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Primordial blackhole formation: exploring chaotic potential with a sharp step via the GLMS perspective
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Abstract
A sharp step on a chaotic potential can enhance primordial curvature fluctuations on smaller scales to the
O
(
10
−
2
)
to form primordial black holes (PBHs). The present study discusses an inflationary potential with a sharp step that results in the formation of PBHs in four distinct mass ranges. Also this inflationary model allows the separate consideration of observable parameters
n
s
and
r
on the CMB scale from the physics at small scales, where PBHs formation occur. In this work we computed the fractional abundance of PBHs (
f
PBH
) using the GLMS approximation of peak theory and also the Press–Schechter (PS) formalism. In the two typical mass windows,
10
−
13
M
⊙
and
10
−
11
M
⊙
,
f
PBH
calculated using the GLMS approximation is nearly equal to 1 and that calculated via PS is of 10
−3
. In the other two mass windows
1
M
⊙
and
6
M
⊙
,
f
PBH
obtained using GLMS approximation is 0.01 and 0.001 respectively, while
f
PBH
calculated via PS formalism yields 10
−5
and 10
−6
. The results obtained via GLMS approximation are found to be consistent with observational constraints. A comparative analysis of
f
PBH
obtained using the GLMS perspective and the PS formalism is also included.
Title: Primordial blackhole formation: exploring chaotic potential with a sharp step via the GLMS perspective
Description:
Abstract
A sharp step on a chaotic potential can enhance primordial curvature fluctuations on smaller scales to the
O
(
10
−
2
)
to form primordial black holes (PBHs).
The present study discusses an inflationary potential with a sharp step that results in the formation of PBHs in four distinct mass ranges.
Also this inflationary model allows the separate consideration of observable parameters
n
s
and
r
on the CMB scale from the physics at small scales, where PBHs formation occur.
In this work we computed the fractional abundance of PBHs (
f
PBH
) using the GLMS approximation of peak theory and also the Press–Schechter (PS) formalism.
In the two typical mass windows,
10
−
13
M
⊙
and
10
−
11
M
⊙
,
f
PBH
calculated using the GLMS approximation is nearly equal to 1 and that calculated via PS is of 10
−3
.
In the other two mass windows
1
M
⊙
and
6
M
⊙
,
f
PBH
obtained using GLMS approximation is 0.
01 and 0.
001 respectively, while
f
PBH
calculated via PS formalism yields 10
−5
and 10
−6
.
The results obtained via GLMS approximation are found to be consistent with observational constraints.
A comparative analysis of
f
PBH
obtained using the GLMS perspective and the PS formalism is also included.
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