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|
# Copyright (c) 2017-2018 Weitian LI <weitian@aaronly.me>
# MIT license
"""
Simulate (giant) radio halos originating from the recent merger
events, which generate cluster-wide turbulence and accelerate the
primary (i.e., fossil) relativistic electrons to high energies to
be synchrotron-bright. This *turbulence re-acceleration* model
is currently most widely accepted to explain the (giant) radio halos.
The simulation method is somewhat based on the statistical (Monte
Carlo) method proposed by [cassano2005]_, but with extensive
modifications and improvements.
References
----------
.. [brunetti2011]
Brunetti & Lazarian 2011, MNRAS, 410, 127
http://adsabs.harvard.edu/abs/2011MNRAS.410..127B
.. [cassano2005]
Cassano & Brunetti 2005, MNRAS, 357, 1313
http://adsabs.harvard.edu/abs/2005MNRAS.357.1313C
.. [cassano2006]
Cassano, Brunetti & Setti, 2006, MNRAS, 369, 1577
http://adsabs.harvard.edu/abs/2006MNRAS.369.1577C
.. [cassano2012]
Cassano et al. 2012, A&A, 548, A100
http://adsabs.harvard.edu/abs/2012A%26A...548A.100C
.. [donnert2013]
Donnert 2013, AN, 334, 615
http://adsabs.harvard.edu/abs/2013AN....334..515D
.. [donnert2014]
Donnert & Brunetti 2014, MNRAS, 443, 3564
http://adsabs.harvard.edu/abs/2014MNRAS.443.3564D
.. [hogg1999]
Hogg 1999, arXiv:astro-ph/9905116
http://adsabs.harvard.edu/abs/1999astro.ph..5116H
.. [miniati2015]
Miniati 2015, ApJ, 800, 60
http://adsabs.harvard.edu/abs/2015ApJ...800...60M
.. [pinzke2017]
Pinzke, Oh & Pfrommer 2017, MNRAS, 465, 4800
http://adsabs.harvard.edu/abs/2017MNRAS.465.4800P
.. [sarazin1999]
Sarazin 1999, ApJ, 520, 529
http://adsabs.harvard.edu/abs/1999ApJ...520..529S
"""
import logging
from functools import lru_cache
import numpy as np
from scipy import integrate
from . import helper
from .solver import FokkerPlanckSolver
from .emission import HaloEmission
from ...share import CONFIGS, COSMO
from ...utils.units import (Units as AU,
UnitConversions as AUC,
Constants as AC)
logger = logging.getLogger(__name__)
class RadioHalo:
"""
Simulate the radio halo properties for a galaxy cluster that is
experiencing an on-going merger or had a merger recently.
Description
-----------
1. Calculate the turbulence persistence time (tau_turb; ~<1 Gyr);
2. Calculate the diffusion coefficient (D_pp) from the systematic
acceleration timescale (tau_acc; ~0.1 Gyr). The acceleration
diffusion is assumed to have an action time ~ tau_turb (i.e.,
only during turbulence persistence), and then is disabled (i.e.,
only radiation and ionization losses later);
3. Assume the electrons are constantly injected and has a power-law
energy spectrum, determine the injection rate by further assuming
that the total injected electrons has energy of a fraction (eta_e)
of the ICM total thermal energy;
4. Set the electron density/spectrum be the accumulated electrons
injected during t_merger time, then evolve it for time_init period
considering only losses and constant injection, in order to derive
an approximately steady electron spectrum for following use;
5. Calculate the magnetic field from the cluster total mass (which
is assumed to be growth linearly from M_main to M_obs);
6. Calculate the energy losses for the coefficients of Fokker-Planck
equation;
7. Solve the Fokker-Planck equation to derive the relativistic
electron spectrum at t_obs (i.e., z_obs);
8. Calculate the synchrotron emissivity from the derived electron
spectrum.
Parameters
----------
M_obs : float
Cluster virial mass at the current observation (simulation end) time.
Unit: [Msun]
z_obs : float
Redshift of the current observation (simulation end) time.
M_main, M_sub : float
The main and sub cluster masses before the (major) merger.
Unit: [Msun]
z_merger : float
The redshift when the (major) merger begins.
