TypeIIbSED#
- class uvex_transients.models.supernovae.IIb.TypeIIbSED(**overrides: Parameter | Quantity | float | int)[source]#
Phenomenological Type IIb supernova SED.
Two superposed Bazin pulses times a cooling blackbody photosphere. Unlike
MoragShockCoolingSED/MoragShockCoolingBlackbodySED, which model only the early shock-cooling phase from first principles, this is a purely empirical light-curve shape intended to span a full Type IIb light curve. It fits real double- and single-peaked Type IIb events better than a single modulated pulse:\[L_\mathrm{bol}(t) = A_0\, \frac{\exp[-(t-t_0)/\tau_{\mathrm{fall},0}]}{1 + \exp[-(t-t_0)/\tau_{\mathrm{rise},0}]} + A_1\, \frac{\exp[-(t-t_1)/\tau_{\mathrm{fall},1}]}{1 + \exp[-(t-t_1)/\tau_{\mathrm{rise},1}]},\]delegated directly to
TwoComponentBazinLightcurve– see that class’s docstring for why an additive superposition of two independent pulses covers both single- and double-peaked light curves. The first component (centered on \(t_0\)) stands in for the early shock-cooling peak, the second (centered on \(t_1\)) for the radioactively powered main/nickel peak. The photospheric temperature follows the same single-power-law cooling law used elsewhere in this package (cooling_temperature_cgs()):\[T(t) = T_\mathrm{floor} + (T_0 - T_\mathrm{floor})\left(1 + \frac{t}{\tau_T}\right)^{-\alpha_T}.\]Parameters
Parameter
Symbol
Description
amplitude_0\(A_0\)
Luminosity normalization of the early, shock-cooling peak.
t0\(t_0\)
Characteristic transition time of the early peak.
rise_0\(\tau_{\mathrm{rise},0}\)
Logistic rise timescale of the early peak.
fall_0\(\tau_{\mathrm{fall},0}\)
Exponential decline timescale of the early peak.
amplitude_1\(A_1\)
Luminosity normalization of the main, radioactively powered peak.
t1\(t_1\)
Characteristic transition time of the main peak.
rise_1\(\tau_{\mathrm{rise},1}\)
Logistic rise timescale of the main peak.
fall_1\(\tau_{\mathrm{fall},1}\)
Exponential decline timescale of the main peak.
T0\(T_0\)
Photospheric temperature at t=0 (the T(t) -> T0 limit, not literally T at peak).
T_floor\(T_\mathrm{floor}\)
Asymptotic late-time photospheric temperature (T(t) -> T_floor as t -> infinity).
tau_T\(\tau_T\)
Photospheric cooling timescale.
alpha_T\(\alpha_T\)
Photospheric cooling power-law index.
Notes
amplitude_0– the early peak’s normalization – is uniform in \(\log_{10}(A_0/\mathrm{erg\,s^{-1}})\) between 39 and 43, spanning several decades from far fainter than the main peak up to brighter than it. This single prior covers both populations at once: draws where the early peak ends up negligible are effectively single-peaked Type IIb light curves, and draws where it is comparable to or exceeds the main peak are double-peaked – roughly a third of draws from the default priors below are double-peaked.t0andT_floorare held fixed; every other parameter is drawn from a broad Uniform (or, foramplitude_1/T0, Normal-in-log) prior over an order-of-magnitude-motivated range, not yet a fit to any specific real Type IIb event (compareTypeIIPSED, whose light-curve priors do come from fitting real SNe).Methods
as_astropy_model([x_type, y_type, y_kind, ...])Build an
Modelof thisSpectralModelfor a given parameter set.as_source_spectrum(t, *[, redshift, ...])Build a
SourceSpectrumgiving the observed flux at one fixed time \(t\).eval(nu, t, **parameters)Evaluate the spectral luminosity at the given frequency and time.
eval_bolometric(t, **parameters)Evaluate the bolometric luminosity at the given time.
eval_bolometric_cgs(t, **parameters)Bolometric luminosity, taking and returning plain cgs numbers.
