TY - JOUR
T1 - Type-III and IV interacting Weyl points
AU - Nissinen, J.
AU - Volovik, G. E.
N1 - | openaire: EC/H2020/694248/EU//TOPVAC
PY - 2017
Y1 - 2017
N2 - 3+1-dimensional Weyl fermions in interacting systems are described by effective quasi-relativistic Green’s functions parametrized by a 16 element matrix eα μin an expansion around the Weyl point. The matrix eα μcan be naturally identified as an effective tetrad field for the fermions. The correspondence between the tetrad field and an effective quasi-relativistic metric gμν governing the Weyl fermions allows for the possibility to simulate different classes of metric fields emerging in general relativity in interacting Weyl semimetals. According to this correspondence, there can be four types of Weyl fermions, depending on the signs of the components g00 and g00 of the effective metric. In addition to the conventional type-I fermions with a tilted Weyl cone and type-II fermions with an overtilted Weyl cone for g00 > 0 and respectively g00 > 0 or g00 < 0, we find additional “type-III” and “type-IV” Weyl fermions with instabilities (complex frequencies) for g00 < 0 and g00 > 0 or g00 < 0, respectively. While the type-I and type-II Weyl points allow us to simulate the black hole event horizon at an interface where g00 changes sign, the type-III Weyl point leads to effective spacetimes with closed timelike curves.
AB - 3+1-dimensional Weyl fermions in interacting systems are described by effective quasi-relativistic Green’s functions parametrized by a 16 element matrix eα μin an expansion around the Weyl point. The matrix eα μcan be naturally identified as an effective tetrad field for the fermions. The correspondence between the tetrad field and an effective quasi-relativistic metric gμν governing the Weyl fermions allows for the possibility to simulate different classes of metric fields emerging in general relativity in interacting Weyl semimetals. According to this correspondence, there can be four types of Weyl fermions, depending on the signs of the components g00 and g00 of the effective metric. In addition to the conventional type-I fermions with a tilted Weyl cone and type-II fermions with an overtilted Weyl cone for g00 > 0 and respectively g00 > 0 or g00 < 0, we find additional “type-III” and “type-IV” Weyl fermions with instabilities (complex frequencies) for g00 < 0 and g00 > 0 or g00 < 0, respectively. While the type-I and type-II Weyl points allow us to simulate the black hole event horizon at an interface where g00 changes sign, the type-III Weyl point leads to effective spacetimes with closed timelike curves.
UR - http://www.scopus.com/inward/record.url?scp=85016480274&partnerID=8YFLogxK
U2 - 10.1134/S0021364017070013
DO - 10.1134/S0021364017070013
M3 - Article
AN - SCOPUS:85016480274
VL - 105
SP - 447
EP - 452
JO - JETP LETTERS / PISMA V ZHURNAL EKSPERIMENTALNOI I TEORETICHESKOI FIZIKI
JF - JETP LETTERS / PISMA V ZHURNAL EKSPERIMENTALNOI I TEORETICHESKOI FIZIKI
SN - 0021-3640
IS - 7
ER -