1202 CHAPTER 34. GELFAND TRIPLES AND RELATED STUFF

≤ ⟨Bu0,u0⟩+2∫ T

0∥Y (r)∥V ′ ∥u

rk (r)∥V dr+ ε

≤ ⟨Bu0,u0⟩+2(∫ T

0∥Y (r)∥p′

V ′ dr)1/p′(∫ T

0∥ur

k (r)∥pV dr

)1/p

+ ε

≤ C (∥Y∥K′ ,∥u∥K)+ ε

whenever k is large enough because these partitions are chosen such that

limk→∞

(∫ T

0∥ur

k (r)∥pV

)1/p

=

(∫ T

0∥u(r)∥p

V

)1/p

and so these are bounded. This has shown that for the dense subset of [0,T ] , D≡ ∪kPk,

supt∈D⟨B(t)u(t) ,u(t)⟩+

∫ T

0

⟨B′u,u

⟩ds <C (∥Y∥K′ ,∥u∥K)+ ε

However, ε was arbitrary and the partitions are nested. Hence the above holds for all ε andso

supt∈D⟨B(t)u(t) ,u(t)⟩+

∫ T

0

⟨B′u,u

⟩ds <C (∥Y∥K′ ,∥u∥K)

By 34.5.29 and the integral equation, there is a set of measure zero including all theearlier sets of measure zero N such that for t /∈ N,ul

n (t) ,urn (t)→ u(t) pointwise in V. Also,

B(t)urn (t)→ Bu(t) in V ′. This last can be obtained from the integral equation solved. t→

Bu(t) is continuous into V ′. Then let t /∈ N. We have urn (t)→ u(t) in V . Now B(t)ur

n (t) =B(t)u(sn) where sn ∈ D and sn→ t. Then Bu(t) = B(t)u(t) and

∥B(sn)u(sn)−B(t)u(t)∥V ′ ≤ ∥(B(sn)−B(t))u(sn)∥V ′ +∥B(t)(u(sn)−u(t))∥V ′

≤Ct ∥B(sn)−B(t)∥+C∥u(sn)−u(t)∥Vwhere Ct is a constant which comes because u(sn)→ u(t) in V and so is bounded. Theconstant C is just maxt∈[0,T ] ∥B(t)∥. Then, since the two terms on the right converge to 0 asn→∞, it follows that as sn→ t,B(sn)u(sn)→ B(t)u(t) = Bu(t) in V ′ while u(sn)→ u(t)in V . It follows that for t /∈ N,

⟨Bu(t) ,u(t)⟩+∫ T

0

⟨B′u,u

⟩ds = lim

n→∞⟨Bu(sn) ,u(sn)⟩+

∫ T

0

⟨B′u,u

⟩ds≤C (∥Y∥K′ ,∥u∥K)

Hence,

supt /∈N⟨Bu(t) ,u(t)⟩+

∫ T

0

⟨B′u,u

⟩ds≤C (∥Y∥K′ ,∥u∥K)

It only remains to verify the claim about weak continuity.Consider now the claim that t→ Bu(t) is weakly continuous on NC. Letting v ∈V,s ∈

NC,limt→s⟨Bu(t) ,v⟩= ⟨Bu(s) ,v⟩= ⟨Bu(s) ,v⟩ (34.5.34)

1202 CHAPTER 34. GELFAND TRIPLES AND RELATED STUFFT< (Buo,uo) +2 f° ( (P)lv link lly ar-+T , 1/p! 7 oT \/pBu.) +2( [I liar) — (["wenieadr) +eC(I) +€IAIAwhenever k is large enough because these partitions are chosen such thatjim (fl oi) i { [ow ve)”and so these are bounded. This has shown that for the dense subset of [0,7], D = Ug”,Tsup (B(1) u(r) ,u(t)) +f (Blu,u)ds <C((\¥ lx lull) +€teHowever, € was arbitrary and the partitions are nested. Hence the above holds for all € andso rsup(B(e) u(t), (e))-+ [ (Brun) ds < (|| ele)teBy 34.5.29 and the integral equation, there is a set of measure zero including all theearlier sets of measure zero N such that for t ¢ N,u/, (t) ,u’, (t) + u(t) pointwise in V. Also,B(t) ul, (t) > Bu(t) in V’. This last can be obtained from the integral equation solved. t >Bu(t) is continuous into V’. Then let t ¢ N. We have u’, (t) > u(t) in V. Now B(t)u? (t) =B(t)u(s,) where s, € D ands, >t. Then Bu(t) = B(t) u(t) and|B (sn) u (Sn) —B(t)u(t)|lyr < ||(B (sn) —B(t)) u (sn) [ly + I/B (t) (us) — u(t) lye<C,||B (sn) —B(t)|| +C||u (sn) —u (2) lywhere C; is a constant which comes because u(s,) — u(t) in V and so is bounded. Theconstant C is just max;<j9,7) ||B (¢)||. Then, since the two terms on the right converge to 0 asn—> , it follows that as sy, + t,B (s,)u(s,) > B(t) u(t) = Bu(t) in V’ while u(s,) > u(t)in V. It follows that fort ¢ N,T T(Bu(1).u(0))-+ [ (Blusu)ds= fim (Bu (sn) 1e(s5)) + [ (Blusu)ds <C (Yall)nooHence,Tsup (Bu(t).u()) + [) (Blu) ds < C( (a lulc)tIt only remains to verify the claim about weak continuity.Consider now the claim that t + Bu (t) is weakly continuous on NC. Letting v € V,s €NC,lim (Bu (t) ,v) = (Bu(s) ,v) = (Bu(s) ,v) (34.5.34)ts