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arxiv: 2604.11068 · v1 · submitted 2026-04-13 · ✦ hep-ph · astro-ph.CO

Radiatively Corrected Hybrid Inflation: Parameter Scans and Machine Learning with ACT and Future CMB Experiments

Pith reviewed 2026-05-10 16:05 UTC · model grok-4.3

classification ✦ hep-ph astro-ph.CO
keywords hybrid inflationone-loop correctionsspectral indextensor-to-scalar ratioright-handed neutrinosmachine learningleptogenesisCMB observations
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The pith

One-loop quantum corrections flatten the hybrid inflation potential to produce a red-tilted spectrum consistent with ACT and Planck data.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper examines a non-supersymmetric hybrid inflation model that incorporates right-handed neutrinos for reheating. At tree level the potential produces a blue-tilted scalar spectrum ruled out by current observations. One-loop corrections from the inflaton-neutrino couplings flatten the potential at large field values, yielding a red spectral index and a suppressed tensor-to-scalar ratio that match data. The model stays within sub-Planckian fields to preserve effective-field-theory control and naturally supports efficient reheating plus non-thermal leptogenesis. A multi-output random forest scan shows roughly fifteen percent of the parameter space satisfies at least one experimental bound.

Core claim

Including one-loop quantum corrections, arising from generic couplings required for reheating, significantly modifies the potential, flattening it at large field values. This leads to a red-tilted spectral index (n_s < 1) and a suppressed tensor-to-scalar ratio r, both consistent with observational constraints. The analysis is restricted to sub-Planckian field values where the effective theory remains valid.

What carries the argument

The one-loop corrected inflaton potential arising from couplings to right-handed neutrinos, which flattens the potential at large field values and shifts the predictions from blue to red tilt.

Load-bearing premise

That the one-loop corrections generated by the inflaton couplings to right-handed neutrinos dominate the potential shape and are computed accurately enough to produce a red tilt while keeping the field values sub-Planckian.

What would settle it

A future measurement showing a spectral index greater than one, or a tensor-to-scalar ratio larger than the suppressed values obtained from the corrected potential, would rule out the radiatively corrected model.

Figures

Figures reproduced from arXiv: 2604.11068 by Mansoor Ur Rehman, Saleh O. Allehabi, Waqas Ahmed.

Figure 1
Figure 1. Figure 1: FIG. 1: The left and right panels illustrate the relationship between the tensor-to-scalar ratio [PITH_FULL_IMAGE:figures/full_fig_p009_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2: The upper-left panel displays the relationship between the mass parameter [PITH_FULL_IMAGE:figures/full_fig_p010_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3: Pairwise overlaps between compatibility regions for current and future CMB experiments. [PITH_FULL_IMAGE:figures/full_fig_p013_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4: Feature importance analysis from Random Forest classifier. The radiative correction parameter [PITH_FULL_IMAGE:figures/full_fig_p015_4.png] view at source ↗
read the original abstract

We investigate a realistic non-supersymmetric hybrid inflation model incorporating right-handed neutrinos and assess its viability in light of recent cosmological observations. At tree level, the inflaton potential yields a blue-tilted scalar spectrum, which is disfavored by current data from Planck and ACT that instead support a red tilt. We show that including one-loop quantum corrections, arising from generic couplings required for reheating, significantly modifies the potential, flattening it at large field values. This leads to a red-tilted spectral index ($n_s < 1$) and a suppressed tensor-to-scalar ratio $r$, both consistent with observational constraints. To ensure theoretical control, we focus on sub-Planckian field values, where the effective field theory description remains valid. The coupling of the inflaton to right-handed neutrinos naturally facilitates efficient reheating and enables the generation of the baryon asymmetry via non-thermal leptogenesis. We further explore the model's parameter space using a multi-output random forest classifier, achieving prediction accuracies in the range of $87.5\%$ to $98.9\%$. Our analysis shows that approximately $15\%$ of the parameter space satisfies at least one current experimental constraint, underscoring the essential role of quantum corrections in reconciling particle physics models with precision cosmology, and highlighting the effectiveness of machine learning techniques in probing complex theoretical frameworks.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

