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Htm (33 of 93)19122005 09:23:48 isotopic spin symmetry of nuclear physics, 464 isotropic three-dimensional simple harmonic oscillator, 40 isovector current, 187 isovector magnetic moment, 101 ITO, 40, 58, 59, 61, 71, 74, 88, 94, 109, 468, 469, 552 j-shell, 45 Jacob and Wick, 60, 239, 557 Jensens inequality, 566 KARMEN, 525, 526 kinetic energy for vector mesons, 250 Klein-Gordon equation, 121, 362 Kohn-Sham (KS) approach, 220, 229 KS wave functions and eigenvalues, 230 lagrangian, 178, 182, 184, 196, 208, 210, 211, 248, 251, 252, 378, 437, 440, 448, 450-455, 458, 463, 514, 549, 559 lagrangian density, 117, 120, 122, 139, 146, 161, optoin, 179, 187, 191, 192, 195, 232, 267, 277, 426 lagrangian for point nucleons, 571 lagrangian of QCD, 254 lagrangian of QED, 570 lagrangian of the standard model, 572 Laguerre polynomials, 42 LAMPF, 504 Landau gauge, 162, 422 large Nc limit of QCD, 378, 381 lattice gauge theory (LGT), 271, 272, 283, 291, 295, 306, 316, 339 lattice sites, 274 binaru and fre Dirac fields, 513, 559 left- and right-handed isospin, 559 left-handed neutrinos, 447, 519 Legendre polynomials, 46 Legendre transformation, 226, 228 lepton current, 433, 456, 467, 569 lepton fields, 431, 446 lepton flavor number, 524 lepton kinetic energy, 447 lepton lagrangian, 569 lepton matrix elements, 480, 481 lepton number, 433, 519, 521 lepton tensor, 384 lepton traces, 481, 482, 488, 533, 534 leptons, 458, 515 level orderings in the nuclear potential, 41, 44 LGT, 329, 351, 356, 359, 360, 409 Lie algebra, 181, 186, 247, 249, 253 Lie algebra s u ( 2 ) ~ su(2)R, 559 light scalar of dynamic origin, 196 line integral, 276 linearization of the equations of motion, 82 link, 274, 275, 280, 281, 291, 299, 303, 331, 353 link variables, 290, 296, 298, 300, 308, 330, 332-335, 339 Liouvilles theorem, 414 liquid drop, 15 local SU(2)w U(l)w gauge invariance, 461 local SU(2) matrix h(z),214, 562 local current and charge density operators, 54, 471 local gauge invariance, 248, 251, 253, 271, 351, 450, 451 local binary option system free transformation, 248, 249, 251 localized nuclear density, 55, 79, 262, 474, 529 localized source, 57, 473 long-range correlations, 35 long-wavelength, 541 long-wavelength expansion, 491 long-wavelength limit, 63, 65, 70, 474, 475 longitudinal multipoles, 468 loops in QCD, 379 Lorentz force, 574 Lorentz transformation, 231, 239, 241, 411, 436 low-mass scalar, 195, 196, 197, 211 M.

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(1983). 6 Partially Uncompetitive Inhibition This inhibition type is a special form of uncompetitive inhibition when the ter- nary EAI complex is still active: 2X100 2X101 2X102 kB1 k2 EA A EA 3 EP k1 I k4 EAIk36 EIP 2. No reversal of current was permissible, else the effect would not manifest. If they had different signs, then l1l2 0.

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The gravitational effect binqry this on Io is to pull it forward in its direction of motion so increasing both the angular momentum and energy of its orbit. We thank all the contributors to this book for their time and effort in preparing the manuscripts, published by [4, 5] are shown in Fig.

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