CC BY
0lopscience
¡opscience.iop.org
Home Search Collections Journals About Contact us My IOPscience
Long-lived light mediator to dark matter and primordial small scale spectrum
This content has been downloaded from IOPscience. Please scroll down to see the full text. View the table of contents for this issue, or go to the journal homepage for more
Download details: IP Address: 195.34.78.149
This content was downloaded on 28/06/2016 at 11:49
Please note that terms and conditions apply.
/ournal of Cosmology and Astroparticle Physics
An IOP and SISSA journal
Long-lived light mediator to dark matter and primordial small scale j
spectrum A
Yue Zhang U1
Walter Burke Institute for Theoretical Physics,
California Institute of Technology, Pasadena, CA 91125, U.S.A.
E-mail: yuezhang@theory.caltech.edu
j Article funded by SCOAP3. Content from this work may be used
Received March 11, 2015 Accepted April 15, 2015 Published May 6, 2015
Abstract. We calculate the early universe evolution of perturbations in the dark matter energy density in the context of simple dark sector models containing a GeV scale light mediator. We consider the case that the mediator is long-lived, with lifetime up to a second, and before decaying it temporarily dominates the energy density of the universe. We show that for primordial perturbations that enter the horizon around this period, the interplay between linear growth during matter domination and collisional damping can generically lead to a sharp peak in the spectrum of dark matter density perturbation. As a result, the population of the smallest DM halos gets enhanced. Possible implications of this scenario are discussed.
Keywords: power spectrum, dark matter theory, particle physics - cosmology connection, cosmological perturbation theory
ArXiv ePrint: 1502.06983
A f .v, rdVhe termlof the Creative Commons Attribution 3.0 License. doi:10.1088/1475-7516/2015/05/008
Any further distribution of this work must maintain attribution to the author(s) and the title of the work, journal citation and DOI.
Contents
1 Introduction 1
2 Simple dark sector models with a light mediator 2
3 Light mediator dominance and perturbations 5
4 Possible testable implications 9
5 Outlook 10
1 Introduction
An important question for the field of particle cosmology is to reveal the nature of dark f
matter (DM). There has been compelling evidence for the existence of DM, most of which are from gravitational effects. There are also various ongoing experiments aiming to discover the DM through possible interactions other than gravity. On the theory side, there are well- ^—^ motivated frameworks like supersymmetry that can accommodate DM candidates as weakly interacting particles. An alternative approach to the theory of DM is using minimality ——^ as guiding principle. The focus of this work is a class of simple models in which the DM candidate talks to the Standard Model (SM) sector through the exchange of a light mediator. This setup has been proposed and explored for several different motivations [1-7]. With a
light mediator it is possible to suppress the direct detection constraints on DM, but still have „___
prospects for other indirect searches. The simple interaction between the light mediator and DM can offer rich dynamics in the dark sector [8-11].
In this note, we investigate the light mediator phenomenology and cosmology in the C context of two simple models, where the mediator is either a vector or scalar boson. Its interaction with the SM sector is via photon kinetic mixing in the vector mediator case, and the Higgs portal in the scalar case. We are interested in the mass range of the mediator at GeV scale, and lifetime as long as a second. This is often a less studied region of parameter space because the portal interaction is so weak that no current experiment is sensitive to it. The aim of this work is to fill this gap by studying the consequences of the mediator's longevity and possible testable implications. We note that the mediator is long-lived because of the tiny portal coupling between the dark and SM sectors — this also implies that the two sectors never reach equilibrium, but evolve with their own temperatures. There could be an interesting impact on the cosmology, if the light mediator becomes non-relativistic and temporarily dominates the energy density of the universe before it decays and releases entropy. We calculate the evolution of density perturbations of DM during the mediator dominance and the imprint of this period on the primordial power spectrum. Because the mediator has become matter-like when it begins to dominate the universe, the DM density perturbation could grow linearly. A competing effect is the collisional damping from the DM-mediator scattering. We find that for perturbations entering the horizon during the mediator domination era, the linear growth effect wins over damping. We show a generic prediction of such long-lived mediator model is a sharp peak in the transfer function right before the exponential cutoff. This corresponds to a characteristic length scale of order 10-4 pc, that is,
Collisional damping
Linear growth
Log growth
O o Oil
S "E. Mediator (f> ^ g domination Q -o
<p decay (~lsec)
Figure 1. History of dark sector and perturbation growth.
size of the minimal DM halos. The peak implies these mini halos are to be more populated than in the usual cold DM case.
