Introduction QC mappings of the whole plane QC mappings on domains The end
Regularity of planar quasiconformal mappings
Mart´ı Prats
September 8th, 2016
Introduction QC mappings of the whole plane QC mappings on domains The end
Introduction
Introduction QC mappings of the whole plane QC mappings on domains The end
Measuring smoothness and integrability in R
d1 p
p“ 1 p“ 8
L4
Lebesgue spacesÑintegrability.
Di↵erentiablility classes Ñ smoothness. Sobolev spacesÑ both together. H¨older continuous spacesÑ fill gaps. Interpolation to generalize.
}f }Lp “`´
|f |p˘1{p, }f }L8 “ ess sup|f |
}f }Cs “ }f }L8` ¨ ¨ ¨ ` }rsf}L8 }f }Ws,p “ }f }Lp` ¨ ¨ ¨ ` }rsf}Lp
}f }Cs “
}f }L8` ¨ ¨ ¨ ` sup|rtsuf|x´y|pxq´rtsutsufpyq|
}f }Ws,p,}f }Bp,qs ,}f }Fp,qs
By means of Sobolev embeddings, we have either continuity or extra integrability.
Introduction QC mappings of the whole plane QC mappings on domains The end
Measuring smoothness and integrability in R
d1 p
s
0 2 4
C3
L4
Lebesgue spacesÑ integrability.
Di↵erentiablility classes Ñsmoothness.
Sobolev spacesÑ both together. H¨older continuous spacesÑ fill gaps. Interpolation to generalize.
}f }Lp “`´
|f |p˘1{p, }f }L8 “ ess sup|f |
}f }Cs “ }f }L8` ¨ ¨ ¨ ` }rsf}L8
}f }Ws,p “ }f }Lp` ¨ ¨ ¨ ` }rsf}Lp
}f }Cs “
}f }L8` ¨ ¨ ¨ ` sup|rtsuf|x´y|pxq´rtsutsufpyq|
}f }Ws,p,}f }Bp,qs ,}f }Fp,qs
By means of Sobolev embeddings, we have either continuity or extra integrability.
Introduction QC mappings of the whole plane QC mappings on domains The end
Measuring smoothness and integrability in R
d1 p
s
0 2 4
W3,4 C3
L4
Lebesgue spacesÑintegrability.
Di↵erentiablility classes Ñsmoothness.
Sobolev spacesÑbothtogether.
H¨older continuous spacesÑ fill gaps. Interpolation to generalize.
}f }Lp “`´
|f |p˘1{p, }f }L8 “ ess sup|f |
}f }Cs “ }f }L8` ¨ ¨ ¨ ` }rsf}L8
}f }Ws,p “ }f }Lp` ¨ ¨ ¨ ` }rsf}Lp
}f }Cs “
}f }L8` ¨ ¨ ¨ ` sup|rtsuf|x´y|pxq´rtsutsufpyq|
}f }Ws,p,}f }Bp,qs ,}f }Fp,qs
By means of Sobolev embeddings, we have either continuity or extra integrability.
Introduction QC mappings of the whole plane QC mappings on domains The end
Measuring smoothness and integrability in R
d1 p
s
0 2 4
W3,4
C1.75
L4
Lebesgue spacesÑ integrability.
Di↵erentiablility classes Ñ smoothness.
Sobolev spacesÑ both together.
H¨older continuous spacesÑ fill gaps.
Interpolation to generalize.
}f }Lp “`´
|f |p˘1{p, }f }L8 “ ess sup|f |
}f }Cs “ }f }L8` ¨ ¨ ¨ ` }rsf}L8
}f }Ws,p “ }f }Lp` ¨ ¨ ¨ ` }rsf}Lp
}f }Cs “
}f }L8` ¨ ¨ ¨ ` sup|rtsuf|x´y|pxq´rtsutsufpyq|
}f }Ws,p,}f }Bp,qs ,}f }Fp,qs
By means of Sobolev embeddings, we have either continuity or extra integrability.
Introduction QC mappings of the whole plane QC mappings on domains The end
Measuring smoothness and integrability in R
d1 p
s
0 2 4
W3,4
C1.75
L4
W3{2,8{5 W1,4{3
Lebesgue spacesÑ integrability.
Di↵erentiablility classes Ñ smoothness.
Sobolev spacesÑ both together.
H¨older continuous spacesÑ fill gaps.
Interpolation to generalize.
}f }Lp “`´
|f |p˘1{p, }f }L8 “ ess sup|f |
}f }Cs “ }f }L8` ¨ ¨ ¨ ` }rsf}L8
}f }Ws,p “ }f }Lp` ¨ ¨ ¨ ` }rsf}Lp
}f }Cs “
}f }L8` ¨ ¨ ¨ ` sup|rtsuf|x´y|pxq´rtsutsufpyq|
}f }Ws,p,}f }Bp,qs ,}f }Fp,qs
By means of Sobolev embeddings, we have either continuity or extra integrability.
