Planck 2018 and Brane Inflation Revisited
We revisit phenomenological as well as string-theoretical aspects of D-brane inflation cosmological models. Phenomenologically these models stand out on par with -attractors, as models with Planck-compatible values of , moving down to the sweet spot in the data with decreasing value of . On the formal side we present a new supersymmetric version of these models in the context of de Sitter supergravity with a nilpotent multiplet and volume modulus stabilization. The geometry of the nilpotent multiplet is evaluated in the framework of string theory.
- 1 Introduction
- 2 Phenomenological D-brane inflation models
- 3 D-brane Dynamics
- 4 D-brane Inflation in String Theory/de Sitter Supergravity
- 5 On stringy origin of the nilpotent geometry
- 6 Brane Inflation with volume stabilization in dS supergravity
- 7 Discussion
- A Other phenomenological models
D-brane inflation models have two aspects, a phenomenological and a string-theoretical. Both became very interesting after the investigation of inflationary models in the Planck 2018 data release Akrami:2018odb (). The Planck 2018 - plane is shown in Fig. 1. The dark (light) blue regions describe the () confidence level for the CMB related data obtained by Planck 2018 and Bicep/Keck2014, additionally including the baryon oscillations (BAO) data. Meanwhile the comparison of predictions of inflationary models with the data in Akrami:2018odb () was based on the CMB related data only, excluding BAO. The corresponding 1 and 2 regions are shown in red in Fig. 1.
The main part of the left hand side of the region in this plane is described by the simplest -attractor model Kallosh:2013yoa (), with the predictions bounded by the two yellow lines corresponding to the -attractor prediction
with the number of e-foldings and . The lower part of the -attractor yellow band covers also the predictions of the Starobinsky model Starobinsky:1980te (), the GL supergravity model Goncharov:1985yu (), and the Higgs inflation model Salopek:1988qh (); Bezrukov:2007ep (). The values of and for -attractor models were shown in Kallosh:2013yoa () and Carrasco:2015pla (), see Fig. 3 here. Special cases with correspond to Starobinsky, Higgs and conformal inflation Kallosh:2013hoa (), corresponds to the GL model Goncharov:1985yu (), correspond to fibre inflation Cicoli:2008gp (); Kallosh:2017wku (). Models with originate from theories with maximal supersymmetry Ferrara:2016fwe (); Kallosh:2017ced ().
As one can see from Akrami:2018odb (), the two yellow lines corresponding to -attractors cover the left hand side of the dark blue (and dark red) areas in Fig. 1. However, the Planck 2018 analysis of inflationary models presented in Table 5 in Akrami:2018odb () reveals yet another class of models, which may match the observations equally well, in a complementary way. It is a class of D-brane inflation models with the potential proportional to , studied in Appendix C of the KKLMMT paper Kachru:2003sx (). Predictions of such models cover the right hand side of the dark blue (and dark red) areas in Fig. 1.
As an example, let us simultaneously plot the predictions of -attractors and of the simplest D-brane inflationary model with in figures representing the Planck 2018 data for on scale, which is more suitable for illustration of the predictions of the models in the limit of small , where both of these classes of models exhibit attractor behavior, see Fig. 2. As one can see from this figure, the combination of the simplest -attractor model and the simplest D-brane inflation model almost completely cover the dark blue (dark purple) area of the Planck 2018 data.
The reason why the predictions of -attractors and of the simplest D-brane inflation match each other in Fig. 2 so perfectly is very simple. According to the investigation in Appendix C of Kachru:2003sx (), the value of in the D-brane inflationary model with in the small (small ) limit is given by
Magically, for -attractors shown by the right yellow line corresponding to in Fig. 2 exactly coincides with for the simplest D-brane inflation models for the left red line with :
Of course, one should remember that exact predictions of these models depend on details of the models, mechanism of reheating, etc., and the position of the region for Planck 2018 depends on the data set (e.g. with or without BAO). Nevertheless the perfect match shown in Fig. 2 is quite striking.
