Empirically, Type Ia supernovae are the most useful, precise, and mature tools for determining astronomical distances. Acting as calibrated candles they revealed the presence of dark energy and are being used to measure its properties. However, the nature of the Type Ia explosion, and the progenitors involved, have remained elusive, even after seven decades of research. But now, new large surveys are bringing about a paradigm shift—we can finally compare samples of hundreds of supernovae to isolate critical variables. As a result of this, and advances in modelling, breakthroughs in understanding all aspects of these supernovae are finally starting to happen.
Guest stars (who could have imagined they were distant stellar explosions?) have been surprising humans for at least 950 years, but probably far longer. They amazed and confounded the likes of Tycho, Kepler and Galileo, to name a few. But it was not until the separation of these events into novae and supernovae by Baade and Zwicky that progress understanding them began in earnest1. This process of splitting a diverse group into related subsamples to yield insights into their origin would be repeated again and again over the years, first by Minkowski when he separated supernovae of Type I (no hydrogen in their spectra) from Type II (have hydrogen)2, and then by Elias et al. when they determined that Type Ia supernovae (SNe Ia) were distinct3. We now define Type Ia supernovae as those without hydrogen or helium in their spectra, but with strong ionized silicon (SiII), which has observed absorption lines at 6,150, 5,800 and 4,000 Å (ref. 4). The progenitor of a Type Ia supernova has never been seen, but the consensus is that they are the result of the thermonuclear explosion of a degenerate carbon-oxygen white dwarf (WD) star5 gaining mass in a binary system6, in contrast to the other types of supernovae, which are thought to result from the collapse of the core of a massive star. Much about them remains unknown—the process of categorizing and trying to understand them continues.
As distance indicators, SNe Ia are capable of better than 6% precision in distance after empirical corrections are made for their lightcurve shape and colour. Just over a decade ago, they were used to deliver perhaps the most shocking scientific discovery in the last half-century: the expansion of the universe is not slowing, but is, instead, accelerating7,8. The 'dark energy' required to power this acceleration is prodigious, and, indeed, must be the dominant constituent of the universe by a factor of 17 over normal matter, and 3 over dark matter (which, despite the name, is probably unrelated). But, because dark energy is so dilute (1 m3 contains the energy equivalent to a few atoms of hydrogen), its effects can only be seen on vast scales. We must compare supernovae across ∼10 Gyr of cosmic time, during which stars and galaxies have undergone substantial evolution. Therefore, it is critical to understand supernovae, if they are to be relied on as the primary distance probe in astrophysics.
We begin by reviewing SN Ia lightcurves and spectra, and their use in cosmology. This has been refined to the point that SNe Ia are now sensitive to subtle, systematic effects. However, many of these are being addressed by comparing large subsamples of hundreds of SNe Ia, which has become possible for the first time only in the last few years.
New multidimensional simulations are revealing once-elusive details of the explosion, such as how asymmetry contributes to the diversity seen in SNe Ia. Advances in understanding progenitors have been proceeding apace, led by new observations. The properties of SNe Ia are being correlated with the stellar populations in their host galaxies, yielding real progenitor constraints. Dramatic new discoveries, like supernovae that appear to require a progenitor above the Chandrasekhar mass, are challenging pre-existing theories. Evidence has been mounting that the long-favoured scenario of accretion from a main sequence or red giant companion star cannot account for all SNe Ia. Instead, the WD merger and even the sub-Chandrasekhar mass explosion models have been experiencing a revival.
Finally, we conclude that empirical SN Ia cosmology remains solid, but is being continually refined by taking into account ever-more-subtle effects and new knowledge. But our understanding of the progenitors of SNe Ia and the explosion process may be undergoing an evolution, as the data from vast new surveys with thousands of supernovae are becoming available.
