In probability theory, a subordinator is a non-negative stochastic process with stationary and independent increments. It is a special type of Lévy process that plays a key role in the theory of local time. Subordinators describe how time evolves within another stochastic process, called the subordinated process, by determining the random number of "time steps" occurring in chronological time. To qualify as a subordinator, the process must be an increasing Lévy process, almost surely, or an additive process.
Definition
A subordinator is a real-valued stochastic process X = ( X t ) t ≥ 0 {\displaystyle X=(X_{t})_{t\geq 0}} that is a non-negative and a Lévy process.6 Subordinators are the stochastic processes X = ( X t ) t ≥ 0 {\displaystyle X=(X_{t})_{t\geq 0}} that have all of the following properties:
- X 0 = 0 {\displaystyle X_{0}=0} almost surely
- X {\displaystyle X} is non-negative, meaning X t ≥ 0 {\displaystyle X_{t}\geq 0} for all t {\displaystyle t}
- X {\displaystyle X} has stationary increments, meaning that for t ≥ 0 {\displaystyle t\geq 0} and h > 0 {\displaystyle h>0} , the distribution of the random variable Y t , h := X t + h − X t {\displaystyle Y_{t,h}:=X_{t+h}-X_{t}} depends only on h {\displaystyle h} and not on t {\displaystyle t}
- X {\displaystyle X} has independent increments, meaning that for all n {\displaystyle n} and all t 0 < t 1 < ⋯ < t n {\displaystyle t_{0}<t_{1}<\dots <t_{n}} , the random variables ( Y i ) i = 0 , … , n − 1 {\displaystyle (Y_{i})_{i=0,\dots ,n-1}} defined by Y i = X t i + 1 − X t i {\displaystyle Y_{i}=X_{t_{i+1}}-X_{t_{i}}} are independent of each other
- The paths of X {\displaystyle X} are càdlàg, meaning they are continuous from the right everywhere and the limits from the left exist everywhere
Examples
The variance gamma process can be described as a Brownian motion subject to a gamma subordinator.7 If a Brownian motion, W ( t ) {\displaystyle W(t)} , with drift θ t {\displaystyle \theta t} is subjected to a random time change which follows a gamma process, Γ ( t ; 1 , ν ) {\displaystyle \Gamma (t;1,\nu )} , the variance gamma process will follow:
X V G ( t ; σ , ν , θ ) := θ Γ ( t ; 1 , ν ) + σ W ( Γ ( t ; 1 , ν ) ) . {\displaystyle X^{VG}(t;\sigma ,\nu ,\theta )\;:=\;\theta \,\Gamma (t;1,\nu )+\sigma \,W(\Gamma (t;1,\nu )).}The Cauchy process can be described as a Brownian motion subject to a Lévy subordinator.8
Representation
Every subordinator X = ( X t ) t ≥ 0 {\displaystyle X=(X_{t})_{t\geq 0}} can be written as
X t = a t + ∫ 0 t ∫ 0 ∞ x Θ ( d s d x ) {\displaystyle X_{t}=at+\int _{0}^{t}\int _{0}^{\infty }x\;\Theta (\mathrm {d} s\;\mathrm {d} x)}where
- a ≥ 0 {\displaystyle a\geq 0} is a scalar and
- Θ {\displaystyle \Theta } is a Poisson process on ( 0 , ∞ ) × ( 0 , ∞ ) {\displaystyle (0,\infty )\times (0,\infty )} with intensity measure E Θ = λ ⊗ μ {\displaystyle \operatorname {E} \Theta =\lambda \otimes \mu } . Here μ {\displaystyle \mu } is a measure on ( 0 , ∞ ) {\displaystyle (0,\infty )} with ∫ 0 ∞ max ( x , 1 ) μ ( d x ) < ∞ {\displaystyle \int _{0}^{\infty }\max(x,1)\;\mu (\mathrm {d} x)<\infty } , and λ {\displaystyle \lambda } is the Lebesgue measure.
The measure μ {\displaystyle \mu } is called the Lévy measure of the subordinator, and the pair ( a , μ ) {\displaystyle (a,\mu )} is called the characteristics of the subordinator.
Conversely, any scalar a ≥ 0 {\displaystyle a\geq 0} and measure μ {\displaystyle \mu } on ( 0 , ∞ ) {\displaystyle (0,\infty )} with ∫ max ( x , 1 ) μ ( d x ) < ∞ {\displaystyle \int \max(x,1)\;\mu (\mathrm {d} x)<\infty } define a subordinator with characteristics ( a , μ ) {\displaystyle (a,\mu )} by the above relation.910
References
Kallenberg, Olav (2002). Foundations of Modern Probability (2nd ed.). New York: Springer. p. 290. /wiki/Olav_Kallenberg ↩
Kallenberg, Olav (2017). Random Measures, Theory and Applications. Switzerland: Springer. p. 651. doi:10.1007/978-3-319-41598-7. ISBN 978-3-319-41596-3. 978-3-319-41596-3 ↩
Applebaum, D. "Lectures on Lévy processes and Stochastic calculus, Braunschweig; Lecture 2: Lévy processes" (PDF). University of Sheffield. pp. 37–53. http://www.applebaum.staff.shef.ac.uk/Brauns2notes.pdf ↩
Applebaum, D. "Lectures on Lévy processes and Stochastic calculus, Braunschweig; Lecture 2: Lévy processes" (PDF). University of Sheffield. pp. 37–53. http://www.applebaum.staff.shef.ac.uk/Brauns2notes.pdf ↩
Li, Jing; Li, Lingfei; Zhang, Gongqiu (2017). "Pure jump models for pricing and hedging VIX derivatives". Journal of Economic Dynamics and Control. 74. doi:10.1016/j.jedc.2016.11.001. /wiki/Doi_(identifier) ↩
Kallenberg, Olav (2002). Foundations of Modern Probability (2nd ed.). New York: Springer. p. 290. /wiki/Olav_Kallenberg ↩
Applebaum, D. "Lectures on Lévy processes and Stochastic calculus, Braunschweig; Lecture 2: Lévy processes" (PDF). University of Sheffield. pp. 37–53. http://www.applebaum.staff.shef.ac.uk/Brauns2notes.pdf ↩
Applebaum, D. "Lectures on Lévy processes and Stochastic calculus, Braunschweig; Lecture 2: Lévy processes" (PDF). University of Sheffield. pp. 37–53. http://www.applebaum.staff.shef.ac.uk/Brauns2notes.pdf ↩
Kallenberg, Olav (2002). Foundations of Modern Probability (2nd ed.). New York: Springer. p. 287. /wiki/Olav_Kallenberg ↩
Kallenberg, Olav (2002). Foundations of Modern Probability (2nd ed.). New York: Springer. p. 290. /wiki/Olav_Kallenberg ↩