Introduction QC mappings of the whole plane QC mappings on domains The end
Measuring smoothness and integrability in R
d1 p
s
sp“ d Supercritical
Subcritical 0
2 4 3
Ws1,p1 Cs1´p1d
Lp1
Ws2,p2
Lp2˚ Lp2 d“ 3
Lebesgue spacesÑ integrability.
Di↵erentiablility classes Ñ smoothness.
Sobolev spacesÑ both together.
H¨older continuous spacesÑ fill gaps.
Interpolation to generalize.
}f }Lp “`´
|f |p˘1{p, }f }L8 “ ess sup|f |
}f }Cs “ }f }L8` ¨ ¨ ¨ ` }rsf}L8
}f }Ws,p “ }f }Lp` ¨ ¨ ¨ ` }rsf}Lp
}f }Cs “
}f }L8` ¨ ¨ ¨ ` sup|rtsuf|x´y|pxq´rtsutsufpyq|
}f }Ws,p,}f }Bp,qs ,}f }Fp,qs
By means of Sobolev embeddings, we have either continuity or extra integrability.
Introduction QC mappings of the whole plane QC mappings on domains The end
Quasiconformal mappings
Conformal mappings Preserves angles
“Circles to circles” Cauchy-Riemann:
1
2pBxf ` iByfq “ 0
Quasiconformal mappings Angle distortion bounded.
“Circles to ellipses”.
|Bf | § k|Bf |
Introduction QC mappings of the whole plane QC mappings on domains The end
Quasiconformal mappings
Conformal mappings Preserves angles
“Circles to circles”
Cauchy-Riemann:
1
2pBxf ` iByfq “ 0
Quasiconformal mappings Angle distortion bounded.
“Circles to ellipses”.
|Bf | § k|Bf |
Introduction QC mappings of the whole plane QC mappings on domains The end
Quasiconformal mappings
Conformal mappings Preserves angles
“Circles to circles”
Cauchy-Riemann:
1
2pBxf ` iByfq “ 0 Bf “ 0
Quasiconformal mappings Angle distortion bounded.
“Circles to ellipses”.
|Bf | § k|Bf |
Introduction QC mappings of the whole plane QC mappings on domains The end
Quasiconformal mappings
Conformal mappings Preserves angles
“Circles to circles”
Cauchy-Riemann:
1
2pBxf ` iByfq “ 0 Bf “ 0
Quasiconformal mappings Angle distortion bounded.
“Circles to ellipses”.
|Bf | § k|Bf |
Introduction QC mappings of the whole plane QC mappings on domains The end
The Beurling transform
The Beurling transform of a function f P LppCq is:
Bf pzq “ 1
´⇡ lim
"Ñ0
ˆ
|w´z|°"
fpwq
pz ´ wq2dmpwq.
It is essential to quasiconformal mappings because Bp¯Bf q “ Bf @f P W1,p. Recall thatB : LppCq Ñ LppCq is bounded for 1 † p † 8.
AlsoB : Ws,ppCq Ñ Ws,ppCq is bounded for 1 † p † 8 and s ° 0.
Introduction QC mappings of the whole plane QC mappings on domains The end
The Beurling transform
The Beurling transform of a function f P LppCq is:
Bf pzq “ 1
´⇡ lim
"Ñ0
ˆ
|w´z|°"
fpwq
pz ´ wq2dmpwq.
It is essential to quasiconformal mappings because Bp¯Bf q “ Bf @f P W1,p.
Recall thatB : LppCq Ñ LppCq is bounded for 1 † p † 8.
AlsoB : Ws,ppCq Ñ Ws,ppCq is bounded for 1 † p † 8 and s ° 0.
Introduction QC mappings of the whole plane QC mappings on domains The end
The Beurling transform
The Beurling transform of a function f P LppCq is:
Bf pzq “ 1
´⇡ lim
"Ñ0
ˆ
|w´z|°"
fpwq
pz ´ wq2dmpwq.
It is essential to quasiconformal mappings because Bp¯Bf q “ Bf @f P W1,p. Recall thatB : LppCq Ñ LppCq is bounded for 1 † p † 8.
AlsoB : Ws,ppCq Ñ Ws,ppCq is bounded for 1 † p † 8 and s ° 0.
Introduction QC mappings of the whole plane QC mappings on domains The end
QC mappings of the whole plane
Introduction QC mappings of the whole plane QC mappings on domains The end
The Beltrami equation
1 p
p“ 1 p“ 8
µ
Let µP L8c pCq with :“ }µ}8† 1.
The Beltrami equation
¯Bf pzq “ µpzqBf pzq has a unique solution f P Wloc1,2such that fpzq “ z ` Op1{zq as z Ñ 8. Consider
h:“ µ ` µBpµq ` µBpµBpµqq ` ¨ ¨ ¨
“pI ´ µBq´1pµq,
since}µ ¨ B}p2,2q§ }B}p2,2q“ † 1. Then, hP L2 and f “ ⇡z1 ˚ h ` z. This remains true if}B}pp,pq† 1{.