Lightcurves and spectra
In a SN Ia, a wave of thermonuclear fusion rips through a degenerate WD star, synthesizing iron-peak elements (Ni, Co, Fe) in the dense inner regions, intermediate mass elements (Si, S, Ca, Mg, O) where burning is incomplete, and sometimes leaving unburned material (C,O) near the outer layers9. Though the explosion provides the kinetic energy of the SN Ia and unbinds the WD, this is not what we see as the supernova. The lightcurve is powered by the radioactive decay of 56Ni (half-life 6.1 days) to 56Co, and ultimately to 56Fe (half-life 77 days). Gamma rays produced in the decays are thermalized, and at peak light ∼85% of the light output of the SN Ia is in the optical, peaking at 4,000 Å, with the remainder mostly radiated in the near-ultraviolet and the near-infrared10.
Figure 1 shows the quasi-bolometric (ultraviolet-optical-infrared) lightcurve evolution of a typical SN Ia, SN 2003du (ref. 11), along with representative spectra. SNe Ia rise to maximum light over ∼13–23 days in the B-band, with a typical rise time of about 17.5 days12. Initially, the time for photons to diffuse out of the dense ejecta is high, so that the rate of deposition of energy by radioactive decay exceeds the energy radiated by the SN. Thus, at early times, spectra show only absorption lines probing the outer layers of the SN. As the SN expands and thins, the light-emitting region (the photosphere) recedes (in mass or velocity coordinates), and spectra start to probe deeper layers. Eventually, the ejecta reach a point where the rate of energy deposition by radioactive decay is equal to the radiated luminosity of the SN, and the SN starts to decline in luminosity13. Around, or after maximum light, spectra show P-Cygni profiles—emission at the rest wavelength (initially weak), and blueshifted absorption. Weeks after maximum light, the spectra start becoming dominated by scattering from permitted lines (at least in the blue)14 and ultimately become dominated by emission features as the ejecta start to become optically thin, and the SN makes the transition from the photospheric to the nebular phase. At late times (hundreds of days), gamma rays can freely escape, but positrons may be trapped15, and the lightcurve slope may match the slope expected from the decay of 56Co, or can be steeper than this in the case of incomplete trapping16. Late time spectra are dominated by emission lines from iron-peak elements, synthesized in the deepest regions where the WD was densest.
Dark energy is often characterized by its ratio of pressure to density, that is, its equation of state, w=P/ρc2 (Fig. 2). If a is an arbitrary length scale in the universe, then the density of some component of the universe evolves as ρ∝a−3(1+w). Normal matter has w=0; it dilutes with volume as space expands. If dark energy has an equation of state w=−1, corresponding to Einstein's cosmological constant, Λ, then it has the strange property that the energy density does not dilute as the universe expands; it must be a property of the vacuum. Other possibilities exist: if w<−1 the dark energy density is ever growing, and will ultimately result in a 'big rip,' destroying galaxies and even subatomic particles. However, w can also be a scalar field with w>−1 (generally known as quintessence), and the value of w can evolve over time.
Measurements of 〈w〉 or w(z) are obtained by building a map of the history of the expansion of the universe using SNe Ia as standardized candles. SNe Ia can show a factor of ten or more difference in peak luminosity, but the luminosity is correlated with the time it takes the supernova to rise and fall in brightness17. Therefore, the width of the lightcurve is measured and used to correct the peak luminosity. Common parametrizations include the 'stretch factor8', s, proportional to lightcurve width, or Δm15(B), the number of magnitudes the B-band lightcurve falls in 15 days after peak brightness, inversely proportional to lightcurve width17. A correction must also be made for colour, since redder SNe are dimmer, both intrinsically, and due to dust18,19. Various techniques are used to determine these parameters by fitting lightcurve models to the data, but leading fitters include MLCS2k2 (ref. 20), SALT2 (ref. 21), and SiFTO22.
