Stability of Matter
By Michael Loss. 2005
217 citations recorded by the source corpus.
Subfields: Atomic and Molecular Physics, and Optics, Mathematical Physics
View Paper: https://www.semanticscholar.org/paper/9a9849b18c40e76752ccca98c17608f68512dc7f
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Atomic and Molecular Physics, and Optics
- Robert Seiringer
- Elliott H. Lieb
- Gerald Teschl
- R. Benguria
- E. W. Mielke
- M. Ashbaugh
- F. Schunck
- Mathieu Lewin
In Mathematical Physics
- Robert Seiringer
- R. Benguria
- Gerald Teschl
- Elliott H. Lieb
- E. W. Mielke
- M. Ashbaugh
- F. Schunck
- Rupert L. Frank
Citations in the corpus
- Isoperimetric Inequalities for Eigenvalues of the Laplacian (2007, background): “In particular, Benguria and Loss [31] have shown a connection between this problem and a special case of the Lieb–Thirring inequalities [120, 117], inequalities which play a fundamental role in Lieb and Thirring’s proof of the stability of matter (see, in particular, [119] and the review article [11”
- Mathematical Methods in Quantum Mechanics (2009, background): “For multi-particle operators from the viewpoint of stability of matter, see Lieb and Seiringer [41].”
- The Stability of Matter in Quantum Mechanics (2009, methodology): “1 LT Inequalities: Formulation The non-relativistic versions of the inequalities discussed in this chapter were invented in 1975 [134, 135] in order to give an alternative, simpler proof of the stability of non-relativistic matter, first proved by Dyson and Lenard [44].”
- General relativistic boson stars (2003, background): “That bosons cannot be localised within their Compton wavelength is guaranteed by Heisenberg’s uncertainty principle [107,186].”
- The Crystallization Conjecture: A Review (2015, unknown): “For such a classical model, Coulomb interaction is not adapted, since the energy tends to −∞ as two particles of opposite charge get closer to each other, and the model is unstable (note, however, that it is stable in the quantum case, as it was proved by Dyson-Lenard [59, 112] and Lieb-Thirring [12”