lc ICERM # at Brandan Jonathan page - oil Qcq ,t ) lk= Qcq ) - - PowerPoint PPT Presentation

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lc ICERM # at Brandan Jonathan page - oil Qcq ,t ) lk= Qcq ) - - PowerPoint PPT Presentation

Talk lc ICERM # at Brandan Jonathan page - oil Qcq ,t ) lk= Qcq ) z=q maybe Work or over . braids plus stand Hecke combinations Hn= type A 1k their of n algebra fryy 7 . 5- g) ( stg ' ) :( -0 relation qeadwti . 65


slide-1
SLIDE 1 Talk at ICERM page #

lc

Jonathan Brandan Work
  • ver
lk= Qcq )
  • r
maybe Qcq ,t ) . z=q
  • oil

Hn= type

A Hecke algebra

fryy ¥7

1k . their combinations
  • f
n stand braids plus 65 4 } 2 , qeadwti relation :( 5- g) ( stg ') .
braid elation
  • f
course !

sysitsi

'

#

5-51=-2 skein relation :

If

  • *
=
  • 2 Tp
Attn :

affie

Hecke algebra
  • add
niolibk generators f• plus relation

¥

=gyn X " ... , Xn Sn ZCAH .) =

|k[X,± ,

. . ,Xn±]
  • AH
, Bernstein cater AH , Hn ,

X.tl

... fo =

T

when
  • n
RH edge Theorem (Dipper
  • Jones
, Francis . Gahan ) ZCAHN) Z ( Hn)
slide-2
SLIDE 2 Talk at ICERM page #

Zd

Jonathan Brandan Basis for ZCHN ) :

{ m×( Xii

. . , Xn ) |× = a partition of n with fist column removed } monomial symmetric polynomial XP ! . . XP " Hsym ) eg his

¥

T

* Size = # partitions of n = #rreps = dim ZCHN) X ,tXztXztX4tXs ± Corollary The

maps

Sym

%-)

ZCHN ) , e. her

CXF

, ... ,

X±n

)

Symmettifuctwi , 7 are asymptotically faithful

n?okaan±=

ODT

"→ Conjecture The map Sym @ Sym ¥045 ZCHN) is asymptotically faithful to .

Difficult computationally

to convert

XY

into X .?s . . . Sage ? Rest of the talk : why ? ?
slide-3
SLIDE 3 Talk at ICERM page #

3f

Jonathan Brandan Heisenberg category :

Heisnft ,t )

c- k€27 central charge lk . hniarstnifmonoidal category Idea ( khouanou ) Monoidal Objects ^ , V T , f = identity adomorphusin ,

h= Heisenberg Liedgebn

presentation ^o^@u=^^v " ' Pn , qn , c Morpwsin ,

%

,

I

Baidelakon , skein relation [ pn ,qm|=

fmmc

^ ccertol
  • f
Invertible , afpieteekealatroi

A

, V Adjuidins

µ=T=4

Seek monoidal category Let

*

i=Vf

. forces P

,9i+2=EiP

, so =~ Ufhy Case k= -2 T <c=k > 17 Gmthudiecknig Declare f)

V

  • V. ]
is invertible
  • K
  • p ,=[^ ]
, q ,=[ v ] t One more data

:vz•=¥HcYded£a

.tn?nsT.trYUiiJ=ytz...Ag

[ p , ,q , ]=k AND SO On !
slide-4
SLIDE 4 Talk at ICERM page #

4c

Jonathan Brandan Basic question now

...

bases for moplusin spaces in '

Heiskk , t )

? eg End ( 11 ) v
  • na
  • v
Bubbles . . . 27

%

~ Follows from earlier conjecture ! Sym @ fgm The point : Heis .

.tt

it )

C ,

nztf

Hn . mod T acts by " induction "

f

acts by " restrictor " Her 's .dz ,t )

G

replace An with level Zcydobmi Hecke algebras :
  • To
finish , I 'll show you the case k=O
  • slightly
easier ! In

fact

, Heisofz ,t ) Is affinitaton of HOMFLY skein category

(

Turaev

)

slide-5
SLIDE 5 Talk at ICERM page #

5b

Jonathan Brandan Let

t=qn

.

DIDIIIDI

' Dim

Uqlgen)

Quantum group long )

ftp.fng.l?ytI...ntEifit2l

Ej=

Eirfrj

  • I
' Erjfir v higher

V

natural representation not

{ fg=

frj

Fir

  • qtfirfrj
" " 4
  • f
dimension m ellneub

Heigcz .tl T

acts as Vxo
  • f
acts as V * @
  • ffunctor
)

D

%

acts as

VxoV@M-sVxoVxOM.R-matmVxoVD.v

( natural transformation )

UqGln)

  • mod
12 acts as V @ M Mxov , Vxom , R . matrix squared . v = t.tt =

9q÷i

, " =

[

n ) Quantum dimension
  • f

slide-6
SLIDE 6 Talk at ICERM page # 6 b Jonathan Brandan

Ennis

.9!H

End ( Ida .ge

. ,.mµl=Z(Uqfsen )) ,€k[xF , ... , xntysn

X ;

=EM§"

" Er ,iDr Frj Dj

(

Ei ,i= Fin . = E '

)

If

m > v
  • m
it

§

, fin " E

Xii

,

Xiii

' ' Xim .

"

i

¥

,,§⇐t±¥"

Eitiiiimfmgmosafetfeifsymmeni, If

meo Similar but I ' in ' place
  • f
x. . . Laurent sgmmeki functions .

The

basis theorem follows °o°

THEIR