Introduction QC mappings of the whole plane QC mappings on domains The end
The Beltrami equation
1 p
µ
Wlocs,p
0 2 s
f
Let µP L8c pCq with :“ }µ}8† 1.
The Beltrami equation
¯Bf pzq “ µpzqBf pzq has a unique solution f P Wloc1,2such that fpzq “ z ` Op1{zq as z Ñ 8.
Consider
h:“ µ ` µBpµq ` µBpµBpµqq ` ¨ ¨ ¨
“pI ´ µBq´1pµq,
since}µ ¨ B}p2,2q§ }B}p2,2q“ † 1. Then, hP L2 and f “ ⇡z1 ˚ h ` z. This remains true if}B}pp,pq† 1{.
Introduction QC mappings of the whole plane QC mappings on domains The end
The Beltrami equation
1 p
µ
Wlocs,p
0 2 s
f
Let µP L8c pCq with :“ }µ}8† 1.
The Beltrami equation
¯Bf pzq “ µpzqBf pzq has a unique solution f P Wloc1,2such that fpzq “ z ` Op1{zq as z Ñ 8.
Consider
h:“ µ ` µBpµq ` µBpµBpµqq ` ¨ ¨ ¨
“pI ´ µBq´1pµq,
since}µ ¨ B}p2,2q§ }B}p2,2q“ † 1. Then, hP L2 and f “ ⇡z1 ˚ h ` z. This remains true if}B}pp,pq† 1{.
Introduction QC mappings of the whole plane QC mappings on domains The end
The Beltrami equation
1 p
µ
Wlocs,p
0 2 s
f
Let µP L8c pCq with :“ }µ}8† 1.
The Beltrami equation
¯Bf pzq “ µpzqBf pzq has a unique solution f P Wloc1,2such that fpzq “ z ` Op1{zq as z Ñ 8.
Consider
h:“ µ ` µBpµq ` µBpµBpµqq ` ¨ ¨ ¨
“pI ´ µBq´1pµq,
since}µ ¨ B}p2,2q§ }B}p2,2q“ † 1. Then, hP L2 and f “ ⇡z1 ˚ h ` z. This remains true if}B}pp,pq† 1{.
Introduction QC mappings of the whole plane QC mappings on domains The end
The Beltrami equation
1 p
µ
Wlocs,p
0 2 s
f
Let µP L8c pCq with :“ }µ}8† 1.
The Beltrami equation
¯Bf pzq “ µpzqBf pzq has a unique solution f P Wloc1,2such that fpzq “ z ` Op1{zq as z Ñ 8.
Consider
h:“ µ ` µBpµq ` µBpµBpµqq ` ¨ ¨ ¨
“pI ´ µBq´1pµq,
since}µ ¨ B}p2,2q§ }B}p2,2q“ † 1.
Then, hP L2 and f “ ⇡z1 ˚ h ` z. This remains true if}B}pp,pq† 1{.
Introduction QC mappings of the whole plane QC mappings on domains The end
The Beltrami equation
1 p
µ
Wlocs,p
0 2 s
f
h
Let µP L8c pCq with :“ }µ}8† 1.
The Beltrami equation
¯Bf pzq “ µpzqBf pzq has a unique solution f P Wloc1,2such that fpzq “ z ` Op1{zq as z Ñ 8.
Consider
h:“ µ ` µBpµq ` µBpµBpµqq ` ¨ ¨ ¨
“pI ´ µBq´1pµq,
since}µ ¨ B}p2,2q§ }B}p2,2q“ † 1.
Then, hP L2
and f “ ⇡z1 ˚ h ` z. This remains true if}B}pp,pq† 1{.
Introduction QC mappings of the whole plane QC mappings on domains The end
The Beltrami equation
1 p
µ
Wlocs,p
0 2 s
f
h
Let µP L8c pCq with :“ }µ}8† 1.
The Beltrami equation
¯Bf pzq “ µpzqBf pzq has a unique solution f P Wloc1,2such that fpzq “ z ` Op1{zq as z Ñ 8.
Consider
h:“ µ ` µBpµq ` µBpµBpµqq ` ¨ ¨ ¨
“pI ´ µBq´1pµq,
since}µ ¨ B}p2,2q§ }B}p2,2q“ † 1.
Then, hP L2 and f “ ⇡z1 ˚ h ` z.
This remains true if}B}pp,pq† 1{.
Introduction QC mappings of the whole plane QC mappings on domains The end
The Beltrami equation
1 p
µ
Wlocs,p
0 2 s
f
h
Let µP L8c pCq with :“ }µ}8† 1.
The Beltrami equation
¯Bf pzq “ µpzqBf pzq has a unique solution f P Wloc1,2such that fpzq “ z ` Op1{zq as z Ñ 8.
