Quick Question (EW gaugino mass relation)

In summary, the CMSSM and mSUGRA models parametrize the universe in terms of 4 variables and a sign, while mSUGRA implements a boundary condition relating m_0,A_0,B_0.
  • #1
samr
12
0
Can't for the life of me remember the characteristic EW gaugino mass relation for CMSSM, nor can I track it down.

Anyone know it off the top of their head or link me a paper?

(to clarify, I mean that mSUGRA is commonly defined by the gaugino mass relation 1:2:6 for [tex]M_1:M_2:M_3[/tex])

(maybe more usefully that's [tex]M_\textrm{bino}:M_\textrm{wino}:M_\textrm{gluino}[/tex])
 
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  • #2
What's the difference between msugra and cmssm, in terms of the boundary conditions? I thought they were interchangable: both have universal gaugino masses at the GUT scale, along with a single A term and universal scalars.
 
  • #3
To be honest it doesn't seem to matter since most papers use them interchangeably. However, they are mostly either oversimplifying (since both are considered gravity mediated) or (possibly) mistaken.

The CMSSM is parametrized in terms of 4 variables and a sign at the GUT scale.
That is [tex]m_0[/tex] the sfermion (scalar) mass, [tex]m_\frac{1}{2}[/tex] the gaugino mass, [tex]A_0[/tex] the trilinear coupling and [tex]\tan(\beta)[/tex] the ratio of the vacuum expectation values of the Higgs fields, and the sign of [tex]\mu[/tex] the Higgs mixing parameter..

mSUGRA however is a more constrained model, it implements a boundary condition relating (among other things, but only directly) [tex]m_0,A_0,B_0[/tex] where [tex]B_0[/tex] is the bilinear coupling. This boundary condition is:
[tex]B_0=A_0-m_0[/tex]
While the implication of this isn't obvious if you think of it interms of the pseudo scalar higgs mass [tex]M_3 = \mu B_0[/tex] this is the same as setting [tex]M_3^2=\mu(A_0-m_0)[/tex] at the GUT scale.
This reduces mSUGRA to 3 parameters and a sign ([tex]m_0,m_\frac{1}{2},A_0,\textrm{sign}(\mu)[/tex]) and now [tex]\tan(\beta)[/tex] is an output.

edit: to clarify the [tex]M_3 [/tex] here is NOT the same as the [tex]M_3[/tex] above. In the first post it is the gluino mass, here it is the pseudoscalar higgs mass (with the [tex]H_1H_2[/tex] term in the lagrangian). A slight ambiguity in my notation - sorry.
 
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  • #4
Without having worked through it , I can't see why it would be any different from mSUGRA (the gaugino mass relation), the RGEs aren't horribly affected by the mSUGRA boundary condition so it should be about the same. Oh well.
 
  • #5
I seem to recall a paper by Nilles and someone called ``The gaugino code''. You might check that one out. Why don't you try downloading softSUSY and just do the running and see?
 
  • #6
Already have done that and it comes out roughly the same as mSUGRA (slight deviations in the last term); and yes I have the Gaugino code about - but in any case they should be the same as I think I said earlier. So it was a bit of a pointless question :D

(And they'd need to be 1:2:6 to be consistent any way)
 
  • #7
Yeah, the slight deviations come from higher order loopy effects that softSUSY calculates, I bet. Most of the RGE flow in both cases comes from the coupling constants, as you probably have surmised :)
 

FAQ: Quick Question (EW gaugino mass relation)

1. What is the "Quick Question (EW gaugino mass relation)"?

The "Quick Question (EW gaugino mass relation)" is a simplified version of the Electroweak Gaugino Mass Relation, which is a mathematical relationship between the masses of the three types of particles called gauginos (neutralino, chargino, and gluino) in the Standard Model of particle physics.

2. How is the Electroweak Gaugino Mass Relation derived?

The Electroweak Gaugino Mass Relation is derived from the supersymmetry theory, which proposes that for every known particle, there exists a corresponding "superpartner" particle. The Electroweak Gaugino Mass Relation is obtained by imposing certain symmetry conditions on the supersymmetry equations.

3. What is the significance of the Electroweak Gaugino Mass Relation?

The Electroweak Gaugino Mass Relation is significant because it provides a prediction for the masses of the gaugino particles, which can be tested experimentally. It also helps to determine the underlying symmetry structure of the Standard Model and can potentially provide evidence for the existence of supersymmetry.

4. Are there any experimental tests or evidence for the Electroweak Gaugino Mass Relation?

Yes, there have been several experiments conducted at the Large Hadron Collider (LHC) and other particle accelerators to test the Electroweak Gaugino Mass Relation. So far, the results have been consistent with the predicted values, providing support for the existence of supersymmetry.

5. What are the potential implications if the Electroweak Gaugino Mass Relation is found to be incorrect?

If the Electroweak Gaugino Mass Relation is found to be incorrect, it would mean that the current understanding of the Standard Model and supersymmetry is incomplete. This could open up new avenues for research and potentially lead to a better understanding of the fundamental laws of nature.

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