12 results on '"Sjoerd Hardeman"'
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2. Organization level research in scientometrics: a plea for an explicit pragmatic approach.
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Sjoerd Hardeman
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- 2013
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3. Spatial scientometrics: Towards a cumulative research program.
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Koen Frenken, Sjoerd Hardeman, and Jarno Hoekman
- Published
- 2009
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4. Research excellence indicators: time to reimagine the ‘making of’?
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Sjoerd Hardeman, Daniel Vertesy, Ângela Guimarães Pereira, and Federico Ferretti
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Public Administration ,media_common.quotation_subject ,05 social sciences ,Geography, Planning and Development ,Management, Monitoring, Policy and Law ,050905 science studies ,Making-of ,Excellence ,0502 economics and business ,Engineering ethics ,Sociology ,0509 other social sciences ,050203 business & management ,media_common - Published
- 2018
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5. Quark matter influence on observational properties of compact stars
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Sjoerd Hardeman
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Physics ,Nuclear and High Energy Physics ,Particle physics ,Astrophysics (astro-ph) ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,Down quark ,Compact star ,Astrophysics ,High Energy Physics - Phenomenology ,Strange matter ,High Energy Physics - Phenomenology (hep-ph) ,Quark star ,Quark–gluon plasma ,Up quark ,Exotic star ,Color superconductivity - Abstract
Densities in compact stars may be such that quarks are no longer confined in hadrons, but instead behave as weakly interacting particles. In this regime perturbative calculations are possible. Yet, due to high pressures and an attractive channel in the strong force, condensation of quarks in a superfluid state is likely. This can have interesting consequences for magnetic fields, especially in relation to the discovery of slow-period free precession in a compact star. In this proceedings there will be a discussion of the mass-radius relations of compact stars made from quark matter and magnetic field behaviour in compact stars with a quark matter core., 4 pages, 2 images. To be published in the proceedings of SEWM 2008, Nucl. Phys. A, in print
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- 2009
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6. Effective theories of single field inflation when heavy fields matter
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Gonzalo A. Palma, Jinn Ouk Gong, Ana Achúcarro, Sjoerd Hardeman, Subodh P. Patil, Laboratoire de Physique Théorique de l'ENS [École Normale Supérieure] (LPTENS), Fédération de recherche du Département de physique de l'Ecole Normale Supérieure - ENS Paris (FRDPENS), École normale supérieure - Paris (ENS-PSL), Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)-École normale supérieure - Paris (ENS-PSL), Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)-Université Pierre et Marie Curie - Paris 6 (UPMC)-Centre National de la Recherche Scientifique (CNRS), Centre de Physique Théorique [Palaiseau] (CPHT), École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique Théorique de l'ENS (LPTENS), Université Pierre et Marie Curie - Paris 6 (UPMC)-Fédération de recherche du Département de physique de l'Ecole Normale Supérieure - ENS Paris (FRDPENS), École normale supérieure - Paris (ENS Paris), Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)-École normale supérieure - Paris (ENS Paris), Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)-Centre National de la Recherche Scientifique (CNRS), and Centre National de la Recherche Scientifique (CNRS)-École polytechnique (X)
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High Energy Physics - Theory ,Nuclear and High Energy Physics ,Cosmology and Nongalactic Astrophysics (astro-ph.CO) ,Spontaneous symmetry breaking ,FOS: Physical sciences ,General Relativity and Quantum Cosmology (gr-qc) ,Astrophysics::Cosmology and Extragalactic Astrophysics ,01 natural sciences ,General Relativity and Quantum Cosmology ,Theoretical physics ,High Energy Physics - Phenomenology (hep-ph) ,Operator (computer programming) ,0103 physical sciences ,Effective field theory ,010306 general physics ,Adiabatic process ,Gauge symmetry ,Physics ,[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th] ,010308 nuclear & particles physics ,Inflaton ,High Energy Physics - Phenomenology ,High Energy Physics - Theory (hep-th) ,[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph] ,Goldstone boson ,[PHYS.GRQC]Physics [physics]/General Relativity and Quantum Cosmology [gr-qc] ,Bispectrum ,Particle Physics - Theory ,Astrophysics - Cosmology and Nongalactic Astrophysics - Abstract