Consider
h:“ µ ` µBpµq ` µBpµBpµqq ` ¨ ¨ ¨
“pI ´ µBq´1pµq,
since}µ ¨ B}p2,2q§ }B}p2,2q“ † 1.
Then, hP L2 and f “ ⇡z1 ˚ h ` z.
This remains true if}B}pp,pq † 1{.
Introduction QC mappings of the whole plane QC mappings on domains The end
Results without boundaries
Wlocs,p
1 p
s
0 2
µ
`1 1
`1
Let µP L8c pCq with :“ }µ}8† 1.
hP Lp for p1
† 1p [A92, AIS01]. µP VMOpˆCq ùñ h P Lp for 1† p † 8. [I]
µP Clocn`" ùñ h P Clocn`"[AIM]. µP Asp,q ùñ h P Asp,q for sp° 2 [CMO].
µP W1,2 ùñ h P W1,2´"for p“ 2 [CFMOZ].
µP W1,p ùñ h P W1,q for p† 2,
1
q °1p`p1 [CFMOZ].
Introduction QC mappings of the whole plane QC mappings on domains The end
Results without boundaries
Wlocs,p
1 p
s
0 2
µ 1 h
p
1 p1
Let µP L8c pCq with :“ }µ}8† 1.
hP Lp for p1
† 1p [A92, AIS01].
µP VMOpˆCq ùñ h P Lp for 1† p † 8. [I]
µP Clocn`" ùñ h P Clocn`"[AIM]. µP Asp,q ùñ h P Asp,q for sp° 2 [CMO].
µP W1,2 ùñ h P W1,2´"for p“ 2 [CFMOZ].
µP W1,p ùñ h P W1,q for p† 2,
1
q °1p`p1 [CFMOZ].
Introduction QC mappings of the whole plane QC mappings on domains The end
Results without boundaries
Wlocs,p
1 p
s
0 2
f
µ 1 h
p
1 p1
Let µP L8c pCq with :“ }µ}8† 1.
hP Lp for p1
† 1p [A92, AIS01].
µP VMOpˆCq ùñ h P Lp for 1† p † 8. [I]
µP Clocn`" ùñ h P Clocn`"[AIM]. µP Asp,q ùñ h P Asp,q for sp° 2 [CMO].
µP W1,2 ùñ h P W1,2´"for p“ 2 [CFMOZ].
µP W1,p ùñ h P W1,q for p† 2,
1
q °1p`p1 [CFMOZ].
Introduction QC mappings of the whole plane QC mappings on domains The end
Results without boundaries
Wlocs,p
1 p
s
0 2
µ 1
p
1 p1
Let µP L8c pCq with :“ }µ}8† 1.
hP Lp for p1
† 1p [A92, AIS01].
µP VMOpˆCq
ùñ h P Lp for 1† p † 8. [I]
µP Clocn`" ùñ h P Clocn`"[AIM]. µP Asp,q ùñ h P Asp,q for sp° 2 [CMO].
µP W1,2 ùñ h P W1,2´"for p“ 2 [CFMOZ].
µP W1,p ùñ h P W1,q for p† 2,
1
q °1p`p1 [CFMOZ].
Introduction QC mappings of the whole plane QC mappings on domains The end
Results without boundaries
Wlocs,p
1 p
s
0 2
µ h
1 p
1 p1
Let µP L8c pCq with :“ }µ}8† 1.
hP Lp for p1
† 1p [A92, AIS01].
µP VMOpˆCq ùñ h P Lp for 1† p † 8. [I]
µP Clocn`" ùñ h P Clocn`"[AIM]. µP Asp,q ùñ h P Asp,q for sp° 2 [CMO].
µP W1,2 ùñ h P W1,2´"for p“ 2 [CFMOZ].
µP W1,p ùñ h P W1,q for p† 2,
1
q °1p`p1 [CFMOZ].
Introduction QC mappings of the whole plane QC mappings on domains The end
Results without boundaries
Wlocs,p
1 p
s
0 2
f
µ h
1 p
1 p1
Let µP L8c pCq with :“ }µ}8† 1.
hP Lp for p1
† 1p [A92, AIS01].
µP VMOpˆCq ùñ h P Lp for 1† p † 8. [I]
µP Clocn`" ùñ h P Clocn`"[AIM]. µP Asp,q ùñ h P Asp,q for sp° 2 [CMO].
µP W1,2 ùñ h P W1,2´"for p“ 2 [CFMOZ].
µP W1,p ùñ h P W1,q for p† 2,
1
q °1p`p1 [CFMOZ].
Introduction QC mappings of the whole plane QC mappings on domains The end
Results without boundaries
Wlocs,p
1 p
s
0 2
µ
1 p
1 p1
Let µP L8c pCq with :“ }µ}8† 1.
hP Lp for p1
† 1p [A92, AIS01].