In the next section, we study the simplest dark sector models with a light vector/scalar mediator. We summarize the current experimental constraints on the light mediator mass and its portal coupling to SM. The allowed region where the mediator can be long-lived and dominate the universe is highlighted. In section III, we do the calculation on the evolution of density perturbations in the early universe, paying attention to the modes entering horizon around the light mediator dominated era. We obtain the relative transfer function by comparing our results with those of the usual cold DM. In section IV, we estimate the characteristic mass and size of the minimal DM halos and discuss possible testable predictions.
2 Simple dark sector models with a light mediator
To set the stage, we sketch in figure 1 the major events happening to the dark sector and their time scales relevant for this study.
Vector mediator case. The first dark sector model we examine contains a massive vector mediator V^,
£ = £sm+ - igxVfj,)x ~ in\\ \ ~+ m2vV^ - . (2.1)
The DM field % is a Dirac fermion and V^ couples to the DM vector current. Both are SM gauge singlets. A kinetic mixing (the k term) between V and the usual photon is introduced.
In the early universe, the DM x and the mediator V^ are in thermal equilibrium through the gauge interaction gx. We focus on the case of light mediator, mx 2> my. In this case, the DM freeze out is controlled by the annihilation xx ~~^ VV. To give the correct relic density to symmetric DM, the thermal annihilation cross section should satisfy
vroi 3 x 10-26cm3/s , ,
Manni = —^ = -C- ' 2"2
where S is the DM number density dilution factor due to any entropy production after the freeze out. For asymmetric DM, the relic density is given the primordial asymmetry in x and x number, and the annihilation cross section has to be larger than the thermal value.
After the DM freeze out, the light mediator V^ takes over all the entropy in the dark sector. We assume the dark sector has its own temperature T', and define its ratio to the
(C) mx=2GeV
(D) mx=2GeV
E137 LSND^H SN1987a --^
BBN exclusion ^VM
my (GeV)
K* ->7r+ +invisible
^-dominance ; /
BBN exclusion
0.001 0.003
0.03 m* (GeV)
Figure 2. Experimental constraints on dark sector models with light mediator, shown in the parameter space of photon/Higgs portal versus mediator mass. We want to highlight the red region where the mediator could dominate the universe before it decays.
visible photon temperature, £ = T;/T7, at very high temperature. After DM annihilation, the comoving V^ number is
nv (Ty)
13Z (3)£3 g*s(Tcd)rr 3
' T 3 g*s(mt) 7
where g*s(T) counts the relativistic SM degree of freedom contributing to entropy density. For this assumption to be valid, the interactions between and the SM particles must be decoupled throughout the history of universe. Because the (kinetic) mixing k is the only portal that communicate the two sectors, it is sufficient to require that the inverse decay rate ff — is less than the Hubble parameter at temperature of universe equal to my We find for m^ < 10 GeV it requires k < 10-7. As shown below, this is well satisfied if the light mediator is long-lived enough to dominate the universe.
There are further phenomenological constraints on k and my. In order to be consistent with standard big-bang nucleosynthesis, a commonly used requirement is to make decay before 1 second or so. This gives a lower bound on k.2 We use the numerical result on the
1Although the other scattering processes such as qq ^ Vg may have larger rates at T > mv because r ~ T, the relevant quantity here is the ratio to the Hubble rate, T/H. Because H ~ T , these constraints are always less important than inverse decay. A key ingredient for this to be valid is that the photon has a universal coupling constant to all fermions. This is not true for the Higgs portal discussed in the next model.
2If there is an additional very light scalar or fermion in the dark sector which the mediator can decay into,
the constraint on k could be evaded. This could lead to extra contribution to effective number of neutrinos,
Neff [13, 14]. In this work, we focus on the minimal model and do not consider such extensions.