We compute the low energy effective field theory (EFT) expansion for single-field inflationary models that descend from a parent theory containing multiple other scalar fields. By assuming that all other degrees of freedom in the parent theory are sufficiently massive relative to the inflaton, it is possible to derive an EFT valid to arbitrary order in perturbations, provided certain generalized adiabaticity conditions are respected. These conditions permit a consistent low energy EFT description even when the inflaton deviates off its adiabatic minimum along its slowly rolling trajectory. By generalizing the formalism that identifies the adiabatic mode with the Goldstone boson of this spontaneously broken time translational symmetry prior to the integration of the heavy fields, we show that this invariance of the parent theory dictates the entire non-perturbative structure of the descendent EFT. The couplings of this theory can be written entirely in terms of the reduced speed of sound of adiabatic perturbations. The resulting operator expansion is distinguishable from that of other scenarios, such as standard single inflation or DBI inflation. In particular, we re-derive how certain operators can become transiently strongly coupled along the inflaton trajectory, consistent with slow-roll and the validity of the EFT expansion, imprinting features in the primordial power spectrum, and we deduce the relevant cubic operators that imply distinct signatures in the primordial bispectrum which may soon be constrained by observations., (v1) 25 pages, 1 figure; (v2) references added and typos corrected, to appear in Journal of High Energy Physics
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- 2012
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7. Mass hierarchies and non-decoupling in multi-scalar field dynamics
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Sjoerd Hardeman, Subodh P. Patil, Jinn Ouk Gong, Gonzalo A. Palma, Ana Achúcarro, Laboratoire de Physique Théorique de l'ENS (LPTENS), Université Pierre et Marie Curie - Paris 6 (UPMC)-Fédération de recherche du Département de physique de l'Ecole Normale Supérieure - ENS Paris (FRDPENS), École normale supérieure - Paris (ENS Paris), Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)-École normale supérieure - Paris (ENS Paris), Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)-Centre National de la Recherche Scientifique (CNRS), Centre de Physique Théorique [Palaiseau] (CPHT), Centre National de la Recherche Scientifique (CNRS)-École polytechnique (X), Laboratoire de Physique Théorique de l'ENS [École Normale Supérieure] (LPTENS), Fédération de recherche du Département de physique de l'Ecole Normale Supérieure - ENS Paris (FRDPENS), École normale supérieure - Paris (ENS-PSL), Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)-École normale supérieure - Paris (ENS-PSL), Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)-Université Pierre et Marie Curie - Paris 6 (UPMC)-Centre National de la Recherche Scientifique (CNRS), and École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS)
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High Energy Physics - Theory ,Nuclear and High Energy Physics ,Cosmology and Nongalactic Astrophysics (astro-ph.CO) ,Geodesic ,Sigma model ,FOS: Physical sciences ,General Relativity and Quantum Cosmology (gr-qc) ,Curvature ,01 natural sciences ,General Relativity and Quantum Cosmology ,[PHYS.ASTR.CO]Physics [physics]/Astrophysics [astro-ph]/Cosmology and Extra-Galactic Astrophysics [astro-ph.CO] ,High Energy Physics - Phenomenology (hep-ph) ,0103 physical sciences ,Effective field theory ,010306 general physics ,Vacuum manifold ,Physics ,Quantum field theory in curved spacetime ,010308 nuclear & particles physics ,[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th] ,Potential energy ,High Energy Physics - Phenomenology ,Classical mechanics ,High Energy Physics - Theory (hep-th) ,[PHYS.GRQC]Physics [physics]/General Relativity and Quantum Cosmology [gr-qc] ,Scalar field ,Particle Physics - Theory ,Astrophysics - Cosmology and Nongalactic Astrophysics - Abstract
