Low scale inflation with a curvaton
Jessica Cook 11/14/17
1608.08625, PRD: J Bramante, J Cook, A Delgado, A Martin The tensor to scalar ratio r < 0.07
φ2 inflation is basically ruled out many of the simplest large field models ruled out large field = Δφ ≥ MP models that are looking good are the strong gravitational coupling models (R2 inflation, Higgs inflation, etc.) and smaller field models, Δφ ≤ MP becomes interesting to ask, what are the best looking smaller field models small field models generally fine tuned.
Note we know the amplitude of the scalar power 2 spectrum: 9 H P⇣ =2.2 10 2 ⇥ ⇡ ✏MP so smaller scalar inflation -> smaller H -> smaller ε
ε sets slope of potential inflation requires a pretty flat potential anyway, need a ‘really’ flat potential as you go to smaller scales means couplings of the inflaton must get smaller too general small field models often look like: 2 3 V = V0 + g1 + g2 + g3 + ... often models either hilltop…
or inflection point… where derivatives of the potential -> 0 at scales relevant to inflation
becomes easier to explain why the potential is so flat at inflation scales Higgs hilltop?
V = V µ2 2 + 4 0 ask where does field have to start, such that you get enough efolds? 60 4M2 · P 2 60 = end e ⌫ have to start ‘really’ close to the top of the hill!
and there is a quantum uncertainty bound, even at temp=0
H 17 =4 10 GeV 2⇡ ⇥ 32 find inflation could only last: N =1.4 10 max ⇥ ideally you could write a model where only two potential terms are really relevant at inflation scales. Like 1 2 2 1 4 V = V0 m V = V 2 0 4 And while these models do work in the large field regime, they don’t in the small field regime. or rather they can generate enough inflation in the small field regime, but will generate totally wrong answers for ns. one can write small field models of the form: V = V g g 2 g 3 + ... 0 1 2 3 but need keep multiple of those g’s and balance them against each other and the tuning of all the parameters will get worse and worse the smaller scale you want to go further the models that work, that give the right As and ns, are so flat, the potential changes so slowly with φ for the V0… end up with leftover dark energy in the end example:
V = (1014)4 (5 1010)3 103 3 ⇥ imagine adding a higher dimensional term to turn potential around, keep it from being tachyonic