Thus, phenomenologically D-brane inflation model after Planck 2018 has acquired a new significance, even independent of its string theory origin. But we will show here that a new progress can be made with regard to string theory implementation of the phenomenologically attractive versions of D-brane inflation model.
The string theory origin of D-brane inflation model is often attributed to KKLMMT model Kachru:2003sx (), where D3-brane--brane interaction was studied in the context of the volume modulus stabilization. Earlier proposals for D-brane inflation relevant to our current discussion were made in Dvali:2001fw (); Burgess:2001fx (); GarciaBellido:2001ky (). The inflationary potentials corresponding to Dp-brane--brane interaction were proposed in the form
In Martin:2013tda () a detailed cosmological analysis of both potentials was performed, with emphasis on the cases and , i.e. for inverse quartic and quadratic potentials. The first potential in (4) was called BI (Brane Inflation), the second one was called KKLTI (KKLT Inflation).
The earlier proposals in Dvali:2001fw (); Burgess:2001fx (); GarciaBellido:2001ky () were made without addressing the volume stabilization issue. A consistent cosmological evolution of Dp-branes in string theory with the fundamental ten-dimensional geometry can be interpreted as an evolution in the four-dimensional Einstein equations under condition that the six-dimensional internal space has a constant volume, not a runaway behavior which destroys the consistency of the four-dimensional cosmology.
In Kachru:2003sx () D3-brane--brane interaction was studied simultaneously with the volume stabilization. The concrete example in string theory was based on strong warping, which is dual to an almost conformal four-dimensional field theory. Therefore the scalar field describing the motion of the brane was conformally coupled to gravity. This was consistent with the choice of the Kähler potential and the KKLT superpotential in the form
However, it is well known that it is difficult to achieve inflation in the theories with a conformally coupled inflaton. This was one of the the main reasons to consider a generalized KKLT superpotential (5) where the dependence on the distance between branes was included in . A specific explicit model of inflation which followed from (5) was presented in Baumann:2007ah (). The corresponding potential, an inflection point potential, has , which is ruled out by the data, see for example Fig. 1. More about the derivation of this model can be found in a review paper on string cosmology Baumann:2014nda ().
The reason for us to revisit the KKLMMT paper Kachru:2003sx () after Planck 2018 is that, in addition and independently of an example of a particular form of the Kähler potential and superpotential (5), Ref. Kachru:2003sx () provided a basis for other, more general approaches to string cosmology. It can be used at present in a form which is in fact supported by the latest data, using in particular equation (2) for the tilt of the spectrum as derived in Appendix C of Kachru:2003sx (). We will therefore start with phenomenological properties of D-brane inflation models following Kachru:2003sx (); Lorenz:2007ze (); Martin:2013tda (), and then we will discuss a possibility to implement such models in supergravity and string theory.
2 Phenomenological D-brane inflation models
2.1 KKLMMT scenario and inverse quartic and quadratic models
A short preview of the phenomenology of the simplest D-brane inflationary models is given in Figure 2. In this section we will study a broad class of phenomenological models of D-brane inflation in greater detail. As in Encyclopedia Inflationaris Martin:2013tda (), we will call the corresponding potentials either BI (Brane Inflation) for a Coulomb-type interaction, or KKLTI (for KKLT Inflation) when the potential takes a form of the inverse harmonic function. The case of the inverse quadratic Coulomb-type interaction is
whereas the potential in a form of the inverse harmonic function is
At small the ‘exact’ non-singular at potential takes the form of . At very large values of the potential tends to a quadratic one, in the area where ,
In the limit , predictions of this model coincide with the predictions of the simplest chaotic inflation model , which is ruled out. However, as we will see soon, in the case this model provides a good fit to Planck 2018 data, see Fig. 4.