To determine cosmological parameters, an observed Hubble diagram (distance versus redshift) is constructed, and cosmological parameters are varied in a model that is fitted to the data. If we express distances as magnitudes, as a distance estimator, we can use23:
where is the peak magnitude of the SN in the B-band (the blue filter where the SN is brightest), s is the lightcurve stretch, c is the colour of the SN (a linear combination of U−B and B−V, relative to some reference colour22,23), α is the slope of the stretch-luminosity relation, β is the slope of the colour-luminosity relation, and M is a measure of the absolute magnitude of the SN combined with the Hubble constant. Note that since relative magnitudes are used, neither the absolute magnitude of the SN, nor the value of the Hubble constant must be known. , s, and c are measured from a fit to each SN lightcurve, while M, α, and β are constants determined from the overall cosmological fit.
Cosmological studies using SNe Ia, have reached a point where over most redshift ranges systematic errors (those that affect many measurements simultaneously in a correlated way) dominate statistical errors (that is, those that are reduced by )24,25,26—see Figure 2. Many systematic uncertainties can be lowered with new methods, improved statistics, by comparing subsamples of supernovae, or breakthroughs in understanding. The primary systematic uncertainties affecting SNe Ia are survey-dependent, but there is general consensus that the largest are calibration to the historic Landolt photometric system, treatment of the ultraviolet, reddening due to dust, the differences supernovae show with respect to environment, and the possible evolution of SNe with redshift. See Table 1 for a summary of recent SN Ia constraints on 〈w〉 and dominant systematic uncertainties.
As supernovae are observed at high redshift, the region of the spectrum seen through a given broadband filter changes. A correction must be made for this, the k-correction, which requires knowledge of the spectral energy distribution of an average supernova27, and precise knowledge of the filter transmission curves and calibration system used for each supernova. Unfortunately, many historical low-redshift supernovae were transformed to the Landolt photometric standard system, which is poorly understood and no longer reproducible, as the filter and instrument transmission curves used to establish it are not known to modern precision and no longer exist. The fact that the low-z SN sample is on the Landolt system has forced many high redshift surveys to transform to it, incurring a systematic uncertainty in zero points and colour terms23. These systematic uncertainties will be reduced once a large new low-redshift sample of SNe is assembled, calibrated onto a new system (for example, Sloan).
At redshifts above z∼0.2, the restframe U-band and ultraviolet is redshifted into the optical region of the spectrum. Unfortunately, there is a great deal of scatter in restframe U observations. Some surveys rely heavily on the restframe U, so uncertainties from this region can translate into dominant systematic uncertainties24. In fact, differences seen between the distances determined by different lightcurve fitters, such as MLCS2k2 (ref. 20), SALT2 (ref. 21), and SiFTO22 boil down largely to the way they treat the restframe U-band.
There are two possibilities for U-band uncertainty: (1) SNe intrinsically show more variation in U28, and/or (2) the U-band is poorly calibrated. The Supernova Legacy Survey (SNLS) has shown that when longer-wavelength high-redshift observations from a well-calibrated single survey are k-corrected to restframe U-band, the dispersion is more than three times lower than for low-redshift data where the U-band is observed directly23. Therefore, discrepancies are most likely due to problematic low-redshift observations where many factors conspire to make U observations difficult, including atmospheric variation, extinction, nonstandard filters, and poor calibrators29. This systematics can be dealt with by building a new, better-calibrated low-redshift sample, and possibly by avoiding the restframe U-band.
Lightcurve fitters must correct for the fact that redder supernovae are dimmer. This is due to a combination of an intrinsic colour-luminosity relation (faint supernovae are intrinsically red18), and reddening due to dust. Although there is consensus that the two effects ought to be corrected for independently, there is disagreement over whether this can be practically achieved given current data limitations.
