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Evading the Lyth Bound in Hybrid Natural Inflation
High Energy Physics - Theory · Submitted 8 May 2013
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We show that this pessimistic conclusion is naturally avoided in a rather broad class of small-field models.
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The abstract, sentence by sentence
Generically, the gravitational-wave or tensor-mode contribution to the primordial curvature spectrum of inflation is tiny if the field-range of the inflaton is much smaller than the Planck scale. We show that this pessimistic conclusion is naturally avoided in a rather broad class of small-field models. More specifically, we consider models where an axion-like shift symmetry keeps the inflaton potential flat (up to non-perturbative cosine-shaped modulations), but inflation nevertheless ends in a waterfall-regime, as is typical for hybrid inflation. In such hybrid natural inflation scenarios (examples are provided by Wilson line inflation and fluxbrane inflation), the slow-roll parameter $\epsilon$ can be sizable during an early period (relevant for the CMB spectrum). Subsequently, $\epsilon$ quickly becomes very small before the tachyonic instability eventually terminates the slow roll regime. In this scenario, one naturally generates a considerable tensor-mode contribution in the curvature spectrum, collecting nevertheless the required amount of e-foldings during the final period of inflation. While non-observation of tensors by Planck is certainly not a problem, a discovery in the medium to long term future is realistic.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Generically, the gravitational-wave or tensor-mode contribution to the primordial curvature spectrum of inflation is tiny if the field-range of the inflaton is much smaller than the Planck scale. | background 1.00 | 0.05 | 0.03 | asserted 0.90 |
| s1 | We show that this pessimistic conclusion is naturally avoided in a rather broad class of small-field models. | contribution 0.49 | 0.88 | 0.69 | asserted 1.00 |
| s2 | More specifically, we consider models where an axion-like shift symmetry keeps the inflaton potential flat (up to non-perturbative cosine-shaped modulations), but inflation nevertheless ends in a waterfall-regime, as is typical for hybrid inflation. | contribution 0.57 | 0.31 | 0.08 | asserted 0.94 |
| s3 | In such hybrid natural inflation scenarios (examples are provided by Wilson line inflation and fluxbrane inflation), the slow-roll parameter $\epsilon$ can be sizable during an early period (relevant for the CMB spectrum). | result 0.44 | 0.67 | 0.13 | asserted 0.54 |
| s4 | Subsequently, $\epsilon$ quickly becomes very small before the tachyonic instability eventually terminates the slow roll regime. | result 0.73 | 0.63 | 0.07 | asserted 1.00 |
| s5 | In this scenario, one naturally generates a considerable tensor-mode contribution in the curvature spectrum, collecting nevertheless the required amount of e-foldings during the final period of inflation. | result 0.99 | 0.77 | 0.65 | asserted 0.97 |
| s6 | While non-observation of tensors by Planck is certainly not a problem, a discovery in the medium to long term future is realistic. | interpretation 0.99 | 0.11 | 0.10 | hedged possibility 0.92 |
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The paper
Original abstract
Generically, the gravitational-wave or tensor-mode contribution to the primordial curvature spectrum of inflation is tiny if the field-range of the inflaton is much smaller than the Planck scale. We show that this pessimistic conclusion is naturally avoided in a rather broad class of small-field models. More specifically, we consider models where an axion-like shift symmetry keeps the inflaton potential flat (up to non-perturbative cosine-shaped modulations), but inflation nevertheless ends in a waterfall-regime, as is typical for hybrid inflation. In such hybrid natural inflation scenarios (examples are provided by Wilson line inflation and fluxbrane inflation), the slow-roll parameter $\epsilon$ can be sizable during an early period (relevant for the CMB spectrum). Subsequently, $\epsilon$ quickly becomes very small before the tachyonic instability eventually terminates the slow roll regime. In this scenario, one naturally generates a considerable tensor-mode contribution in the curvature spectrum, collecting nevertheless the required amount of e-foldings during the final period of inflation. While non-observation of tensors by Planck is certainly not a problem, a discovery in the medium to long term future is realistic.
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References
How the literature uses it
12 arXiv papers cite this in 16 sentences
Papers whose main result relates to this one's
States a conflicting result 1 paper
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This shows that non-trivial dynamics can't evade the Lyth bound.
A Field Range Bound for General Single-Field Inflation · 0.81
Papers citing it · 12 sentences without a confident label
Uses its data or values 1 paper
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There, a constraint on $f$ coming from an embedding of the effective potential of Eq. [ref] into a string theory guide the authors to choose the fiducial bound $f≲√(3)/4π$ giving an upper bound $r≃7.6 ×10^-4$ [ref] .
General bounds in Hybrid Natural Inflation · Hybrid Natural Inflation, bounds in the restricted case · 0.88
Compares with it 2 papers
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The achievable enhancement of $r$ is bounded by the amount of running $α≲0.01$ of the spectral index $n_s$ allowed by data (see e.g. [ref] where similarly the $r$-enhancement is bounded by the allowed running $α$.) * Inflation is driven by a combination of the volume modulus and its $C_4$ RR-form axion partner on one of two local symmetrically arranged saddle/inflection points.
Accidental Inflation from K\"ahler Uplifting · Introduction · 0.90
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This corresponds to the situation where $ϵ$ and therefore the tensor to scalar ratio $r = 16ϵ$ is maximal and given by [equation] This is smaller than the value $r ≃7.6·10^-4$ found in the related work [ref] .
D7-Brane Moduli Space in Axion Monodromy and Fluxbrane Inflation · Consequences of Experimental Constraints · 0.99
Cites it as background 1 paper
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In Ref. [ref] , HNI was already given a detailed analysis for its feasibility to reach large values of $r$, for sub-Planckian axion decay constant and sub-Planckian field range.
General bounds in Hybrid Natural Inflation · Hybrid Natural Inflation, bounds in the restricted case · 0.80
What it cites · 68 sentences without a confident label
Uses data or values from 1 paper
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Now, the most recent value [ref] for the power spectrum is $Δ_R^2≡A_S ≃2.2 ×10^-9$ at the fiducial scale $k = 0.05 Mpc^-1$.
Planck 2013 results. XXII. Constraints on inflation · Production of Primordial Black Holes · 0.99
Compares with 1 paper
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By contrast, the authors of [ref] achieve waterfall near the minimum through field theory model building, but they do not consider tensor modes. ] From the fluxbrane perspective, however, things look different: The energy of the two-brane system is minimized in a situation where the branes come very close to each other.
Inflationary models with a flat potential enforced by non-abelian discrete gauge symmetries · Introduction · 0.95
Cites as background 39 papers
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This coupling may provide an efficient channel for reheating [ref] .] This discussion can be taken to the more advanced level of supergravity, where it takes the form of arguing about natural sizes of higher-order terms in the Kähler potential [ref] .
Gauge Field Production in Axion Inflation: Consequences for Monodromy, non-Gaussianity in the CMB, and Gravitational Waves at Interferometers · Introduction · 0.81
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This coupling may provide an efficient channel for reheating [ref] .] This discussion can be taken to the more advanced level of supergravity, where it takes the form of arguing about natural sizes of higher-order terms in the Kähler potential [ref] .
False Vacuum Inflation with Einstein Gravity · Introduction · 0.81
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This coupling may provide an efficient channel for reheating [ref] .] This discussion can be taken to the more advanced level of supergravity, where it takes the form of arguing about natural sizes of higher-order terms in the Kähler potential [ref] .
Hybrid Inflation in Supergravity · Introduction · 0.81
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