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Compensation for large tensor modes with iso-curvature perturbations in CMB anisotropies
Cosmology and Nongalactic Astrophysics · Submitted 24 Mar 2014
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim To realize such a suppression, we consider anti-correlated iso-curvature perturbations which could be realized in the simple curvaton model.
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The abstract, sentence by sentence
Recently, BICEP2 has reported the large tensor-to-scalar ratio $r=0.2^{+0.07}_{-0.05}$ from the observation of the cosmic microwave background (CMB) B-mode at degree-scales. Since tensor modes induce not only CMB B-mode but also the temperature fluctuations on large scales, to realize the consistent temperature fluctuations with the Planck result we should consider suppression of scalar perturbations on corresponding large scales. To realize such a suppression, we consider anti-correlated iso-curvature perturbations which could be realized in the simple curvaton model.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Recently, BICEP2 has reported the large tensor-to-scalar ratio $r=0.2^{+0.07}_{-0.05}$ from the observation of the cosmic microwave background (CMB) B-mode at degree-scales. | background 0.99 | 0.04 | 0.04 | asserted 1.00 |
| s1 | Since tensor modes induce not only CMB B-mode but also the temperature fluctuations on large scales, to realize the consistent temperature fluctuations with the Planck result we should consider suppression of scalar perturbations on corresponding large scales. | background 0.84 | 0.10 | 0.17 | asserted 0.85 |
| s2 | To realize such a suppression, we consider anti-correlated iso-curvature perturbations which could be realized in the simple curvaton model. | method 0.75 | 0.41 | 0.25 | hedged possibility 0.99 |
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The paper
Original abstract
Recently, BICEP2 has reported the large tensor-to-scalar ratio $r=0.2^{+0.07}_{-0.05}$ from the observation of the cosmic microwave background (CMB) B-mode at degree-scales. Since tensor modes induce not only CMB B-mode but also the temperature fluctuations on large scales, to realize the consistent temperature fluctuations with the Planck result we should consider suppression of scalar perturbations on corresponding large scales. To realize such a suppression, we consider anti-correlated iso-curvature perturbations which could be realized in the simple curvaton model.
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References
How the literature uses it
17 arXiv papers cite this in 25 sentences
Papers whose main result relates to this one's
States the same result 1 paper
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We show that the tension in the bound on the tensor-to-scalar ratio $r$ between Planck and BICEP2 can be resolved by introducing the anti-correlated isocurvature perturbations.
Isocurvature perturbations and tensor mode in light of Planck and BICEP2 · 0.96
Papers citing it · 15 sentences without a confident label
Cites it as background 10 papers
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To relieve this tension, some possible extensions to the $Λ$CDM+$r$ model have been discussed such as the ruining spectral index [ref] introduced by BICEP2 (see also in Refs. [ref] ), the additional relativistic degrees of freedom beyond the three active neutrinos and photons [ref] , the suppression of the adiabatic perturbations on large scales [ref] , the blue tilted tensor [ref] , and the isocurvature mode [ref] and so on.
Reconciling the Tension Between Planck and BICEP2 Through Early Dark Energy · Introduction · 0.82
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Inflationary modifications include a large running of the scalar tilt [ref] ; more explicit features in the inflationary scalar spectra [ref] ; or anticorrelated isocurvature perturbations [ref] .
Neutrinos help reconcile Planck measurements with both Early and Local Universe · Introduction · 0.84
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Some possible extensions of the model to resolve the tension have been discussed since the data release of BICEP2 such as the running spectral index [ref] , the suppression of the adiabatic perturbations on large scales [ref] , the presence of the extra relativistic particles [ref] , blue-tilted tensor spectrum [ref] , the existence of anti-correlated isocurvature mode [ref] , and so on.
Isocurvature perturbations and tensor mode in light of Planck and BICEP2 · Introduction · 0.89
What it cites · 21 sentences without a confident label
Uses data or values from 3 papers
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Although these papers used different parameterization from that used in Ref. [ref] , obtained results are consistent.], by using the WMAP3 and other data sets the constraints on the value of $B_m$ and $r$ are respectively given by $B_m cosθ_m ≥- 0.13$ and $r ≤0.49$.
Cosmological Constraints on Isocurvature and Tensor Perturbations · Compensation caused by iso-curvature perturbations · 0.88
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The latter gives the upper bound on the tensor-to-scalar ratio as $r < 0.11$ obtained from the combined analysis of the CMB temperature fluctuations and other data sets [ref] .
Planck 2013 results. XVI. Cosmological parameters · Introduction · 0.85
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The latter gives the upper bound on the tensor-to-scalar ratio as $r < 0.11$ obtained from the combined analysis of the CMB temperature fluctuations and other data sets [ref] .
Planck 2013 results. XXII. Constraints on inflation · Introduction · 0.85
Cites as background 20 papers
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Based on this result, there have appeared a number of interesting papers [ref] .
Hint of relic gravitational waves in the Planck and WMAP data · Introduction · 0.97
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Based on this result, there have appeared a number of interesting papers [ref] .
Higgs Chaotic Inflation and the Primordial B-mode Polarization Discovered by BICEP2 · Introduction · 0.97
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Based on this result, there have appeared a number of interesting papers [ref] .
Solving the Tension between High-Scale Inflation and Axion Isocurvature Perturbations · Introduction · 0.97
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