Circumstellar disc

Around the Solar System

• The asteroid belt is a reservoir of small bodies in the Solar System located between the orbit of Mars and Jupiter. It is a source of interplanetary dust.
• Edgeworth-Kuiper belt, beyond the orbit of Neptune
• Scattered disc, beyond the orbit of Neptune
• Hills cloud; only the inner Oort cloud has a toroid-like shape. The outer Oort cloud is more spherical in shape.

Binary system

The infall of gas onto a binary system allows the formation of circumstellar and circumbinary discs. The formation of such a disc will occur for any binary system in which infalling gas contains some degree of angular momentum. A general progression of disc formation is observed with increasing levels of angular momentum:

• Circumprimary disc is one which orbits the primary (i.e. more massive) star of the binary system. This type of disc will form through accretion if any angular momentum is present in the infalling gas.
• Circumsecondary disc is one which orbits around the secondary (i.e. less massive) star of the binary star system. This type of disc will only form when a high enough level of angular momentum is present within the infalling gas. The amount of angular momentum required is dependent on the secondary-to-primary mass ratio. A circumsecondary disk is sometimes seen transiting in front of the primary.
• Circumbinary disc is one which orbits about both the primary and secondary stars. Such a disc will form at a later time than the circumprimary and circumsecondary discs, with an inner radius much larger than the orbital radius of the binary system. A circumbinary disc may form with an upper mass limit of approximately 0.005 solar masses, at which point the binary system is generally unable to perturb the disc strongly enough for gas to be further accreted onto the circumprimary and circumsecondary discs. An example of a circumbinary disc may be seen around the star system GG Tauri.
• Given the formation of a circumbinary disc, the formation of an inner cavity surrounding the binary is inevitable. This cavity is the result of spiral density waves located at Lindblad resonances, specifically the outer Lindblad resonances. The exact resonances which excise the cavity depend on the eccentricity of the binary ${\displaystyle e_b}$, but in each case the size of the cavity is proportional to the binary separation ${\displaystyle a_b}$.

Accretion variability

Short-term variability

The indicative timescale that governs the short-term evolution of accretion onto binaries within circumbinary disks is the binary's orbital period ${\displaystyle P_b}$. Accretion into the inner cavity is not constant, and varies depending on ${\displaystyle e_b}$ and the behavior of the gas along the innermost region of the cavity. For non-eccentric binaries, accretion variability coincides with the Keplerian orbital period of the inner gas, which develops lumps corresponding to ${\displaystyle m=1}$ outer Lindblad resonances. This period is approximately five times the binary orbital period. For eccentric binaries, the period of accretion variability is the same as the binary orbital period due to each binary component scooping in matter from the circumbinary disk each time it reaches the apocenter of its orbit.

Long-term variability

Eccentric binaries also see accretion variability over secular timescales hundreds of times the binary period. This corresponds to the apsidal precession rate of the inner edge of the cavity, which develops its own eccentricity ${\displaystyle e_d}$, along with a significant region of the inner circumbinary disk up to ${\displaystyle \sim 10a_b}$. This eccentricity may in turn affect the inner cavity accretion as well as dynamics further out in the disk, such as circumbinary planet formation and migration.

Orbital evolution

It was originally believed that all binaries located within circumbinary disk would evolve towards orbital decay due to the gravitational torque of the circumbinary disk, primarily from material at the innermost edge of the excised cavity. This decay is no longer guaranteed when accretion from the circumbinary disk onto the binary occurs, and can even lead to increased binary separations. The dynamics of orbital evolution depend on the binary's parameters, such as the mass ratio ${\displaystyle q_b}$ and eccentricity ${\displaystyle e_b}$, as well as the thermodynamics of the accreting gas.

Misaligned disks

Once a circumstellar disk has formed, spiral density waves are created within the circumstellar material via a differential torque due to the binary's gravity. The majority of these discs form axisymmetric to the binary plane, but it is possible for processes such as the Bardeen-Petterson effect, a misaligned dipole magnetic field and radiation pressure to produce a significant warp or tilt to an initially flat disk.

Strong evidence of tilted disks is seen in the systems Her X-1, SMC X-1, and SS 433 (among others), where a periodic line-of-sight blockage of X-ray emissions is seen on the order of 50–200 days; much slower than the systems' binary orbit of ~1 day. The periodic blockage is believed to result from precession of a circumprimary or circumbinary disk, which normally occurs retrograde to the binary orbit as a result of the same differential torque which creates spiral density waves in an axissymmetric disk.

Evidence of tilted circumbinary disks can be seen through warped geometry within circumstellar disks, precession of protostellar jets, and inclined orbits of circumplanetary objects (as seen in the eclipsing binary TY CrA). For disks orbiting a low secondary-to-primary mass ratio binary, a tilted circumbinary disc will undergo rigid precession with a period on the order of years. For discs around a binary with a mass ratio of one, differential torques will be strong enough to tear the interior of the disc apart into two or more separate, precessing discs.

A study from 2020 using ALMA data showed that circumbinary disks around short period binaries are often aligned with the orbit of the binary. Binaries with a period longer than one month showed typically a misalignment of the disk with the binary orbit.

Dust

• Debris discs consist of planetesimals along with fine dust and small amounts of gas generated through their collisions and evaporation. The original gas and small dust particles have been dispersed or accumulated into planets.
• Zodiacal cloud or interplanetary dust is the material in the Solar System created by collisions of asteroids and evaporation of comet seen to observers on Earth as a band of scattered light along the ecliptic before sunrise or after sunset.
• Exozodiacal dust is dust around another star than the Sun in a location analogous to that of the Zodiacal Light in the Solar System.