The case of the inverse quartic Coulomb-type interaction is
whereas the potential in a form of the inverse harmonic function is
Here again, at small the ‘exact’ non-singular at potential takes the form of . At very large values of the potential tends to a quartic one, in the area where ,
The -attractor models have
For Dp-brane--brane inflation models with , the general formula for small is
This was also given in Burgess:2001fx () and in Martin:2013tda () in slightly different notation. For example in Martin:2013tda () the formula is in terms of and is given as . Note that for the polynomial potentials
This means that the brane inflation spectral index at small coincides with of inflation in a theory with a polynomial potential with
The quartic brane inflation for D3- model at small has the same Kachru:2003sx () as the one for :
in agreement with with the general equation (13) for .
The quadratic brane inflation model, with D5- potential, at small has the same GarciaBellido:2001ky () as inflation in a theory with a linear potential ,
in agreement with the general equation (13) for .111Note that the models with , such as , , and , can be described by string theory monodromy models Silverstein:2008sg (); McAllister:2008hb (); Dong:2010in (); McAllister:2014mpa (). The corresponding models that we describe give the same values of , for related to by the rules (13), (15), but for smaller range of .
On the left side in Fig. 4 we have an -attractor band which starts at and moves down in a straight line. Next is the inverse quartic brane inflation model which at small is in the position corresponding to , both for BI and KKLTI models, and continues straight. The inverse quadratic brane inflation at small at the right panel in Fig. 4 at small is in a position corresponding to , both for BI and KKLTI models, and continues straight. These three models pretty much cover all admissible area in the plane below .
To understand the reason of similarity between predictions of -attractors and D-brane inflation, we show in Fig. 5 two potentials. One of them is the potential of the -attractor model with with . The second one is of the inverse quartic D-brane inflation type, for . This figure shows that in both cases we have plateau potentials at large fields, and for some choice of parameters (e.g. for and ) one can even make these potentials look even more similar, even though predictions of these models for continue to be slightly different.
The value of for -attractors depends on ,
Meanwhile in brane inflation models the value of depends on . In quartic case, using Kachru:2003sx () for one finds
In particular, for , we find . Using eq. (5.332) of Martin:2013tda (), we find a more general expression for for ,
For an inverse quadratic potential with we find
In particular, for , we find .
It is instructive to compare these results with the ones presented in Fig. 4. One can see that with the decrease of the results for in the BI and KKLTI models converge to each other at the values of approximately corresponding to , just as one could expect by comparing to each other the potentials of these models.
Thus here we have presented our analysis of quartic and quadratic BI and KKLTI models inside region of Planck 2018. As we see, the combination of these models covers the main part of the area in the Planck 2018 data in Fig. 4. This is explained by the similarity of potentials of these models illustrated by Fig. 5. Our results are compatible with the ones found in Martin:2013tda ().
2.2 Inverse linear case with D6- potential
In the previous discussion we concentrated on investigation of inverse quadratic and inverse quartic mode, as in the Planck 2018 analysis in Akrami:2018odb (). Both cases are associated with type IIB string theory, where moduli stabilization was viewed as possible due to KKLT and LVS constructions. However, there was a progress recently with regard to an uplifting role of the brane in Kallosh:2018nrk () and de Sitter vacua in type IIA string theory in Blaback:2018hdo ().
Therefore we would like to add here an example of D6- potential using the general equations above to find out the phenomenology of these models. This is the case of ,
Note that the variable is not a coordinate, but a distance in the moduli space, , which is why the potentials depend on .
At large , the predictions of the model converge to the predictions of the theory with a simple linear potential . However, at small it predicts the same value of as the theory with .
At large and small (for ), the predictions are
For this gives , which is within the Planck area for small .
3 D-brane Dynamics
3.1 String theory analysis
To understand the D-brane dynamics in string theory in application to inflation it is useful to consider the original Polchinski’s computation of the energy between two parallel Dirichlet p-branes at the distance from each other Polchinski:1996na (); Bachas:1998rg (), see Fig. 6. In eq. (90) in Polchinski:1996na () there is an answer for
two D-branes222 An open string theory computation of the related diagram is presented in Kiritsis:1997hj ().. Here we present it both for two D-branes, with the negative contribution from the open string R sector, as well as for one D-brane-anti-D-brane with the positive contribution from the open string R sector
where and all functions are defined in eq. (49) in Polchinski:1996na () and is world sheet modulus. This takes into account that the world-sheet fermions that are periodic around the cylinder correspond to R-R exchange, while the ones which are anti-periodic come from NS-NS exchange.