eval_bolometric_log(t, **parameters)Natural log of the bolometric luminosity, given physical-unit inputs.
eval_bolometric_log_cgs(t, **parameters)Natural log of the bolometric luminosity, taking and returning plain cgs numbers.
eval_cgs(nu, t, **parameters)Spectral luminosity, taking and returning plain cgs numbers.
eval_from_arrays(nu, t, *parameters)Positional-argument form of
eval().eval_log(nu, t, **parameters)Natural log of the spectral luminosity, given physical-unit inputs.
eval_log_cgs(nu, t, **parameters)Natural log of the spectral luminosity, taking and returning plain cgs numbers.
eval_spectrum(nu, t, **parameters)Evaluate the normalized spectral shape at the given frequency and time.
eval_spectrum_cgs(nu, t, **parameters)Return the normalized spectral shape as plain cgs numbers; see
eval_log_cgs().eval_spectrum_log(nu, t, **parameters)Natural log of the normalized spectral shape, given physical-unit inputs.
eval_spectrum_log_cgs(nu, t, **parameters)Natural log of the normalized spectral shape, taking and returning plain cgs numbers.
flux(nu, t, *[, redshift, ...])Evaluate the observed flux density at the given frequency and time.
flux_band(nu, throughput, t, *[, redshift, ...])Evaluate the throughput-weighted mean observed flux density over a band.
flux_band_cgs(nu, throughput, t, redshift, ...)Band-averaged observed flux density as plain cgs numbers; see
flux_band_log_cgs().flux_band_log(nu, throughput, t, *[, ...])Natural log of the band-averaged observed flux density, given physical-unit inputs.
flux_band_log_cgs(nu, throughput, t, ...[, ...])Natural log of the throughput-weighted mean flux density over a band, plain cgs numbers.
flux_bolometric(t, *[, redshift, ...])Evaluate the observed bolometric flux at the given time.
flux_bolometric_cgs(t, redshift, ...)Observed bolometric flux, taking and returning plain cgs numbers.
flux_bolometric_log(t, *[, redshift, ...])Natural log of the observed bolometric flux, given physical-unit inputs.
flux_bolometric_log_cgs(t, redshift, ...)Natural log of the observed bolometric flux, taking and returning plain cgs numbers.
flux_cgs(nu, t, redshift, luminosity_distance, *)Observed flux density, taking and returning plain cgs numbers.
flux_log(nu, t, *[, redshift, ...])Natural log of the observed flux density, given physical-unit inputs.
flux_log_cgs(nu, t, redshift, ...[, ...])Natural log of the observed flux density, taking and returning plain cgs numbers.
get(k[,d])items()keys()mag(nu, t, *[, redshift, ...])Evaluate the apparent AB magnitude at the given frequency and time.
mag_band(nu, throughput, t, *[, redshift, ...])Evaluate the apparent AB magnitude of the band-averaged flux density.
mag_band_cgs(nu, throughput, t, redshift, ...)Apparent AB magnitude of the band-averaged flux density.
mag_bandpass(bandpass, t, *[, redshift, ...])Evaluate the apparent AB magnitude of the flux averaged over bandpass.
mag_cgs(nu, t, redshift, luminosity_distance, *)Apparent AB magnitude: \(m_\mathrm{AB} = -2.5 \log_{10}(F_\nu / F_{\mathrm{AB},0})\).
pack_params_to_arrays(**parameters)Convert a dict of parameter values into an ordered sequence.
sample_parameters([size, rng, parameters])Draw random samples of some or all of this model's parameters.
simulate(nu, t[, size, rng])Draw random parameter realizations and evaluate the model at the given frequency and time.
simulate_photometry(t, exptime, detector, ...)Simulate noisy synthetic photometry of this model at given time(s), against a real detector.
temperature(t, **parameters)\(T(t)\) in Kelvin.
unpack_params_from_arrays(*parameters)Convert an ordered sequence of parameter values back into a dict.
values()