Perturbation theory for particles in one-dimensional, central- or axial-symmetric fields

1997 ◽  
Vol 112 (1) ◽  
pp. 888-891
Author(s):  
Yu. I. Polyakov
1990 ◽  
Vol 68 (2) ◽  
pp. 198-205 ◽  
Author(s):  
Heinrich Hoff

Taking into account the dependence of the heat capacity and heat conductivity on temperature, one obtains a nonlinear field equation of temperature. This nonlinear partial differential equation is resolved by perturbation theory for the particular case of a homogeneous system. The solution is checked by some criteria of control derived from thermostatics, from steady state transport, and from spatial symmetry. It forms the theoretical framework of nonlinear heat waves to be discussed in a future paper.


1990 ◽  
Vol 02 (04) ◽  
pp. 479-494 ◽  
Author(s):  
PETER D. HISLOP ◽  
SHU NAKAMURA

Spectral properties of one-dimensional Schrödinger operators with unbounded potentials are studied. The main example is the Stark Hamiltonian with unbounded Anderson-type random perturbations. In this case, it is shown that if the perturbation is o(x) then the spectrum is the real line and absolutely continuous except for eigenvalues with no accumulation points. If the perturbation is larger than O(x), then the Hamiltonian has no absolutely continuous spectrum. The methods of proof involve the Mourre estimate and trace-class perturbation theory as recently used by Simon and Spencer.


10.14311/1257 ◽  
2010 ◽  
Vol 50 (5) ◽  
Author(s):  
P. Amore ◽  
F. M. Fernández

We study a harmonic molecule confined to a one-dimensional box with impenetrable walls. We explicitly consider the symmetry of the problem for the cases of different and equal masses. We propose suitable variational functions and compare the approximate energies given by the variation method and perturbation theory with accurate numerical ones for a wide range of values of the box length. We analyze the limits of small and large box size.


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