µP VMOpˆCq ùñ h P Lp for 1† p † 8. [I]
µP Clocn`"
ùñ h P Clocn`"[AIM]. µP Asp,q ùñ h P Asp,q for sp° 2 [CMO].
µP W1,2 ùñ h P W1,2´"for p“ 2 [CFMOZ].
µP W1,p ùñ h P W1,q for p† 2,
1
q °1p`p1 [CFMOZ].
Introduction QC mappings of the whole plane QC mappings on domains The end
Results without boundaries
Wlocs,p
1 p
s
0 2
µ h
1 p
1 p1
Let µP L8c pCq with :“ }µ}8† 1.
hP Lp for p1
† 1p [A92, AIS01].
µP VMOpˆCq ùñ h P Lp for 1† p † 8. [I]
µP Clocn`" ùñ h P Clocn`"[AIM].
µP Asp,q ùñ h P Asp,q for sp° 2 [CMO].
µP W1,2 ùñ h P W1,2´"for p“ 2 [CFMOZ].
µP W1,p ùñ h P W1,q for p† 2,
1
q °1p`p1 [CFMOZ].
Introduction QC mappings of the whole plane QC mappings on domains The end
Results without boundaries
Wlocs,p
1 p
s
0 2
f
µ h
1 p
1 p1
Let µP L8c pCq with :“ }µ}8† 1.
hP Lp for p1
† 1p [A92, AIS01].
µP VMOpˆCq ùñ h P Lp for 1† p † 8. [I]
µP Clocn`" ùñ h P Clocn`"[AIM].
µP Asp,q ùñ h P Asp,q for sp° 2 [CMO].
µP W1,2 ùñ h P W1,2´"for p“ 2 [CFMOZ].
µP W1,p ùñ h P W1,q for p† 2,
1
q °1p`p1 [CFMOZ].
Introduction QC mappings of the whole plane QC mappings on domains The end
Results without boundaries
Wlocs,p
1 p
s
0 2
µ
1 p
1 p1
Let µP L8c pCq with :“ }µ}8† 1.
hP Lp for p1
† 1p [A92, AIS01].
µP VMOpˆCq ùñ h P Lp for 1† p † 8. [I]
µP Clocn`" ùñ h P Clocn`"[AIM].
µP Asp,q
ùñ h P Asp,q for sp° 2 [CMO].
µP W1,2 ùñ h P W1,2´"for p“ 2 [CFMOZ].
µP W1,p ùñ h P W1,q for p† 2,
1
q °1p`p1 [CFMOZ].
Introduction QC mappings of the whole plane QC mappings on domains The end
Results without boundaries
Wlocs,p
1 p
s
0 2
µ h
1 p
1 p1
Let µP L8c pCq with :“ }µ}8† 1.
hP Lp for p1
† 1p [A92, AIS01].
µP VMOpˆCq ùñ h P Lp for 1† p † 8. [I]
µP Clocn`" ùñ h P Clocn`"[AIM].
µP Asp,q ùñ h P Asp,q for sp° 2 [CMO].
µP W1,2 ùñ h P W1,2´"for p“ 2 [CFMOZ].
µP W1,p ùñ h P W1,q for p† 2,
1
q °1p`p1 [CFMOZ].
Introduction QC mappings of the whole plane QC mappings on domains The end
Results without boundaries
Wlocs,p
1 p
s
0 2
f
µ h
1 p
1 p1
Let µP L8c pCq with :“ }µ}8† 1.
hP Lp for p1
† 1p [A92, AIS01].
µP VMOpˆCq ùñ h P Lp for 1† p † 8. [I]
µP Clocn`" ùñ h P Clocn`"[AIM].
µP Asp,q ùñ h P Asp,q for sp° 2 [CMO].
µP W1,2 ùñ h P W1,2´"for p“ 2 [CFMOZ].
µP W1,p ùñ h P W1,q for p† 2,
1
q °1p`p1 [CFMOZ].
Introduction QC mappings of the whole plane QC mappings on domains The end
Results without boundaries
Wlocs,p
1 p
s
0 2
µ
1 p
1 p1
Let µP L8c pCq with :“ }µ}8† 1.
hP Lp for p1
† 1p [A92, AIS01].
µP VMOpˆCq ùñ h P Lp for 1† p † 8. [I]
µP Clocn`" ùñ h P Clocn`"[AIM].
µP Asp,q ùñ h P Asp,q for sp° 2 [CMO].
µP W1,2
ùñ h P W1,2´"for p“ 2 [CFMOZ].
µP W1,p ùñ h P W1,q for p† 2,
1
q °1p`p1 [CFMOZ].
Introduction QC mappings of the whole plane QC mappings on domains The end
Results without boundaries
Wlocs,p
1 p
s
0 2
µ h
1 p
1 p1
Let µP L8c pCq with :“ }µ}8† 1.
hP Lp for p1
† 1p [A92, AIS01].
