Perfectly invisible P T $$ \mathcalP}\mathcal{T} $$ -symmetric zero-gap systems, conformal field theoretical kinks, and exotic nonlinear supersymmetry

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Perfectly invisible P T $$ \mathcalP}\mathcal{T} $$ -symmetric zero-gap systems, conformal field theoretical kinks, and exotic nonlinear supersymmetry ; volume:2017 ; number:12 ; day:12 ; month:12 ; year:2017 ; pages:1-36 ; date:12.2017
Journal of high energy physics ; 2017, Heft 12 (12.12.2017), 1-36, 12.2017

Classification: Physik

Creator: Guilarte, Juan Mateos

Contributor: Plyushchay, Mikhail S.
SpringerLink (Online service)

DOI: 10.1007/JHEP12(2017)061

URN: urn:nbn:de:1111-2018021012489

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 14.08.2025, 11:01 AM CEST

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Guilarte, Juan Mateos
Plyushchay, Mikhail S.
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

$Conformal bridge transformation, PT $$ \mathcalPT} $$ - and supersymmetry$

Conformal bridge transformation, PT $$ \mathcalPT} $$ - and supersymmetry

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

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

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

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

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

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

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

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

$C P $$ \mathcalC}\mathcal{P} $$ violation with an unbroken C P $$ \mathcalC}\mathcal{P} $$ transformation$

C P $$ \mathcalC}\mathcal{P} $$ violation with an unbroken C P $$ \mathcalC}\mathcal{P} $$ transformation

$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

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

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

$Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity$

Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity

$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

$Conformal bridge transformation, PT $$ \mathcalPT} $$ - and supersymmetry$

Conformal bridge transformation, PT $$ \mathcalPT} $$ - and supersymmetry

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

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

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

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

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

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

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

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

$C P $$ \mathcalC}\mathcal{P} $$ violation with an unbroken C P $$ \mathcalC}\mathcal{P} $$ transformation$

C P $$ \mathcalC}\mathcal{P} $$ violation with an unbroken C P $$ \mathcalC}\mathcal{P} $$ transformation

$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

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

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

$Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity$

Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity

$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

$Conformal bridge transformation, PT $$ \mathcalPT} $$ - and supersymmetry$

Conformal bridge transformation, PT $$ \mathcalPT} $$ - and supersymmetry

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

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

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

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

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

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

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

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

$C P $$ \mathcalC}\mathcal{P} $$ violation with an unbroken C P $$ \mathcalC}\mathcal{P} $$ transformation$

C P $$ \mathcalC}\mathcal{P} $$ violation with an unbroken C P $$ \mathcalC}\mathcal{P} $$ transformation

$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

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

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

$Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity$

Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity

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Perfectly invisible P T $$ \mathcalP}\mathcal{T} $$ -symmetric zero-gap systems, conformal field theoretical kinks, and exotic nonlinear supersymmetry

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Other Objects (12)

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

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

Conformal bridge transformation, PT $$ \mathcalPT} $$ - and supersymmetry

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

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

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

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

C P $$ \mathcalC}\mathcal{P} $$ violation with an unbroken C P $$ \mathcalC}\mathcal{P} $$ transformation

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

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

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

Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity

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

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

Conformal bridge transformation, PT $$ \mathcalPT} $$ - and supersymmetry

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

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

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

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

C P $$ \mathcalC}\mathcal{P} $$ violation with an unbroken C P $$ \mathcalC}\mathcal{P} $$ transformation

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

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

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

Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity

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

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

Conformal bridge transformation, PT $$ \mathcalPT} $$ - and supersymmetry

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

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

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

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

C P $$ \mathcalC}\mathcal{P} $$ violation with an unbroken C P $$ \mathcalC}\mathcal{P} $$ transformation

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

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

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

Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity

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