Abstract

If the fifth dimension is a one-dimensional connected manifold, up to diffeomorphism, the only possible space–times will be M 4 × R 1 , M 4 × R 1 / Z 2 , M 4 × S 1 and M 4 × S 1 / Z 2 . And there exist two possibilities for the cosmological constant along the fifth dimension: the cosmological constant is constant, and the cosmological constant is sectionally constant. We construct general models with parallel 3-branes and constant/sectionally constant cosmological constant along the fifth dimension on those kinds of the space–times. Moreover, we point out that for a compact fifth dimension, the sum of the brane tensions is zero, and for a non-compact fifth dimension, the sum of the brane tensions is positive. Furthermore, we assume the observable brane which includes our world should have positive tension, and obtain that the gauge hierarchy problem can be solved in those scenarios. We also discuss some simple models.

Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.