These three terms for two Dp-branes sum to zero by the ‘abstruse identity,’ since in this case the open string spectrum is supersymmetric. But in case of D-brane-anti-D-brane, when R-sector has a different sign, they sum up since
Thus for two D-branes
In terms of the closed string exchange, this reflects the fact that D-branes are BPS states, the net forces from NS-NS and R-R exchanges canceling. For D-brane-anti-D-brane
We are interested in the limit which is dominated by the lowest lying modes in the closed string spectrum. In such case
Here is a massless propagator in the Euclidean dimension. The corresponding equation is
For example, for D3 case it is and
Thus for two D-branes the net force between Ramond-Ramond repulsion and gravitational plus dilaton attraction cancels. For D-brane-anti-D-brane the force between Ramond-Ramond attraction and gravitational plus dilaton attraction doubles.
At large distances one can use an approximated expression for the cylinder amplitude at (30). At short distances blows up, but it means that our approximation where only low lying string states are taken into account is not valid and the full tower of string states contributes as shown in eq. (28).
From the perspective of string theory computation with the result in (28) it would be confusing to use the concept of the brane-anti-brane annihilation. D-branes and anti-D-branes are not particles with the opposite charge which annihilate and disappear. When the distance between them is small one should not use the approximation which allows to use the harmonic function in eq. (30) and the corresponding potential energy of the brane-anti-brane system. It is the difference between particles and strings which becomes essential at small distances which has to be taken into account in attempts to provide an interpretation of this physical system.
In application to cosmology we will be interested in both potentials in eq. (32). But we will be particularly interested in the region where the difference between these two is not significant.
3.2 On potential in the space-time picture
Now we follow the strategy in KKLMMT paper Kachru:2003sx () where in Sec. 2 and in Appendix B a computation of the D3/ potential in warped geometries is proposed. This is also related to a discussion above were we followed Polchinski:1996na (); Bachas:1998rg () in their computation of the cylinder diagram directly in string theory. It is also useful to follow Lorenz:2007ze () where the same procedure is explained conveniently, not necessarily requiring a warped 5d geometry. The review of inflation in string theory in Baumann:2014nda () is also helpful here. Note that here we assume that we already have a space-time picture. This means that the full string theory computation in (28) is already approximated by the case where limit is taken. But we will see a different way how the harmonic function in the Euclidean space shows up and defines the potential of the D3/ system.
D3-brane is perturbing the background and we calculate the resulting energy of the -brane in this perturbed geometry. This gives the same answer for the potential energy of the brane-anti-brane pair. We start with 10d geometry
In case that the moving D3-brane is at a position at a radial location in the six-dimensional space and the -brane is at a fixed position the corresponding harmonic function in the six-dimensional space is given in KKLMMT as
Here is a characteristic length scale of the geometry, and is the five-form charge. This expression is valid for strongly warped geometries. In Lorenz:2007ze () a general form of a harmonic function is used, namely for a position of the moving brane , which has a canonical kinetic term following from the D-brane action
where are some constants. This choice is more in the spirit of the analysis in the previous section where an inverse harmonic function in a six-dimensional Euclidean space for the D3/ potential is an approximation to the stringy computation of the cylinder diagram in Fig. 6.
The Born-Infeld and Chern-Simons actions of the -brane in the background of a moving D3-brane are given by the following expression:
Therefore, the action representing D3/ interaction for slow velocities leads to the action of the inflaton field
From the D-brane action . Thus
At the potential , at the potential . At the only potential which is left is a KKLT potential corresponding to an uplift of dS vacuum, as defined in (57).