MLCS2k2 attempts to separate intrinsic and dust reddening and make different corrections for each20. SALT2 and SiFTO work under the assumption that it is difficult or impossible to separate the effects of dust and intrinsic reddening, so they make an empirical reddening correction by solving for the slope of the colour-luminosity relation, β. If this reddening were only due to dust, then β=RB=RV+1. For Milky Way dust, RB=4.1. However, as shown in Figure 3, shallower slopes are found for β. This may result from the conflation of dust and intrinsic SN reddening, and would indicate that the intrinsic SN Ia reddening-luminosity relation has a shallower slope than the dust relation. However, since the lightcurve shape-luminosity relation is already factored out in this method23; it means there must be a component of intrinsic colour that does not correlate with lightcurve shape19. An alternative is that the dust along the line of sight to SNe Ia is intrinsically different, or that scattering effects in the circumstellar environment result in a different apparent reddening law30.
One way to separate the intrinsic/dust reddening degeneracy is through infrared observations, where the effects of dust are minimized. Infrared observations have shown that many SNe seem to have a sub-Milky Way value of RV, sometimes as low as RV=1.531,32. There are hints that lightly reddened SNe may have an RV close to that in the Milky Way, whereas heavily extincted SNe Ia have lower values (Fig. 3)33. However, this is opposite to earlier findings from optical data34, and the small sample size makes it difficult to draw reliable conclusions.
There are indications that supernovae with higher velocity ejecta have lower inferred RV values35 (Fig. 3). As the colour is correlated with physical SN features, this may indicate that sometimes an intrinsic colour difference in SNe is wrongly ascribed to dust reddening (though this can be mitigated by making a colour cut), or perhaps that there are different progenitor scenarios, with different circumstellar dust-scattering properties, that produce SNe with different velocities.
Various authors have exploited the low sensitivity to dust in the infrared to make infrared Hubble diagrams. This is doubly attractive, because SNe Ia intrinsically show reduced scatter in the infrared36—in the H-band SNe Ia have an r.m.s dispersion of only 0.15 mag without correction for lightcurve shape or colour37. This is theoretically expected, in part because less luminous SNe are cooler and radiate a larger fraction of their luminosity in the infrared38. Although heroic attempts have been made to produce high redshift infrared Hubble diagrams of SNe Ia39, the massive amount of observing time required, and the fact that the restframe infrared is redshifted to even longer wavelengths, has made serious cosmological constraints from this method elusive.
Populations and evolution
Even before SNe Ia were used for cosmology, it was known that the most luminous SNe Ia (those with the broadest lightcurves), occur only in late-type galaxies40. Likewise, subluminous SNe Ia are preferentially found in galaxies with a significant old population41. SN lightcurve width and luminosity have now been shown to correlate with host galaxy star formation rate, galaxy mass, and metallicity10,42,43,44.
Because star formation increases by a factor of 10 up to redshift 1.5, and bright, broad-lightcurve supernovae favour star forming hosts, it is expected that the mix of supernovae will change with redshift. Indeed, it has been shown that supernovae at z=1 are intrinsically ∼12% more luminous than local SNe Ia45. The spectra of high-redshift supernovae also show fewer intermediate mass elements, consistent with the idea that they make more iron-peak elements to power their luminosity46. A changing mix of supernovae with redshift is not necessarily problematic for cosmology, if lightcurve shape and colour corrections allow all supernovae to be corrected to the same absolute magnitude. Unfortunately, they do not44,47—as is shown in Figure 4, supernovae in high- and low-mass galaxies each correct to an absolute magnitude different by 0.08±0.02 mag. This trend is also present (though weaker), if SNe are split by host star formation rate, or metallicity. If not corrected, this can lead to a ∼0.04 systematic error in w44. Therefore, aside from colour and lightcurve shape, a third correction, one for host galaxy properties, must be applied to SNe Ia to avoid systematic residuals with respect to the Hubble diagram.
