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The phase diagram of an SU(2)_L x SU(2)_R lattice Higgs-Yukawa model withfinite lambda is constructed using mean field theory. The phase diagram bears asuperficial resemblance to that for infinite lambda, however as lambda isdecreased the paramagnetic region shrinks in size. For small lambda the phasetransitions remain second order, and no new first order transitions are seen.Comment: 9 pages, 3 postscript figures, RevTex. To appear in PR

physical review. d. particles, fields, gravitation, and cosmology/physical review. d. particles and fields

Mean field phase diagram of an SU(2<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi mathvariant="italic">L</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>×SU(2<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi mathvariant="italic">R</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>lattice…

Mean field phase diagram of an SU(2)L×SU(2)Rlattice…