Quantization
and
generalized
Kohler
structures Work
in
progress
with
Francis
Bischoff
Quantization Kohler structures and generalized Work Bischoff - - PowerPoint PPT Presentation
Quantization Kohler structures and generalized Work Bischoff Francis with in progress Based arXiv 1804.05412 our paper : : on . . . - model The Zunino 2nd 19-79 r : Is Nig ) } { csih ) ( ( Lorentz Riemann II - I N
Quantization
and
generalized
Kohler
structures Work
in
progress
with
Francis
Bischoff
Based
paper
:arXiv
:
1804.05412
19-79
Zunino
:The
2nd
r
{ csih )
Is
Nig ) }
(Lorentz
( RiemannInherits
N -6,2 ) Susy
from
Koike
I
!TMO
II
19-84
Gates
is
truefor
generalized
Kahler
( It
, I . )g
complex
structures
St
.d¥=o
,dd'±w±#
wt
, wforms
Katherine
g%=z¥Zz
( U
,#
, ,Zn ))
complex
chart
,K
E(
U
, IR )Zunino :
Use
complex
str
.to
extend
9
:S
→M to
asuper field
I
:E
→M
Then
action
is
{ oI*K
droke
Q1ianalogofkforgen.tiihler.IT
Quantization
I koihler
,w=gI
may
Pre
to
(
L
, H17 )
(
(
He !!
at:3 with
FCP )
line
bundle
⇒
It
=HMM
, L )using
Je
D
"
⑦,E①L①
I
Q2iAnalogofkandt-forGenka.hu?
G
Poi
try
:Hitchin
2006
,
MiG
.2007,2010
( Itt
I
Insist :*
." " " " "
#T=I±QtiQI±hpphu+e
QCT
't)In
the
usual
Kiihler
case ,QA
= w "and
T±
=QB
= ODeform
aKahler
structure
to
a Gkwith a.
to
Construction
GK
( M
, I . ) =a p2
T EHo I
MT )
=HYP?
013 ) )
← ←at
91
,
,
Wo
=Fubini
Kainer ←
at
it
lenient
'
Ii
tr init
⇒
I
veCOL TM )
sit
.JV
=o(
Wo )
Hit
{ Cv ,r]=o
I
+ =4 ! ( I
.)Itt
a =So
"145 It
w .ds
fg.It.I-lgeuerahzedkiihleroncp2.se
Summary
:want
Gen
.Kahler
potential
K
want
aPre )
He ,
A
key
geometrical input
:holomorphic
Poisson geometry
E
TheKoihlerpotenti#
according
to (
Donaldson
' 01 ) w =i 25
Ka
=I t.in#Ka)=5Aa,AaEr9Ua )
Aa
holomorphic
[ Aap]
eHt #-)
Glue
Tie
,to
Tq
,
/←ahkrc
using
translation
by
Aap
i⇐÷÷÷÷÷
'I
Result
Z
=II
TEKE
(
r )
symplectic
with
rly
=d (
Real
.L
is
[
Lagrangian for
Imr
Symplectic
for
Re R
" I!! Effie!:# entia.LisanA-braneforlmr.LT
Ex
( P
' ,Wes )
Z
=affine
bundle
with
class [ w ]
eH' I
r
' )=¥÷÷: :
inte
r
=dxidy
Lz
L
={
real
locus }
Moritaca-te.org
Weinstein
:study
poisson
( X
, r )via
its symplectic
realizations
i÷:
" i
"t IT
lnvolutire
is
Poisson ( X
, 't )( X
, ol( x
' , r ' )Morita
2- category ( Weinstein)
Hr )
sp
¥ip
Mort I
x , X ' ) =( xp ,
sit
.Ker t*
I
Kent '*
i.Mor
' I 2- it ')
=local
isos
ft ,r )
→LZ
' ,r
')Mor Pic ( X
, r ) = {§!!! ) µ
Picard
group
.Identity
inPic
is
adistinguished
self
Weinstein grouper'd
.⇒
: :::::÷.÷ :* :*
"
Z
=T*g
,r
=scan
a
.( X
x Indy )
2-
=a'
xet
aI
x ,y , a , b )Z
sf
It
sf It
Ceax , ytxb )
X
r=
dandlytxb
)
theorem ( Bischoff
,
M.G. , Zab zine ) (Assuming
QI
' =F
exists)
A
Generalized
Kahler
structure
Cg ,
It
, Iis
equivalent
to
aHot
. symplecticMorita
equivalence
CZ , r ) :(
x.
rt
→ txt ,q)together
with
anondegenerate C
'sbrane bisection
.
'
. .
is
z
It
f- )
( Xt , rt )
X
.ELE
Xt
t
foliations
induce
It
, IL
.Is
Z
It
F
real
and
F'
' ' ' ' +It
=F
' " "g
( X
.f- )
( Xt , rt )
unique
symmetric
tensor
S 'T
't
require
Riemannian
.Potential
function
" ii.
art
dry
=rly
isread 1mHz )
=dk
Ke
LU , R )
⇒n=2i2K
⇒
g
determined by
real
smooth
function
K
.E
( X
a
' ,x Indy )
( Z ,r )
:L X. DO
2-
=a'
xeh
a(
x ,y , a , b ). if
it :*
. ,
r=
damn dlyntnxeb )
tdlszlrdx
I
I
I
Pi
9
,Pz
192
Darboux
chat
.{
K'
19212
⇒
complete
Gen
.Kohler
metric
EZ
Quantization
Gutowitfen
:embed
( M
, w )into
( Z
,r
)
sit
.n/µ=
w#
r )
ie
.mis : :;s÷:* :*:L:3
⇒
two
branes
M
,Zee
(
L
Space filling
brane Lagrangian
brave
⇒
H=HomlM,Z#T
proposalforquautization-LC.CZ
,SL )
:two
branes
in
A
brane
Morita
( £
,Imr )
bisection
equivalence
.H=Hom(L,Zcc€
Construction
GK
( M
, I . ) =a p2
T EHo I
MT )
=HYP?
013 ) )
← ←at
91
,
,
Wo
=Fubini
Kainer ←
at
it
lenient
'
Ii
tr init
⇒
I
veCOL TM )
sit
.JV
=o(
Wo )
Hit
{ Cv ,r]=o
I
+ =4 ! ( I
.)Itt
a =So
"145 It
w .ds
fg.It.I-lgeuerahzedkiihleroncp2.se
Iterate
the
construction
,⇐
, :( X.
DO
Z
, z£12
723
Ly
d
y I
a ,
d
a,t
n ,
X
X
Xo
X
,Xz
Xz
t-qtO.HomCLoqZ.IT
algebra
lndep
.Hamiltonian
deforms
for
IP
' ,Mor
Pic
( P
' ) =PG ↳ ( a )
xPic C P
' )( 4
,Ocn ) )
If
wecompute
inthis
case
Id
A
=to Ho ( IP
' ,Ockn ) )
\k >
Id
Ay
Vandenbergh
noncommutative
deformation
A
,