English (United Kingdom)

https://curated-unify.zendy.io/wp-json/zendy-region/v1/featured_content/oa?rat=en

https://curated-unify.zendy.io/wp-json/zendy-region/v1/highlighted_journal/

Global: Zendy Tools annual

Presents the keyphrase highlighting as premium feature

Keyphrase Highlighting

Presents the summarisation as premium feature

Summarisation

Insights

Presents the pdf analysis as premium feature

PDF Analysis

Presents the zaia usage as premium feature

ZAIA

Global: Zendy Tools monthly

Global: Zendy Plus monthly

Presents the access of premium content as premium feature

Premium Content

Global: Zendy Plus annual

Global: Zendy Free Plan

With use of a 6-form field strength of ten-dimensional type IIA supergravityover AdS_4 x CP^3, when S^7/Z_k is considered as a S^1 Hopf fibration on CP^3,we earn a fully localized solution in the bulk of Euclideanized AdS_4. Indeed,this object appears in the external space because of wrapping a D4(M5)-braneover some parts of the respective internal spaces. Interestingly, thissupersymmetry breaking SU(4)x U(1)-singlet mode exists in already known spectrawhen one uses the 8_c gravitino representation of SO(8). To adjust the boundarytheory, we should swap the original 8_s and 8_c representations forsupercharges and fermions in the Aharony-Bergman-Jafferis-Maldacena model. Theprocedure could later be interpreted as adding an anti-D4(M5)-brane to theprime N=6 membrane theory resulting in a N=0 antimembrane theory while othersymmetries are preserved. Then, according to the well-known state-operatorcorrespondence rules, we find a proper dual operator with the conformaldimension of {\Delta}=3 that matches to the bulk massless pseudoscalar state.After that, by making use of some fitting ansatzs for the used matter fields,we arrive at an exact boundary solution and comment on the other related issuesas well.

New Instantons in AdS_4/CFT_3 from D4-Branes Wrapping Some of CP^3