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Jiro Kodaira and QCD Analysis of Structure Functions
Dedicated to the memory of Jiro Kodaira T. Uematsu (Kyoto Univ.) at KEK workshop “Towards precision QCD physics” March 10, 2007
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Jiro Kodaira’s Personal History
Born in Nagano,Japan in 1951 Graduated from Kyoto Univ. in 1974 Finished Ph.D in 1979 1979 -1980 RA at YITP, Kyoto Univ. 1980 - JSPS Fellow at SLAC 1982 - RA at Kobe University 1983 - RA & AP at Hiroshima Univ. 2005 - Professor at KEK
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Asymptotic freedom ’73 Kodaira’s paper EMC effects ’88 LHC starting ’07 1951 ’70 ’74 1979 2005 2006 ’80 ’82 ’83 under grad. SLAC Hiroshima KEK Born in Nagano Graduate course in Kyoto Univ. Kobe Yukawa Inst.
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Kodaira’s contributions to perturbative QCD
QCD higher order corrections to the polarized deep inelastic scattering Kyoto Group flavor-singlet nucleon polarized structure function Kodaira 1979 Soft gluon resummation Kodaira & Trentadue Spin correlation in top quark production Kodaira & Parke, … Axial Anomaly plays an important role NLL order
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QCD Higher Order Effects
Physical quantity Anomalous dim. Next-Leading-log Leading-log Kyoto Group Kodaira et al flavor non-singlet Phys.Rev.D20 (1979) 627; Nucl.Phys. B159 (1979) 99
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Polarized DIS & Structure Functions
nucleon spin incident lepton scattered quark scattered lepton or Structure tensor Unpolarized structure fns. polarized structure fns.
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Flavor Singlet Case Axial anomaly Kodaira QCD correction
Axial vector current Flavor Singlet Case Axial anomaly Triangle anomaly 2-loop anomalous dim. does not vanish + other diagram Kodaira Nucl.Phys. B165 (1980)129 : # of flavors QCD correction
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Parton distribution functions are scheme-dependent
1988 EMC at CERN “Spin Crisis” Altarelli-Ross Phys. Lett B212 (1988) 391 Gluon polarization contributes due to anomaly Or Parton distribution functions are scheme-dependent J. Kodaira and T. U. Nucl. Phys. B141 (1978) 497
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Kodaira’s other contributions to pQCD
Twist-3 effects & BC sum rule in Yasui, Tanaka, Nasuno, Tochimura; Sasaki, Matsuda, T.U. Twist-4 effects in Kawamura, Yasui, T.U. Spin correlation in top quark production Parke, Nasuno, Kiyo, Hori, Morii Polarized Drell-Yan processes Kawamura, Tanaka, Shimizu, Yokoya Small-x of in resummation Kiyo, Tochimura
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Higher-twist effects in polarized structure fns.
Twist-3 and twist-4 operators Tanaka's talk characteristics of higher-twist operators Represents quark and gluon correlations The number of relevant composite operators increases as n increases Renormalization of higher-twist operators Operator mixing through renormalization becomes quite complicated
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Twist-3 effects in twist-2 twist-3 quark-gluon operators
Mixing very complicated Burkhardt-Cottingham sum rule
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Twist-4 effects on spin structure fn
Flavor non-singlet Twist-4 effects Flavor singlet Off-shell Green’s functions in covariant gauge
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KEK An expert in the field of pQCD and expected to advise experimentalists about physics at LHC and ILC from deep understanding of the theory Leader’s role of “Minami-Tateya” (numerical analysis) group doing automatic computation of Feynman graphs and various simulations for the analyses of data from collider experiments International collaborations just started LAPTH Annecy, NIKHEF (GRACE-FORM project), …
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Kodaira’s connections in the world
SLAC S. Parke (Fermilab), L. Trentadue (Parma), L. Dixon, S. Drell, S. Brodsky,… RIKEN-BNL R.L.Jaffe (MIT), X.Ji (Maryland), W. Vogelsang, D. Boer, M. Stratmann,.. DESY Zeuthen J. Bluemlein, S. Moch, … NIKHEF J. Vermaseren, … LAPTH D. Perret-Gallix, F. Boudjema,.. CERN G. Altarelli, …. Firenze S. Catani, … Collaboration with KEK Minami-tateya Group
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7th International Symposium on Radiative Corrections
APPLICATION OF QUANTUM FIELD THEORY TO PHENOMENOLOGY Shonan Village, Japan October 2-7, 2005
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Concluding remarks Very sad but his achievements will remain
Take over Kodaira’s spirit for the research in high-energy physics and pass it to the younger generations Efforts should be taken toward precisions of QCD as well as Electro-weak physics Promote the international collaborations as Jiro Kodaira had tried to establish
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Conclusion QCD is a Theory of Strong Interaction
From Jiro’s Slide in Aug06 Conclusion QCD is a Theory of Strong Interaction Non-abelin Gauge Theory One of the “most” beautiful The. in 20th Century Forced to solve (at least) two problems now 1. do calculation for practical purpose (LHC, ILC, …) 2. reveal dynamics of gauge theory using the simplest but the most difficult one namely QCD
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