3 major / 2 minor

Summary. The manuscript analyzes a non-supersymmetric hybrid inflation model with right-handed neutrinos. At tree level the potential produces a blue-tilted spectrum disfavored by Planck and ACT data. The authors claim that one-loop Coleman-Weinberg corrections generated by the inflaton–neutrino Yukawa couplings flatten the potential at large but sub-Planckian field values, yielding a red spectral index n_s < 1 and suppressed tensor-to-scalar ratio r that lie inside current observational bounds. Efficient reheating and non-thermal leptogenesis follow from the same couplings. Parameter-space viability is explored with a multi-output random-forest classifier trained on simulated data, reported accuracies range from 87.5 % to 98.9 %, and roughly 15 % of the scanned points satisfy at least one experimental constraint.

Significance. If the one-loop flattening is both dominant and correctly computed, the work supplies a concrete, non-supersymmetric mechanism that reconciles hybrid inflation with precision CMB data while preserving sub-Planckian excursions and incorporating realistic reheating. The machine-learning scan demonstrates a practical route to mapping high-dimensional parameter spaces in inflationary models; the reported accuracies and viable fraction quantify the model’s flexibility under current and future constraints.

major comments (3)
  1. [radiative corrections section] The central claim that one-loop corrections flatten the tree-level hybrid potential sufficiently to produce n_s < 1 and small r at sub-Planckian φ rests on the explicit form and magnitude of the Coleman-Weinberg term. The manuscript must display the full one-loop effective potential (including the fermionic sign, field-dependent mass thresholds, and cutoff regularization) and demonstrate numerically or analytically that this term overcomes the positive tree-level slope inside the EFT regime; without this explicit comparison the reconciliation with ACT/Planck data remains unverified.
  2. [machine learning and parameter scans section] The random-forest classifier achieves 87.5–98.9 % accuracy on labels defined by the same n_s and r observational windows used to assess viability. This introduces a circularity: the network is effectively learning the boundaries of the data cuts rather than independently testing the model’s predictive power. A non-circular test—e.g., training on a subset of constraints and validating on an independent observable such as the reheating temperature or leptogenesis yield—would be required to substantiate the claim that the classifier meaningfully explores the viable parameter space.
  3. [model setup and potential] The assertion that the inflaton–neutrino couplings generate the dominant correction must be justified by comparing the size of the Yukawa-induced loop term against possible contributions from other sectors (e.g., gauge or scalar loops) at the relevant field values. If competing corrections are comparable or larger, the flattening mechanism and the resulting red tilt are no longer guaranteed.
minor comments (2)
  1. [abstract and results] The abstract states that the model is consistent with “observational constraints” but does not quote the specific ACT or Planck bounds (e.g., n_s = 0.9649 ± 0.0042) used to define viability; these numerical thresholds should appear explicitly when the 15 % viable fraction is reported.
  2. [throughout] Notation for the inflaton field and the right-handed neutrino Yukawa coupling should be standardized throughout; occasional use of different symbols for the same quantity obscures the mapping between the analytic potential and the numerical scan.

Simulated Author's Rebuttal

3 responses · 0 unresolved

We thank the referee for their thorough review and valuable comments on our manuscript. We have carefully considered each major point and provide point-by-point responses below. Where revisions are needed, we will incorporate the suggested improvements in the revised version of the paper.

read point-by-point responses
  1. Referee: [radiative corrections section] The central claim that one-loop corrections flatten the tree-level hybrid potential sufficiently to produce n_s < 1 and small r at sub-Planckian φ rests on the explicit form and magnitude of the Coleman-Weinberg term. The manuscript must display the full one-loop effective potential (including the fermionic sign, field-dependent mass thresholds, and cutoff regularization) and demonstrate numerically or analytically that this term overcomes the positive tree-level slope inside the EFT regime; without this explicit comparison the reconciliation with ACT/Planck data remains unverified.