In this work we study the effects of field space curvature on scalar field perturbations around an arbitrary background field trajectory evolving in time. Non-trivial imprints of the 'heavy' directions on the low energy dynamics arise when the vacuum manifold of the potential does not coincide with the span of geodesics defined by the sigma model metric of the full theory. When the kinetic energy is small compared to the potential energy, the field traverses a curve close to the vacuum manifold of the potential. The curvature of the path followed by the fields can still have a profound influence on the perturbations as modes parallel to the trajectory mix with those normal to it if the trajectory turns sharply enough. We analyze the dynamical mixing between these non-decoupled degrees of freedom and deduce its non-trivial contribution to the low energy effective theory for the light modes. We also discuss the consequences of this mixing for various scenarios where multiple scalar fields play a vital role, such as inflation and low-energy compactifications of string theory., Comment: 16 pages, 2 figures, typeset in PRD style. v2: Minor changes throughout to emphasize that the analysis also applies to sharp and/or prolonged turns. References added
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- 2010
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8. Consistent Decoupling of Heavy Scalars and Moduli in N=1 Supergravity
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Kepa Sousa, Ana Achúcarro, and Sjoerd Hardeman
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Physics ,High Energy Physics - Theory ,Nuclear and High Energy Physics ,Particle physics ,Compactification (physics) ,Supergravity ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,Supersymmetry ,Expectation value ,General Relativity and Quantum Cosmology (gr-qc) ,General Relativity and Quantum Cosmology ,Moduli ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,High Energy Physics - Theory (hep-th) ,De Sitter universe ,Effective action ,Mathematical physics ,Ansatz - Abstract
We consider the conditions for integrating out heavy chiral fields and moduli in N=1 supergravity, subject to two explicit requirements. First, the expectation values of the heavy fields should be unaffected by low energy phenomena. Second, the low energy effective action should be described by N=1 supergravity. This leads to a working definition of decoupling in N=1 supergravity that is different from the usual condition of gravitational strength couplings between sectors, and that is the relevant one for inflation with moduli stabilization, where some light fields (the inflaton) can have long excursions in field space. It is also important for finding de Sitter vacua in flux compactifications and KKLT scenarios, since failure of the decoupling condition invalidates the implicit assumption that the stabilization and uplifting potentials have a low energy supergravity description. We derive a sufficient condition for supersymmetric decoupling, namely, that the Kahler invariant function G = K + log |W|^2 is of the form G = L(light, (heavy)) with H and L arbitrary functions, which includes the particular case G = L(light) + H(heavy). The consistency condition does not hold in general for the ansatz K = K(light) + K(heavy), W = W(light) + W(heavy) and we discuss under what circumstances it does hold., Comment: 5 pages, LaTeX. Discussion clarified, PRD-version
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- 2008
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9. Decoupling limits in multi-sector supergravities
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Johannes M. Oberreuter, Ana Achúcarro, Sjoerd Hardeman, Ted van der Aalst, and Koenraad Schalm
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High Energy Physics - Theory ,Physics ,Cosmology and Nongalactic Astrophysics (astro-ph.CO) ,Supergravity ,High Energy Physics::Phenomenology ,Superpotential ,FOS: Physical sciences ,Astronomy and Astrophysics ,Expectation value ,Supersymmetry ,Decoupling (cosmology) ,Cosmology ,High Energy Physics - Phenomenology ,High Energy Physics::Theory ,General Relativity and Quantum Cosmology ,Theoretical physics ,High Energy Physics - Phenomenology (hep-ph) ,High Energy Physics - Theory (hep-th) ,Quantum field theory ,Scaling ,Astrophysics - Cosmology and Nongalactic Astrophysics - Abstract