I—1 UI
decay rate in [12] including the hadronic channels. On the other hand, k also controls the direct detection cross section of DM x,
where aX = gX/(4n). For weak scale DM, the current LUX [15] experiment places the strongest upper limit on k. In order to satisfy both constraints, the mediator VM should be heavier than ~ 50 MeV.3 This is shown in the panel (A) of figure 2. We also notice that with a weak scale DM, the direct detection constraint on k — mv parameter space is stronger than many of the limits on models with dark photon only. On the other hand, if the DM is lighter than around 4GeV, the direct detection limits from LUX and CDMSlite [17] (which C_| covers the lower mass region down to mX = 4GeV) are both evaded. However, as shown in panel (C) of figure 2, the other constraints from, e.g., Supernova 1987a, are also very strong [18-20] (for an exception see [21])—not much parameter space could be opened in the lower mv region.
We want to highlight a less constrained region where 10-12 < k < 10-9 and mv is at GeV scale. In this case, the V particle is long-lived enough and becomes non-relativistic before it decays; the total energy density of the universe could experience a temporary period of V-matter domination. To find the minimum lifetime of V^ for this to happen, one can —^ compare its energy density with that of the visible radiation species,
__ n2 /g (T )N 4/3
PV(Ty) = mvnv(Ty)e ) , pr(Ty) = — g*(Ty)T4
3The momentum exchange for DM scattering on xenon nucleus is roughly 50 MeV. Thus for mediator
lighter than this value, the cross section will get saturated by the momentum exchange, and the bound could
be slightly weakened [16]. We find this only slightly affects the lower bound on the mediator mass.
g*s (Ty)\ 4/3 ( )
30* ^ \g*s(mt)J ' (.)
Here g*(T) counts the relativistic SM degree of freedom contributing to energy density. After
T' < mv, the mediator becomes non-relativistic, and pv scales as T~3, while for radiation ____
pr scales as T-4 up to the changes in g*s. In order for pv to be ever larger than pr, we find
the lower bound on the lifetime, o
rv > 0.004«-6(ImV)"2 sec . (2.6) 8
Note 0.004 second corresponds to around a temperature of the universe at 15 MeV. Scalar mediator case. The Lagrangian for a dark sector with scalar mediator is
L = Lsm + Xidx — mxXX + 1 — m^2 + VxXX^
+^lh(H— v2/2)0 + A^HW + Ai^4 , (2.7)
where the DM x is a Dirac fermion, and the mediator 0 is a real scalar, and both are SM singlets.
In early universe x and 0 are in thermal equilibrium via their Yukawa coupling yX. For mX » mi, the DM relic density is controlled by the process xX ^ 00. For symmetric DM, correct thermal relic density requires the annihilation cross section satisfy
9naXTcd 3 x 10-26cm3/s
Manni=9nar=—S—L. (2.8)
This is a p-wave annihilation and Tcd & mx/26 is the chemical decoupling temperature. Again we assume the dark sector has its own temperature T'. After DM freeze out the comoving 0 number is given by
= ^g^t3 . (2.9)
» 2n2 g*s (mt) 7 In this model, there are two ways that 0 could communicate to SM. First, if the coefficient of cross quartic term X»h is large, 0 will experience a similar freeze out via s-channel Higgs exchange. Second, the term in the Lagrangian induces a mixing between 0 and the Higgs boson and is responsible for 0 to scatter and decay. Because of the Higgs portal, the 0-top quark scattering is most important in bringing 0 into equilibrium with SM than inverse decay. As said, we are primarily interested in a similar parameter space as the vector mediator case, where A»h, are small enough so that they never bring 0 into equilibrium with the SM sector. This requires, \»h < 10-7 and < 10-7, respectively.
The BBN and direct detection could further constrain h and m». For the 0 decay rate we use a result including the hadronic channels [22, 23]. The direct detection cross section
of DM x is O
^ ^ 4axf2mN^ (210)
^SI --^^-, (2.10)
where ax = yX/(4n). It was noted in [7] that if DM is heavier than ~ 5GeV, 0 must weigh
more than twice of the muon mass, m» > 210 MeV. This can be seen from panel (B) of ^ figure 2.
Because there are fewer constraints on a light scalar mediator than a vector one, for DM mass at GeV scale, we find it possible to lift the direct detection constraint, and make 0 as light as MeV. There is still an upper bound on 0-Higgs mixing from the low energy K+
— Et process [24], as shown in panel (D) of figure 2. In together with the decay before BBN requirement, there is a narrow window still allowed for the parameter 10-5 < < 10-4. However, in this window, 0 will always be thermalized with SM
particles at high temperature, which fixes £ = 1.