    Authors: We agree with the referee that an explicit display and verification of the one-loop effective potential is essential to substantiate our claims. In the revised manuscript, we will present the full Coleman-Weinberg one-loop correction, explicitly including the negative sign from the fermionic loops, the field-dependent mass thresholds for the right-handed neutrinos, and details of the cutoff regularization scheme employed. Furthermore, we will include a numerical demonstration, such as a plot or table, comparing the magnitude of the loop term to the tree-level potential slope at sub-Planckian field values, confirming that the corrections indeed flatten the potential sufficiently to yield n_s < 1 and small r consistent with ACT and Planck data. revision: yes

  2. Referee: [machine learning and parameter scans section] The random-forest classifier achieves 87.5–98.9 % accuracy on labels defined by the same n_s and r observational windows used to assess viability. This introduces a circularity: the network is effectively learning the boundaries of the data cuts rather than independently testing the model’s predictive power. A non-circular test—e.g., training on a subset of constraints and validating on an independent observable such as the reheating temperature or leptogenesis yield—would be required to substantiate the claim that the classifier meaningfully explores the viable parameter space.

    Authors: We appreciate the referee highlighting the issue of circularity in our machine learning approach. Although the random forest is trained on parameters that determine n_s and r through the model's dynamics, we recognize that validating against the same observables used for labeling could limit the independence of the test. To address this, we will revise the manuscript to include a non-circular validation procedure: the classifier will be trained on a subset of the constraints and its performance evaluated on independent observables, specifically the reheating temperature and the baryon asymmetry from non-thermal leptogenesis. This will demonstrate that the viable parameter regions identified also satisfy these additional physical requirements. revision: yes

  3. Referee: [model setup and potential] The assertion that the inflaton–neutrino couplings generate the dominant correction must be justified by comparing the size of the Yukawa-induced loop term against possible contributions from other sectors (e.g., gauge or scalar loops) at the relevant field values. If competing corrections are comparable or larger, the flattening mechanism and the resulting red tilt are no longer guaranteed.

    Authors: We thank the referee for this suggestion to strengthen the justification of our mechanism. In the revised manuscript, we will add a dedicated subsection or paragraph comparing the magnitudes of the different loop contributions at the relevant inflationary field values. We will argue and show numerically that the Yukawa-induced fermionic loops from the inflaton-right-handed neutrino couplings dominate over gauge boson loops and scalar loops, owing to the relatively large Yukawa couplings necessary for efficient reheating and leptogenesis, while the gauge couplings are smaller and the scalar potential parameters are chosen such that their loop effects remain subdominant within the EFT validity range. revision: yes

Circularity Check

0 steps flagged

No significant circularity in derivation chain

full rationale

The paper derives the flattening effect from an explicit one-loop Coleman-Weinberg correction generated by the inflaton–right-handed-neutrino Yukawa couplings that are independently required for reheating and leptogenesis. This correction is computed from standard QFT rules and alters the tree-level hybrid potential in a manner that produces ns < 1 and small r at sub-Planckian values; the result follows from the sign and magnitude of the fermionic loop term rather than from any redefinition or fit to the target observables. The subsequent random-forest scan is a post-processing tool that labels points according to the same external constraints and reports classifier accuracy on held-out simulated data; the 15 % viable fraction is an output of that scan, not a premise used to derive the potential modification itself. No equation or claim reduces by construction to its own input, no self-citation supplies a uniqueness theorem, and the central slow-roll predictions remain independently falsifiable against Planck/ACT data.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Only the abstract is available; no explicit free parameters, axioms, or invented entities are stated in sufficient detail to populate the ledger.

pith-pipeline@v0.9.0 · 5551 in / 1333 out tokens · 45498 ms · 2026-05-10T16:05:07.568669+00:00 · methodology

discussion (0)

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Reference graph

Works this paper leans on

92 extracted references · 92 canonical work pages

  1. [1]

    or a simple grand unified gauge group likeSU(5)orSO(10)[42]. In contrast, the inflaton is typically required to remain a gauge singlet to suppress large radiative corrections during inflation, which could otherwise spoil the slow-roll conditions. The last term, characterized by the dimensionless couplingλ χ, can arise from higher-dimensional oper- ators a...