µP VMOpˆCq ùñ h P Lp for 1† p † 8. [I]
µP Clocn`" ùñ h P Clocn`"[AIM].
µP Asp,q ùñ h P Asp,q for sp° 2 [CMO].
µP W1,2 ùñ h P W1,2´"for p“ 2 [CFMOZ].
µP W1,p ùñ h P W1,q for p† 2,
1
q °1p`p1 [CFMOZ].
Introduction QC mappings of the whole plane QC mappings on domains The end
Results without boundaries
Wlocs,p
1 p
s
0
2 f
µ h
1 p
1 p1
Let µP L8c pCq with :“ }µ}8† 1.
hP Lp for p1
† 1p [A92, AIS01].
µP VMOpˆCq ùñ h P Lp for 1† p † 8. [I]
µP Clocn`" ùñ h P Clocn`"[AIM].
µP Asp,q ùñ h P Asp,q for sp° 2 [CMO].
µP W1,2 ùñ h P W1,2´"for p“ 2 [CFMOZ].
µP W1,p ùñ h P W1,q for p† 2,
1
q °1p`p1 [CFMOZ].
Introduction QC mappings of the whole plane QC mappings on domains The end
Results without boundaries
Wlocs,p
1 p
s
0 2
µ
1 p
1 p1
Let µP L8c pCq with :“ }µ}8† 1.
hP Lp for p1
† 1p [A92, AIS01].
µP VMOpˆCq ùñ h P Lp for 1† p † 8. [I]
µP Clocn`" ùñ h P Clocn`"[AIM].
µP Asp,q ùñ h P Asp,q for sp° 2 [CMO].
µP W1,2 ùñ h P W1,2´"for p“ 2 [CFMOZ].
µP W1,p
ùñ h P W1,q for p† 2,
1
q °1p`p1 [CFMOZ].
Introduction QC mappings of the whole plane QC mappings on domains The end
Results without boundaries
Wlocs,p
1 p
s
0 2
µ h
1 p
1 p1
Let µP L8c pCq with :“ }µ}8† 1.
hP Lp for p1
† 1p [A92, AIS01].
µP VMOpˆCq ùñ h P Lp for 1† p † 8. [I]
µP Clocn`" ùñ h P Clocn`"[AIM].
µP Asp,q ùñ h P Asp,q for sp° 2 [CMO].
µP W1,2 ùñ h P W1,2´"for p“ 2 [CFMOZ].
µP W1,p ùñ h P W1,q for p† 2,
1
q °1p`p1 [CFMOZ].
Introduction QC mappings of the whole plane QC mappings on domains The end
Results without boundaries
Wlocs,p
1 p
s
0
2 f
µ h
1 p
1 p1
Let µP L8c pCq with :“ }µ}8† 1.
hP Lp for p1
† 1p [A92, AIS01].
µP VMOpˆCq ùñ h P Lp for 1† p † 8. [I]
µP Clocn`" ùñ h P Clocn`"[AIM].
µP Asp,q ùñ h P Asp,q for sp° 2 [CMO].
µP W1,2 ùñ h P W1,2´"for p“ 2 [CFMOZ].
µP W1,p ùñ h P W1,q for p† 2,
1
q °1p`p1 [CFMOZ].
Introduction QC mappings of the whole plane QC mappings on domains The end
Recent progress
Theorem (P.)
Let 0† s † 2, 1 † p † 8, let µ P Ws,pX L8, with µ§ D and let f be the principal solution to the Beltrami equation ¯Bf “ µBf .
If s“ 2p, then
Bf P W¯ s,q for every 1 q ° 1
p. If s† 2p and 1p † p11 ´p1 “ 1´1`, then
¯Bf P Ws,q for every 1 q ° 1
p` 1 p
.
See [Clop, Faraco, Ruiz] for previous weaker results and Bais´on’s thesis for a stronger result in the critical setting with s° 1{2.
It remains unclear if the condition 1p † p11
´p1 can be replaced by 1p †p11, which is more natural and is achieved for s“ 1.
Introduction QC mappings of the whole plane QC mappings on domains The end
Recent progress
Theorem (P.)
Let 0† s † 2, 1 † p † 8, let µ P Ws,pX L8, with µ§ D and let f be the principal solution to the Beltrami equation ¯Bf “ µBf .
If s“ 2p, then
Bf P W¯ s,q for every 1 q ° 1
p. If s† 2p and 1p † p11 ´p1 “ 1´1`, then
¯Bf P Ws,q for every 1 q ° 1
p` 1 p
.
See [Clop, Faraco, Ruiz] for previous weaker results and Bais´on’s thesis for a stronger result in the critical setting with s° 1{2.
It remains unclear if the condition 1p † p11
´p1 can be replaced by 1p †p11, which is more natural and is achieved for s“ 1.
Introduction QC mappings of the whole plane QC mappings on domains The end
Recent progress
Theorem (P.)