Similar to the vector mediator case, we are interested in the possibility that 0 temporarily dominates the total energy density of the universe before it decays. Using (2.9) we derive the minimal lifetime of 0 for this to happen,
* * °.01«-6( tsV r sec. (2.11)
This happens if 10-10 < < 10-8, and is highlighted in the red region of figure 2(B).
To close this section, we have summarized the experimental constraints on two simple models of dark sector with light mediator, V or 0, and showed the regions in the parameter space that allow the mediator to temporarily dominate the universe as matter. The next few sections are devoted to the study of the implication of this possible era on the DM primordial spectrum.
3 Light mediator dominance and perturbations
To calculate the perturbation to energy densities in early universe, we define the metric in the conformal Newton gauge
ds2 = -(1 + 2^)di2 + (1 + 2$)a%-dxW . (3.1)
Figure 3. Evolution of the energy densities of DM x, light mediator (j> and SM radiation r. In the shaded region, the universe is 4> dominated.
The perturbations satisfy \I> = —$ in the absence of quadrupole moment.
There are three species in the universe,4 DM %■> light, mediator <fi and SM radiation r. The radiation includes all relativist.ic SM particles which tightly couple to each other. For each species, the stress-energy tensor and the perturbations are
T»v = (1 + w)p( 1 + 6)nW + wp( 1 + 5)(fv , (3.2)
where w = p/p, and u^ = (1 — v). The next-to-leading order quantities are 5 and v.
Using the continuity of !)„,, the decay of (f) into usual radiation with DM as a spectator can be described as [25]
px + 3 Hpx = 0, Pl + 3(1 + w^HpQ = —r^pi, (3.3)
pr + 4Hpx = r^pi .
where an over dot means d/dt. The Hubble expansion rate is
.-> 87TG , . ,
H = — (Px + P4> + Pr) ■ (3-4)
We include the process where the light, mediator 0 changes from radiation-like (w^ = 1/3) to matter-like {w^ —> 0) as the temperature drops. As assumed throughout, this work, after DM freeze out. the total number of % no longer change, and so does that of <fi until it. begins to decay to radiation species of the SM sector.
We present, the results using a. set. of sample input, parameters, m^ = 10 GeV r^ = 1 sec, £ = 1, and mx = 1 TeV. We also choose the initial temperature to be Tj„i = mx/26 » m^ right, after freeze out., and define the Hubble radius at this time to be ao = 1. As a. good approximation, T7 = T^ = T-m; at the time ao- The initial conditions for (3.3) are
27T2 ■ 7T2 7T2
px(a,i) = S x (5.4 GeV) x rib—g^T^T^ , p^cu) = —Tj4;, pr(ai) = —g*(T-mi)T4ni .
4In this section we will proceed the discussion a with scalar light mediator <p. The results for vector mediator case are very similar.
m^ = 10GeV, 7"^=lsec, ^=1 = lOGeV, 7"^=lsec, ^=1
Figure 4. Evolution of primordial perturbations of different wavelengths that enter the horizon before, during and after the 4> domination regime. Different colors correspond to wave numbers k/keq = fO9'5 (cyan), fO9 1 (red), fO8'8 (magenta), 108 (orange), fO7'5 (yellow), fO7 (green) and fO6 (blue), respectively. The dashed part of curves means sign change in the perturbation due to acoustic oscillation.
where % = n^/s = 0.9 x 10 10 is the baryon-to-entropy ratio today, and the dilution factor S due to entropy release from 0 decay is fixed a posteriori from solving eqs. (3.3),
5= (44)3/1 , (3.5)
\Px(af)J XpMi);
where a,/ corresponds to an epoch well after 0 decay.
Figure 3 shows the evolution of the p's. During the period 103 < a < 3 x 105, the energy density of (f) beats that of radiation and dominates the total energy in the universe. This happens until the (f) particles decay away, and dump a significant amount entropy into radiation. With the above set of parameters, S ~ 60, and matter-radiation equality happens at Oeq = 2.8 x 1011.