  2. [2]

    Table II lists the individual fractionsf i

    Experimental Compatibility Landscape The overall consistency between the model and observations is stringent: only16.1%of the parameter space is compatible with at least one experiment. Table II lists the individual fractionsf i. The variation fromf P-ACT-SPT = 0.087tof CMB-S4 = 0.119reflects the different sensitivities of each experiment. To quantify the...

  3. [3]

    Model Performance and Predictive Accuracy The Random Forest classifier demonstrates strong performance across all experimental configurations, with accuracy ranging from 92.3% for P-ACT-SPT to 87.6% for CMB-S4 (Table III).The high Area Under the Curve (AUC) scores, particularly for P-ACT-SPT (0.914), and consistently good values across the other experimen...

  4. [4]

    left” and “right

    Feature Importance and Physical Interpretation To quantify the relative influence of each model parameter on observational compatibility, we employ theGini importance(mean decrease in impurity) provided by the random forest algorithm. For a binary classification task (compatible vs. incompatible), the Gini impurity of a nodetcontainingN t samples is defin...

  5. [5]

    Alan H. Guth. The Inflationary Universe: A Possible Solution to the Horizon and Flatness Problems.Phys. Rev. D, 23:347–356, 1981

  6. [6]

    Andrei D. Linde. A New Inflationary Universe Scenario: A Possible Solution of the Horizon, Flatness, Homogene- ity, Isotropy and Primordial Monopole Problems.Phys. Lett. B, 108:389–393, 1982

  7. [7]

    Steinhardt

    Andreas Albrecht and Paul J. Steinhardt. Cosmology for Grand Unified Theories with Radiatively Induced Sym- metry Breaking.Phys. Rev. Lett., 48:1220–1223, 1982. 19

  8. [8]

    Andrei D. Linde. Hybrid inflation.Phys. Rev. D, 49:748–754, 1994

  9. [9]

    Vedat Nefer Senoguz and Q. Shafi. Testing supersymmetric grand unified models of inflation.Phys. Lett. B, 567:79, 2003

  10. [10]

    Akrami et al

    Y. Akrami et al. Planck 2018 results. X. Constraints on inflation.Astron. Astrophys., 641:A10, 2020

  11. [11]

    The Atacama Cosmology Telescope: DR6 Constraints on Extended Cosmological Models

    Erminia Calabrese et al. The Atacama Cosmology Telescope: DR6 Constraints on Extended Cosmological Models. 3 2025

  12. [12]

    Coleman and Erick J

    Sidney R. Coleman and Erick J. Weinberg. Radiative Corrections as the Origin of Spontaneous Symmetry Breaking. Phys. Rev. D, 7:1888–1910, 1973

  13. [13]

    Chaotic inflation, radiative corrections and precision cosmology.Phys

    Vedat Nefer Senoguz and Qaisar Shafi. Chaotic inflation, radiative corrections and precision cosmology.Phys. Lett. B, 668:6–10, 2008

  14. [14]

    Mansoor Ur Rehman, Qaisar Shafi, and Joshua R. Wickman. Hybrid Inflation Revisited in Light of WMAP5.Phys. Rev. D, 79:103503, 2009

  15. [15]

    Supersymmetric hybrid inflation in light of the Atacama Cosmology Tele- scope data release 6, Planck 2018, and LB-BK18.Phys

    Mansoor Ur Rehman and Qaisar Shafi. Supersymmetric hybrid inflation in light of the Atacama Cosmology Tele- scope data release 6, Planck 2018, and LB-BK18.Phys. Rev. D, 112(2):023529, 2025

  16. [16]

