Witten anomaly in 4d heterotic compactificaitons with N $$ \mathcalN} $$ = 2 supersymmetry

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Witten anomaly in 4d heterotic compactificaitons with N $$ \mathcalN} $$ = 2 supersymmetry ; volume:2020 ; number:7 ; day:24 ; month:7 ; year:2020 ; pages:1-15 ; date:7.2020
Journal of high energy physics ; 2020, Heft 7 (24.7.2020), 1-15, 7.2020

Creator: Enoki, Yuichi
Sato, Yotaro
Watari, Taizan

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP07(2020)180

URN: urn:nbn:de:101:1-2020092001051125355400

Rights: Open Access; Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 14.08.2025, 10:49 AM CEST

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Enoki, Yuichi
Sato, Yotaro
Watari, Taizan
SpringerLink (Online service)

Other Objects (12)

$Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry$

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

$Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry$

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

$Superpotential of three dimensional N $$ \mathcalN} $$ = 1 heterotic supergravity$

Superpotential of three dimensional N $$ \mathcalN} $$ = 1 heterotic supergravity

$On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions$

On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

$Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity$

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

$Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry$

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

$Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets$

Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

$Gravitational couplings in N $$ \mathcalN} $$ = 2 heterotic compactifications with Wilson lines$

Gravitational couplings in N $$ \mathcalN} $$ = 2 heterotic compactifications with Wilson lines

$Defect multiplets of N = 1 $$ \mathcalN}=1 $$ supersymmetry in 4d$

Defect multiplets of N = 1 $$ \mathcalN}=1 $$ supersymmetry in 4d

$Basis for non-factorizable superamplitudes in N $$ \mathcalN} $$ = 1 supersymmetry$

Basis for non-factorizable superamplitudes in N $$ \mathcalN} $$ = 1 supersymmetry

Anomaly corrected heterotic horizons

$N $$ \mathcalN} $$ =2 heterotic string compactifications on orbifolds of K3 × T 2$

N $$ \mathcalN} $$ =2 heterotic string compactifications on orbifolds of K3 × T 2

$Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry$

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

$Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry$

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

$Superpotential of three dimensional N $$ \mathcalN} $$ = 1 heterotic supergravity$

Superpotential of three dimensional N $$ \mathcalN} $$ = 1 heterotic supergravity

$On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions$

On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

$Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity$

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

$Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry$

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

$Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets$

Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

$Gravitational couplings in N $$ \mathcalN} $$ = 2 heterotic compactifications with Wilson lines$

Gravitational couplings in N $$ \mathcalN} $$ = 2 heterotic compactifications with Wilson lines

$Defect multiplets of N = 1 $$ \mathcalN}=1 $$ supersymmetry in 4d$

Defect multiplets of N = 1 $$ \mathcalN}=1 $$ supersymmetry in 4d

$Basis for non-factorizable superamplitudes in N $$ \mathcalN} $$ = 1 supersymmetry$

Basis for non-factorizable superamplitudes in N $$ \mathcalN} $$ = 1 supersymmetry

Anomaly corrected heterotic horizons

$N $$ \mathcalN} $$ =2 heterotic string compactifications on orbifolds of K3 × T 2$

N $$ \mathcalN} $$ =2 heterotic string compactifications on orbifolds of K3 × T 2

$Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry$

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

$Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry$

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

$Superpotential of three dimensional N $$ \mathcalN} $$ = 1 heterotic supergravity$

Superpotential of three dimensional N $$ \mathcalN} $$ = 1 heterotic supergravity

$On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions$

On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

$Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity$

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

$Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry$

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

$Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets$

Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

$Gravitational couplings in N $$ \mathcalN} $$ = 2 heterotic compactifications with Wilson lines$

Gravitational couplings in N $$ \mathcalN} $$ = 2 heterotic compactifications with Wilson lines

$Defect multiplets of N = 1 $$ \mathcalN}=1 $$ supersymmetry in 4d$

Defect multiplets of N = 1 $$ \mathcalN}=1 $$ supersymmetry in 4d

$Basis for non-factorizable superamplitudes in N $$ \mathcalN} $$ = 1 supersymmetry$

Basis for non-factorizable superamplitudes in N $$ \mathcalN} $$ = 1 supersymmetry

Anomaly corrected heterotic horizons

$N $$ \mathcalN} $$ =2 heterotic string compactifications on orbifolds of K3 × T 2$

N $$ \mathcalN} $$ =2 heterotic string compactifications on orbifolds of K3 × T 2

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Witten anomaly in 4d heterotic compactificaitons with N $$ \mathcalN} $$ = 2 supersymmetry

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Other Objects (12)

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

Superpotential of three dimensional N $$ \mathcalN} $$ = 1 heterotic supergravity

On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

Gravitational couplings in N $$ \mathcalN} $$ = 2 heterotic compactifications with Wilson lines

Defect multiplets of N = 1 $$ \mathcalN}=1 $$ supersymmetry in 4d

Basis for non-factorizable superamplitudes in N $$ \mathcalN} $$ = 1 supersymmetry

Anomaly corrected heterotic horizons

N $$ \mathcalN} $$ =2 heterotic string compactifications on orbifolds of K3 × T 2

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

Superpotential of three dimensional N $$ \mathcalN} $$ = 1 heterotic supergravity

On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

Gravitational couplings in N $$ \mathcalN} $$ = 2 heterotic compactifications with Wilson lines

Defect multiplets of N = 1 $$ \mathcalN}=1 $$ supersymmetry in 4d

Basis for non-factorizable superamplitudes in N $$ \mathcalN} $$ = 1 supersymmetry

Anomaly corrected heterotic horizons

N $$ \mathcalN} $$ =2 heterotic string compactifications on orbifolds of K3 × T 2

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

Superpotential of three dimensional N $$ \mathcalN} $$ = 1 heterotic supergravity

On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

Gravitational couplings in N $$ \mathcalN} $$ = 2 heterotic compactifications with Wilson lines

Defect multiplets of N = 1 $$ \mathcalN}=1 $$ supersymmetry in 4d

Basis for non-factorizable superamplitudes in N $$ \mathcalN} $$ = 1 supersymmetry

Anomaly corrected heterotic horizons

N $$ \mathcalN} $$ =2 heterotic string compactifications on orbifolds of K3 × T 2

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