The physical origins for the differences in supernova properties in spiral and elliptical galaxies have been elusive40,41,42—are they related to progenitor age, metallicity or entirely different progenitors? The recently discovered trend that galaxy mass may have the most significant role in determining SN properties10,44 would seem to implicate metallicity, as higher mass galaxies retain more metals in their deeper potential wells. Still, the age-metallicity degeneracy precludes firm conclusions on this evidence alone48. Theoretically, there are reasons that high metallicity progenitors should produce subluminous SNe Ia49: increased 22Ne in high metallicity WDs provides more neutrons during the nucleosynthesis that occurs during the explosion, and thus yields more stable 58Ni and less of the radioactive lightcurve-powering 56Ni. However, this has only a ∼10% effect on SN luminosity, perhaps indicating that an as-yet unknown metallicity effect or progenitor age is the more important in controlling 56Ni yield and SN luminosity10.
If progenitor age is the predominant effect controlling SN luminosity, this has implications for SN progenitors. In the single degenerate scenario the time to explosion is controlled by the main sequence lifetime of the secondary (mass-transferring) star, as the mass transfer timescale is thought to be negligible, only ∼107 years. Therefore, in this model, the delay time is a direct indication of the secondary star's mass. In the double degenerate (DD) model, where two WDs merge, gravitational wave radiation ultimately brings the stars together, but they may have a head start if they have drawn closer, by orbiting in the common envelope of one of the stars as it is evolving. Age may still have a role in determining luminosity, because at early times the only WDs will be massive ones derived from the more massive stars.
Explosion theory and observational constraints
In what might be called the standard model for a SN Ia, a carbon-oxygen (CO) WD accretes matter until it compresses to the point that carbon is ignited just before the Chandrasekhar limit (note that the common misconception that the WD goes over the Chandrasekhar limit is wrong—this would lead to collapse to a neutron star). The evidence that the exploding star is a WD is strong, albeit circumstantial: neither hydrogen nor helium is seen in the spectrum of a SN Ia50, SNe Ia can happen long after star formation has ceased, the explosive process may implicate degenerate matter, the energy obtained by the thermonuclear burning of a WD minus the binding energy roughly matches the kinetic energy of SNe Ia, and simulations of the process have been successful at reproducing SN Ia lightcurves and spectra9,51,52.
The WD may have a 'simmering' phase of order a thousand years following unstable carbon ignition, where thermonuclear runaway is prevented by convection53. Ultimately, however, explosive burning is ignited and the WD is incinerated in seconds.
If a WD near the Chandrasekhar mass is detonated (that is, the burning occurs supersonically), then the WD burns at such a high density that the fusion products consist almost entirely of iron-peak elements54. This does not match the spectra or lightcurves of SNe Ia. A deflagration (subsonic burning), on the other hand, gives the SN time to pre-expand. Burning at a lower density can produce intermediate mass elements and reproduce many of the observational features of SNe Ia51. However, pure deflagrations fail to produce the high velocity material (Fig. 1) that seems to be nearly ubiquitous in SNe Ia in the outer layers55, and in two- and three dimensional simulations they leave too much carbon and oxygen unburned56. Therefore, the consensus is that in a Chandrasekhar mass explosion, the flame must start out subsonically, but at some point become supersonic52. Though the physics remains poorly understood, models that start as a deflagration but impose a transition to a detonation under certain conditions have been successful at reproducing normal SN Ia lightcurves and spectra, and even lightcurve width-luminosity relations and metallicity effects57. Explosions dominated by deflagration produce more intermediate mass elements (dimmer SNe Ia), while those dominated by detonation produce brighter and more 56Ni-rich SNe Ia (Fig. 5)57.
It is possible to gain insight into the explosion physics with spectropolarimetry or other techniques that reveal asphericity—recent work indicates that some of the dispersion in SN properties results from broken symmetries57. SN asymmetry can be measured via spectropolarimetry, since asymmetric electron scattering leads to polarization vectors that do not cancel. Most normal SNe Ia are found to be spherically symmetric58,59. The first convincing evidence for significant deviations from spherical symmetry was seen in a subluminous SN Ia60, which may make sense if they are deflagration-dominated. However, supernovae with high velocity features often show even stronger spectropolarimetric signatures of asymmetry, possibly due to clumpy ejecta58,61.
