2020
DOI: 10.48550/arxiv.2012.12491
|View full text |Cite
Preprint
|
Sign up to set email alerts
|

Superconducting instabilities in a spinful Sachdev-Ye-Kitaev model

Étienne Lantagne-Hurtubise,
Vedangi Pathak,
Sharmistha Sahoo
et al.

Abstract: We introduce a spinful variant of the complex Sachdev-Ye-Kitaev model with time reversal symmetry, which can be solved exactly in the limit of a large number N of degrees of freedom. At low temperature, the phase diagram of the model includes a compressible non-Fermi liquid and a strongly-correlated spin singlet superconductor that shows a tunable enhancement of the gap ratio predicted by BCS theory. The two phases are separated by a first-order phase transition, in the vicinity of which a gapless superconduct… Show more

Help me understand this report
View published versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

0
2
0

Year Published

2021
2021
2021
2021

Publication Types

Select...
1

Relationship

0
1

Authors

Journals

citations
Cited by 1 publication
(2 citation statements)
references
References 34 publications
0
2
0
Order By: Relevance
“…The model is originally in 0 + 1 − d dimensions and its fermionic fields are Majorana neutral fermions. This feature, if taken seriously, already implies that the charge and spin degrees of freedom have been dropped out of the model 45 , when describing the electronic carriers. Indeed Majorana Fermions are neutral and interaction J grows to infinity but is fully local and momentum is not conserved.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…The model is originally in 0 + 1 − d dimensions and its fermionic fields are Majorana neutral fermions. This feature, if taken seriously, already implies that the charge and spin degrees of freedom have been dropped out of the model 45 , when describing the electronic carriers. Indeed Majorana Fermions are neutral and interaction J grows to infinity but is fully local and momentum is not conserved.…”
Section: Discussionmentioning
confidence: 99%
“…The transferred momentum q is a 3 − d vector in the liquid, but it is only defined in two dimensions in the J E −k,−ω J E k,ω term. We overcame the same difficulty in Eq.s (45,47), by considering the convolution (with k− integration) as in Eq. (56) of Subsection III.B, which corresponds to averaging in space, but by assuming that the fluctuation correlations are localized within a volume ∼ ã2 .…”
Section: A Marginal Fermi Liquid (Mfl) For T T Cohmentioning
confidence: 99%