Stages

Stages in circumstellar discs refer to the structure and the main composition of the disc at different times during its evolution. Stages include the phases when the disc is composed mainly of submicron-sized particles, the evolution of these particles into grains and larger objects, the agglomeration of larger objects into planetesimals, and the growth and orbital evolution of planetesimals into the planetary systems, like the Solar System or many other stars.

Major stages of evolution of circumstellar discs:

• Protoplanetary discs: In this stage large quantities of primordial material (e.g., gas and dust) are present and the discs are massive enough to have potential to be planet-forming.
• Transition discs: At this stage, the disc shows significant reduction in the presence of gas and dust and presents properties between protoplanetary and debris discs.
• Debris discs: In this stage the circumstellar disc is a tenuous dust disc, presenting small gas amounts or even no gas at all. It is characterized by having dust lifetimes smaller than the age of the disc, hence indicating that the disc is second generation rather than primordial.

Disc dissipation and evolution

Material dissipation is one of the processes responsible for circumstellar discs evolution. Together with information about the mass of the central star, observation of material dissipation at different stages of a circumstellar disc can be used to determine the timescales involved in its evolution. For example, observations of the dissipation process in transition discs (discs with large inner holes) estimate the average age of a circumstellar disc to be approximately 10 Myr.

Dissipation process and its duration in each stage is not well understood. Several mechanisms, with different predictions for discs' observed properties, have been proposed to explain dispersion in circumstellar discs. Mechanisms like decreasing dust opacity due to grain growth, photoevaporation of material by X-ray or UV photons from the central star (stellar wind), or the dynamical influence of a giant planet forming within the disc are some of the processes that have been proposed to explain dissipation.

Dissipation is a process that occurs continuously in circumstellar discs throughout the lifetime of the central star, and at the same time, for the same stage, is a process that is present in different parts of the disc. Dissipation can be divided in inner disc dissipation, mid-disc dissipation, and outer disc dissipation, depending on the part of the disc considered.

Inner disc dissipation occurs at the inner part of the disc (< 0.05–0.1 AU). Since it is closest to the star, this region is also the hottest, thus material present there typically emits radiation in the near-infrared region of the electromagnetic spectrum. Study of the radiation emitted by the very hot dust present in that part of the disc indicates that there is an empirical connection between accretion from a disc onto the star and ejections in an outflow.

Mid-disc dissipation, occurs at the mid-disc region (1–5 AU) and is characterized for the presence of much more cooler material than in the inner part of the disc. Consequently, radiation emitted from this region has greater wavelength, indeed in the mid-infrared region, which makes it very difficult to detect and to predict the timescale of this region's dissipation. Studies made to determine the dissipation timescale in this region provide a wide range of values, predicting timescales from less than 10 up to 100 Myr.

Outer disc dissipation occurs in regions between 50–100 AU, where temperatures are much lower and emitted radiation wavelength increases to the millimeter region of the electromagnetic spectrum. Mean dust masses for this region has been reported to be ~ 10⁻⁵ solar masses. Studies of older debris discs (10⁷–10⁹ yr) suggest dust masses as low as 10⁻⁸ solar masses, implying that diffusion in outer discs occurs on a very long timescale.

As mentioned, circumstellar discs are not equilibrium objects, but instead are constantly evolving. The evolution of the surface density ${\displaystyle \mathrm{\Sigma }}$ of the disc, which is the amount of mass per unit area so after the volume density at a particular location in the disc has been integrated over the vertical structure, is given by: ${\displaystyle \frac{\mathrm{\partial }\mathrm{\Sigma }}{\mathrm{\partial }t}=\frac{3}{r}\frac{\mathrm{\partial }}{\mathrm{\partial }r}\left[r^{1/2}\frac{\mathrm{\partial }}{\mathrm{\partial }r}\nu \mathrm{\Sigma }{r}^{1/2}\right]}$ where ${\displaystyle r}$ is the radial location in the disc and ${\displaystyle \nu }$ is the viscosity at location ${\displaystyle r}$. This equation assumes axisymmetric symmetry in the disc, but is compatible with any vertical disc structure.

Viscosity in the disc, whether molecular, turbulent or other, transports angular momentum outwards in the disc and most of the mass inwards, eventually accreting onto the central object. The mass accretion onto the star ${\displaystyle \dot{M}}$ in terms of the disc viscosity ${\displaystyle \nu }$ is expressed: ${\displaystyle \dot{M}=3\pi \nu \mathrm{\Sigma }{\left[1-\sqrt{\frac{r_{\text{in}}}{r}}\right]}^{-1}}$ where ${\displaystyle r_{\text{in}}}$ is the inner radius.

Direct imaging

Protoplanetary disks and debris disks can be imaged with different methods. If the disk is seen edge-on, the disk can sometimes block the light of the star and the disk can be directly observed without a coronagraph or other advanced techniques (e.g. Gomez's Hamburger or Flying Saucer). Other edge-on disks (e.g. Beta Pictoris or AU Microscopii) and face-on disks (e.g. IM Lupi or AB Aurigae) require a coronagraph, adaptive optics or differential images to take an image of the disk with a telescope. These optical and infrared observations, for example with SPHERE, usually take an image of the star light being scattered on the surface of the disk and trace small micron-sized dust particles. Radio arrays like ALMA on the other hand can map larger millimeter-sized dust grains found in the mid-plane of the disk. Radio arrays like ALMA can also detect narrow emission from the gas of the disk. This can reveal the velocity of the gas within and around the disk. In some cases an edge-on protoplanetary disk (e.g. CK 3 or ASR 41) can cast a shadow onto the surrounding dusty material. This cast shadow works like a shadow play, and the projection of the disk is much larger than the true size of the disk.