Attributes
----------
fpsolver : `~FokkerPlanckSolver`
The solver instance to calculate the electron spectrum evolution.
radius : float
The halo radius
Unit: [kpc]
gamma : 1D float `~numpy.ndarray`
The Lorentz factors of the adopted logarithmic grid to solve the
equation.
_acceleration_disabled : bool
Whether the turbulence acceleration is intentionally disabled?
"""
# Component name
compID = "extragalactic/halos"
name = "giant radio halos"
def __init__(self, M_obs, z_obs, M_main, M_sub, z_merger,
configs=CONFIGS):
self.M_obs = M_obs
self.z_obs = z_obs
self.age_obs = COSMO.age(z_obs)
self.M_main = M_main
self.M_sub = M_sub
self.z_merger = z_merger
self.age_merger = COSMO.age(z_merger)
self._acceleration_disabled = False
self._set_configs(configs)
self._set_solver()
def _set_configs(self, configs):
comp = self.compID
self.configs = configs
self.f_acc = configs.getn(comp+"/f_acc")
self.f_radius = configs.getn(comp+"/f_radius")
self.zeta_ins = configs.getn(comp+"/zeta_ins")
self.eta_turb = configs.getn(comp+"/eta_turb")
self.eta_e = configs.getn(comp+"/eta_e")
self.x_cr = configs.getn(comp+"/x_cr")
self.gamma_min = configs.getn(comp+"/gamma_min")
self.gamma_max = configs.getn(comp+"/gamma_max")
self.gamma_np = configs.getn(comp+"/gamma_np")
self.buffer_np = configs.getn(comp+"/buffer_np")
if self.buffer_np == 0:
self.buffer_np = None
self.time_step = configs.getn(comp+"/time_step")
self.time_init = configs.getn(comp+"/time_init")
self.injection_index = configs.getn(comp+"/injection_index")
self.fiducial_freq = configs.getn(comp+"/fiducial_freq")
self.fiducial_factor = configs.getn(comp+"/fiducial_factor")
self.f_rc = configs.getn(comp+"/f_rc")
self.beta = configs.getn(comp+"/beta")
def _set_solver(self):
self.fpsolver = FokkerPlanckSolver(
xmin=self.gamma_min,
xmax=self.gamma_max,
x_np=self.gamma_np,
tstep=self.time_step,
f_advection=self.fp_advection,
f_diffusion=self.fp_diffusion,
f_injection=self.fp_injection,
buffer_np=self.buffer_np,
)
@property
@lru_cache()
def gamma(self):
"""
The logarithmic grid adopted for solving the equation.
"""
return self.fpsolver.x
@property
def age_begin(self):
"""
The cosmic time when the merger begins.
Unit: [Gyr]
"""
return self.age_merger
def time_turbulence(self, t=None):
"""
The duration that the compressive turbulence persists, which is
estimated as:
τ_turb ≅ L / v_impact = 2*R_turb / v_impact.
During this period, the merger-induced turbulence is regarded
to accelerate the relativistic electrons effectively.
Unit: [Gyr]
"""
t_merger = self._merger_time(t)
mass_main = self.mass_main(t=t_merger)
mass_sub = self.mass_sub(t=t_merger)
z_merger = COSMO.redshift(t_merger)
vi = helper.velocity_impact(mass_main, mass_sub, z_merger) # [km/s]
distance = 2 * self.radius_turbulence(t_merger)
uconv = AUC.kpc2km * AUC.s2Gyr # [s kpc/km] => [Gyr]
time = uconv * distance / vi # [Gyr]
return time
def mach_turbulence(self, t=None):
"""
The turbulence Mach number determined from its velocity dispersion.
"""
t_merger = self._merger_time(t)
cs = helper.speed_sound(self.kT(t_merger)) # [km/s]
v_turb = self._velocity_turb(t_merger) # [km/s]
return v_turb / cs
@property
def radius_virial_obs(self):
"""
The virial radius of the "current" cluster (``M_obs``) at ``z_obs``.
Unit: [kpc]
"""
return helper.radius_virial(mass=self.M_obs, z=self.z_obs)
@property
def radius(self):
"""
The estimated radius of the simulated radio halo.
