Skip to main content
U.S. Department of Energy
Office of Scientific and Technical Information

The nonrelativistic limit of the Dirac operator: Splitting of the operator and classification of the discrete spectrum

Thesis/Dissertation ·
OSTI ID:6895508
Two problems related to the non-relativistic limit of the Dirac operator are discussed. The first is can the Dirac operator be explicitly split into an electron and a positron part. The second is whether the discrete spectrum can be classified into electron energy levels and positron energy levels, and if so, how. Our main results are: (1)Given a relative boundedness condition on the potentials, the Dirac operator H(c) has a spectral gap of the form ({minus}mc{sup 2}+l, mc{sub 2}{minus}1) for c large enough. (2)A condition on the potential V which is sufficient to ensure that H(c) has a spectral gap at zero. (3)The standard theorems on resolvent convergence generalize to the case of pseudoresolvent convergence. (4){plus minus}H(c) {minus}mc{sup 2} converges to H{sup {plus minus}}P{sup {plus minus}} in the norm pseudoresolvent sense, where H{sup +} and H{sup {minus}} are the associated Pauli-Schroedinger operators and P{sup +} and P{sup {minus}} are the projections on the upper and lower spaces of spinors. (5)The constant {minus}l from (1) is a lower bound for H{sup +} and H{sup {minus}}.(6) Result 1 can be sharpened as follows: If {minus}K and {minus}L are lower bounds for H{sup {minus}} and H{sup +}, respectively, and {var epsilon} > 0, then H(c) has a spectral gap of the form ({minus}mc{sup 2} + K + {var epsilon}, mc{sup 2} - L - {var epsilon}) for c large enough. (7)In analogy with 4, we have ({plus minus}H(c) - mc{sup 2})Q{sup {plus minus}}(c) {yields} H{sup {plus minus}}P{sup {plus minus}} in the norm pseudoresolvent sense, where Q{sup +}(c) and Q{sup {minus}}(c) are the spectral projections of H(c) corresponding to the positive and negative halves of the spectrum respectively. (8)Using 7, the Dirac operator splits into an electron part, a positron part, and a rest mass part. (9)The existence of a spectral gap classifies the discrete spectrum into electron energy levels and positron energy levels.
Research Organization:
California Univ., Los Angeles, CA (USA)
OSTI ID:
6895508
Country of Publication:
United States
Language:
English