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Xisco Jimenez Forteza
RDStackingProject
Commits
d748699c
Commit
d748699c
authored
4 years ago
by
Francisco Jimenez Forteza
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rdown.py
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# Copyright (C) 2021 Xisco Jimenez Forteza
#
# This program is free software; you can redistribute it and/or modify it
# under the terms of the GNU General Public License as published by the
# Free Software Foundation; either version 3 of the License, or (at your
# option) any later version.
#
# This program is distributed in the hope that it will be useful, but
# WITHOUT ANY WARRANTY; without even the implied warranty of
# MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General
# Public License for more details.
#
# You should have received a copy of the GNU General Public License along
# with this program; if not, write to the Free Software Foundation, Inc.,
# 51 Franklin Street, Fifth Floor, Boston, MA 02110-1301, USA.
#
# =============================================================================
#
# Preamble
#
# =============================================================================
#
# Module to generate RD waveforms.
import
numpy
as
np
import
qnm
import
os
f_fpars
=
[[
2.95845
,
-
2.58697
,
0.0533469
],
[
2.12539
,
-
1.78054
,
0.0865503
],
[
1.74755
,
-
1.44776
,
0.123666
],
[
1.78287
,
-
1.53203
,
0.129475
],
[
2.04028
,
-
1.83224
,
0.112497
]]
q_fpars
=
[[
0.584077
,
1.52053
,
-
0.480658
],
[
0.00561441
,
0.630715
,
-
0.432664
],
[
-
0.197965
,
0.515956
,
-
0.369706
],
[
-
0.275097
,
0.455691
,
-
0.331543
],
[
-
0.287596
,
0.398514
,
-
0.309799
]]
class
Ringdown_Spectrum
:
"""
RDown model generator
"""
def
__init__
(
self
,
mf
,
af
,
l
,
m
,
n
=
4
,
s
=-
2
,
time
=
[],
fixed
=
False
):
self
.
mf
=
mf
self
.
af
=
af
self
.
l
=
l
self
.
m
=
m
self
.
n
=
n
self
.
time
=
time
self
.
grav_220
=
[
qnm
.
modes_cache
(
s
=
s
,
l
=
self
.
l
,
m
=
self
.
m
,
n
=
i
)
for
i
in
range
(
0
,
self
.
n
+
1
)]
self
.
dim
=
self
.
n
+
1
self
.
fixed
=
fixed
if
len
(
self
.
time
)
==
0
:
self
.
time
=
np
.
arange
(
0
,
100
,
0.1
)
if
self
.
fixed
:
omegas_new
=
np
.
asarray
([
self
.
grav_220
[
i
](
a
=
self
.
af
)[
0
]
for
i
in
range
(
0
,
self
.
dim
)])
self
.
w
=
(
np
.
real
(
omegas_new
))
/
self
.
mf
self
.
tau
=-
1
/
(
np
.
imag
(
omegas_new
))
*
self
.
mf
def
QNM_spectrum
(
self
):
"""
It computes the RD frequencies and damping times in NR units.
"""
omegas_new
=
np
.
asarray
([
self
.
grav_220
[
i
](
a
=
self
.
af
)[
0
]
for
i
in
range
(
0
,
self
.
n
+
1
)])
w_m_a
=
(
np
.
real
(
omegas_new
))
/
self
.
mf
tau_m_a
=-
1
/
(
np
.
imag
(
omegas_new
))
*
self
.
mf
return
(
w_m_a
,
tau_m_a
)
def
w_fpars_Berti
(
self
,
n
):
return
f_fpars
[
n
]
def
tau_qpars_Berti
(
self
,
n
):
return
q_fpars
[
n
]
def
mass_from_wtau
(
self
,
n
,
w
,
tau
):
f1
,
f2
,
f3
=
w_fpars_Berti
(
n
)
q1
,
q2
,
q3
=
tau_qpars_Berti
(
n
)
res
=
(
f1
+
f2
*
(
2
**
(
-
1
/
q3
)
*
((
-
2
*
q1
+
w
*
tau
)
/
q2
)
**
(
1
/
q3
))
**
f3
)
/
w
return
res
def
spin_from_wtau
(
self
,
n
,
w
,
tau
):
f1
,
f2
,
f3
=
w_fpars_Berti
(
n
)
q1
,
q2
,
q3
=
tau_qpars_Berti
(
n
)
res
=
1
-
2
**
(
-
1
/
q3
)
*
((
-
2
*
q1
+
w
*
tau
)
/
q2
)
**
(
1
/
q3
)
return
res
def
mass_from_wtau_loop
(
self
,
w
,
tau
,
l
,
m
):
res
=
[
None
]
*
dim
for
n
in
range
(
0
,
dim
):
f1
,
f2
,
f3
=
w_fpars_Berti
(
n
)
q1
,
q2
,
q3
=
tau_qpars_Berti
(
n
)
res
[
n
]
=
(
f1
+
f2
*
(
2
**
(
-
1
/
q3
)
*
((
-
2
*
q1
+
w
[
n
]
*
tau
[
n
])
/
q2
)
**
(
1
/
q3
))
**
f3
)
/
w
[
n
]
return
res
def
spin_from_wtau_loop
(
self
,
w
,
tau
,
l
,
m
):
res
=
[
None
]
*
dim
for
n
in
range
(
0
,
dim
):
f1
,
f2
,
f3
=
w_fpars_Berti
(
n
)
q1
,
q2
,
q3
=
tau_qpars_Berti
(
n
)
res
[
n
]
=
1
-
2
**
(
-
1
/
q3
)
*
((
-
2
*
q1
+
w
[
n
]
*
tau
[
n
])
/
q2
)
**
(
1
/
q3
)
return
res
def
rd_model_wtau
(
self
,
theta
):
"""
RD model parametrized with the damping time tau.