The equations for the evolution of perturbations in the fluid densities and in the metric are
<jx + — + 3$ = 0 , a
K + H0X + ^ = + T-HO* - 0X),
¿V + (1 + W^ + 3(1 + = , 0* + (1 - 3wJHOt + ^ - =
a I + Wfi a I + Wfi
oCt Pr
^ + (H + 3Wa~2) $ = JF {px6x + P+ Pr8r) '
where 9 = aV • v for each species. We derived these equations following the notations in [26-29]. Notice again the over dot means d/dt here. The rate r"1 is related to the scattering
process 0x ^ 0x which keeps the DM in kinetic equilibrium with 0, and it is given by
where the first bracket is the 0x ^ 0X cross section5 at T ^ mx, and the second bracket represents the ratio of collision time to the thermal relaxation time [30]. The relative velocity = 1 when T > m$, and = ^j3T/m$ at low temperature. For ax = 0.1 and mx = 1 TeV, this rate falls below Hubble at akd — 104 (around T ~ 10MeV). With this input, the sound speed cs of the the x fluid is, c2s = 5px/5px = 2T$/(3mx) before kinetic decoupling (a < akd), and more suppressed for a > akd. The back reaction of the scattering on the 6$ equation has C j been neglected because 0 is much more populated than x. ^^
The primordial scalar perturbations does not evolve until entering the horizon. The initial conditions for (3.6) can be obtained by simplifying these equations for super-horizon modes. At time a0, the universe is still radiation dominated, thus, h^
5x(ao) = 5$(ao) = 45r(ao) = 2$o , 6x(ao) = 6$(ao) = 6r(ao) = -2Hf(ao) ' (3.7)
where $0 is the primordial scalar perturbation in the metric.
We solve the set of equations in (3.6) for modes that enter the horizon before, during and after the 0 domination regime. The results on $ and Sx are shown in figure 4. From the $ plot one could infer when a mode enters the horizon, while the Sx plot shows the impact of 0-x scattering and the era of 0 matter domination on different scales. ____
During the period when > pr, the universe is temporarily matter dominated, and it is well known that in this period the density perturbations of 0 itself and DM x both
grow linearly. This feature is shown in figure 4, where 0 domination depicted by the shaded region. For modes entering the horizon in this period, $ drops slowly allowing 6X to grow, which then serves as the source for the linear growth of Sx. After 0 begins to decay and the universe returns to radiation dominated, these perturbations grow logarithmically. Because all 0 particles eventually decay away, only the DM density perturbation Sx matters for later structure formation at this scale, and it still remembers the 0-domination history. The enhancement in Sx implies it will reach the nonlinear growth regime much earlier than the usual cold DM case.
At earlier time, the effect of 0-x scattering plays an important role. The scattering term rc-1 couples the 0 fluid tightly to the DM x fluid. Because in this regime 0 still carries non-negligible kinetic energy and has a larger sound speed, it drives the acoustic oscillation and causes collisional damping in Sx until the rate falls below H at akd. At very high wavenumber k, the resulting damping factor in the Sx spectrum can be estimated as [32],
Ddamp(k) = exp f. (3.8)
V kcut /
where we find kcut corresponds to the mode entering the horizon at the moment of 0 domination begins. For modes entering the horizon during 0 dominated era, they are less affected
5For the vector mediator model, the Vx ^ Vx cross section is that of Thomson scattering, 8naX/(3mX
k/kf. q
Figure 5. The transfer function normalized to that of collision-less cold DM. keq corresponds to the mode that enters the horizon at matter-radiation equality.
by the collisional damping effects, although the kinetic decoupling happens afterwards. This can be understood because both 0 and x have become effectively non-relativistic, and their perturbations satisfy the same equation with the same initial condition. The momentum exchange term r~l{9(f> — 9X) is also not important because 9^ and 9X evolve hand in hand with each other.
To obtain the transfer function T(k), we evolve the DM density perturbation 5X to the time of matter-radiation equality, and normalize the perturbations to those of a cold DM. The result is shown in figure 5. The relative transfer function T(k)/TcDM(k) exhibits a peak at wavenumber ~ 108fceq right, before the exponential cutoff. The enhancement factor in this case in the density perturbation can be as large as 100 — 1000.
This peak-plus-cutoff feature is a unique prediction of dark sector models where DM couples to a long-lived light mediator. This result also does not depend on whether the DM is symmetric or asymmetric.