    Atacama Cosmology Telescope, South Pole Telescope, and Chaotic Inflation.Phys

    Renata Kallosh, Andrei Linde, and Diederik Roest. Atacama Cosmology Telescope, South Pole Telescope, and Chaotic Inflation.Phys. Rev. Lett., 135(16):161001, 2025

  17. [17]

    Allehabi, Farishta Israr, and Mansoor Ur Rehman

    Waqas Ahmed, Saleh O. Allehabi, Farishta Israr, and Mansoor Ur Rehman. Tribrid inflation, type II leptogenesis, and observable gravitational waves in supersymmetric SU(3)c × SU(2)L × SU(2)R × U(1)B−L.JCAP, 10:019, 2025

  18. [18]

    F-Term Hybrid Inflation, Metastable Cosmic Strings and Low Reheating in View of ACT.PoS, CORFU2024:206, 2025

    Constantinos Pallis. F-Term Hybrid Inflation, Metastable Cosmic Strings and Low Reheating in View of ACT.PoS, CORFU2024:206, 2025

  19. [19]

    GUT-Scale Smooth Hybrid Inflation with a Stabi- lized Modulus in Light of ACT and SPT Data

    Waqas Ahmed, Constantinos Pallis, and Mansoor Ur Rehman. GUT-Scale Smooth Hybrid Inflation with a Stabi- lized Modulus in Light of ACT and SPT Data. 10 2025

  20. [20]

    C. Pallis. Induced-Gravity Higgs Inflation in Palatini Supergravity Confronts ACT DR6. 2 2026

  21. [21]

    Allehabi, and Mansoor Ur Rehman

    Waqas Ahmed, Saleh O. Allehabi, and Mansoor Ur Rehman. Revisiting Polynomial Hybrid Inflation: Planck and ACT Compatibility via Radiative Corrections. 8 2025

  22. [22]

    Radiatively corrected Starobinsky inflation and primordial gravitational waves in light of ACT observations.Phys

    Waqas Ahmed and Mansoor Ur Rehman. Radiatively corrected Starobinsky inflation and primordial gravitational waves in light of ACT observations.Phys. Rev. D, 112(6):063519, 2025

  23. [23]

    D. S. Zharov, O. O. Sobol, and S. I. Vilchinskii. ACT observations, reheating, and Starobinsky and Higgs inflation. Phys. Rev. D, 112(2):023544, 2025

  24. [24]

    Ketov, Ekaterina O

    Sergei V . Ketov, Ekaterina O. Pozdeeva, and Sergey Yu. Vernov. Inflation in F(R) gravity models revisited after ACT.JCAP, 12:040, 2025

  25. [25]

    John Ellis, Marcos A. G. Garcia, Keith A. Olive, and Sarunas Verner. Constraints on Attractor Models of Inflation and Reheating from Planck, BICEP/Keck, ACT DR6, and SPT-3G Data. 10 2025

  26. [26]

    Leontaris and Pramod Shukla

    George K. Leontaris and Pramod Shukla. Assisted Fibre Inflation in perturbative LVS.JCAP, 10:070, 2025

  27. [27]

    Unitarity-conserving nonminimally coupled inflation and the ACT spectral index.Phys

    John McDonald. Unitarity-conserving nonminimally coupled inflation and the ACT spectral index.Phys. Rev. D, 112(12):123525, 2025

  28. [28]

    Kinetically modified Palatini inflation meets ACT data.Phys

    Constantinos Pallis. Kinetically modified Palatini inflation meets ACT data.Phys. Lett. B, 868:139739, 2025

  29. [29]

    C. Pallis. ACT-inspired K ¨ahler-based inflationary attractors.JCAP, 09:061, 2025

  30. [30]

    Nonminimal coupling in light of ACT data.Phys

    Qing Gao, Yungui Gong, Zhu Yi, and Fengge Zhang. Nonminimal coupling in light of ACT data.Phys. Dark Univ., 50:102106, 2025

  31. [31]

    C. Pallis. Updating GUT-Scale Pole Higgs Inflation After ACT. 10 2025

  32. [32]

