REVIEW
On the Possibility of Large Axion Decay Constants
High Energy Physics - Theory · Submitted 28 Mar 2003 · 18 references
Pith's verdict: The high-harmonics objection is the real contribution, and it is better grounded than the reader's report suggests; the genuine gap is the missing explicit V(θ), not the harmonic step.
T0 · AI review
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Referee report
The paper
The paper claims
Across heterotic, Type I, Type II and M-theory vacua, the authors argue that any axion with a decay constant above the Planck scale also picks up order-one high harmonics, leaving it no better an inflaton than a Planck-scale axion.
The reading
Extended reading notes
Core claim
The paper's load-bearing assertion is stated in the conclusions: 'In each case the required axion field arises from the components of a p-form gauge potential along a p-cycle in the limit that the cycle shrinks to zero size. There are always light states and/or low action instantons, which arise in this limit, and give rise to rapidly varying contributions to the axion potential ... which effectively rescale the decay constant to the Planck scale.' If correct, no controlled string vacuum supplies a periodic field with a decay constant parametrically above the Planck scale and a potential flat enough for natural inflation.
Load-bearing premise
The argument depends on the premise that whenever the naive decay constant exceeds the Planck scale, the Fourier coefficients of the axion effective action at harmonic number n of order f_A/M_p are unsuppressed, so the potential genuinely varies on Planck-scale distances in the canonical field. This is asserted from instanton and light-state estimates (for example the paragraph after Eq. 22 in section 3.3, and the membrane-instanton discussion around Eq. 29 in section 4) but is never computed for any example. If the low harmonics happened to dominate despite high-n terms being present, natural inflation could still proceed, and the central claim would fail even with every decay-constant formula in the paper intact.
Original abstract
The decay constant of the QCD axion is required by observation to be small compared to the Planck scale. In theories of "natural inflation," and certain proposed anthropic solutions of the cosmological constant problem, it would be interesting to obtain a large decay constant for axion-like fields from microscopic physics. String theory is the only context in which one can sensibly address this question. Here we survey a number of periodic fields in string theory in a variety of string vacua. In some examples, the decay constant can be parameterically larger than the Planck scale but the effective action then contains appreciable harmonics of order $f_A/M_p$. As a result, these fields are no better inflaton candidates than Planck scale axions.
The compiled record
The paper's own sentences, arranged, kept beside the review and separate from it. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
The abstract, sentence by sentence
The decay constant of the QCD axion is required by observation to be small compared to the Planck scale. In theories of "natural inflation," and certain proposed anthropic solutions of the cosmological constant problem, it would be interesting to obtain a large decay constant for axion-like fields from microscopic physics. String theory is the only context in which one can sensibly address this question. Here we survey a number of periodic fields in string theory in a variety of string vacua. In some examples, the decay constant can be parameterically larger than the Planck scale but the effective action then contains appreciable harmonics of order $f_A/M_p$. As a result, these fields are no better inflaton candidates than Planck scale axions.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The decay constant of the QCD axion is required by observation to be small compared to the Planck scale. | background 1.00 | 0.06 | 0.06 | asserted 1.00 |
| s1 | In theories of "natural inflation," and certain proposed anthropic solutions of the cosmological constant problem, it would be interesting to obtain a large decay constant for axion-like fields from microscopic physics. | background 0.90 | 0.04 | 0.03 | hedged possibility 0.50 |
| s2 | String theory is the only context in which one can sensibly address this question. | background 0.75 | 0.06 | 0.04 | asserted 1.00 |
| s3 | Here we survey a number of periodic fields in string theory in a variety of string vacua. | contribution 0.89 | 0.86 | 0.03 | asserted 0.95 |
| s4 | In some examples, the decay constant can be parameterically larger than the Planck scale but the effective action then contains appreciable harmonics of order $f_A/M_p$. | result 0.98 | 0.70 | 0.17 | hedged possibility 0.56 |
| s5 | As a result, these fields are no better inflaton candidates than Planck scale axions. | interpretation 0.84 | 0.68 | 0.54 | asserted 1.00 |
What was examined, and what was not
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References
How later papers used it
182 later papers cite it
1 later paper by other authors is listed below: 1 cited it as support.
Cites it as support 1 of 25 papers with this label
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This is borne out in examples [ref] , where it is very difficult to realize $f ≫M_pl$ in a controlled manner.
Instanton Expansions and Phase Transitions (2020) · Introduction · 1.00
How the literature uses it
164 arXiv papers cite this in 232 sentences
Papers citing it · 181 sentences without a confident label
Contests it 1 paper
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In all cases, their decay constants were found to be bounded above as $f ≲M_Pl$.[ [ref] incorrectly claims the model-independent heterotic axion, i.e., the 4d dual of $B_μν$, has $f = M_Pl$.
The Weak Gravity Conjecture: A Review · Axions in string theory · contest 0.72
Uses its method or tool 1 paper
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We will use ([ref]), ([ref]), guided by [ref] , to determine the decay constants in our specific examples below.
Gravity Waves and Linear Inflation from Axion Monodromy · Axion Kinetic Terms · 0.95
Uses its data or values 1 paper
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Given that we expect $A$ and $B$ to be $O(1)$ numbers, once again we have failed to find a large mass hierarchy – once again we use the result of [ref] for the axion decay constant of the canonically-normalized field.
Axion Inflation and Gravity Waves in String Theory · KL racetrack models · 1.00
Cites it as support 20 papers
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Within the framework of string theory we expect $f$ to be at most as large as the string scale $M_String ≤M_Pl$ [ref] .[Because of the rather high value of the observed tensor modes we expect large values for the potential $V^1/4 ∼ 2· 10^16 GeV$ and a rather high value $M_String≥V^1/4$ of the string scale as well.] Values of $M_String$ and $f$ larger than $M_Pl$ would lead us to the uncontrollable regime of strongly interacting string theory where a meaningful discussion of the flatness of a potential will be impossible.
Aligned Natural Inflation: Monodromies of two Axions · Introduction · 0.96
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However, as shown in [ref] (and reviewed above) such decay constants are not available in this regime of string theory.
Axion Inflation and Gravity Waves in String Theory · KKLT: an exact volume-axion mass ratio · 0.97
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Present indications are that such decay constants will not occur in a consistent theory of quantum gravity [ref] .
An Ignoble Approach to Large Field Inflation · Introduction · 0.96
Cites it as background 26 papers
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Theories of light axions may be subject to theoretical constraints including the weak gravity and swampland conjectures [ref] , and perhaps related to these constraints, there can be limitations on physically allowed objects and dynamical processes, particularly involving large excursions of the scalar in spacetime [ref] .
Virtual and Thermal Schwinger Processes · Bounds on Field Excursions · 0.89
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But it was already noticed by the authors of [ref] that the embedding of extra-natural inflation to string theory was difficult, and this point was further examined in [ref] .
Large Field Inflation Models from Higher-Dimensional Gauge Theories · Introduction · 0.80
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String theory compactifications can provide many axions descending from the various $p$-form potentials of ten-dimensional supergravity (see [ref] for a comprehensive discussion), but there exist no complete examples in which the decay constants are suitably large and the construction is parametrically controlled.[See, however, [ref] for recent proposals to obtain large decay constants in string theory.] Indeed, there are generic arguments that suggest that it is quite difficult to obtain large decay constants in which the string construction is under good control [ref] .
Aligned Natural Inflation in String Theory · Natural Inflation and Decay Constant Alignment · 0.88
Discussion
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