4 D-brane Inflation in String Theory/de Sitter Supergravity
We propose to use a shift symmetric Kähler potential of the form
This kind of shift symmetric Kähler potentials were used in the past for a class of string theory cosmological models in the context of compactification Dasgupta:2002ew (); Hsu:2003cy (); Hsu:2004hi (); Kallosh:2007ig (); Haack:2008yb (). See also review of string cosmology models with unwarped branes in Baumann:2014nda (). It is interesting that the relevant stringy D3/D7 models of inflation, called D-term inflation in its supergravity version, generically has and is now practically ruled out. However, its investigation gave us a useful tool: shift symmetric Kähler potential (41).
4.1 Inflaton shift symmetry and quantum corrections
It is known that at the classical level in string theory/supergravity one can find situations, like a choice of compactification manifold, when the shift symmetry as shown in eq. (41) is possible. It was actually derived in Hsu:2004hi () in case of compactification, using the special Kähler geometry and the corresponding holomorphic section , which, in the special coordinate symplectic frame, is expressed in terms of a prepotential depending on closed string moduli as well as open string moduli, including a position of D3 brane.
However, quantum corrections may break this symmetry to some extent. The corresponding studies were performed in Berg:2004ek (); McAllister:2005mq (), mostly in the context of the stringy version of the D3/D7 brane inflation. The situation there may be summarized as follows with regard to detailed studies in D3/D7 brane inflation Haack:2008yb () in notation of that paper, where , is the torus complex structure, and is the axion-dilaton. With account taken of quantum corrections to gauge coupling of D7 brane, the non-perturbative superpotential dependence on the position of D3 brane was given in the form where quadratic and quartic corrections to
where , and is a function of and , depending on complex structure modulus , given in eq. (F.18) of Haack:2008yb (). Here is some group theoretical factor, represent string theory theta functions. The function was introduced in Berg:2005ja (). In Haack:2008yb () the effect of this dependence of the superpotential on the mobile D3 position was taken into account in the potential. As a result, in addition to a standard supergravity D-term potential, there are quantum corrections of the form of a mass term with a parameter and a quartic term with the parameter . Few examples were studied and plotted in Figs. 4 and 7 in Haack:2008yb (). These examples have shown some region of complex structure modulus where the corrections to as well as to are small. The conclusion was made that with some fine-tuning of the value of , defined by fluxes, it was possible to make quantum corrections to the potential of D3/D7 brane inflation small. But the problem of D3/D7 brane inflation with and without quantum corrections is that none of these models fit the data from Planck 2018.
For D-brane inflation models with compactification, quantum corrections to superpotential have not been studied. If the calculations of quantum corrections associated with gaugino condensation in D3/D7 brane inflation would apply also to D-brane inflation models, one would expect that fine tuning is necessary to make these corrections small. It would be interesting to investigate this issue and describe the situations when such corrections are small, since without quantum corrections D-brane inflation models fit the data from Planck 2018 so well.
In particular, one may study the case where KKLT-type volume stabilization proceeds via a superpotential generated by Euclidean D3-branes Witten:1996bn (), not by gaugino condensation. The nonperturbative effects in absence of a background flux require that the relevant four-cycle satisfies a topological condition derived in Witten:1996bn (). However, it was shown in Gorlich:2004qm (); Bergshoeff:2005yp () that these topological conditions are changed in the presence of flux. In this case the one-loop correction comes from an instanton fluctuation determinant, which has not been computed in the context of the cosmological models that we study here. It would be important to find out whether such computation can be performed and what it would entail.
