>i have thougth: levy measure in a jump diffusion process is:a * f(x)where a is >= 0 and f(x) is the probability density function of jumps (size).>this is true if you are talking about finite activity (finite number of jumps on every compact interval) Levy process e.g. compound Poisson process. Gamma process has infinite activity. Yes you can write its Levy measure as v(dx)= e^(-x)/x dx , but e^(-x)/x is no a density...Gamma process has infinite activity. >so if you know f(x) (it is necessary to know the form of characteristic function anyway) you can say, seeing the levy measure, if the process is:continuous( levy measure =0), jump-diffusion (levy measure has form a*f(x)) or a pure jump process (otherwise).>yes, you can do this. It's known that there are three popular methods to construct a Levy process:C1) Specify a Levy triplet (b, c, v) = (drift, Gaussian coeff., Levy Measure);C2) Specify an infinitely divisible r.v. as the density of L_1;C3) Time-changing Brownian motion with an independent increasing Levy process T (subordinator).My original question was: Let L_t be a Levy process. Suppose all we know is the density function of L_1 (so we specify Levy process using method C2). How do we find out whether our process is a pure jump process? (see
http://math.nyu.edu/faculty/varadhan/sp ... emset2.pdf )For example, in case of Gamma process, we know the density of L_1. Then we can calculate the characteristic function of L_t, and then we would need to find a way to write it in the Levy-Khinchine form. Then by looking at it (using arguments you suggeste) we can figure out what the Levy measure looks like and hence the jump structure of our process.