Physical Foundations of Cosmology

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412 Bibliography


153 (1968), 1. Nonequilibrium hydrogen recombination is considered. The roles of
Lyman-alpha quanta and two-quanta decay of the 2Slevel are noted.

Particle physics and early universe (Chapter 4)


Yang, C., Mills, R. Conservation of isotopic spin and isotopic gauge invariance.Physical
Review, 96 (1954), 191. The first non-Abelian gauge theory based on theSU(2) group
of isotopic spin conservation is constructed.
Gell-Mann, M. A schematic model of baryons and mesons.Physics Letters, 8 (1964), 214;
Zweig, G. CERN Preprints TH 401 and TH 412 (1964) (unpublished). The quark
model is proposed.
Greenberg, O. Spin and unitary spin independence in a paraquark model of baryons and
mesons.Physical Review Letters, 13 (1964), 598; Han, M., Nambu, Y., Three triplet
model with doubleSU( 3 )symmetry.Physical Review B, 139 (1965), 1006; Bardeen,
W., Fritzsch, H., Gell-Mann, M. Light cone current algebra,π^0 decay, ande+e−
annihilation. InScale and Conformal Symmetry in Hadron Physics, ed. Gatto, R.
(1973) p. 139, New York: Wiley. It is found from baryon systematics and from the rate
of neutral pion decay into two photons that quarks of each flavor must come in three
colors.
Stuckelberg, E., Petermann, A. The normalization group in quantum theory.Helvetica Phys-
ica Acta, 24 (1951), 317; La normalisation des constantes dans la theorie des quanta.
Helvetica Physica Acta, 26 (1953), 499; Gell-Mann, M., Low, F. Quantum electro-
dynamics at small distances.Physical Review, 95 (1954), 1300. The renormalization
group method is proposed.
Gross, D., Wilczek, F. Ultraviolet behavior of non-Abelian gauge theories.Physical Review
Letters, 30 (1973), 1343; Politzer, H. Reliable perturbative results for strong interac-
tions?Physical Review Letters, 30 (1973), 1346. The asymptotic freedom of the strong
interaction is discovered using the renormalization group method. The asymptotic free-
dom and its physical implications in theλφ^4 theory, with negativeλ, are discussed
in the earliar papers by: Symanzik K. A field theory with computable large-momenta
behavior.Lettere al Nuovo Cimento, 6 (1973), 77; and Parisi, G. Deep inelastic scat-
tering in a field theory with computable large-momenta behavior.Lettere al Nuovo
Cimento, 7 (1973), 84.
Chodos, A., Jaffe, R., Johnson, K., Thorn, C., Weisskopf, V. A new extended model of
hadrons.Physical Review D, 9 (1974), 3471. The bag model is proposed (see Section
4.2.2).
Glashow, S. Partial symmetries of weak interactions.Nuclear Physics, 22 (1961), 579;
Salam, A., Ward, J. Electromagnetic and weak interactions.Physics Letters, 13 (1964),



  1. TheSU( 2 )×U( 1 )group structure is discussed in relation to electromagnetic and
    weak interactions.
    Higgs, P. Broken symmetries, massless particles and gauge fields.PhysicsLetters, 12 (1964),
    132; Broken symmetries and the masses of gauge bosons.Physics Letters, 13 (1964),
    508; Englert, F., Brout, R. Broken symmetry and the mass of gauge vector mesons.
    Physical Review Letters, 13 (1964), 321; Guralnik, G., Hagen, C., Kibble, T. Global
    conservation laws and massless particles.Physical Review Letters, 13 (1964), 585.
    The mechanism of the generation of the mass of gauge bosons via interaction with a
    classical scalar field is discovered.
    Weinberg, S. A model of leptons.Physical Review Letters, 19 (1967), 1264; Salam, A. Weak
    and electromagnetic interactions. InElementary Particle Theory, Proceedings of the

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