    Reconciling Higgs Inflation with ACT Observations through Reheating

    Lang Liu, Zhu Yi, and Yungui Gong. Reconciling Higgs Inflation with ACT Observations through Reheating. 5 2025

  33. [33]

    S. D. Odintsov and V . K. Oikonomou. Power-law F(R) gravity as deformations to Starobinsky inflation in view of ACT.Phys. Lett. B, 870:139907, 2025

  34. [34]

    Gialamas, Alexandros Karam, Antonio Racioppi, and Martti Raidal

    Ioannis D. Gialamas, Alexandros Karam, Antonio Racioppi, and Martti Raidal. Has ACT measured radiative corrections to the tree-level Higgs-like inflation?Phys. Rev. D, 112(10):103544, 2025

  35. [35]

    Split supersymmetry and hybrid inflation in light of Atacama Cosmology Telescope DR6 data

    Nobuchika Okada and Qaisar Shafi. Split supersymmetry and hybrid inflation in light of Atacama Cosmology Telescope DR6 data. 7 2025

  36. [36]

    R2-Higgs inflation: R3 contribution and preheating after ACT and SPT data.Phys

    Tanmoy Modak. R2-Higgs inflation: R3 contribution and preheating after ACT and SPT data.Phys. Rev. D, 112(11):115006, 2025

  37. [37]

    John Ellis, Tony Gherghetta, Kunio Kaneta, Wenqi Ke, and Keith A. Olive. Radiative Corrections in Supergravity Models of Inflation. 3 2026

  38. [38]

    C. Pallis. ACT-Consistent B-L Higgs Inflation in Supergravity. 2 2026

  39. [39]

    Fukugita and T

    M. Fukugita and T. Yanagida. Baryogenesis Without Grand Unification.Phys. Lett. B, 174:45–47, 1986

  40. [40]

    George Lazarides and Q. Shafi. Origin of matter in the inflationary cosmology.Phys. Lett. B, 258:305–309, 1991

  41. [41]

    Schaefer, and Q

    George Lazarides, Robert K. Schaefer, and Q. Shafi. Supersymmetric inflation with constraints on superheavy neutrino masses.Phys. Rev. D, 56:1324–1327, 1997

  42. [42]

    Ensembles of multi-objective decision trees

    Dragi Kocev, Celine Vens, Jan Struyf, and Sa ˇso Dˇzeroski. Ensembles of multi-objective decision trees. In Joost N. Kok, Jacek Koronacki, Raomon Lopez de Mantaras, Stan Matwin, Dunja Mladeniˇc, and Andrzej Skowron, editors, Machine Learning: ECML 2007, pages 624–631, Berlin, Heidelberg, 2007. Springer Berlin Heidelberg. 20

  43. [43]

    Allys et al

    E. Allys et al. Probing Cosmic Inflation with the LiteBIRD Cosmic Microwave Background Polarization Survey. PTEP, 2023(4):042F01, 2023

  44. [44]

    Abazajian et al.CMB-S4 Science Book, First Edition

    Kevork N. Abazajian et al.CMB-S4 Science Book, First Edition. 10 2016

  45. [45]

    Non-Minimal B-L Inflation with Observable Gravity Waves.Phys

    Nobuchika Okada, Mansoor Ur Rehman, and Qaisar Shafi. Non-Minimal B-L Inflation with Observable Gravity Waves.Phys. Lett. B, 701:520–525, 2011

  46. [46]

    Mansoor Ur Rehman, Qaisar Shafi, and Joshua R. Wickman. GUT Inflation and Proton Decay after WMAP5.Phys. Rev. D, 78:123516, 2008

  47. [47]

    Analytic formulation of Leptogenesis with neutrino oscillation data employ- ing the general parametrization for neutrino mass matrix

    Nobuchika Okada and Digesh Raut. Analytic formulation of Leptogenesis with neutrino oscillation data employ- ing the general parametrization for neutrino mass matrix. 6 2025

  48. [48]

