Abstract:As potential candidates of dark matter, primordial black holes (PBHs) are within the core scopes of various astronomical observations. In light of the explosive development of gravitational wave (GW) and radio astronomy, we thoroughly analyze a stochastic background of cosmological GWs, induced by overly large primordial density perturbations, with several spikes that was inspired by the sound speed resonance effect and can predict a particular pattern on the mass spectrum of PBHs. With a specific mechanism fo… Show more
“…The amplitude difference after horizon crossing between two resonant polarization modes originates mainly from the phase difference of h R and h L before the horizon crossing (see Fig. 4), which results from the difference of their equations of motion (14) when the Chern-Simons coupling is considered. Similar results can also be found in the other two cases.…”
Section: Figmentioning
confidence: 99%
“…The parameter resonance amplification of scalar perturbations during inflation has been widely discussed [13][14][15][16][17]. In this paper, we investigate the similar amplification of tensor perturbations with parity-violation caused by the gravitational Chern-Simons term coupled to an axion field that drives inflation while they are deep inside the horizon during inflation.…”
We investigate axion inflation where the gravitational Chern–Simons term is coupled to a periodic function of the inflaton. We find that tensor perturbations with different polarizations are amplified in different ways by the Chern–Simons coupling. Depending on the model parameters, the resonance amplification results in a parity-violating peak or a board plateau in the energy spectrum of gravitational waves, and the sharp cutoff in the infrared region constitutes a characteristic distinguishable from stochastic gravitational wave backgrounds produced by matter fields in Einstein gravity.
“…The amplitude difference after horizon crossing between two resonant polarization modes originates mainly from the phase difference of h R and h L before the horizon crossing (see Fig. 4), which results from the difference of their equations of motion (14) when the Chern-Simons coupling is considered. Similar results can also be found in the other two cases.…”
Section: Figmentioning
confidence: 99%
“…The parameter resonance amplification of scalar perturbations during inflation has been widely discussed [13][14][15][16][17]. In this paper, we investigate the similar amplification of tensor perturbations with parity-violation caused by the gravitational Chern-Simons term coupled to an axion field that drives inflation while they are deep inside the horizon during inflation.…”
We investigate axion inflation where the gravitational Chern–Simons term is coupled to a periodic function of the inflaton. We find that tensor perturbations with different polarizations are amplified in different ways by the Chern–Simons coupling. Depending on the model parameters, the resonance amplification results in a parity-violating peak or a board plateau in the energy spectrum of gravitational waves, and the sharp cutoff in the infrared region constitutes a characteristic distinguishable from stochastic gravitational wave backgrounds produced by matter fields in Einstein gravity.
“…Furthermore, the PBHs formation is followed by the generation of the induced gravitational waves (GWs), when the primordial curvature perturbations enhance significantly [59][60][61][62][63][64][65][66][67][68][69][70][71][72][73][74]. In other words, after the horizon re-entry, the collapse of the overdense regions can generate large metric perturbations besides PBHs.…”
Within the framework of inflationary model with field-dependent kinetic term for quartic and natural potentials, we investigate generation of the primordial black holes (PBHs) and induced gravitational waves (GWs). In this setup, we consider a kinetic function as $$G(\phi )=g_I(\phi )\big (1+g_{II}(\phi )\big )$$
G
(
ϕ
)
=
g
I
(
ϕ
)
(
1
+
g
II
(
ϕ
)
)
and show that in the presence of first term $$g_I(\phi )$$
g
I
(
ϕ
)
both quartic and natural potentials, in contrast to the standard model of inflation, can be consistent, with the 68% CL of Planck observations. Besides, the second term $$g_{II}(\phi )$$
g
II
(
ϕ
)
can cause a significant enhancement in the primordial curvature perturbations at the small scales which results the PBHs formation. For the both potentials, we obtain an enhancement in the scalar power spectrum at the scales $$k\sim 10^{12}~{\mathrm{Mpc}}^{-1}$$
k
∼
10
12
Mpc
-
1
, $$10^{8}~{\mathrm{Mpc}}^{-1}$$
10
8
Mpc
-
1
, and $$10^{5}~{\mathrm{Mpc}}^{-1}$$
10
5
Mpc
-
1
, which causes PBHs production in mass scales around $$10^{-13}M_{\odot }$$
10
-
13
M
⊙
, $$10^{-5}M_{\odot }$$
10
-
5
M
⊙
, and $$10 M_{\odot }$$
10
M
⊙
, respectively. Observational constraints confirm that PBHs with a mass scale of $$10^{-13}M_{\odot }$$
10
-
13
M
⊙
can constitute the total of dark matter in the universe. Furthermore, we estimate the energy density parameter of induced GWs which can be examined by the observation. Also we conclude that it can be parametrized as a power-law function $$\Omega _{\mathrm{GW}}\sim (f/f_c)^n$$
Ω
GW
∼
(
f
/
f
c
)
n
, where the power index equals $$n=3-2/\ln (f_c/f)$$
n
=
3
-
2
/
ln
(
f
c
/
f
)
in the infrared limit $$f\ll f_{c}$$
f
≪
f
c
.
“…constraints on various aspects of fundamental physics, see e.g. [124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146] (see also the reviews [147,148]).…”
We consider two stable Interacting Dark Matter -Dark Energy models and confront them against current Cosmic Microwave Background data from the Planck satellite. We then generate luminosity distance measurements from O(10 3 ) mock Gravitational Wave events matching the expected sensitivity of the proposed Einstein Telescope. We use these to forecast how the addition of Gravitational Wave standard sirens data can improve current limits on the Dark Matter -Dark Energy coupling strength (ξ). We find that the addition of Gravitational Waves data can reduce the current uncertainty by a factor of 5. Moreover, if the underlying cosmological model truly features Dark Matter -Dark Energy interactions with a value of ξ within the currently allowed 1σ upper limit, the addition of Gravitational Wave data would help disentangle such an interaction from the standard case of no interaction at a significance of more than 3σ. 98.80.Cq, 95.35.+d, 95.36.+x, 98.80.Es.
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