Strangely, SNe Ia whose spectroscopic features start off with high velocity and evolve rapidly, often show nebular lines that appear redshifted, while SNe Ia with slower velocity evolution show blueshifted nebular lines62. This probably indicates asymmetry in the explosion, in qualitative agreement with models where a deflagration burns off-center, and is followed by a detonation.
The progenitor question
Even if there is agreement that the primary star in a SN Ia is a WD, the identity of the secondary star in the binary system is uncertain. There are three broad classes of models: (1) single degenerate6, where the companion is a main sequence or red giant star that loses mass via either Roche lobe overflow, or a wind (symbiotic star), (2) DD, where two WDs merge and explode63,64, and (3) sub-Chandra65, where a layer of helium builds up on the surface of a WD below the Chandrasekhar mass until it detonates.
In the single degenerate model, a WD ignites carbon burning, causing it to explode, by accreting matter from a nondegenerate companion to near the Chandra mass. Since CO WDs are thought to start no larger than ∼1–1.2 solar masses, a significant amount of accretion from a secondary star is required. However, hydrogen must be accreted at a rate between 10−7 and 10−8 M⊙ yr−1 to steadily burn to carbon or oxygen on the surface of the WD66. If it accretes faster, it will form a red giant-like envelope. Slower accretion is thought to lead to the build up of matter that results in novae, and mass being lost from the system. The apparently required steady burning generates supersoft X-rays, and as a result, systems in this phase of their evolution are observable as supersoft X-ray sources67. However, the observed rates of supersoft sources in the Milky Way and external galaxies can only account for ∼5% of the SN Ia rate68,69, possibly favouring the DD model, although many of these systems ought to pass through a supersoft phase as well70.
White dwarf mergers
In the DD scenario, two WDs merge to achieve the Chandra mass63,64. The less massive WD is disrupted into a disk that will eventually accrete onto the more massive WD71. In this case, carbon may be ignited on the surface of the more massive WD during the accretion process, resulting in non-explosive carbon burning, converting the star to an O-Ne WD. This should ultimately undergo accretion induced collapse to a neutron star rather than producing a SN Ia72, though it may be possible to avoid this fate under certain conditions73. The simulated merger of two equal mass 0.9 M⊙ WDs has been shown to lead to a SN Ia, although it was subluminous74, due to the low central density of a 0.9 M⊙ WD. More massive equal-mass mergers may produce normal, or even overluminous SNe Ia, but would be more rare. Lower-mass mergers should be common, though it is not clear if they lead to SNe Ia75. The merger of two WDs is a very complicated three dimensional process (necessitating approximations in current models), and very few simulations have been completed.
The WD merger scenario has a natural explanation for greater SN luminosity in young environments: younger and more massive stars produce more massive WDs. Massive WD mergers have more potential fuel than less massive mergers.
Sub-Chandrasekhar mass explosions
Although approaching the Chandra mass is a convenient method for triggering carbon burning, there is no hard evidence that the Chandra mass is required. In the classical sub-Chandra models65, known as 'double detonation' or 'edge-lit detonations,' a layer of accreted helium (∼0.2 M⊙) is built up either by burning accreted hydrogen to helium or by accretion from a helium-rich donor. When the pressure at the base of the helium layer reaches a critical threshold, it detonates, driving a shock into the core of the WD. This causes a second detonation, resulting in a flame propagating outward from the core (or near it), destroying the WD. Because the sub-Chandra WD has a lower density throughout, a simple detonation does not burn the entire star to iron-peak elements. This model thus has the advantage that an ad hoc deflagration to detonation transition is avoided. However, the significant outer helium layer is efficiently burned to 56Ni, resulting in early time spectra that should be rich in 56Ni, which does not match observations76. If helium can detonate with a smaller layer, which some studies hint77, then sub-Chandra simulations can reproduce many of the observed properties of SNe Ia78. Some of the elegance of the model is undercut by the required narrow range of WD masses: ∼0.9–1.1 M⊙, in order to achieve the central densities necessary to produce iron-peak elements.
