1918 CHAPTER 59. BASIC PROBABILITY

Then this can be used to find moments of the random variable assuming they exist. The kth

moment is defined as

E(

Xk).

This can be done by using the dominated convergence theorem to differentiate the charac-teristic function with respect to t and then plugging in t = 0. For example,

φ′X (t) = E (iX exp(itX))

and now plugging in t = 0 you get iE (X) . Doing another differentiation you obtain

φ′′X (t) = E

(−X2 exp(itX)

)and plugging in t = 0 you get −E

(X2)

and so forth.An important case is where X is normally distributed with mean 0 and variance σ2. In

this case, as shown above, the characteristic function is

e−12 t2σ2

Also all moments exist when X is normally distributed. So what are these moments?

Dt

(e−

12 t2σ2

)=−tσ2e−

12 t2σ2

and plugging in t = 0 you find the mean equals 0 as expected.

Dt

(−tσ2e−

12 t2σ2

)=−σ

2e−12 t2σ2

+ t2σ

4e−12 t2σ2

and plugging in t = 0 you find the second moment is σ2. Then do it again.

Dt

(−σ

2e−12 t2σ2

+ t2σ

4e−12 t2σ2

)= 3σ

4te−12 t2σ2 − t3

σ6e−

12 t2σ2

Then E(X3)= 0.

Dt

(3σ

4te−12 t2σ2 − t3

σ6e−

12 t2σ2

)= 3σ

4e−12 t2σ2 −6σ

6t2e−12 t2σ2

+ t4σ

8e−12 t2σ2

and so E(X4)= 3σ4. By now you can see the pattern. If you continue this way, you find

the odd moments are all 0 and

E(X2m)=Cm

2)m. (59.17.40)

This is an important observation.

1918 CHAPTER 59. BASIC PROBABILITYThen this can be used to find moments of the random variable assuming they exist. The k’”moment is defined asE (x*) ,This can be done by using the dominated convergence theorem to differentiate the charac-teristic function with respect to ¢ and then plugging in t = 0. For example,oe (1) = E (iX exp (itX))and now plugging in t = 0 you get iE (X). Doing another differentiation you obtain{(t)=E (—x? exp (itX))and plugging in t = 0 you get —E (X*) and so forth.An important case is where X is normally distributed with mean 0 and variance o7. Inthis case, as shown above, the characteristic function iseyeAlso all moments exist when X is normally distributed. So what are these moments?D, (ee) — —te2er2 ©and plugging in ¢ = 0 you find the mean equals 0 as expected.D; (- toe 2! ‘e*) = GeO 4 Pote 3”and plugging in t = 0 you find the second moment is 67. Then do it again.D, (-o oe 4 ote 2 ‘e) = 364 {e738 _ Bg 6-3 O*Then E (X?) =0.D; (Bote 3°" — pose 30")6p2—-5PO* 1 44 8-30?= xP? +t’ ore= 30°e —60and so E (X*) = 30+. By now you can see the pattern. If you continue this way, you findthe odd moments are all 0 andE (X°") =Cn (o?)”. (59.17.40)This is an important observation.