Exceptional collections and the geometry of partial flag varieties
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2 exceptional collections in derived categories of coherent sheaves on partial flag varieties G/P The first half of the seminar is dedicated to the general
Department of Mathematics — Fall/Winter 2015 - Illinois Math
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A parallel geometry seminar, the Geometric Potpourri seminar Beberman award “for exceptional contributions to the field of teacher
CV – Anthony Ashmore
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[18] “The exceptional generalised geometry of supersymmetric AdS flux backgrounds” Organiser for Particle Theory Seminar series at University of Chicago
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10 déc 2019 F19 enumerative geometry seminar notes geometry is a case of this Looking at the structure of the exceptional fiber vs H,
Seminar: Lie groups, Lie algebras and symmetric spaces
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In the first part of the seminar we mainly follow the lecture notes by Wolf- gang Ziller [12] 2 Geometric significance of the exceptional Lie
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Exceptional collections and rationality Algebraic Geometry Seminar University of Michigan, Ann Arbor March 2021 Some comments on semi-orthogonal
derived categories and variation of geometric invariant theory
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SEMINAR: DERIVED CATEGORIES AND VARIATION OF GEOMETRIC Then, for a triangulated category T , define the notion of a (full) exceptional collection; for
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4 oct 2018 KCL/UCL Junior Geometry Seminar [Griffiths–Harris, Principle of algebraic geometry] Mirko Mauri is called exceptional divisor
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By contrast, the theory of manifolds of exceptional holonomy is a wide-open field: ern California Symplectic Geometry Seminar Vol 196 Amer Math
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X
n X !0 (1;1) za ! 0=iX a;bg abdzad z b; (gab) !0 X !0 [!0]2H2(X;) ! =!0+i@ @ gab g ab+@2 @z a@ z b: (1;1) K 1X= nTX =i@ @L;L L= g ab+@2 @z a@ z b : S X =!= 1; 10 c1(X) S= c1(X);[!] c1(X) [!] S !=Lv! v Lv v= 0 v @! @t =! : @! @t =i@ @S; = 1= 0 = 1 = 1 X
E (X;!0)
c1(E) = 0 E E E SO(E) c1(S)<0 X L (X;L) (X;L)
X :X! L!X
L
(X;L) 1(1) XLj 1(1)=Lr r X X X0= 1(0) X0= 1(0) L
0
(X0;L0) k! 1 H0(X0;Lk0) (X) (X;L) (X)0 X
X X
X c1(L) (X;L) X0 c1(L0)X0 S1
HX0
(X) =Z X
0(S ^S)H d;
S X0^S S
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P L
P(f) =Z
@P fd AZ P fd; A LP f Z P f d= 0;Z P f x id= 0 xi f f=frg frg QPL f P f2QPL LP(f)>0 fP L
P(f)>0
>0 f2QPL L
P(f)Z
P jfjd: ^K (X;L) P X X0 X 2 1 (!s) = (1 s)+s!s; (1;1) !t X ti! 1 t0i (X;!t0i) Z (X;!t) t! 1 Z=X X X Z
X
Z X nX =! (2)n(n+1)n X=n =g g K Z p2Z p Zp Z p(f) =r!0 Brjfj r;
Br r Z p
T=()rN WN W T r= 1 W W 0 4 (X) (X)>1 (X) =k!1k(X) k=D(X;D): kDP iDi siH0 k=H0(X;K kX) kH0 k 1 [!0] H
H=f:!0+i@
@ >0g: H kk2=Z X ()2d; d !n/n! H (X;!0) H S1 (1;1) Ω(0;1)S1XΩn+1= 0 H 1 H F F=Z X ()(S ^S)d;
S ^S
H H C1;1 H V ! !0 V !n0=!n 0 !0
F() =Z
X V Vd0+J0(); J 0=Z X ()0^!n 1: FC1;1 H F H H L1
L2
E
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L1 E1 H (M;g) mp2M p p (M;g) G
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G2SO(7) (7)SO(8) 7 ;;
V m m92< p < m 2
pV GL(V) GL(V) m= 7p= 3 V 23V V v7!iv()^iv()^: 7V 3 3 GL+(V) GL+(V) 3 G2 3 g
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g jj2= 7 g g W=V t 3 4 Ω =^dt+24(W): ΩGL+(W) (7) SO(7) A GL+(W)Ω 4W A 64 21 = 43 A
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Z
W
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C ~D
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M
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M V
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Q() =d
dV dt =kdk2; G2 Pc G2 7
N/
3 G2 0
MH1(M;) =
0
G2 S7 G2 G2 G2 K 1Z K 1Z G2 G2
MH3(M;)
b3 p1(M)2 H
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3 S4
G2 G2 (7)/G2 G
2
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2S1 Y S2
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