1983
DOI: 10.1103/physrevlett.51.1830
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Mass Inequalities for Quantum Chromodynamics

Abstract: For n-flavor lattice QCD rigorous lower bounds are derived on the masses of baryons, for even n^6, and on the masses of flavor-nonsinglet mesons, for even n ^ 2. The lower bounds are proportional to the pion mass. The consequence of these inequalities for chiral-symmetry breaking is considered.

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Cited by 230 publications
(223 citation statements)
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“…By contrast, the situation for scalar and pseudo-scalar correlators is quite different, as we will discuss better by looking at spatial correlation functions in the next subsection, and indicates that at this temperature we do not yet see evidence of the restoration of the U(1) A symmetry. Notice that the correlation functions still satisfy the Weingarten's mass inequalities [59].…”
Section: Temporal Correlation Functionsmentioning
confidence: 99%
“…By contrast, the situation for scalar and pseudo-scalar correlators is quite different, as we will discuss better by looking at spatial correlation functions in the next subsection, and indicates that at this temperature we do not yet see evidence of the restoration of the U(1) A symmetry. Notice that the correlation functions still satisfy the Weingarten's mass inequalities [59].…”
Section: Temporal Correlation Functionsmentioning
confidence: 99%
“…We observe that above the critical temperature the measured Ps and V effective masses change their order and increase ∝ T , feature shared with the "free" mesons. The inversion in the order of the masses essentially implies that the propagators are not dominated by a narrow state (compare [25]), however not every wide spectral function leads to this inversion, therefore this similarity may have significance. After we tuned the free quarks to simulate the (full) data in the ρ channel, the pseudo-scalar remains, however, still well below the "free" results (a similar observation has been made in [7]).…”
Section: Effective Mass Of Ee-pp Propagators At Nonzero Tmentioning
confidence: 99%
“…Likewise one can show that naive hopping yields a repulsive interaction for the vector channel (spin wave function: ↑↓ + ↓↑), i.e. despite all approximations, the Weingarten inequality [16] is satisfied for our model.…”
Section: A Solutions Withmentioning
confidence: 99%