4 Possible testable implications
From DM density perturbation spectrum one can calculate the DM structure formation at later time. The peak before the cutoff in the primordial spectrum corresponds to a special scale of the smallest DM halos/clumps. The peak right before the cutoff indicates that these smallest objects are most likely formed. Here we estimate their properties. From figure 5, we get the wavenumber at the peak in spectrum,
fcpeak ^ 108fceq- The mass of the smallest objects today can be determined fcpeak, evaluated using [31],
where we used today's DM relic density Q[Jm = 0.26, today's critical density p°c = 8.5 x 10-30gem-3, fceq = 0.073Mpc-1QpM/?2, h = 0.673, and M© is the solar mass.
The size of these halos is given by the length scale of the mode at the time when the DM density perturbation ¿x(a„i) approaches to 1 [33],
Clearly Rpeak is more sensitive to the linear growth during 0 domination. To get ani, we first assume scale invariance in the primordial scalar perturbation and fix the initial value of $0 — 8 x 10-6 from the Harrison-Zel'Dovich-Peebles spectrum in the large scale structure observation [34]. From this, we find for the mode corresponding to the peak of figure 5, ¿x(kpeak) will reach nonlinear growth shortly after recombination, and Rpeak ~ 1014 cm. The average DM density inside such mini halos is about 109 times higher than the local DM density in the usual case.
Therefore, the first formed DM halos have a typical mass similar to that of the earth, and typical size similar to the earth-sun distance. After the formation, these halos may merge into larger objects or be destroyed by gravitational tidal forces. A more precise calculation of the small scale structure formation and properties of such objects today calls for simulation |
and is beyond the scope of this work. Today, if the smallest halos still takes substantial ^^ fraction of total Milky Way galaxy mass, the average distance of two nearby such objects is ~ 1016 cm. Thus the solar system would run into such objects every 50-100 years and the direct detection rates will get enhanced periodically. Another way to observe these clumps is indirect detection signals from, e.g., DM annihilation from inside. For asymmetric DM case, if the self-interaction allows DM bound states to exist and form, as discussed in the context of Yukawa bound states [7] or the case of dark atom [35], the indirect detection
signal is also available. It could be enhanced if the bound state formation makes these _^
clumps dissipate enough and further reduce their sizes. There have also been suggestions k » that large primordial density perturbations could lead to micro-lensing effect if DM forms more compact objects [36, 37].
5 Outlook
To summarize, in the context of simple dark sector models containing a long-lived light mediator, we notice the mediator's longevity can be closely connected to an era of temporary matter domination. We have calculated the early universe evolution of dark matter density perturbations, especially during the mediator domination era when the perturbation could o grow linearly. We showed this scenario can result in a sharp peak in the transfer function compared to that of collision-less cold dark matter. This leaves us with more structures on small scales to look for, and could provide additional handle in testing light mediator models with very weak interactions to the standard model. More dedicated simulation of the small scale structure formation would help to obtain more concrete prediction in the properties of these mini dark matter halos.
We note a temporary matter dominated universe before BBN has been discussed in various warm DM models, such as wino DM produced from late decaying moduli [38], and keV sterile neutrino DM diluted by long-lived right handed neutrinos [39-41]. In the moduli decay case, the free streaming of boosted wino always washes out most structures on small scales [27, 28]. The free streaming nature of light sterile neutrino will result in the same suppression. In contrast, in the light mediator models discussed in the present work, the key for the primordial small scale structures to survive is that the long-lived mediator cannot decay to DM, and the DM itself remains cold.
Acknowledgments
We thank Sean Carroll, Clifford Cheung, Francis-Yan Cyr-Racine, Hooman Davoudiasl, Jonathan Feng, Michael Graesser, Hong-Jian He, Goran Senjanovic, Tim Tait, Mark Wise,
Hai-bo Yu for useful conversations and comments on the draft. This work is supported by the Gordon and Betty Moore Foundation through Grant #776 to the Caltech Moore Center for Theoretical Cosmology and Physics, and by the DOE Grant DE-FG02-92ER40701, and also by a DOE Early Career Award under Grant No. DE-SC0010255.
References
[4] [5;
[8] [9] 10 11 12
M. Pospelov, A. Ritz and M.B. Voloshin, Secluded WIMP dark matter, Phys. Lett. B 662 (2008) 53 [arXiv:0711.4866] [inSPIRE].