Constraints on progenitors from rates
Different progenitor scenarios lead to different delay times between the birth of the binary system and the explosion as a SN Ia79. So there is hope of constraining the progenitors by measuring the delay time distribution (DTD; Fig. 6). One approach is to measure the lag between the cosmic star formation rate and the SN Ia rate as a function of redshift. However, large uncertainties in each make this particularly difficult, leading authors to different conclusions even when using largely the same data80,81.
Another approach is to use the relative SN rates in different types of galaxies to constrain the DTD. The fact that the SN Ia rate per unit mass is higher by a factor of ∼20 in late-type galaxies indicates that there is a significant population of short-lived thermonuclear SN progenitors82. Whereas there has been much argument about whether the SN Ia DTD is bimodal83, a leap forward came with the application of spectral energy distribution fitting techniques to SN host galaxies by modelling their stellar populations42. This has allowed more complicated DTDs to be determined: authors using likely SNe Ia from the Subaru-XMM/Newton Deep Survey84 (squares in Fig. 6), or in clusters85 (filled circles), find a power law DTD proportional to t−1. It is difficult to explain the power law DTD results using the single degenerate scenario alone79,84, though there is at least one claim86.
Host galaxy spectroscopy contains even more information to constrain progenitors. New studies using different methods and different data sets87,88, but the same galaxy fitting code, have determined the relative rates of supernovae in 0–0.42 Gyr (prompt), 0.42–2.4 Gyr (medium), and >2.4 Gyr (delayed) bins (stars Fig. 6). They find that 'prompt' and 'delayed' supernovae are required at several sigma. They also confirm earlier findings that bright, broad-lightcurve supernovae favour a prompt population, while dim, narrow-lightcurve SNe Ia favour a delayed population.
Pinpointing the locations of SNe Ia relative to the stellar populations in which they reside can give some information on progenitors, even if it is imprecise due to the probability that the SN has migrated from its birth site. Comparing the distributions of SNe Ia to the blue light in galaxies reveals that even 'prompt' SNe Ia are significantly delayed, with delay times 200–500 Myr89. Additional constraints have been obtained by comparing SN Ia remnants in the Magellanic clouds (triangles in Fig. 6) to their local resolved stellar populations90. At a >99% confidence level, 'prompt' SNe Ia that explode within 330 Myr of star formation are required.
Surviving or preceding material
If WDs grow to become SNe Ia via hydrogen accretion, then it ought to be possible to see this hydrogen in the SN Ia in some form (Figure 7). However, despite decades of searching, no such smoking gun has been found. No SN Ia has ever been seen in the radio91, establishing an upper limit on steady mass loss of material before the SN of ∼3×10−8 M⊙ yr−1. This disfavours the symbiotic star hypothesis, where the WD accretes matter from the stellar wind of its companion. If, on the other hand, the WD is accreting from Roche lobe overflow of a companion, the outer hydrogen layers of the secondary ought to become stripped and entrained in the SN ejecta, where it will show up at low velocities when the ejecta become optically thin92. However, in a couple of well-observed SNe Ia, upper limits on the amount of hydrogen detected are 0.01 M⊙, which would seem to rule out this scenario50, at least for these SNe. In a few cases, apparent SNe Ia have been seen interacting with pre-existing hydrogen, as in SN93, although it is not clear these are really SNe Ia94, and even if they are, these systems are the exception rather than the rule.
The impact of the SN ejecta on any companion star would shock the ejecta, leaving observational signatures along certain lines of sight for several days, long after the ejecta has overtaken the companion95. This would lead to distortions in the early-time lightcurves of SNe Ia around 10% of the time, especially in the ultraviolet to B regions of the spectrum. If the companion star is a red giant, particularly large distortions ought to be seen—the fact that they would have never seem to be problematic for this scenario96.