Unit: [kpc]
"""
return self.radius_turbulence(self.age_merger) * self.f_radius
@lru_cache()
def radius_turbulence(self, t):
"""
The radius of the turbulence injection region, which is calculated
as the mean of the stripping radius of the sub-cluster and the core
radius of the main cluster.
Unit: [kpc]
"""
z = COSMO.redshift(t)
M_main = self.mass_main(t)
M_sub = self.mass_sub(t)
rs = helper.radius_stripping(M_main, M_sub, z, configs=self.configs)
R_vir = helper.radius_virial(M_main, z)
return (R_vir + rs) / 2
@property
def angular_radius(self):
"""
The angular radius of the radio halo.
Unit: [arcsec]
"""
DA = COSMO.DA(self.z_obs) * 1e3 # [Mpc] -> [kpc]
theta = self.radius / DA # [rad]
return theta * AUC.rad2arcsec
@property
def volume(self):
"""
The halo volume, calculated from the above radius.
Unit: [kpc^3]
"""
return (4*np.pi/3) * self.radius**3
@property
def B_obs(self):
"""
The magnetic field strength at the simulated observation
time (i.e., cluster mass of ``self.M_obs``), will be used
to calculate the synchrotron emissions.
Unit: [uG]
"""
return helper.magnetic_field(mass=self.M_obs, z=self.z_obs,
configs=self.configs)
@property
def kT_obs(self):
"""
The ICM mean temperature of the cluster at ``z_obs``.
Unit: [keV]
"""
return helper.kT_cluster(self.M_obs, z=self.z_obs,
configs=self.configs)
@lru_cache()
def kT(self, t):
"""
The ICM mean temperature of the merged cluster.
Unit: [keV]
"""
M_main = self.mass_main(t)
M_sub = self.mass_sub(t)
z = COSMO.redshift(t)
return helper.kT_cluster(mass=M_main+M_sub, z=z, configs=self.configs)
def tau_acceleration(self, t):
"""
Calculate the electron acceleration timescale due to turbulent
waves, which describes the turbulent acceleration efficiency.
The turbulent acceleration timescale has order of ~0.1 Gyr.
Here we consider the turbulence cascade mode through scattering
in the high-β ICM mediated by plasma instabilities (firehose,
mirror) rather than Coulomb scattering. Therefore, the fast modes
damp by TTD (transit time damping) on relativistic rather than
thermal particles, and the diffusion coefficient is given by:
D_pp = (4π * p^2 * ζ / X_cr / L_turb) * <v_turb^2>^2 / c_s^3
where:
ζ: efficiency factor for the effectiveness of plasma instabilities
X_cr: relative energy density of cosmic rays
L_turb: turbulence injection scale
v_turb: turbulence velocity dispersion
c_s: sound speed
Thus the acceleration timescale is:
τ_acc = p^2 / (4*D_pp)
= (X_cr * c_s^3 * L_turb) / (16π * ζ * <v_turb^2>^2)
WARNING
-------
Current test shows that a very large acceleration timescale (e.g.,
1000 or even larger) will cause problems (maybe due to some
limitations within the current calculation scheme), for example,
the energy losses don't seem to have effect in such cases, so the
derived initial electron spectrum is almost the same as the raw
input one, and the emissivity at medium/high frequencies even
decreases when the turbulence acceleration begins!
By carrying out some tests, the value of 10 [Gyr] is adopted for
the maximum acceleration timescale.
Parameters
----------
t : float, optional
The cosmic time when to determine the acceleration timescale.
Unit: [Gyr]
Returns
-------
tau : float
The acceleration timescale at the requested time.
Unit: [Gyr]
References
----------
* Ref.[pinzke2017],Eq.(37)
* Ref.[miniati2015],Eq.(29)
"""
# Maximum acceleration timescale when no turbulence acceleration
# NOTE: see the above WARNING!
tau_max = 10.0 # [Gyr]
if not self._is_turb_active(t):
return tau_max
t_merger = self._merger_time(t)
L_turb = 2 * self.radius_turbulence(t_merger) # [kpc]
cs = helper.speed_sound(self.kT(t_merger)) # [km/s]
v_turb = self._velocity_turb(t_merger) # [km/s]
tau = (self.x_cr * cs**3 * L_turb /
(16*np.pi * self.zeta_ins * v_turb**4)) # [s kpc/km]
tau *= AUC.s2Gyr * AUC.kpc2km # [Gyr]
tau *= self.f_acc # custom tune parameter
# Impose the maximum acceleration timescale
if tau > tau_max:
tau = tau_max
return tau
@property
@lru_cache()
def injection_rate(self):
"""
The constant electron injection rate assumed.
