By Jyh-Ping Hsu
Offers a self-contained reference/text introducing usual difficulties linked to particleparticle, particle-surface, and surface-surface interactions, focusing on stable levels dispersed in a liquid part. DLC: floor chemistry.
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11]). Similarly as above, we can force the system to provide the required n-point functions by introducing external currents besides Jx ; Rxy . k/ denoted by Rx1 :::xn (k D 1; : : : ; n): iS ! k/ with respect to these sources will give us the k-point functions. We require that the fully connected part coincide with the predefined values. k/ through Vk . The physical value of the vertices comes from the requirements ı ŒVk =ıVj D 0. Since we fixed all the correlation functions up to the n-point 40 2 Finite Temperature Field Theories: Review functions, the perturbative expansion should contain only n-particle-irreducible (nPI) diagrams, which remain connected even after cutting n internal lines.
11]). Similarly as above, we can force the system to provide the required n-point functions by introducing external currents besides Jx ; Rxy . k/ denoted by Rx1 :::xn (k D 1; : : : ; n): iS ! k/ with respect to these sources will give us the k-point functions. We require that the fully connected part coincide with the predefined values. k/ through Vk . The physical value of the vertices comes from the requirements ı ŒVk =ıVj D 0. Since we fixed all the correlation functions up to the n-point 40 2 Finite Temperature Field Theories: Review functions, the perturbative expansion should contain only n-particle-irreducible (nPI) diagrams, which remain connected even after cutting n internal lines.
We require only two features for S0 : it should provide a solvable system, and its predictions should be close to the true physical characterization of the system. If these are fulfilled, then we may hope that the small deviations of the leading-order predictions from the exact characteristic quantities can be gradually taken into account by some perturbative series. 2/, as was expected in naive perturbation theory. This consideration has far-reaching consequences: in fact, the choice of the unperturbed Lagrangian, and thus the perturbation theory itself, is already an interpretation of the physical system.