2002
DOI: 10.1016/s0370-2693(01)01430-7
|View full text |Cite
|
Sign up to set email alerts
|

Anomalies in orbifold field theories

Abstract: We study the constraints on models with extra dimensions arising from local anomaly cancellation. We consider a five-dimensional field theory with a U(1) gauge field and a charged fermion, compactified on the orbifold S1/(Z2×Z2′). We show that, even if the orbifold projections remove both fermionic zero modes, there are gauge anomalies localized at the fixed points. Anomalies naively cancel after integration over the fifth dimension, but gauge invariance is broken, spoiling the consistency of the theory. We di… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

8
118
0

Year Published

2002
2002
2020
2020

Publication Types

Select...
6
3

Relationship

0
9

Authors

Journals

citations
Cited by 94 publications
(126 citation statements)
references
References 16 publications
8
118
0
Order By: Relevance
“…K is the usual modified Bessel function [30]. The singularities of E 1 can arise for specific values of s, from poles of the Gamma functions in the rhs of the first line in 16 16 An alternative to using (C.6) is to make a simple binomial expansion of the parenthesis under the sum in (C. The singularities of E1 given in (C.8) arise now from either the Gamma functions (if s is a negative integer or zero) and from the usual singularity of ζ-function at 2k + 2s = 1, (if s is ±1/2, −3/2, −5/2, −7/2, · · ·).…”
Section: Jhep03(2005)009mentioning
confidence: 99%
“…K is the usual modified Bessel function [30]. The singularities of E 1 can arise for specific values of s, from poles of the Gamma functions in the rhs of the first line in 16 16 An alternative to using (C.6) is to make a simple binomial expansion of the parenthesis under the sum in (C. The singularities of E1 given in (C.8) arise now from either the Gamma functions (if s is a negative integer or zero) and from the usual singularity of ζ-function at 2k + 2s = 1, (if s is ±1/2, −3/2, −5/2, −7/2, · · ·).…”
Section: Jhep03(2005)009mentioning
confidence: 99%
“…This result was derived in Ref. 52 within the equivalent formulation of this model as an S 1 /(Z 2 × Z ′ 2 ) orbifold, as described before. It has also been shown in Ref.…”
Section: Bulk Fermions On Smentioning
confidence: 66%
“…The orbifold allows us to obtain chiral fermions, and the fermion fields generally contribute to anomalies at boundaries [80,81]. In our model, U(1) V charges of the fermion fields that have the Neumann boundary condition at y = 0 tend to become anomalous.…”
Section: Overview Of the E 6 Modelmentioning
confidence: 99%