Unit: [cm^-3 Gyr^-1]
The injection rate is parametrized by assuming that the total
energy injected in the relativistic electrons during the cluster
life (e.g., ``age_obs`` here) is a fraction (``self.eta_e``)
of the total thermal energy of the cluster.
The electrons are assumed to be injected throughout the cluster
ICM/volume, i.e., do not restricted inside the halo volume.
Qe(γ) = Ke * γ^(-s),
int[ Qe(γ) γ me c^2 ]dγ * t_cluster = η_e * e_th
=>
Ke = [(s-2) * η_e * e_th * γ_min^(s-2) / (me * c^2 * t_cluster)]
References
----------
Ref.[cassano2005],Eqs.(31,32,33)
"""
s = self.injection_index
e_th = helper.density_energy_thermal(self.M_obs, self.z_obs,
configs=self.configs)
term1 = (s-2) * self.eta_e * e_th # [erg cm^-3]
term2 = self.gamma_min**(s-2)
term3 = AU.mec2 * self.age_obs # [erg Gyr]
Ke = term1 * term2 / term3 # [cm^-3 Gyr^-1]
return Ke
@property
def electron_spec_init(self):
"""
The electron spectrum at ``age_begin`` to be used as the initial
condition for the Fokker-Planck equation.
This initial electron spectrum is derived from the accumulated
electron spectrum injected throughout the ``age_begin`` period,
by solving the same Fokker-Planck equation, but only considering
energy losses and constant injection, evolving for a period of
``time_init`` in order to obtain an approximately steady electron
spectrum.
Units: [cm^-3]
"""
# Accumulated electrons constantly injected until ``age_begin``
n_inj = self.fp_injection(self.gamma)
n0_e = n_inj * (self.age_begin - self.time_init)
logger.debug("Deriving the initial electron spectrum ...")
self._acceleration_disabled = True
tstart = self.age_begin
tstop = self.age_begin + self.time_init
self.fpsolver.tstep = self.time_step * 3 # To save time
n_e = self.fpsolver.solve(u0=n0_e, tstart=tstart, tstop=tstop)
self._acceleration_disabled = False
self.fpsolver.tstep = self.time_step
return n_e
def calc_electron_spectrum(self, tstart=None, tstop=None, n0_e=None,
fiducial=False):
"""
Calculate the relativistic electron spectrum by solving the
Fokker-Planck equation.
Parameters
----------
tstart : float, optional
The (cosmic) time from when to solve the Fokker-Planck equation
for relativistic electrons evolution.
Default: ``self.age_begin``.
Unit: [Gyr]
tstop : float, optional
The (cosmic) time when to derive final relativistic electrons
spectrum for synchrotron emission calculations.
Default: ``self.age_obs``.
Unit: [Gyr]
n0_e : 1D `~numpy.ndarray`, optional
The initial electron spectrum (number distribution).
Default: ``self.electron_spec_init``
Unit: [cm^-3]
fiducial : bool
Whether to disable the turbulent acceleration and derive the
fiducial electron spectrum?
Default: ``False``
Returns
-------
n_e : float 1D `~numpy.ndarray`
The solved electron spectrum.
Unit: [cm^-3]
"""
if tstart is None:
tstart = self.age_begin
if tstop is None:
tstop = self.age_obs
if n0_e is None:
n0_e = self.electron_spec_init
if fiducial:
self._acceleration_disabled = True
self.fpsolver.tstep = self.time_step * 2 # To save time
logger.debug("Calculating the %s electron spectrum ..." %
("[fiducial]" if fiducial else ""))
n_e = self.fpsolver.solve(u0=n0_e, tstart=tstart, tstop=tstop)
self._acceleration_disabled = False
self.fpsolver.tstep = self.time_step
return n_e
def is_genuine(self, n_e):
"""
Check whether the radio halo is genuine/observable by comparing the
radio flux density to the fiducial value, which is calculated from
the fiducial electron spectrum derived with turbulent acceleration
turned off.
