In astronomy, the binary mass function or simply mass function is a function that constrains the mass of the unseen component (typically a star or exoplanet) in a single-lined spectroscopic binary star or in a planetary system. It can be calculated from observable quantities only, namely the orbital period of the binary system, and the peak radial velocity of the observed star. The velocity of one binary component and the orbital period provide information on the separation and gravitational force between the two components, and hence on the masses of the components.

The binary mass function follows from Kepler's third law when the radial velocity of one binary component is known.^[1] Kepler's third law describes the motion of two bodies orbiting a common center of mass. It relates the orbital period with the orbital separation between the two bodies, and the sum of their masses. For a given orbital separation, a higher total system mass implies higher orbital velocities. On the other hand, for a given system mass, a longer orbital period implies a larger separation and lower orbital velocities.

Because the orbital period and orbital velocities in the binary system are related to the masses of the binary components, measuring these parameters provides some information about the masses of one or both components.^[2] However, the true orbital velocity is often unknown, because velocities in the plane of the sky are much more difficult to determine than velocities along the line of sight.^[1]

Radial velocity is the velocity component of orbital velocity in the line of sight of the observer. Unlike true orbital velocity, radial velocity can be determined from Doppler spectroscopy of spectral lines in the light of a star,^[3] or from variations in the arrival times of pulses from a radio pulsar.^[4] A binary system is called a single-lined spectroscopic binary if the radial motion of only one of the two binary components can be measured. In this case, a lower limit on the mass of the other, unseen component can be determined.^[1]

The true mass and true orbital velocity cannot be determined from the radial velocity because the orbital inclination is generally unknown. (The inclination is the orientation of the orbit from the point of view of the observer, and relates true and radial velocity.^[1]) This causes a degeneracy between mass and inclination.^[5][6] For example, if the measured radial velocity is low, this can mean that the true orbital velocity is low (implying low mass objects) and the inclination high (the orbit is seen edge-on), or that the true velocity is high (implying high mass objects) but the inclination low (the orbit is seen face-on).

The peak radial velocity ${\displaystyle K}$ is the semi-amplitude of the radial velocity curve, as shown in the figure. The orbital period ${\displaystyle P_{\text{orb}}}$ is found from the periodicity in the radial velocity curve. These are the two observable quantities needed to calculate the binary mass function.^[2]

The observed object of which the radial velocity can be measured is taken to be object 1 in this article, its unseen companion is object 2.

Let ${\displaystyle M_{1}}$ and ${\displaystyle M_{2}}$ be the stellar masses, with ${\displaystyle M_{1}+M_{2}=M_{\mathrm {tot} }}$ the total mass of the binary system, ${\displaystyle v_{1}}$ and ${\displaystyle v_{2}}$ the orbital velocities, and ${\displaystyle a_{1}}$ and ${\displaystyle a_{2}}$ the distances of the objects to the center of mass. ${\displaystyle a_{1}+a_{2}=a}$ is the semi-major axis (orbital separation) of the binary system.

We start out with Kepler's third law, with ${\displaystyle \omega _{\mathrm {orb} }=2\pi /P_{\mathrm {orb} }}$ the orbital frequency and ${\displaystyle G}$ the gravitational constant,

$${\displaystyle GM_{\text{tot}}=\omega _{\text{orb}}^{2}a^{3}.}$$

Using the definition of the center of mass location, ${\displaystyle M_{1}a_{1}=M_{2}a_{2}}$,^[1] we can write

$${\displaystyle a=a_{1}+a_{2}=a_{1}\left(1+{\frac {a_{2}}{a_{1}}}\right)=a_{1}\left(1+{\frac {M_{1}}{M_{2}}}\right)={\frac {a_{1}}{M_{2}}}(M_{1}+M_{2})={\frac {a_{1}M_{\mathrm {tot} }}{M_{2}}}.}$$

Inserting this expression for ${\displaystyle a}$ into Kepler's third law, we find

$${\displaystyle GM_{\mathrm {tot} }=\omega _{\mathrm {orb} }^{2}{\frac {a_{1}^{3}M_{\mathrm {tot} }^{3}}{M_{2}^{3}}}.}$$

which can be rewritten to

$${\displaystyle {\frac {M_{2}^{3}}{M_{\mathrm {tot} }^{2}}}={\frac {\omega _{\mathrm {orb} }^{2}a_{1}^{3}}{G}}.}$$

The peak radial velocity of object 1, ${\displaystyle K}$, depends on the orbital inclination ${\displaystyle i}$ (an inclination of 0° corresponds to an orbit seen face-on, an inclination of 90° corresponds to an orbit seen edge-on). For a circular orbit (orbital eccentricity = 0) it is given by^[7]

$${\displaystyle K=v_{1}\sin i=\omega _{\text{orb}}a_{1}\sin i.}$$

After substituting ${\displaystyle a_{1}}$ we obtain

$${\displaystyle {\frac {M_{2}^{3}}{M_{\text{tot}}^{2}}}={\frac {K^{3}}{G\omega _{\text{orb}}\sin ^{3}i}}.}$$

The binary mass function ${\displaystyle f}$ (with unit of mass) is^{[8][7][2][9][1][6][10]}

$${\displaystyle f={\frac {M_{2}^{3}\sin ^{3}i}{(M_{1}+M_{2})^{2}}}={\frac {P_{\mathrm {orb} }\ K^{3}}{2\pi G}}.}$$

For an estimated or assumed mass ${\displaystyle M_{1}}$ of the observed object 1, a minimum mass ${\displaystyle M_{\mathrm {2,min} }}$ can be determined for the unseen object 2 by assuming ${\displaystyle i=90^{\circ }}$. The true mass ${\displaystyle M_{2}}$ depends on the orbital inclination. The inclination is typically not known, but to some extent it can be determined from observed eclipses,^[2] be constrained from the non-observation of eclipses,^[8][9] or be modelled using ellipsoidal variations (the non-spherical shape of a star in binary system leads to variations in brightness over the course of an orbit that depend on the system's inclination).^[11]

Limits

In the case of ${\displaystyle M_{1}\gg M_{2}}$ (for example, when the unseen object is an exoplanet^[8]), the mass function simplifies to

$${\displaystyle f\approx {\frac {M_{2}^{3}\ \sin ^{3}i}{M_{1}^{2}}}.}$$

In the other extreme, when ${\displaystyle M_{1}\ll M_{2}}$ (for example, when the unseen object is a high-mass black hole), the mass function becomes^[2]

$${\displaystyle f\approx M_{2}\sin ^{3}i,}$$

and since ${\displaystyle 0\leq \sin(i)\leq 1}$ for ${\displaystyle 0^{\circ }\leq i\leq 90^{\circ }}$, the mass function gives a lower limit on the mass of the unseen object 2.^[6]

In general, for any ${\displaystyle i}$ or ${\displaystyle M_{1}}$,

$${\displaystyle M_{2}>\max \left(f,f^{1/3}M_{1}^{2/3}\right).}$$

In an orbit with eccentricity ${\displaystyle e}$, the mass function is given by^[7][12]

$${\displaystyle f={\frac {M_{2}^{3}\sin ^{3}i}{(M_{1}+M_{2})^{2}}}={\frac {P_{\mathrm {orb} }\ K^{3}}{2\pi G}}\left(1-e^{2}\right)^{3/2}.}$$