 1973 paper by Kobayashi and Maskawa.

The neutrino oscillation phenomena, as predicted by Maki, Nakagawa and Sakata, has been experimentally confirmed (2015 Nobel prize in physics).

Kent Staley (2004) describes the historical background to their paper, emphasizing the largely forgotten[clarification needed] role of theorists at Nagoya University and the "Nagoya model" they developed. Several of the authors of the Nagoya model embraced the philosophy of dialectical materialism, and he discusses the role that such metaphysical commitments play in physical theorizing. Both theoretical and experimental developments that generated great interest in Japan, and ultimately stimulated Kobayashi and Maskawa's 1973 work, went almost entirely unnoticed in the U.S. The episode exemplifies both the importance of untestable "themata" in developing new theories, and the difficulties that may arise, when two parts of a research community work in relative isolation from one another.[22]

Missed out on Nobel Prize[edit]

Shoichi Sakata's "Sakata model" inspired Murray Gell-Mann and George Zweig's quark model, but the 1969 prize was only awarded to Murray Gell-Mann. Afterward, Ivar Waller, the member of Nobel Committee for Physics was sorry that Sakata had not received a prize.[23]

In September 1970, Hideki Yukawa politely wrote to Waller informing him that Sakata had been ill when the nomination was written; since then, his condition had worsened significantly. Three weeks later, Sakata died. Yukawa informed Waller that a prize to Sakata would have brought him much honor and encouragement. He, then, in the name of leading Japanese particle physicists, asked to know what the Nobel committee thought of Sakata's merits, for that would perhaps bring them consolation.[23]



  1. ^ a b Nussbaum, Louis-Frédéric. (2005). "Sakata Shōichi" in Japan Encyclopedia, p. 812, p. 812, at Google Books; n.b., Louis-Frédéric is pseudonym of Louis-Frédéric Nussbaum, see Deutsche Nationalbibliothek Authority File Archived 2012-05-24 at
  2. ^ Hideki YUKAWA; Shoichi SAKATA; Minoru KOBAYASHI; Mitsuo TAKETANI (1938). "On the Interaction of Elementary Particles IV". Proc. Phys.-Math. Soc. Jpn. 20: 319.
  3. ^ Shoichi SAKATA; Takesi INOUE (1942). "Chukanshi to Yukawa ryushi no Kankei ni tuite. (in Japanese)". Nippon Suugaku-Butsuri Gakkaishi. 16. doi:10.11429/subutsukaishi1927.16.232.
  4. ^ Shoichi SAKATA; Takesi INOUE (1946). "On the Correlations between Mesons and Yukawa Particles". Prog. Theor. Phys. 1 (4): 143–150. Bibcode:1946PThPh...1..143S. doi:10.1143/PTP.1.143.
  5. ^ a b T. Nakano; K. Nishijima (1953). "Charge Independence for V-particles". Prog. Theor. Phys. 10 (5): 581–582. Bibcode:1953PThPh..10..581N. doi:10.1143/PTP.10.581.
  6. ^ a b K. Nishijima (1954). "Some Remarks on Even-odd Rule". Prog. Theor. Phys. 12 (1): 107–108. Bibcode:1954PThPh..12..107N. doi:10.1143/PTP.12.107.
  7. ^ M. Gell-Mann (1956). "The Interpretation of the New Particles as Displaced Charge Multiplets". Nuovo Cimento. 4 (Suppl 2): 848–866. Bibcode:1956NCim....4S.848G. doi:10.1007/BF02748000.
  8. ^ Shoichi SAKATA (1956). "On a Composite Model for the New Particles". Prog. Theor. Phys. 16 (6): 686–688. Bibcode:1956PThPh..16..686S. doi:10.1143/PTP.16.686.
  9. ^ E. Fermi; C.N. Yang (1949). "Are Mesons Elementary Particles?". Phys. Rev. 76 (12): 1739–1743. Bibcode:1949PhRv...76.1739F. doi:10.1103/PhysRev.76.1739.
  10. ^ Mineo IKEDA; Shuzo OGAWA; Yoshio OHNUKI (1959). "A Possible Symmetry in Sakata's Model for Bosons-Baryons System". Prog. Theor. Phys. 22 (5): 715–724. Bibcode:1959PThPh..22..715I. doi:10.1143/PTP.22.715.
  11. ^ Mineo IKEDA; Shuzo OGAWA; Yoshio OHNUKI (1960). "A Possible Symmetry in Sakata's Model for Bosons-Baryons System II". Prog. Theor. Phys. 23 (6): 1073–1099. Bibcode:1960PThPh..23.1073I. doi:10.1143/PTP.23.1073.
  12. ^ Yoshio YAMAGUCHI (1959). "A Composite Theory of Elementary Particles". Prog. Theor. Phys. Suppl. 11: 1–36. Bibcode:1959PThPS..11....1Y. doi:10.1143/PTPS.11.1.
  13. ^ Yoshio YAMAGUCHI (1959). "A Model of Strong Interactions". Prog. Theor. Phys. Suppl. 11: 37–51. Bibcode:1959PThPS..11...37Y. doi:10.1143/PTPS.11.37.
  14. ^ Murray GELL-MANN (1961). "The Eightfold Way: A Theory of Strong Interaction Symmetry". doi:10.2172/4008239. Cite journal requires |journal= (help)
  15. ^ Harry J. Lipkin (January 2002). Lie Group for Pedestrians. Dover Books on Physics. ISBN 978-0486421858.
  16. ^ L.B. Okun. Weak Interaction of Elementary Particles. Pergamon Press. ISBN 978-0706505634.
  17. ^ A. GAMBA; R.E. MARSHAK; S. OKUBO (1959). "On a Symmetry in Weak Interaction". PNAS. 45 (6): 881–885. doi:10.1073/pnas.45.6.881. PMC 222657. PMID 16590464.
  18. ^ Ziro MAKI; Masami NAKAGAWA; Yoshio OHNUKI; Shoichi SAKATA (1960). "A Unified Model for Elementary Particles". Prog. Theor. Phys. 23 (6): 1174–1180. Bibcode:1960PThPh..23.1174M. doi:10.1143/PTP.23.1174.
  19. ^ Ziro MAKI; Masami NAKAGAWA; Shoichi SAKATA (1962). "Remarks on the Unified Model of Elementary Particles". Prog. Theor. Phys. 28 (5): 870–880. Bibcode:1962PThPh..28..870M. doi:10.1143/PTP.28.870.
  20. ^ Yasuhisa KATAYAMA; Ken-iti MATUMOTO; Sho TANAKA; Eiji YAMADA (1962). "Possible Unified Models of Elementary Particles with Two Neutrinos". Prog. Theor. Phys. 28 (4): 675–689. Bibcode:1962PThPh..28..675K. doi:10.1143/PTP.28.675.
  21. ^ Asia News & Thailand News Archived 2012-09-09 at
  22. ^ Kent W. Staley; Lost Origins of the Third Generation of Quarks: Theory, Philosophy: Pages 210-229 in Physics in Perspective (PIP), Birkhäuser, Basel (2004). ISSN 1422-6944
  23. ^ a b Robert Marc Friedman, The Politics of Excellence: Behind the Nobel Prize in Science. New York: Henry Holt & Company (October 2001)


External links[edit]