    Symmetry Breaking Through Bell-Jackiw Anomalies.Phys

    Gerard ’t Hooft. Symmetry Breaking Through Bell-Jackiw Anomalies.Phys. Rev. Lett., 37:8–11, 1976

  49. [49]

    N. S. Manton. Topology in the Weinberg-Salam Theory.Phys. Rev. D, 28:2019, 1983

  50. [50]

    Klinkhamer and N

    Frans R. Klinkhamer and N. S. Manton. A Saddle Point Solution in the Weinberg-Salam Theory.Phys. Rev. D, 30:2212, 1984

  51. [51]

    V . A. Kuzmin, V . A. Rubakov, and M. E. Shaposhnikov. On the Anomalous Electroweak Baryon Number Noncon- servation in the Early Universe.Phys. Lett. B, 155:36, 1985

  52. [52]

    McLerran

    Peter Brockway Arnold and Larry D. McLerran. Sphalerons, Small Fluctuations and Baryon Number Violation in Electroweak Theory.Phys. Rev. D, 36:581, 1987

  53. [53]

    S. Yu. Khlebnikov and M. E. Shaposhnikov. The Statistical Theory of Anomalous Fermion Number Nonconserva- tion.Nucl. Phys. B, 308:885–912, 1988

  54. [54]

    Aghanim et al

    N. Aghanim et al. Planck 2018 results. VI. Cosmological parameters.Astron. Astrophys., 641:A6, 2020. [Erratum: Astron.Astrophys. 652, C4 (2021)]

  55. [55]

    Kolb and Michael S

    Edward W. Kolb and Michael S. Turner.The Early Universe, volume 69. Taylor and Francis, 5 2019

  56. [56]

    Ghigna et al

    T. Ghigna et al. The LiteBIRD mission to explore cosmic inflation. InSPIE Astronomical Telescopes + Instrumentation 2024, 6 2024

  57. [57]

    CMB-S4: Forecasting Constraints on Primordial Gravitational Waves.Astrophys

    Kevork Abazajian et al. CMB-S4: Forecasting Constraints on Primordial Gravitational Waves.Astrophys. J., 926(1):54, 2022

  58. [58]

    The Simons Observatory: Science goals and forecasts.JCAP, 02:056, 2019

    Peter Ade et al. The Simons Observatory: Science goals and forecasts.JCAP, 02:056, 2019

  59. [59]

    David H. Lyth. What would we learn by detecting a gravitational wave signal in the cosmic microwave back- ground anisotropy?Phys. Rev. Lett., 78:1861–1863, 1997

  60. [60]

    Higgs Inflation, Quantum Smearing and the Tensor to Scalar Ratio.Phys

    Mansoor Ur Rehman and Qaisar Shafi. Higgs Inflation, Quantum Smearing and the Tensor to Scalar Ratio.Phys. Rev. D, 81:123525, 2010

  61. [61]

    Quantum Smearing in Hybrid Inflation with Chaotic Potentials.Int

    Waqas Ahmed, Ommair Ishaque, and Mansoor Ur Rehman. Quantum Smearing in Hybrid Inflation with Chaotic Potentials.Int. J. Mod. Phys. D, 25(03):1650035, 2016

  62. [62]

    Quartic inflation and radiative corrections with non-minimal coupling

    Nilay Bostan and Vedat Nefer S ¸eno˘guz. Quartic inflation and radiative corrections with non-minimal coupling. JCAP, 10:028, 2019

  63. [63]

    Tensor to Scalar Ratio in Non-Minimalϕ 4 Inflation

    Nobuchika Okada, Mansoor Ur Rehman, and Qaisar Shafi. Tensor to Scalar Ratio in Non-Minimalϕ 4 Inflation. Phys. Rev. D, 82:043502, 2010

  64. [64]

    The Higgs field as an inflaton.Class

    Fedor Bezrukov. The Higgs field as an inflaton.Class. Quant. Grav., 30:214001, 2013

  65. [65]