N. Arkani-Hamed, D.P. Finkbeiner, T.R. Slatyer and N. Weiner, A theory of dark matter, Phys. Rev. D 79 (2009) 015014 [arXiv:0810.0713] [inSPIRE].
D.E. Kaplan, M.A. Luty and K.M. Zurek, Asymmetric dark matter, Phys. Rev. D 79 (2009) 115016 [arXiv:0901.4117] [inSPIRE].
H. An, S.-L. Chen, R.N. Mohapatra and Y. Zhang, Leptogenesis as a common origin for matter and dark matter, JHEP 03 (2010) 124 [arXiv:0911.4463] [inSPIRE].
H. An, S.-L. Chen, R.N. Mohapatra, S. Nussinov and Y. Zhang, Energy dependence of direct detection cross section for asymmetric mirror dark matter, Phys. Rev. D 82 (2010) 023533 OH
[arXiv:1004.3296] [inSPIRE].
D.E. Kaplan, G.Z. Krnjaic, K.R. Rehermann and C.M. Wells, Atomic dark matter, JCAP 05 (2010) 021 [arXiv:0909.0753] [inSPIRE].
M.B. Wise and Y. Zhang, Stable bound states of asymmetric dark matter, Phys. Rev. D 90 (2014) 055030 [arXiv:1407.4121] [inSPIRE]. |—
M.B. Wise and Y. Zhang, Yukawa bound states of a large number of fermions, JHEP 02 (2015) 023 [arXiv:1411.1772] [inSPIRE].
J.L. Feng, M. Kaplinghat, H. Tu and H.-B. Yu, Hidden charged dark -matter, JCAP 07 (2009) 004 [arXiv:0905.3039] [inSPIRE].
M.R. Buckley and P.J. Fox, Dark matter self-interactions and light force carriers, Phys. Rev. D o 81 (2010) 083522 [arXiv:0911.3898] [inSPIRE]. QQ
S. Tulin, H.-B. Yu and K.M. Zurek, Beyond collisionless dark matter: particle physics dynamics for dark matter halo structure, Phys. Rev. D 87 (2013) 115007 [arXiv:1302.3898] [inSPIRE].
B. Batell, M. Pospelov and A. Ritz, Probing a secluded U(1) at B-factories, Phys. Rev. D 79 (2009) 115008 [arXiv:0903.0363] [inSPIRE].
S. Weinberg, Goldstone bosons as fractional cosmic neutrinos, Phys. Rev. Lett. 110 (2013) 241301 [arXiv:1305.1971] [inSPIRE].
B. Bertoni, S. Ipek, D. McKeen and A.E. Nelson, Reducing cosmological small scale structure via a large dark matter-neutrino interaction: constraints and consequences, JHEP 04 (2015) 170 [arXiv:1412.3113] [inSPIRE].
LUX collaboration, D.S. Akerib et al., First results from the LUX dark matter experiment at the Sanford Underground Research Facility, Phys. Rev. Lett. 112 (2014) 091303 [arXiv:1310.8214] [inSPIRE].
M. Kaplinghat, S. Tulin and H.-B. Yu, Direct detection portals for self-interacting dark matter, Phys. Rev. D 89 (2014) 035009 [arXiv:1310.7945] [inSPIRE].
SuperCDMS collaboration, R. Agnese et al., Search for low-mass weakly interacting massive particles using voltage-assisted calorimetric ionization detection in the SuperCDMS experiment, Phys. Rev. Lett. 112 (2014) 041302 [arXiv:1309.3259] [inSPIRE].
[18 [19 [20 [21 [22 [23
[34 [35
E. Bertschinger, The effects of cold dark matter decoupling and pair annihilation on cosmological perturbations, Phys. Rev. D 74 (2006) 063509 [astro-ph/0607319] [inSPIRE].
J.D. Bjorken, R. Essig, P. Schuster and N. Toro, New fixed-target experiments to search for dark gauge forces, Phys. Rev. D 80 (2009) 075018 [arXiv:0906.0580] [inSPIRE].
R. Essig et al., Working group report: new light weakly coupled particles, arXiv:1311.0029 [inSPIRE].
J.B. Dent, F. Ferrer and L.M. Krauss, Constraints on light hidden sector gauge bosons from supernova cooling, arXiv:1201.2683 [inSPIRE].
