The chiral phase transition at finite temperature is investigated in the linear sigma model, which is regarded as a low energy effective theory of QCD with three momentum cutoff, in the variational method with the Gaussian approximation in the functional Schrödinger picture. It is shown that the Goldstone theorem is retained and the meson pair excitations are automatically included by taking into account the linear response to the external fields. It is pointed out that the behavior of chiral phase transition depends on the three-momentum cutoff, which leads to the careful treatment of the problem.Subject Index: 233 §1. IntroductionIt is well known that the chiral symmetry plays an essential role in the quark and hadronic world governed by the quantum chromodynamics (QCD). Especially, the spontaneous chiral symmetry breaking leads to the existence of the pion, 1) which plays an important role in the nuclear and hadron physics. One of the recent interests in the hadron physics is the chiral symmetry restoration in the context of the BNL Relativistic Heavy Ion Collider (RHIC) and/or the CERN Large Hadron Collider (LHC). 2) It is believed that the chiral symmetry is restored in the high temperature and/or high baryon density, which might or may be created in the above mentioned experiments.The finite temperature phase transition in the field theoretical treatment was investigated in the context of the phase transition in the early universe. 3) Systematically, the field theoretical treatment for the systems at finite temperature was developed in the early stage. 4), 5) Further, another approach 6) to the finite temperature systems was devised with the variational technique in terms of the functional Schrödinger picture with Gaussian approximation 7), 8) for the bosonic field theory. In this paper, we intend to adopt a slight different variational approach to the bosonic field theory at finite temperature.As for the low energy region of the strong interaction, the low energy effective theories of QCD give very useful tool until now to understand the physics of hadrons, especially, based on the chiral symmetry, while the lattice QCD simulation is developed for the problems related to the chiral symmetry. In the low energy region of QCD, the pion and its chiral partner, namely sigma meson, are important ingredients. As an effective theory of QCD, the linear sigma model 9) gives a powerful tool to understand the many properties of low energy hadron physics, which contains pions and sigma meson paying attention to the chiral symmetry.