Parameters
----------
n_e : float 1D `~numpy.ndarray`
The finally derived electron spectrum.
Unit: [cm^-3]
Returns
-------
genuine : bool
"""
haloem = HaloEmission(gamma=self.gamma, n_e=n_e,
B=self.B_obs, radius=self.radius,
redshift=self.z_obs)
flux = haloem.calc_flux(self.fiducial_freq)
ne_fiducial = self.calc_electron_spectrum(fiducial=True)
haloem.n_e = ne_fiducial
flux_fiducial = haloem.calc_flux(self.fiducial_freq)
return flux >= flux_fiducial * self.fiducial_factor
def fp_injection(self, gamma, t=None):
"""
Electron injection (rate) term for the Fokker-Planck equation.
NOTE
----
The injected electrons are assumed to have a power-law spectrum
and a constant injection rate.
Qe(γ) = Ke * γ^(-s),
Ke: constant injection rate
Parameters
----------
gamma : float, or float 1D `~numpy.ndarray`
Lorentz factors of electrons
t : None
Currently a constant injection rate is assumed, therefore
this parameter is not used. Keep it for the consistency
with other functions.
Returns
-------
Qe : float, or float 1D `~numpy.ndarray`
Current electron injection rate at specified energies (gamma).
Unit: [cm^-3 Gyr^-1]
References
----------
Ref.[cassano2005],Eqs.(31,32,33)
"""
Ke = self.injection_rate # [cm^-3 Gyr^-1]
Qe = Ke * gamma**(-self.injection_index)
return Qe
def fp_diffusion(self, gamma, t):
"""
Diffusion term/coefficient for the Fokker-Planck equation.
The diffusion is directly related to the electron acceleration
which is described by the ``tau_acc`` acceleration timescale
parameter.
WARNING
-------
A zero diffusion coefficient may lead to unstable/wrong results,
since it is not properly taken care of by the solver.
Parameters
----------
gamma : float, or float 1D `~numpy.ndarray`
The Lorentz factors of electrons
t : float
Current (cosmic) time when solving the equation
Unit: [Gyr]
Returns
-------
diffusion : float, or float 1D `~numpy.ndarray`
Diffusion coefficients
Unit: [Gyr^-1]
References
----------
Ref.[donnert2013],Eq.(15)
"""
tau_acc = self.tau_acceleration(t)
gamma = np.asarray(gamma)
diffusion = gamma**2 / 4 / tau_acc
return diffusion
def fp_advection(self, gamma, t):
"""
Advection term/coefficient for the Fokker-Planck equation,
which describes a systematic tendency for upward or downward
drift of particles.
This term is also called the "generalized cooling function"
by [donnert2014], which includes all relevant energy loss
functions and the energy gain function due to turbulence.
Returns
-------
advection : float, or float 1D `~numpy.ndarray`
Advection coefficient.
Unit: [Gyr^-1]
"""
if self._is_turb_active(t):
# Turbulence acceleration and beyond
advection = (abs(self._energy_loss(gamma, t)) -
(self.fp_diffusion(gamma, t) * 2 / gamma))
else:
# To derive the initial electron spectrum
advection = abs(self._energy_loss(gamma, self.age_begin))
return advection
def _merger_time(self, t=None):
"""
The (cosmic) time when the merger begins.
Unit: [Gyr]
"""
return self.age_merger
def mass_merged(self, t=None):
"""
The mass of the merged cluster.
Unit: [Msun]
"""
return self.M_main + self.M_sub
def mass_sub(self, t=None):
"""
The mass of the sub cluster.
Unit: [Msun]
"""
return self.M_sub
def mass_main(self, t):
"""
Calculate the main cluster mass at the given (cosmic) time.
Unit: [Msun]
NOTE
----
Since we currently only consider the last major merger event,
there may be a long time between ``z_merger`` and ``z_obs``.
So we assume that the main cluster grows linearly in time from
(M_main, z_merger) to (M_obs, z_obs).
"""
t0 = self.age_begin
rate = (self.M_obs - self.M_main) / (self.age_obs - t0)
mass = rate * (t - t0) + self.M_main # [Msun]
return mass
def magnetic_field(self, t):
"""
Calculate the mean magnetic field strength of the main cluster mass
at the given (cosmic) time.
