The light CP-even MSSM Higgs mass resummed to fourth logarithmic order

Abstract We present the calculation of the light neutral CP-even Higgs mass in the MSSM for a heavy SUSY spectrum by resumming enhanced terms through fourth logarithmic order (N$$^{3}$$ 3 LL), keeping terms of leading order in the top Yukawa coupling $$\alpha _t$$ αt , and NNLO in the strong couplin...

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Main Authors: R. V. Harlander, J. Klappert, A. D. Ochoa Franco, A. Voigt
Format: Article
Language:English
Published: SpringerOpen 2018-10-01
Series:European Physical Journal C: Particles and Fields
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-018-6351-6
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spelling doaj-add5ee863fc640f9ba600dfc7fb2ead92020-11-25T00:13:53ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522018-10-01781011610.1140/epjc/s10052-018-6351-6The light CP-even MSSM Higgs mass resummed to fourth logarithmic orderR. V. Harlander0J. Klappert1A. D. Ochoa Franco2A. Voigt3Institute for Theoretical Particle Physics and Cosmology, RWTH Aachen UniversityInstitute for Theoretical Particle Physics and Cosmology, RWTH Aachen UniversityInstitute for Theoretical Particle Physics and Cosmology, RWTH Aachen UniversityInstitute for Theoretical Particle Physics and Cosmology, RWTH Aachen UniversityAbstract We present the calculation of the light neutral CP-even Higgs mass in the MSSM for a heavy SUSY spectrum by resumming enhanced terms through fourth logarithmic order (N$$^{3}$$ 3 LL), keeping terms of leading order in the top Yukawa coupling $$\alpha _t$$ αt , and NNLO in the strong coupling $$\alpha _s$$ αs . To this goal, the three-loop matching coefficient for the quartic Higgs coupling of the SM to the MSSM is derived to order $$\alpha _t^2\alpha _s^2$$ αt2αs2 by comparing the perturbative EFT to the fixed-order expression for the Higgs mass. The new matching coefficient is made available through an updated version of the program Himalaya. Numerical effects of the higher-order resummation are studied using specific examples, and sources of theoretical uncertainty on this result are discussed.http://link.springer.com/article/10.1140/epjc/s10052-018-6351-6
collection DOAJ
language English
format Article
sources DOAJ
author R. V. Harlander
J. Klappert
A. D. Ochoa Franco
A. Voigt
spellingShingle R. V. Harlander
J. Klappert
A. D. Ochoa Franco
A. Voigt
The light CP-even MSSM Higgs mass resummed to fourth logarithmic order
European Physical Journal C: Particles and Fields
author_facet R. V. Harlander
J. Klappert
A. D. Ochoa Franco
A. Voigt
author_sort R. V. Harlander
title The light CP-even MSSM Higgs mass resummed to fourth logarithmic order
title_short The light CP-even MSSM Higgs mass resummed to fourth logarithmic order
title_full The light CP-even MSSM Higgs mass resummed to fourth logarithmic order
title_fullStr The light CP-even MSSM Higgs mass resummed to fourth logarithmic order
title_full_unstemmed The light CP-even MSSM Higgs mass resummed to fourth logarithmic order
title_sort light cp-even mssm higgs mass resummed to fourth logarithmic order
publisher SpringerOpen
series European Physical Journal C: Particles and Fields
issn 1434-6044
1434-6052
publishDate 2018-10-01
description Abstract We present the calculation of the light neutral CP-even Higgs mass in the MSSM for a heavy SUSY spectrum by resumming enhanced terms through fourth logarithmic order (N$$^{3}$$ 3 LL), keeping terms of leading order in the top Yukawa coupling $$\alpha _t$$ αt , and NNLO in the strong coupling $$\alpha _s$$ αs . To this goal, the three-loop matching coefficient for the quartic Higgs coupling of the SM to the MSSM is derived to order $$\alpha _t^2\alpha _s^2$$ αt2αs2 by comparing the perturbative EFT to the fixed-order expression for the Higgs mass. The new matching coefficient is made available through an updated version of the program Himalaya. Numerical effects of the higher-order resummation are studied using specific examples, and sources of theoretical uncertainty on this result are discussed.
url http://link.springer.com/article/10.1140/epjc/s10052-018-6351-6
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