Conventional approaches to cosmology in supergravity assume the existence of multiple sectors that only communicate gravitationally. In principle these sectors decouple in the limit Planck mass to infinity. In practice such a limit is delicate: for generic supergravities, where sectors are combined by adding their Kahler functions, the separate superpotentials must contain non-vanishing vacuum expectation values supplementing the naive global superpotential. We show that this requires non-canonical scaling in the naive supergravity superpotential couplings to recover independent sectors of globally supersymmetric field theory in the decoupling limit Planck Mass to infinity., 10 pages; v2, published version, refined wording and clarifying comments throughout, references added
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- 2013
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10. Features of heavy physics in the CMB power spectrum
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Jinn Ouk Gong, Sjoerd Hardeman, Subodh P. Patil, Ana Achúcarro, Gonzalo A. Palma, Laboratoire de Physique Théorique de l'ENS (LPTENS), Université Pierre et Marie Curie - Paris 6 (UPMC)-Fédération de recherche du Département de physique de l'Ecole Normale Supérieure - ENS Paris (FRDPENS), École normale supérieure - Paris (ENS Paris), Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)-École normale supérieure - Paris (ENS Paris), Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)-Centre National de la Recherche Scientifique (CNRS), Centre de Physique Théorique [Palaiseau] (CPHT), Centre National de la Recherche Scientifique (CNRS)-École polytechnique (X), Laboratoire de Physique Théorique de l'ENS [École Normale Supérieure] (LPTENS), Fédération de recherche du Département de physique de l'Ecole Normale Supérieure - ENS Paris (FRDPENS), École normale supérieure - Paris (ENS-PSL), Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)-École normale supérieure - Paris (ENS-PSL), Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)-Université Pierre et Marie Curie - Paris 6 (UPMC)-Centre National de la Recherche Scientifique (CNRS), and École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS)
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High Energy Physics - Theory ,Cosmology and Nongalactic Astrophysics (astro-ph.CO) ,Cosmic microwave background ,FOS: Physical sciences ,General Relativity and Quantum Cosmology (gr-qc) ,Astrophysics::Cosmology and Extragalactic Astrophysics ,01 natural sciences ,General Relativity and Quantum Cosmology ,High Energy Physics - Phenomenology (hep-ph) ,Non-Gaussianity ,0103 physical sciences ,Effective field theory ,010306 general physics ,Adiabatic process ,Inflation (cosmology) ,Physics ,Slow roll ,[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th] ,010308 nuclear & particles physics ,Spectral density ,Astronomy and Astrophysics ,Inflaton ,High Energy Physics - Phenomenology ,Classical mechanics ,High Energy Physics - Theory (hep-th) ,[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph] ,[PHYS.GRQC]Physics [physics]/General Relativity and Quantum Cosmology [gr-qc] ,Astrophysics - Cosmology and Nongalactic Astrophysics - Abstract
The computation of the primordial power spectrum in multi-field inflation models requires us to correctly account for all relevant interactions between adiabatic and non-adiabatic modes around and after horizon crossing. One specific complication arises from derivative interactions induced by the curvilinear trajectory of the inflaton in a multi-dimensional field space. In this work we compute the power spectrum in general multi-field models and show that certain inflaton trajectories may lead to observationally significant imprints of `heavy' physics in the primordial power spectrum if the inflaton trajectory turns, that is, traverses a bend, sufficiently fast (without interrupting slow roll), even in cases where the normal modes have masses approaching the cutoff of our theory. We emphasise that turning is defined with respect to the geodesics of the sigma model metric, irrespective of whether this is canonical or non-trivial. The imprints generically take the form of damped superimposed oscillations on the power spectrum. In the particular case of two-field models, if one of the fields is sufficiently massive compared to the scale of inflation, we are able to compute an effective low energy theory for the adiabatic mode encapsulating certain relevant operators of the full multi-field dynamics. As expected, a particular characteristic of this effective theory is a modified speed of sound for the adiabatic mode which is a functional of the background inflaton trajectory and the turns traversed during inflation. Hence in addition, we expect non-Gaussian signatures directly related to the features imprinted in the power spectrum., Comment: 41 pages, 6 figures, references updated, minor modifications. Version to appear in JCAP. v4: Equations (4.28) and (4.30) and Figures 5 and 6 corrected