Let 0† s † 2, 1 † p † 8, let µ P Ws,pX L8, with µ§ D and let f be the principal solution to the Beltrami equation ¯Bf “ µBf .
If s“ 2p, then
Bf P W¯ s,q for every 1 q ° 1
p. If s† 2p and 1p † p11 ´p1 “ 1´1`, then
¯Bf P Ws,q for every 1 q ° 1
p` 1 p
.
See [Clop, Faraco, Ruiz] for previous weaker results and Bais´on’s thesis for a stronger result in the critical setting with s° 1{2.
It remains unclear if the condition 1p † p11 ´p1 can be replaced by p1 †p11, which is more natural and is achieved for s“ 1.
Introduction QC mappings of the whole plane QC mappings on domains The end
Idea
Ws,p
1 p
s
0 2
µ
µ
1 p
1 p1
µP L8X Ws,p
h :“ pI ´ µBq´1pµq h“ µBh ` µ.
BµBh P Lq, qP pp1, pq: H¨older rDs, µsBh P Lq: Kato-Ponce
s“ 1
Bh “ BpµBhq ` Bµ Bh “ µBBh ` BµBh ` Bµ Bh “ µBBh ` BµBh ` Bµ pI ´ µBqBh “ BµBh ` Bµ Bh “ pI ´ µBq´1pBµBh ` Bµq
s† 1
Dsh“ DspµBhq ` Dsµ
Dsh“ µDsBh ´ rDs, µspBhq ` Dsµ Dsh“ µBDsh´ rDs, µspBhq ` Dsµ pI ´ µBqDsh“ ´rDs, µspBhq ` Dsµ Dsh“ pI ´µBq´1pDsµ´rDs, µspBhqq
Introduction QC mappings of the whole plane QC mappings on domains The end
Idea
Ws,p
1 p
s
0 2
h µ
1 p
1 p1
µP L8X Ws,p h :“ pI ´ µBq´1pµq
h“ µBh ` µ.
BµBh P Lq, qP pp1, pq: H¨older rDs, µsBh P Lq: Kato-Ponce
s“ 1
Bh “ BpµBhq ` Bµ Bh “ µBBh ` BµBh ` Bµ Bh “ µBBh ` BµBh ` Bµ pI ´ µBqBh “ BµBh ` Bµ Bh “ pI ´ µBq´1pBµBh ` Bµq
s† 1
Dsh“ DspµBhq ` Dsµ
Dsh“ µDsBh ´ rDs, µspBhq ` Dsµ Dsh“ µBDsh´ rDs, µspBhq ` Dsµ pI ´ µBqDsh“ ´rDs, µspBhq ` Dsµ Dsh“ pI ´µBq´1pDsµ´rDs, µspBhqq
Introduction QC mappings of the whole plane QC mappings on domains The end
Idea
Ws,p
1 p
s
0 2
h µ
1 p
1 p1
µP L8X Ws,p h :“ pI ´ µBq´1pµq h“ µBh ` µ.
BµBh P Lq, qP pp1, pq: H¨older rDs, µsBh P Lq: Kato-Ponce
s“ 1
Bh “ BpµBhq ` Bµ Bh “ µBBh ` BµBh ` Bµ Bh “ µBBh ` BµBh ` Bµ pI ´ µBqBh “ BµBh ` Bµ Bh “ pI ´ µBq´1pBµBh ` Bµq
s† 1
Dsh“ DspµBhq ` Dsµ
Dsh“ µDsBh ´ rDs, µspBhq ` Dsµ Dsh“ µBDsh´ rDs, µspBhq ` Dsµ pI ´ µBqDsh“ ´rDs, µspBhq ` Dsµ Dsh“ pI ´µBq´1pDsµ´rDs, µspBhqq
Introduction QC mappings of the whole plane QC mappings on domains The end
Idea
Ws,p
1 p
s
0 2
h µ
1 p
1 p1
µP L8X Ws,p h :“ pI ´ µBq´1pµq h“ µBh ` µ.
BµBh P Lq, qP pp1, pq: H¨older rDs, µsBh P Lq: Kato-Ponce
s“ 1
Bh “ BpµBhq ` Bµ Bh “ µBBh ` BµBh ` Bµ Bh “ µBBh ` BµBh ` Bµ pI ´ µBqBh “ BµBh ` Bµ Bh “ pI ´ µBq´1pBµBh ` Bµq
s† 1
Dsh“ DspµBhq ` Dsµ
Dsh“ µDsBh ´ rDs, µspBhq ` Dsµ Dsh“ µBDsh´ rDs, µspBhq ` Dsµ pI ´ µBqDsh“ ´rDs, µspBhq ` Dsµ Dsh“ pI ´µBq´1pDsµ´rDs, µspBhqq
Introduction QC mappings of the whole plane QC mappings on domains The end
Idea
Ws,p
1 p
s
0 2
h µ
1 p
1 p1
µP L8X Ws,p h :“ pI ´ µBq´1pµq h“ µBh ` µ.
