Statements (24)
| Predicate | Object |
|---|---|
| gptkbp:instanceOf |
gptkb:mathematical_concept
|
| gptkbp:appliesTo |
two-dimensional systems
one-dimensional systems |
| gptkbp:author |
gptkb:Herbert_Wagner
gptkb:N._David_Mermin |
| gptkbp:compatibleWith |
three-dimensional systems
|
| gptkbp:field |
condensed matter physics
statistical physics |
| https://www.w3.org/2000/01/rdf-schema#label |
Mermin–Wagner theorem
|
| gptkbp:influenced |
low-dimensional magnetism
theory of phase transitions |
| gptkbp:namedAfter |
gptkb:Herbert_Wagner
gptkb:N._David_Mermin |
| gptkbp:publicationYear |
1966
|
| gptkbp:publishedIn |
gptkb:Physical_Review_Letters
|
| gptkbp:relatedTo |
gptkb:Ising_model
gptkb:Goldstone_theorem gptkb:XY_model spontaneous symmetry breaking |
| gptkbp:state |
Continuous symmetries cannot be spontaneously broken at finite temperature in systems with sufficiently short-range interactions in one or two dimensions.
|
| gptkbp:yearProposed |
1966
|
| gptkbp:bfsParent |
gptkb:Landau–Peierls_instability
gptkb:N._David_Mermin |
| gptkbp:bfsLayer |
6
|