Unit: [uG]
"""
z = COSMO.redshift(t)
mass = self.mass_main(t) # [Msun]
return helper.magnetic_field(mass=mass, z=z, configs=self.configs)
@lru_cache()
def _gas_density_profile_f(self, t):
"""
The gas density profile of the merged cluster.
Returns
-------
f(r) : function
A function that calculates the gas density of unit [Msun/kpc^3].
"""
z = COSMO.redshift(t)
M_main = self.mass_main(t)
M_sub = self.mass_sub(t)
return helper.calc_gas_density_profile(mass=M_main+M_sub, z=z,
f_rc=self.f_rc, beta=self.beta)
@lru_cache()
def _velocity_turb(self, t):
"""
Calculate the turbulence velocity dispersion (i.e., turbulence Mach
number).
NOTE
----
During the merger, a fraction of the merger kinetic energy is
transferred into the turbulence within the region of radius R_turb.
Then estimate the turbulence velocity dispersion from its energy.
Merger energy:
E_merger ≅ 0.5 * f_gas * M_sub * v_vir^2
v_vir = sqrt(G*M_main / R_vir)
Turbulence energy:
E_turb ≅ η_turb * E_merger
≅ 0.5 * M_turb * <v_turb^2>
=> Velocity dispersion:
<v_turb^2> ≅ v_vir^2 * η_turb*f_gas * (M_sub/M_turb)
where:
M_turb = int_0^R_turb ρ_gas(r)*4ᴨ*r^2 dr
Returns
-------
v_turb : float
The turbulence velocity dispersion
Unit: [km/s]
"""
z = COSMO.redshift(t)
rho_gas_f = self._gas_density_profile_f(t)
R_turb = self.radius_turbulence(t) # [kpc]
M_turb = 4*np.pi * integrate.quad(lambda r: rho_gas_f(r) * r**2,
a=0, b=R_turb)[0] # [Msun]
M_main = self.mass_main(t)
M_sub = self.mass_sub(t)
R_vir = helper.radius_virial(M_main+M_sub, z) # [kpc]
R_vir *= AUC.kpc2cm # [cm]
v2_vir = (AC.G * M_main*AUC.Msun2g / R_vir) * AUC.cm2km**2
v2_turb = v2_vir * self.eta_turb*COSMO.baryon_fraction * (M_sub/M_turb)
return np.sqrt(v2_turb)
def _is_turb_active(self, t):
"""
Is the turbulence acceleration is active at the given time?
"""
if self._acceleration_disabled:
return False
t_merger = self._merger_time(t)
t_turb = self.time_turbulence(t_merger)
return (t >= t_merger) and (t <= t_merger + t_turb)
def _energy_loss(self, gamma, t):
"""
Energy loss mechanisms:
* inverse Compton scattering off the CMB photons
* synchrotron radiation
* Coulomb collisions
Reference: Ref.[sarazin1999],Eqs.(6,7,9)
Parameters
----------
gamma : float, or float 1D `~numpy.ndarray`
The Lorentz factors of electrons
t : float
The cosmic time/age
Unit: [Gyr]
Returns
-------
loss : float, or float 1D `~numpy.ndarray`
The energy loss rates
Unit: [Gyr^-1]
"""
gamma = np.asarray(gamma)
z = COSMO.redshift(t)
B = self.magnetic_field(t) # [uG]
mass = self.mass_main(t)
n_th = helper.density_number_thermal(mass, z) # [cm^-3]
loss_ic = -4.32e-4 * gamma**2 * (1+z)**4
loss_syn = -4.10e-5 * gamma**2 * B**2
loss_coul = -3.79e4 * n_th * (1 + np.log(gamma/n_th) / 75)
return loss_ic + loss_syn + loss_coul
class RadioHaloAM(RadioHalo):
"""
Simulate the radio halo properties for a galaxy cluster with all its
on-going merger and past merger events taken into account.
Parameters
----------
M_obs : float
Cluster virial mass at the observation (simulation end) time.
Unit: [Msun]
z_obs : float
Redshift of the observation (simulation end) time.
M_main, M_sub : list[float]
List of main and sub cluster masses at each merger event,
from current to earlier time.