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- 2011
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11. F-term uplifting and the supersymmetric integration of heavy moduli
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Sjoerd Hardeman, Kepa Sousa, and Ana Achúcarro
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High Energy Physics - Theory ,Inflation (cosmology) ,Physics ,Nuclear and High Energy Physics ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,Scalar potential ,Cosmological constant ,Physics::Geophysics ,Moduli ,Maxima and minima ,symbols.namesake ,Theoretical physics ,High Energy Physics - Theory (hep-th) ,Saddle point ,symbols ,F-term ,Hubble's law - Abstract
We study in detail the stability properties of the simplest F-term uplifting mechanism consistent with the integration of heavy moduli. This way of uplifting vacua guarantees that the interaction of the uplifting sector with the moduli sector is consistent with integrating out the heavy fields in a supersymmetric way. The interactions between light and heavy fields are characterized in terms of the Kahler invariant function, G = K + log |W|^2, which is required to be separable in the two sectors. We generalize earlier results that when the heavy fields are stabilized at a minimum of the Kahler function G before the uplifting (corresponding to stable AdS maxima of the potential), they remain in a perturbatively stable configuration for arbitrarily high values of the cosmological constant (or the Hubble parameter during inflation). By contrast, supersymmetric minima and saddle points of the scalar potential are always destabilized for sufficiently large amount of uplifting. We prove that these results remain unchanged after including gauge couplings in the model. We also show that in more general scenarios, where the Kahler function is not separable in the light and heavy sectors, the minima of the Kahler function still have better stability properties at large uplifting than other types of critical points., Comment: 25 pages, 1 figure, corrects typo in JHEP-version
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- 2008
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12. The everpresent η-problem: knowledge of all hidden sectors required
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Koenraad Schalm, Sjoerd Hardeman, Ted van der Aalst, Gonzalo A. Palma, Johannes M. Oberreuter, and String Theory (ITFA, IoP, FNWI)
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Inflation (cosmology) ,Physics ,High Energy Physics - Theory ,Nuclear and High Energy Physics ,Cosmology and Nongalactic Astrophysics (astro-ph.CO) ,Supergravity ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,Supersymmetry ,General Relativity and Quantum Cosmology (gr-qc) ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Inflaton ,Supersymmetry breaking ,General Relativity and Quantum Cosmology ,Standard Model ,Hidden sector ,Theoretical physics ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,High Energy Physics - Theory (hep-th) ,Mixing (physics) ,Astrophysics - Cosmology and Nongalactic Astrophysics - Abstract
We argue that the eta-problem in supergravity inflation cannot be solved without knowledge of the ground state of hidden sectors that are gravitationally coupled to the inflaton. If the hidden sector breaks supersymmetry independently, its fields cannot be stabilized during cosmological evolution of the inflaton. We show that both the subsequent dynamical mixing between sectors as well as the lightest mass of the hidden sector are set by the scale of supersymmetry breaking in the hidden sector. The true cosmological eta-parameter arises from a linear combination of the lightest mode of the hidden sector with the inflaton. Generically, either the true eta deviates considerably from the na\"ive eta implied by the inflaton sector alone, or one has to consider a multifield model. Only if the lightest mass in the hidden sector is much larger than the inflaton mass and if the inflaton mass is much larger than the scale of hidden sector supersymmetry breaking, is the effect of the hidden sector on the slow-roll dynamics of the inflaton negligible., Comment: 27 pages, 6 figures; v2, published version, minor adjustments to the introduction, minor corrections to section 2.2 for improved clarity, references added
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