The Higgs transverse momentum distribution at NNLL and its theoretical errors

In this letter, we present the NNLL-NNLO transverse momentum Higgs distribution arising from gluon fusion. In the regime p [subscript ⊥] ∼ m [subscript h] we include the resummation of the large logs at next to next-to leading order and then match on to the α [subscript s] [superscript 2] fixed orde...

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Bibliographic Details
Main Authors: Vaidya, Varun (Author), Rothstein, Ira Z. (Author), Neill, Duff Austin (Contributor)
Other Authors: Massachusetts Institute of Technology. Center for Theoretical Physics (Contributor), Massachusetts Institute of Technology. Department of Physics (Contributor)
Format: Article
Language:English
Published: Springer Berlin Heidelberg, 2016-06-24T19:15:25Z.
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Online Access:Get fulltext
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100 1 0 |a Vaidya, Varun  |e author 
100 1 0 |a Massachusetts Institute of Technology. Center for Theoretical Physics  |e contributor 
100 1 0 |a Massachusetts Institute of Technology. Department of Physics  |e contributor 
100 1 0 |a Neill, Duff Austin  |e contributor 
700 1 0 |a Rothstein, Ira Z.  |e author 
700 1 0 |a Neill, Duff Austin  |e author 
245 0 0 |a The Higgs transverse momentum distribution at NNLL and its theoretical errors 
260 |b Springer Berlin Heidelberg,   |c 2016-06-24T19:15:25Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/103334 
520 |a In this letter, we present the NNLL-NNLO transverse momentum Higgs distribution arising from gluon fusion. In the regime p [subscript ⊥] ∼ m [subscript h] we include the resummation of the large logs at next to next-to leading order and then match on to the α [subscript s] [superscript 2] fixed order result near p [subscript ⊥] ∼ m [subscript h]. By utilizing the rapidity renormalization group (RRG) we are able to smoothly match between the resummed, small p [subscript ⊥] regime and the fixed order regime. We give a detailed discussion of the scale dependence of the result including an analysis of the rapidity scale dependence. Our central value differs from previous results, in the transition region as well as the tail, by an amount which is outside the error band. This difference is due to the fact that the RRG profile allows us to smoothly turn off the resummation. 
520 |a United States. Department of Energy (contracts DOE-ER-40682-143 and DEACO2-C6H03000) 
546 |a en 
655 7 |a Article 
773 |t Journal of High Energy Physics