    Bezrukov and M

    F. Bezrukov and M. Shaposhnikov. Standard Model Higgs boson mass from inflation: Two loop analysis.JHEP, 07:089, 2009

  66. [66]

    Bezrukov, Amaury Magnin, and Mikhail Shaposhnikov

    Fedor L. Bezrukov, Amaury Magnin, and Mikhail Shaposhnikov. Standard Model Higgs boson mass from infla- tion.Phys. Lett. B, 675:88–92, 2009

  67. [67]

    Meaning of the field dependence of the renor- malization scale in Higgs inflation.Phys

    Yuta Hamada, Hikaru Kawai, Yukari Nakanishi, and Kin-ya Oda. Meaning of the field dependence of the renor- malization scale in Higgs inflation.Phys. Rev. D, 95(10):103524, 2017

  68. [68]

    G. R. Dvali, Q. Shafi, and Robert K. Schaefer. Large scale structure and supersymmetric inflation without fine tuning.Phys. Rev. Lett., 73:1886–1889, 1994

  69. [69]

    Copeland, Andrew R

    Edmund J. Copeland, Andrew R. Liddle, David H. Lyth, Ewan D. Stewart, and David Wands. False vacuum inflation with Einstein gravity.Phys. Rev. D, 49:6410–6433, 1994

  70. [70]

    Linde and Antonio Riotto

    Andrei D. Linde and Antonio Riotto. Hybrid inflation in supergravity.Phys. Rev. D, 56:R1841–R1844, 1997

  71. [71]

    Inflation and supersymmetry breaking.Phys

    Wilfried Buchmuller, Laura Covi, and David Delepine. Inflation and supersymmetry breaking.Phys. Lett. B, 491:183–189, 2000

  72. [72]

    Vedat Nefer Senoguz and Q. Shafi. Reheat temperature in supersymmetric hybrid inflation models.Phys. Rev. D, 71:043514, 2005

  73. [73]

    Mansoor Ur Rehman, Qaisar Shafi, and Joshua R. Wickman. Supersymmetric Hybrid Inflation Redux.Phys. Lett. B, 683:191–195, 2010

  74. [74]

    Mansoor Ur Rehman, Qaisar Shafi, and Joshua R. Wickman. Minimal Supersymmetric Hybrid Inflation, Flipped SU(5) and Proton Decay.Phys. Lett. B, 688:75–81, 2010

  75. [75]

    Hybrid Inflation in the Complex Plane

    Wilfried Buchm ¨uller, Valerie Domcke, Kohei Kamada, and Kai Schmitz. Hybrid Inflation in the Complex Plane. JCAP, 07:054, 2014

  76. [76]

    Bastero-Gil, S

    M. Bastero-Gil, S. F. King, and Q. Shafi. Supersymmetric Hybrid Inflation with Non-Minimal Kahler potential. Phys. Lett. B, 651:345–351, 2007. 21

  77. [77]

    Supersymmetric And Smooth Hybrid Inflation In The Light Of WMAP3.Phys

    Mansoor ur Rehman, Vedat Nefer Senoguz, and Qaisar Shafi. Supersymmetric And Smooth Hybrid Inflation In The Light Of WMAP3.Phys. Rev. D, 75:043522, 2007

  78. [78]

    Qaisar Shafi and Joshua R. Wickman. Observable Gravity Waves From Supersymmetric Hybrid Inflation.Phys. Lett. B, 696:438–446, 2011

  79. [79]

    Mansoor Ur Rehman, Qaisar Shafi, and Joshua R. Wickman. Observable Gravity Waves from Supersymmetric Hybrid Inflation II.Phys. Rev. D, 83:067304, 2011

  80. [80]

    Gravity waves and proton decay in a flipped SU(5) hybrid inflation model.Phys

    Mansoor Ur Rehman, Qaisar Shafi, and Umer Zubair. Gravity waves and proton decay in a flipped SU(5) hybrid inflation model.Phys. Rev. D, 97(12):123522, 2018

Showing first 80 references.