BµBh P Lq, qP pp1, pq: H¨older rDs, µsBh P Lq: Kato-Ponce
s“ 1
Bh “ BpµBhq ` Bµ
Bh “ µBBh ` BµBh ` Bµ Bh “ µBBh ` BµBh ` Bµ pI ´ µBqBh “ BµBh ` Bµ Bh “ pI ´ µBq´1pBµBh ` Bµq
s† 1
Dsh“ DspµBhq ` Dsµ
Dsh“ µDsBh ´ rDs, µspBhq ` Dsµ Dsh“ µBDsh´ rDs, µspBhq ` Dsµ pI ´ µBqDsh“ ´rDs, µspBhq ` Dsµ Dsh“ pI ´µBq´1pDsµ´rDs, µspBhqq
Introduction QC mappings of the whole plane QC mappings on domains The end
Idea
Ws,p
1 p
s
0 2
h µ
1 p
1 p1
µP L8X Ws,p h :“ pI ´ µBq´1pµq h“ µBh ` µ.
BµBh P Lq, qP pp1, pq: H¨older rDs, µsBh P Lq: Kato-Ponce
s“ 1
Bh “ BpµBhq ` Bµ
Bh “ µBBh ` BµBh ` Bµ Bh “ µBBh ` BµBh ` Bµ pI ´ µBqBh “ BµBh ` Bµ Bh “ pI ´ µBq´1pBµBh ` Bµq
s† 1
Dsh“ DspµBhq ` Dsµ
Dsh“ µDsBh ´ rDs, µspBhq ` Dsµ Dsh“ µBDsh´ rDs, µspBhq ` Dsµ pI ´ µBqDsh“ ´rDs, µspBhq ` Dsµ Dsh“ pI ´µBq´1pDsµ´rDs, µspBhqq
Introduction QC mappings of the whole plane QC mappings on domains The end
Idea
Ws,p
1 p
s
0 2
h µ
1 p
1 p1
µP L8X Ws,p h :“ pI ´ µBq´1pµq h“ µBh ` µ.
BµBh P Lq, qP pp1, pq: H¨older rDs, µsBh P Lq: Kato-Ponce
s“ 1
Bh “ BpµBhq ` Bµ
Bh “ µBBh ` BµBh ` Bµ Bh “ µBBh ` BµBh ` Bµ pI ´ µBqBh “ BµBh ` Bµ Bh “ pI ´ µBq´1pBµBh ` Bµq
s† 1
Dsh“ DspµBhq ` Dsµ
Dsh“ µDsBh ´ rDs, µspBhq ` Dsµ Dsh“ µBDsh´ rDs, µspBhq ` Dsµ pI ´ µBqDsh“ ´rDs, µspBhq ` Dsµ Dsh“ pI ´µBq´1pDsµ´rDs, µspBhqq
Introduction QC mappings of the whole plane QC mappings on domains The end
Idea
Ws,p
1 p
s
0 2
h µ
1 p
1 p1
µP L8X Ws,p h :“ pI ´ µBq´1pµq h“ µBh ` µ.
BµBh P Lq, qP pp1, pq: H¨older rDs, µsBh P Lq: Kato-Ponce
s“ 1
Bh “ BpµBhq ` Bµ Bh “µBBh ` BµBh` Bµ
Bh “ µBBh ` BµBh ` Bµ pI ´ µBqBh “ BµBh ` Bµ Bh “ pI ´ µBq´1pBµBh ` Bµq
s† 1
Dsh“ DspµBhq ` Dsµ
Dsh“ µDsBh ´ rDs, µspBhq ` Dsµ Dsh“ µBDsh´ rDs, µspBhq ` Dsµ pI ´ µBqDsh“ ´rDs, µspBhq ` Dsµ Dsh“ pI ´µBq´1pDsµ´rDs, µspBhqq
Introduction QC mappings of the whole plane QC mappings on domains The end
Idea
Ws,p
1 p
s
0 2
h µ
1 p
1 p1
µP L8X Ws,p h :“ pI ´ µBq´1pµq h“ µBh ` µ.
BµBh P Lq, qP pp1, pq: H¨older rDs, µsBh P Lq: Kato-Ponce
s“ 1
Bh “ BpµBhq ` Bµ Bh “ µBBh ` BµBh ` Bµ Bh “ µBBh` BµBh ` Bµ
pI ´ µBqBh “ BµBh ` Bµ Bh “ pI ´ µBq´1pBµBh ` Bµq
s† 1
Dsh“ DspµBhq ` Dsµ
Dsh“ µDsBh ´ rDs, µspBhq ` Dsµ Dsh“ µBDsh´ rDs, µspBhq ` Dsµ pI ´ µBqDsh“ ´rDs, µspBhq ` Dsµ Dsh“ pI ´µBq´1pDsµ´rDs, µspBhqq