noboru kawamoto (hokkaido university) in collaboration with k.asaka , a.d’adda and y.kondo
DESCRIPTION
Exact Lattice Supersymmetry at the Quantum Level for N=2 Wess-Zumino Models in Lower Dimensions. Noboru Kawamoto (Hokkaido University) In collaboration with K.Asaka , A.D’Adda and Y.Kondo. D’Adda , Feo , Kanamori , N.K., Saito . JHEP 1203 (2012) 043, JHEP 1009 (2010) 059. - PowerPoint PPT PresentationTRANSCRIPT
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Exact Lattice Supersymmetry at the Quantum Level for N=2 Wess-Zumino Models
in Lower Dimensions
Noboru Kawamoto (Hokkaido University)
In collaboration with
K.Asaka, A.D’Adda and Y.Kondo
JHEP 1203 (2012) 043, JHEP 1009 (2010) 059
D’Adda, Feo, Kanamori, N.K., Saito
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Major difficulties for lattice SUSY
(1) Difference operator does not satisfy Leibniz rule.
(2) Species doublers of lattice chiral fermion copies appear: unbalance of d.o.f. between bosons and fermions
Let’s consider the simplest lattice SUSY algebra:
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Difficulties in lattice
( 1 ) No Leibniz rule in coordinate space
( 2 ) Species doublers on lattice unbalance of fermion and boson
Solutions
Leibniz rule in momentum space latt. mom. conservation
Doublers as super partners of extended SUSY
Proposal of solution for the difficulties
No chiral fermion problem !
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Solution to (1):
Coordinate:
Momentum:
Good:
Short comings: product is non-local
loss of translational invariance
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Interpretation of (2):
translation generator of
half translation generator
Brilliuon zone
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Essense of Lattice SUSY transformation: D=N=1
species doublers
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Truncation of d.o.f. (chiral condition: D=N=2)
identification
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Wess-Zumino action in two dimensions
Kinetic term
Interaction term
Super charge exact form exact lattice SUSY inv.
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D=N=2 lattice SUSY transformation
Chiral
Anti-chiral
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N=2 Wess-Zumino actions in coordinate
product actions in two dimensions
Kinetic term
Interaction term
SUSY algebra with Leibniz rule is satisfied on product !
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Ward Identity: SUSY exact in quantum level ?
When lattice SUSY is exact:
Suppose we choose:
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Tree level Ward Identity
Tree level W.I. is satisfied.
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One loop Ward Identity:
one loop W.I. tree W.I.
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Two loop Ward Identity:
two loop W.I. tree W.I.
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Subtleties of integration domain
equal ?
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Summary of the formulation (non-gauge theory: D=N=2)
Good: Exact lattice SUSY with correct Leibniz rule on the product, quantum level exactness No chiral fermion problems (species doublers are truncated by chiral conditions)Short comings: non-local field theory Loss of translational invariance (recover at )
super Yang-Mills ?
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Breakdown of associativity
Integration region
(A)
(B)
Since and are different fields, associativity is broken
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Even though the associativity is broken the following product is well defined.
In the formulation of lattice super Yang-Mills the breakdown of the associativity is problem.
non-gauge lattice SUSY has exact symmetry
SUSY transformation is linear in fields while gauge transformation is non-linear.
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Conclusions
Exactly SUSY invariant formulation in mom. and coordinate space is found.
A new star product is defined where exact lattice SUSY algebra is fulfilled.
Another solution to chiral fermion problemSpecies doublers are physical
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N=1
N=2
=
species doubler
Momentum representation
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SUSY transformation in momentum space (N=2 in 1-dim.)
N=2 lattice SUSY algebra
continuum momentum:
species doubler
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Lattice super covariant derivative
Chiral lattice SUSY algebra (D=1,N=2)
No influence to the cont. limit
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N=2species doubler as supermultiplets
bi-local nature of SUSY transformation
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chiral
anti-chiral
Chiral conditions truncation of species doub. d.o.f.
rescaled field ! meaning ?
1-dim.
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Exact Lattice SUSY action for N=2 D=1
lattice momentum conservation
Super charge exact form exact lattice SUSY invariant
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New * product and Leibniz rule(coordinate rep.)
New star * product
Leibniz rule in lattice momentum space
Leibniz rule on * product (coordinate rep.)
Action on * product
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D=N=2 Lattice SUSY transformation
Chiral algebra
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has 4 species doublers
truncation needed
chiral conditions
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D=N=2 super covariant derivative
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Chiral conditions for D=N=2
chiral fields
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D=N=2 lattice SUSY transformation
Chiral suffix (s,s) is omitted
Anti-chiralsuffix (a,a) is omitted
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Wess-Zumino action in two dimensions
Kinetic term
Interaction term
Super charge exact form exact lattice SUSY inv.
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N=2 Wess-Zumino actions in coordinate
product actions in two dimensions
Kinetic term
Interaction term
SUSY algebra with Leibniz rule is satisfied on product !
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Conclusions
Exactly SUSY invariant formulation in mom. and coordinate space is found.
A new star product is defined where exact lattice SUSY algebra is fulfilled.
Another solution to chiral fermion problemSpecies doublers are physical
Higer dimensions, gauge extension, quantum…
the first example
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Symmetric difference operator No Leibniz rule
Possible solutions:
(1) Link approach:
(2) New star product: Leibniz rule ?
Hopf algebraic symmetry
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“inconsistency”When
BruckmannKok
but if we introduce the following “mild non-commutativity”:
then
In general
Two Problems
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Conjecture
-product formulation and link approach are equivalent.
non-locality non-commutativity
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Chiral condition
Anti-chiral condition
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Lattice super covariant derivative
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Species doublers as super multiplets in lattice supersymmetry :
Noboru KAWAMOTO Hokkaido University
In collaboration with A. D’Adda, A. Feo, I. Kanamori and J. Saito
Exact supersymmetry with interactions for D=1 N=2
JHEP 016P 0710 (hep-lat:1006.2046)
Extension to higher dimensions: D=N=2
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Lattice SUSY transformati o n
=
half lattice shift translation (1dim.)
alternating signspecies doublers as supermultiplets
+
Exact SUSY in momentum space with
New (commutative) star product in coordinate space
difference operator Link approach
Lebniz rule
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Lattice superfield:
SUSY transformation:
role of supercoordinate
hermiticity
alternating sign key of the lattice SUSY
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D=1 N=2 Lattice SUSY
Fourier transform
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Kinetic term
Mass term
Interaction term
Momentum representation
exact lattice SUSY invariance under and
Lattice mom. conservation
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Since difference operator does not satisfy Leibniz rule “ How can algebra be consistent ?”
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Symmetric difference operator No Leibniz rule
Possible solutions:
(1) Link approach:
(2) New star product: Leibniz rule ?
Hopf algebraic symmetry
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Lattice momentum:
New star product in coordinate space:
Leibniz rule in mom.
commutative
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star product Leibniz rule
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Exact SUSY invariance in coordinate space on star product actions
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