Unit: [Msun]
z_merger : list[float]
The redshifts at each merger event, from small to large.
merger_num : int
Number of merger events traced for the cluster.
"""
def __init__(self, M_obs, z_obs, M_main, M_sub, z_merger,
merger_num, configs=CONFIGS):
self.merger_num = merger_num
M_main = np.asarray(M_main[:merger_num])
M_sub = np.asarray(M_sub[:merger_num])
z_merger = np.asarray(z_merger[:merger_num])
super().__init__(M_obs=M_obs, z_obs=z_obs,
M_main=M_main, M_sub=M_sub,
z_merger=z_merger, configs=configs)
@property
def age_begin(self):
"""
The cosmic time when the merger begins, i.e., the earliest merger.
Unit: [Gyr]
"""
return self.age_merger[-1]
def _merger_idx(self, t):
"""
Determine the index of the merger event within which the given
time is located, i.e.:
age_merger[idx-1] >= t > age_merger[idx]
"""
return (self.age_merger > t).sum()
def _merger_time(self, t):
"""
Determine the beginning time of the merger event within which
the given time is located.
"""
idx = self._merger_idx(t)
return self.age_merger[idx]
def _merger(self, t):
"""
Return the merger event at cosmic time ``t``.
"""
idx = self._merger_idx(t)
return {
"idx": idx,
"M_main": self.M_main[idx],
"M_sub": self.M_sub[idx],
"z": self.z_merger[idx],
"age": self.age_merger[idx],
}
def mass_merged(self, t):
"""
The mass of merged cluster at the given (cosmic) time.
Unit: [Msun]
"""
if t >= self.age_obs:
return self.M_obs
else:
merger = self._merger(t)
return (merger["M_main"] + merger["M_sub"])
def mass_sub(self, t):
"""
The mass of the sub cluster at the given (cosmic) time.
Unit: [Msun]
"""
merger = self._merger(t)
return merger["M_sub"]
def mass_main(self, t):
"""
Calculate the main cluster mass at the given (cosmic) time.
Parameters
----------
t : float
The (cosmic) time/age.
Unit: [Gyr]
Returns
-------
mass : float
The mass of the main cluster.
Unit: [Msun]
"""
merger1 = self._merger(t)
idx1 = merger1["idx"]
mass1 = merger1["M_main"]
t1 = merger1["age"]
if idx1 == 0:
mass0 = self.M_obs
t0 = self.age_obs
else:
idx0 = idx1 - 1
mass0 = self.M_main[idx0]
t0 = self.age_merger[idx0]
rate = (mass0 - mass1) / (t0 - t1)
return (mass1 + rate * (t - t1))
@property
def time_turbulence_avg(self):
"""
Calculate the time-averaged turbulence acceleration active time
within the period from ``age_begin`` to ``age_obs``.
Unit: [Gyr]
"""
dt = self.time_step
xt = np.arange(self.age_begin, self.age_obs+dt/2, step=dt)
t_turb = np.array([self.time_turbulence(t) for t in xt])
return np.sum(t_turb * dt) / (len(xt) * dt)
@property
def mach_turbulence_avg(self):
"""
Calculate the time-averaged turbulence Mach number within the
period from ``age_begin`` to ``age_obs``.
"""
dt = self.time_step
xt = np.arange(self.age_begin, self.age_obs+dt/2, step=dt)
mach = np.array([self.mach_turbulence(t) for t in xt])
return np.sum(mach * dt) / (len(xt) * dt)
@property
def tau_acceleration_avg(self):
"""
Calculate the time-averaged turbulence acceleration timescale
(i.e., efficiency) within the period from ``age_begin`` to
``age_obs``.
Unit: [Gyr]
"""
dt = self.time_step
xt = np.arange(self.age_begin, self.age_obs+dt/2, step=dt)
tau = np.array([self.tau_acceleration(t) for t in xt])
return np.sum(tau * dt) / (len(xt) * dt)
@property
def time_acceleration_fraction(self):
"""
Calculate the fraction of time within the period from
``age_begin`` to ``age_obs`` that the turbulence acceleration
is active.
"""
dt = self.fpsolver.tstep
xt = np.arange(self.age_begin, self.age_obs+dt/2, step=dt)
active = np.array([self._is_turb_active(t) for t in xt], dtype=int)
return active.mean()
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