Y. Zhang, Supernova cooling in a dark matter smog, JCAP 11 (2014) 042 [arXiv:1404.7172] [inSPIRE].
M.B. Voloshin, Once again about the role of gluonic mechanism in interaction of light Higgs boson with hadrons, Sov. J. Nucl. Phys. 44 (1986) 478 [Yad.. Fiz. 44 (1986) 738] [inSPIRE].
J.D. Clarke, R. Foot and R.R. Volkas, Phenomenology of a very light scalar (100 MeV <mh < 10 GeV) 'mixing with the SM Higgs, JHEP 02 (2014) 123 [arXiv:1310.8042] [inSPIRE].
L.A. Anchordoqui et al., Weinberg's Higgs portal confronting recent LUX and LHC results together with upper limits on B+ and K+ decay into invisibles, Phys. Rev. D 89 (2014) 083513 [arXiv:1312.2547] [inSPIRE].
R.J. Scherrer and M.S. Turner, Decaying particles do not heat up the universe, Phys. Rev. D 31 (1985) 681 [inSPIRE].
C.-P. Ma and E. Bertschinger, Cosmological perturbation theory in the synchronous and conformal Newtonian gauges, Astrophys. J. 455 (1995) 7 [astro-ph/9506072] [inSPIRE].
A.L. Erickcek and K. Sigurdson, Reheating effects in the matter power spectrum and
implications for substructure, Phys. Rev. D 84 (2011) 083503 [arXiv:1106.0536] [inSPIRE]. I—
J. Fan, O. Ozsoy and S. Watson, Nonthermal histories and implications for structure
formation, Phys. Rev. D 90 (2014) 043536 [arXiv:1405.7373] [inSPIRE]. *___-
S. Hofmann, D.J. Schwarz and H. Stoecker, Damping scales of neutralino cold dark matter, Phys. Rev. D 64 (2001) 083507 [astro-ph/0104173] [inSPIRE]. 00
A. Loeb and M. Zaldarriaga, The small-scale power spectrum of cold dark matter, Phys. Rev. D 71 (2005) 103520 [astro-ph/0504112] [inSPIRE].
A.M. Green, S. Hofmann and D.J. Schwarz, The first wimpy halos, JCAP 08 (2005) 003 [astro-ph/0503387] [inSPIRE].
A.V. Gurevich, K.P. Zybin and V.A. Sirota, Small scale structure of dark matter and microlensing, Sov. Phys. Usp. 167 (1997) 913 [astro-ph/9801314] [inSPIRE].
S. Dodelson, Modern cosmology, Academic Press, U.S.A. (2003).
L. Pearce, K. Petraki and A. Kusenko, Signals from dark atom formation in halos, Phys. Rev. D 91 (2015) 083532 [arXiv:1502.01755] [inSPIRE].
A.L. Erickcek and N.M. Law, Astrometric Microlensing by Local Dark Matter Subhalos, Astrophys. J. 729 (2011) 49 [arXiv:1007.4228] [inSPIRE].
F. Li, A. L. Erickcek and N.M. Law, A new probe of the small-scale primordial power spectrum: astrometric microlensing by ultracompact minihalos, Phys. Rev. D 86 (2012) 043519 [arXiv:1202.1284] [inSPIRE].
B.S. Acharya, G. Kane, S. Watson and P. Kumar, A non-thermal WIMP miracle, Phys. Rev. D 80 (2009) 083529 [arXiv:0908.2430] [inSPIRE].
[39] T. Asaka, M. Shaposhnikov and A. Kusenko, Opening a new window for warm dark matter, Phys. Lett. B 638 (2006) 401 [hep-ph/0602150] [inSPIRE].
[40] M. Nemevsek, G. Senjanovic and Y. Zhang, Warm dark matter in low scale left-right theory, JCAP 07 (2012) 006 [arXiv:1205.0844] [inSPIRE].
[41] F. Bezrukov, H. Hettmansperger and M. Lindner, keV sterile neutrino dark matter in gauge extensions of the standard model, Phys. Rev. D 81 (2010) 085032 [arXiv:0912.4415] [inSPIRE].
2 O M U1