Variable sodium lines have been seen in high-resolution spectra of some SNe Ia, and their variability, assumed to be from ionization of circumstellar clouds by the SN, has been taken to be evidence of significant circumstellar material. This ostensibly favours the single degenerate scenario97, although maybe only in rare cases—variable sodium was only seen in 6% of cases in a sample of 31 observations, and then only in the most reddened SNe Ia98. Not all variable sodium SNe Ia are reddened, however, nor do all reddened supernovae show variable sodium99. There have also been doubts that this material is truly circumstellar100.
SN remnants provide more clues to the origin of SNe Ia. They may reveal the progenitor's metallicity101, for example. But even more exciting is the prospect that they may house a surviving progenitor star. Tycho's remnant (SN 1572), long suspected of being a SN Ia, has been definitively revealed to be so by modern spectroscopic observations of the SN light, delayed in transit by reflections off of distant interstellar clouds102. In the single degenerate scenario, the secondary star should survive the SN explosion, but may be stripped of its outer layers, and heated, such that it takes of order 1,000 years to return to thermal equilibrium92. One star, Tycho G, has been claimed as evidence for a surviving progenitor103, though there are many doubts about this hypothesis. It is too displaced from the centre of the remnant, and its proper motion shows that it did not come from that direction. Also, it was not apparently out of thermal equilibrium, and does not have the expected rotational characteristics104.
Beginning with SNLS-03D3bb105, aka SN 2003fg, several supernovae have shown luminosities indicating a nickel yield alone of 1.3–1.8 M⊙ (refs 106, 107), possibly indicating a super-Chandrasekhar mass progenitor. Such energetic explosions ought to have more kinetic energy, and, thus, higher velocity ejecta, but this class of SNe counterintuitively have much slower than average ejecta. This may result from the increased binding energy of a super-Chandra WD105, or from the ejecta plowing into a dense shell of circumstellar material resulting106. These SNe also show rare lines of CII near maximum light, possibly indicating less complete burning. They may also favour a young stellar population. This class of SNe Ia would seem to implicate the merger of two WDs, but no simulation has yet reproduced one.
SN Ia are mature probes of cosmology: systematic uncertainties now dominate statistical uncertainties up to z=1, and the systematic uncertainties are well characterized. Still, there is plenty of room for improvement in the use of SNe Ia as standard candles.
It is possible that no single model can describe all SNe Ia. Perhaps some SNe Ia are sub-Chandra, some are the result of mergers, and some are caused by Roche Lobe overflow. The explosion of a WD may be similar no matter how it is triggered. If it is not required that a model explain all SNe, this opens the door to scenarios that do not have high expected event rates.
In the study of SNe Ia, we have left the 'serendipity era,' when we could only discover what nature happened to tell us through chance encounters with nearby supernovae, and we are entering the 'database era,' where we can proactively ask and answer questions about supernovae by comparing large subsamples. The legacy yields of the multi-year second-generation SN surveys are just becoming apparent. Meanwhile, some third-generation surveys like the Palomar Transient Factory, Pan-STARRS, the Dark Energy Survey, and Skymapper, have already started to produce results, and promise thousands more SNe Ia in the next few years. Finally, fourth-generation surveys, the Large Synoptic Survey Telescope, and possible space missions promise unimaginable riches on the horizon. New techniques like comparing large subsamples, using ultraviolet and infrared data, state of the art calibration, using host galaxy observations, and three-dimensional modelling, have started to yield results, but are still in their infancy. The next decade holds real promise of making serious progress in understanding of nearly every aspect of SNe Ia, from their explosion physics, to their progenitors, to their use as standard candles. And with this knowledge may come the key to unlocking the darkest secrets of dark energy.
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D.A.H. acknowledges support from LCOGT.
The author declares no competing financial interests.
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Howell, D. Type Ia supernovae as stellar endpoints and cosmological tools. Nat Commun 2, 350 (2011). https://doi.org/10.1038/ncomms1344
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