higgs couplings in heft

Asked by zheng

Hello,

My questions is mainly about understanding the higgs couplings in heft.

I wanted to modify the Higgs to top quark couplings. In the file "couplings.f" of SM model, there is only ghtop(1) and ghtop(2) representing left-handed and right-handed couplings respectively. In heft_v4 model, there are two additional couplings, gh3top(1) and gh3top(2), do I need to modify this two couplings defined by gh3top at the same time? I don't quite understand the difference between gh3top and ghtop.

The second question is that after I modified the Higgs to top couplings, do I need to modify the Higgs to gluon gluon couplings accordingly because top loop contributes to the H-g-g coupling? I found the expressions of Higgs to gluon couplings in "couplings.f" but I am not sure if the relation between Higgs to top couplings has be correlated automatically.

Thank you very much.

Question information

Language:
English Edit question
Status:
Solved
For:
MadGraph5_aMC@NLO Edit question
Assignee:
Rikkert Frederix Edit question
Solved by:
Rikkert Frederix
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Rikkert Frederix (frederix) said :
#1

Hello,

The gh3top coupling is not used by default, and was implemented to simulate a pseudo-scalar Higgs. Therefore, you don't need to change that coupling. However, both ghtop and gh3top are NOT used for the g-g-H effective vertex, but only for the Higgs Yukawa coupling. The g-g-h and g-g-g-h effective coupling constants are GH and GH4, respectively. They are computed in the m_top->infinity limit, but also some subleading terms in the Taylor expansion around tau=(m_higgs/2*m_top)^2 are kept.

So, you have to change the ghtop, gh and gh4 couplings consistently to change the strength of the Higgs coupling to top quarks.

Best regards,
Rikkert

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zheng (yjzheng218) said :
#2

Thanks Rikkert Frederix, that solved my question.

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zheng (yjzheng218) said :
#3

Hi Rikkert,

Thanks to the heft model, I get what I need from your codes.

But I am still curious about the approximation expansion that in the limit of \tau->0 to the 3rd order and \tau_W->0 to the 6th order. The relevant original function is arcsin[sqrt{tau}], which can be directly computed by fortran, I am wondering why don't we just put the original function inside the code rather than make series expansion to a certain order? Thank you.

Best regards,
Ya-Juan

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Best Rikkert Frederix (frederix) said :
#4

Dear Ya-Juan,
Indeed, if one is just interested in gg-> h (or h-> gamma gamma) then one could use the full form factor (the arcsin function). However, that is not the correct factor for Higgs+one jet production. Therefore we have decided to use an intermediate solution which is to expand the coupling to the first couple of orders.
Kind regards,
Rikkert

Revision history for this message
zheng (yjzheng218) said :
#5

Thanks Rikkert Frederix, that solved my question.