11.2. LAPLACE TRANSFORM 267

Now it follows from that section that the integrand converges to −te−stφ (t). Therefore, itonly is required to obtain an estimate and use the dominated convergence theorem. Thene−st e−ht−1

h φ (t) =∣∣∣∣e−(s+h)t 1− eht

hφ (t)

∣∣∣∣≤Ceλ t∣∣∣∣1− eht

h

∣∣∣∣e−(s+h) ≤Cte−(s+h−λ )t∣∣∣∣1− eht

th

∣∣∣∣Now

∣∣∣e−(s+h−λ )t∣∣∣ = e−(Re(s+h)−λ )t ≤ e−εt whenever |h| is small enough because of the

assumption that Res > λ . eht −1 =∫ t

0 hehudu and so the last expression is∣∣∣∣∫ t0 hehudu

th

∣∣∣∣≤ 1t

∣∣∣∣∫ t

0ehudu

∣∣∣∣≤ 1t

∫ t

0e|h|udu≤ et|h|,

and so for |h| small enough, say smaller than ε/2, the integrand in 11.1 is no larger thanCte−εte

ε2 t =Cte−

ε2 t which is in L1 and so the dominated convergence theorem applies and it

follows that f ′ (s) =∫

0 (−t)e−stφ (t)dt whenever Re(s)> λ . Continuing similarly, yieldsall the derivatives. However, the existence of all the derivatives will follow from generalresults on analytic functions presented later. ■

The whole approach for Laplace transforms in differential equations is based on theassertion that if L ( f ) = L (g) , then f = g. However, this is not even true because if youchange the function on a set of measure zero, you don’t change the transform. However, iff ,g are continuous, then it will be true. Actually, it is shown here that if L ( f ) = 0, andf is continuous, then f = 0. The approach here is based on the Weierstrass approximationtheorem or rather a case of it.

Lemma 11.2.3 Suppose q is a continuous function defined on [0,1] . Also suppose thatfor all n = 0,1,2, · · · , that

∫ 10 q(x)xndx = 0. Then it follows that q = 0.

Proof: By assumption, for p(x) any polynomial,∫ 1

0 q(x) p(x)dx = 0. Now let {pn (x)}be a sequence of polynomials which converge uniformly to q(x) by Corollary 3.1.3. Saymaxx∈[0,1] |q(x)− pn (x)|< 1

n . Then from this uniform convergence, of pn to q,

∫ 1

0q2 (x)dx = lim

n→∞

∫ 1

0q(x) pn (x)dx = 0.

By continuity, it must be the case that q(x) = 0 for all x since otherwise, there would be asmall interval on which q2 (x) is positive and so the integral could not have been 0 after all.■

Lemma 11.2.4 Suppose | f (t)| ≤Ce−δ t for some δ > 0 and all t > 0 and also that f iscontinuous. Suppose that

∫∞

0 e−st f (t)dt = 0 for all s > 0. Then f = 0.

Proof: First note that limt→∞ | f (t)| = 0. Next change the variable letting x = e−t andso x ∈ [0,1]. Then this reduces to

∫ 10 xs−1 f (− ln(x))dx. Now if you let q(x) = f (− ln(x)) ,

it is not defined when x = 0, but x = 0 corresponds to t → ∞. Thus limx→0+ q(x) = 0.Defining q(0)≡ 0, it follows that it is continuous and letting s−1 be various integers, forall n = 0,1,2, · · · ,

∫ 10 xnq(x)dx = 0 and so q(x) = 0 for all x from Lemma 11.2.3. Thus

f (− ln(x)) = 0 for all x ∈ (0,1] and so f (t) = 0 for all t ≥ 0. ■

11.2. LAPLACE TRANSFORM 267Now it follows from that section that the integrand converges to —te~"@ (t). Therefore, itonly is required to obtain an estimate and use the dominated convergence theorem. Theneost onal (t) =1—eth“(5 1 —eltc rn IE 9)1 —elt< CeS Ce hJeon < Cte (Sth-Alt= e (Re(sth)—A)t_ < e-& whenever |h| is small enough because of theNow Jeonassumption that Res >A. eM —1= fo he! du and so the last expression ist[ edu0and so for |h| small enough, say smaller than ¢/2, the integrand in 11.1 is no larger thanCte~®e3! =Cte~ >! which is in L! and so the dominated convergence theorem applies and itfollows that f’(s) = fo (—t)e~@ (t) dt whenever Re (s) > A. Continuing similarly, yieldsall the derivatives. However, the existence of all the derivatives will follow from generalresults on analytic functions presented later.The whole approach for Laplace transforms in differential equations is based on theassertion that if 2 (f) = & (g), then f = g. However, this is not even true because if youchange the function on a set of measure zero, you don’t change the transform. However, iff,g are continuous, then it will be true. Actually, it is shown here that if “(f) = 0, andf is continuous, then f = 0. The approach here is based on the Weierstrass approximationtheorem or rather a case of it.1<-| Jo heldutth1 t< - | oll du < ell<a <Lemma 11.2.3 Suppose q is a continuous function defined on [0,1]. Also suppose thatfor alln=0,1,2,+++, that fo q(x)x"dx = 0. Then it follows that q = 0.Proof: By assumption, for p (x) any polynomial, fo q(x) p(x) dx = 0. Now let {p, (x)}be a sequence of polynomials which converge uniformly to g(x) by Corollary 3.1.3. Saymax y<(0,1] 14 (x) — Pa (x)| < 4. Then from this uniform convergence, of pn to q,1 1| ¢ (x)dx = lim | q(x) Pn (x) dx = 0.0 neo JQBy continuity, it must be the case that g(x) = 0 for all x since otherwise, there would be asmall interval on which q? (x) is positive and so the integral could not have been 0 after all.aLemma 11.2.4 Suppose |f (t)| <Ce~®* for some & > 0 and allt > 0 and also that f iscontinuous. Suppose that [, e—" f (t)dt =0 for all s > 0. Then f =0.Proof: First note that lim,_,.. |f (t)| = 0. Next change the variable letting x = e~’ andso x € [0, 1]. Then this reduces to fo x°—! £ (—In (x)) dx. Now if you let g(x) = f (—In(x)),it is not defined when x = 0, but x = 0 corresponds to t > oo. Thus lim,,94q¢ (x) = 0.Defining q (0) = 0, it follows that it is continuous and letting s — | be various integers, forall n =0,1,2,--- So x"q (x) dx = 0 and so q(x) = 0 for all x from Lemma 11.2.3. Thusf (—In(x)) =0 for all x € (0, 1] and so f (t) =0 for allt > 0.