4.2 A nilpotent multiplet in -attractors
An additional tool we use here is a nilpotent multiplet , representing an uplifting -brane, Ferrara:2014kva (); Kallosh:2014wsa (); Bergshoeff:2015jxa (); Kallosh:2015nia (). de Sitter supergravity Bergshoeff:2015tra (); Hasegawa:2015bza () is a local version of non-linearly realized global Volkov-Akulov supersymmetry Volkov:1972jx (). Using the nilpotent multiplet we will build de Sitter supergravity for the brane inflation models compatible with the data. An important ingredient of cosmological models in dS supergravity is the Kähler metric of the nilpotent superfield , which depends on other moduli
It has been observed in the past McDonough:2016der (); Kallosh:2017wnt () that the Kähler metric of the nilpotent superfield might carry the information about the inflationary potential. For example, it was shown in Kallosh:2017wnt () that the simplest -attractor model with the potential
can be presented by a particular dS supergravity with the following nilpotent superfield geometry
where . Here is a disk variable of the hyperbolic geometry, and the cosmological constant at the exit from inflation is given by the difference between two constants, .
In case of Dp-brane inflationary models we will show below that the dependence of the nilpotent field geometry on the inflaton superfield has an interesting explanation. It comes in the context of the KKLMMT construction combined with the recent investigation in Kallosh:2018nrk () of the dictionary between string theory models with local sources in ten dimensions and the four-dimensional de Sitter supergravity.
5 On stringy origin of the nilpotent geometry
Recently the dictionary between string theory models and and for dS supergravities with closed string moduli was established in Kallosh:2018nrk (). In case of open string moduli the analogous analysis was not performed yet. Here we will consider a very particular situation, known from cosmology, where it is possible to identify the relevant geometry of the nilpotent multiplet from the first principles of string theory with D-branes.
Consider modifications of and due to the presence of the nilpotent multiplet,
Here the superpotential has a simple dependence on as in (47). When are closed string moduli we have shown in Kallosh:2018nrk () why is computable: for each set of ingredients in 10d of the so-called ‘full-fledged string theory models’ one can compute in 4d as a function of the overall volume, the dilaton and the volume moduli of the supersymmetric cycles on which the -branes are wrapped.
Since the nilpotent multiplet does not have a scalar component, the new potential has an additional term, but it still depends on the same closed string moduli. The new F-term potential acquires an additional nowhere vanishing positive term, associated with Volkov-Akulov non-linearly realized supersymmetry
is the standard supergravity potential without the nilpotent multiplet (without the brane in string theory). It is important to stress here that there is a dictionary between string theory models in ten dimensions described by supergravity with fluxes and local sources, Dp-branes and Op-planes. Upon compactification on calibrated manifolds these string theory models lead to specific choices of and in four-dimensional supergravity, see Kallosh:2018nrk () and references therein.
The reason why the nilpotent field metric, is computable in string theory is that on one hand, the corrected potential due to presence of -brane has a simple dependence on moduli, under condition that , as shown in eqs. (47), (49). Thus, the extra potential has a simple dependence on geometry of the nilpotent superfield
On the other hand, the addition to potential due to -brane action can be inferred from the knowledge of the bosonic -brane action. By comparing these two we have identified in Kallosh:2018nrk () the values of as functions of closed string moduli,
Here the corresponding action for the brane wrapped on a supersymmetric cycle is given by the following expression, and it depends on various closed string moduli, including the volume of the supersymmetric cycles,
More details about this action can be found in Kallosh:2018nrk (). This leaves us with the dictionary between the nilpotent field geometry in presence of a pseudo-calibrated -brane and string theory models with closed string moduli,
Here we study a particular case of the computation of , where is an open string moduli. The new relation between the energy and geometry is an analog of eq. (51)
Thus if we know the dependence of the potential on moduli which is added to the standard supergravity action via a nilpotent field, we can find the geometry using eq. (55). The corresponding geometry of the nilpotent superfield is determined by the total potential
5.1 KKLT uplift
A manifestly supersymmetric version of the KKLT uplifting was proposed in the form in which the -brane is represented by a nilpotent multiplet with , corresponding to Volkov-Akulov non-linearly realized supersymmetry Ferrara:2014kva (); Kallosh:2014wsa (); Bergshoeff:2015jxa (); Kallosh:2015nia (). In this case the new and are given by (in unwarped case)
This is in agreement with using only closed string moduli and action. At present there is a consensus that eqs. (57) and (58) represent a manifestly supersymmetric version of the KKLT uplift. It involves a nilpotent multiplet representing an brane in the framework of de Sitter supergravity with a non-linearly realized supersymmetry.