"""
assert
int
(
len
(
theta
)
/
4
)
==
self
.
dim
,
'
Please recheck your n and parameters
'
wvars
=
theta
[
:
(
self
.
dim
)]
tvars
=
theta
[(
self
.
dim
)
:
2
*
(
self
.
dim
)]
xvars
=
theta
[
2
*
(
self
.
dim
)
:
3
*
(
self
.
dim
)]
yvars
=
theta
[
3
*
(
self
.
dim
)
:
]
ansatz
=
0
for
i
in
range
(
0
,
self
.
dim
):
ansatz
+=
(
xvars
[
i
]
*
np
.
exp
(
1j
*
yvars
[
i
]))
*
np
.
exp
(
-
self
.
time
/
tvars
[
i
])
*
(
np
.
cos
(
wvars
[
i
]
*
self
.
time
)
-
1j
*
np
.
sin
(
wvars
[
i
]
*
self
.
time
))
# -1j to agree with SXS convention
return
ansatz
def
rd_model_wq
(
self
,
theta
):
"""
RD model parametrized with the quality factor q.
"""
assert
int
(
len
(
theta
)
/
4
)
==
self
.
dim
,
'
Please recheck your n and parameters
'
wvars
=
theta
[
:
(
self
.
dim
)]
qvars
=
theta
[(
self
.
dim
)
:
2
*
(
self
.
dim
)]
xvars
=
theta
[
2
*
(
self
.
dim
)
:
3
*
(
self
.
dim
)]
yvars
=
theta
[
3
*
(
self
.
dim
)
:
]
ansatz
=
0
for
i
in
range
(
0
,
self
.
dim
):
ansatz
+=
(
xvars
[
i
]
*
np
.
exp
(
1j
*
yvars
[
i
]))
*
np
.
exp
(
-
self
.
time
*
np
.
pi
*
wvars
[
i
]
/
qvars
[
i
])
*
(
np
.
cos
(
wvars
[
i
]
*
self
.
time
)
-
1j
*
np
.
sin
(
wvars
[
i
]
*
self
.
time
))
# -1j to agree with SXS convention
return
ansatz
def
rd_model_wq_fixed
(
self
,
theta
):
"""
RD model parametrized with the damping time tau and with the QNM spectrum fixd to GR.
"""
xvars
=
theta
[
:
(
self
.
dim
)]
yvars
=
theta
[(
self
.
dim
)
:
2
*
(
self
.
dim
)]
ansatz
=
0
for
i
in
range
(
0
,
self
.
dim
):
ansatz
+=
(
xvars
[
i
]
*
np
.
exp
(
1j
*
yvars
[
i
]))
*
np
.
exp
(
-
self
.
time
/
self
.
tau
[
i
])
*
(
np
.
cos
(
self
.
w
[
i
]
*
self
.
time
)
-
1j
*
np
.
sin
(
self
.
w
[
i
]
*
self
.
time
))
# -1j to agree with SXS convention
return
ansatz
def
rd_model_wq_m_a
(
self
,
theta
):
"""
RD model parametrized with the damping time tau and with the QNM spectrum fixd to GR. The QNM spectrum is given from the mass and spin.
"""
xvars
=
theta
[
:
(
self
.
dim
)]
yvars
=
theta
[(
self
.
dim
)
:
2
*
(
self
.
dim
)]
mass_vars
=
theta
[
-
2
]
spin_vars
=
theta
[
-
1
]
w_m_a
,
tau_m_a
=
QNM_spectrum
ansatz
=
0
for
i
in
range
(
0
,
dim
):
ansatz
+=
(
xvars
[
i
]
*
np
.
exp
(
1j
*
yvars
[
i
]))
*
np
.
exp
(
-
timesrd_final_tsh
/
tau_m_a
[
i
])
*
(
np
.
cos
(
w_m_a
[
i
]
*
timesrd_final_tsh
)
-
1j
*
np
.
sin
(
w_m_a
[
i
]
*
timesrd_final_tsh
))
# -1j to agree with SXS convention
return
ansatz
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