5.2 Inflationary uplift
Here we consider the situation where at the end of inflation the uplifting energy is due to an brane which is at some fixed point in the manifold Kachru:2003sx (); Kachru:2003aw (), for example on a top of an O3-plane, as discussed more recently in Kallosh:2015nia ().
Our new proposal here is to look for a combination of potentials due to KKLT uplift to dS vacua, and an additional uplift by the inflationary energy depending on open string modulus. In case of D3-brane inflation, the new term depends on the energy of D3/ interaction. Our proposal means that the corresponding geometry of the nilpotent superfield will be defined by the total potential
In addition to we have now added the energy of the system depending on open string modulus. In such case, it follows from (56) that
This is our definition of the inflationary uplift in the case of D3/ inflation. We will demonstrate below that it is very useful for inflationary model building.
6 Brane Inflation with volume stabilization in dS supergravity
6.1 D-brane inflaton potentials
It could also be a potential of the form
where the terms with have to be added to remove the singularity at . We will see below that the cosmological evolution with strong volume modulus stabilization as proposed in Kallosh:2011qk (); Linde:2011ja (); Dudas:2012wi () works well for the inflationary models we study below. Namely we can use either KKLT type volume stabilization assuming that to avoid volume destabilization during inflation Kallosh:2004yh (), or using the KL mechanism with two exponents Kallosh:2004yh (); BlancoPillado:2005fn (); Kallosh:2014oja (). In both cases the process of inflation does not affect the volume modulus stabilization and vice versa, inflation is not affected by the volume modulus stabilization. One should note that the geometric approach used in our paper may impose certain constraints on the gravitino mass, which should be taken into account in the model building Hasegawa:2017nks ().
6.2 Unifying inflation and strong volume stabilization
We consider a general theory of volume stabilization in combination of the inflationary potential and discuss the back-reaction of the inflaton potential on the moduli. We use the following set of Kähler and superpotential
where is a volume modulus multiplet, is an inflaton multiplet, is an nilpotent multiplet, respectively. depends on where the is, and in the warped case, , in the unwarped case, . The Kähler coupling gives rise to inflaton potential, see (60). The scalar potential is given by
In all models to be considered, inflation occurs along a stable inflationary trajectory . We will also consider . In that case, the general expression for the potential of the inflaton field and of the volume modulus is given by
In what follows, we will consider two models where the potential ensures strong stabilization of the volume modulus near its post-inflationary value , such that during inflation one has . Also, one can ensure that the post-inflationary vacuum energy is many orders of magnitude smaller than the inflaton potential. In that case, the potential during inflation can be represented by a very simple expression
This expression shows that one can easily combine strong moduli stabilization with construction of inflationary models with arbitrary potentials (67). Similar, but slightly more complicated methods were used in the past in the phenomenological inflationary models without nilpotent superfield Kallosh:2011qk (); Linde:2011ja (); Dudas:2012wi ().
6.3 D-brane inflation and strongly stabilized KKLT model
We consider the KKLT moduli stabilization with inflationary potential and discuss the back-reaction of the inflaton potential on the moduli. We use the following set of Kähler and superpotential 333We do not assume that in the superpotential has a significant dependence on . :
where being a volume modulus multiplet, being an inflaton multiplet, being an nilpotent multiplet, respectively. depends on where the is, and in the warped case, , in the unwarped case, . The Kähler coupling gives rise to inflaton potential, see (67).
Let us first consider the simplest case and . In this case, the scalar potential is simply given by
where we have minimized with respect to and is the value at which is satisfied. We denote the minimum of this potential as , which satisfies
We assume that at the minimum of . From (almost) vanishing cosmological constant condition, we find
For simplicity, let us choose , and one finds
Tuning on the inflaton dependence , the potential minimum of is no longer . Let us call the deviation from as . We expand the potential with respect to and minimize it, which gives the following effective potential,