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(Elliptic) multiple zeta valuesin open superstring amplitudes
Johannes BroedelHumboldt University Berlin
based on joint work with Carlos Mafra, Nils Matthes and Oliver SchlottererarXiv:1412.5535, arXiv:1507.02254
Selected Topics in Theoretical High Energy Physicstbilisi, sakartvelo, September 21st, 2015
IntroductionGoal: scattering amplitudes/cross sections in a field or string theory• standard method: Feynman/worldsheet graphs, useful and cumbersome• alternative idea: add symmetry→ obtain a more symmetric/constrained theory
→ learn about structure→ remove symmetry→ what remains• typical results: new language: special functions for particular theory
(e.g. spinor-helicity for massless theories)recursion relations: relate N -point to (N − 1)-point
• best scenario: avoid Feynman calculations completely/S-matrix approach
This talk:Open string theory as a simple (and very symmetric) testing ground• tree-level: polylogarithms (language) and Drinfeld associator (recursion)• one-loop elliptic iterated integrals (language) and elliptic multiple zeta values• Outlook: link to number theory/algebraic geometry
Johannes Broedel: (Elliptic) multiple zeta values in open superstring amplitudes 1/16
State of the art: open string theoryTree-level:• Calculation of all amplitudes based on [Broedel, Schlotterer
Stieberger ]multiple polylogarithms and multiple zeta values [Goncharov][Brown][Zagier]and the algebraic structure of string corrections at tree-level. [Schlotterer
Stieberger ]• Drinfeld associator avoids necessity of solving integrals at all.[ Broedel, Schlotterer
Stieberger, Terasoma]Complete calculation boiled down to recursive application of linear algebra.
Loop-level:• calculation based on elliptic iterated integrals and elliptic multiple zeta
values [ Broedel, MafraMatthes, Schlotterer][ Broedel
Matthes, Schlotterer]• no analogue of the Drinfeld method so far: integrals can not be replaced com-
pletely yet . . .
Johannes Broedel: (Elliptic) multiple zeta values in open superstring amplitudes 2/16
Why open string theory?Iterated integrals are essential in calculations in field and string theory:• same building blocks
field theory: multiple polylogarithms at loop level. Divergences appear.string theory: multiple polylogarithms at tree level. No divergences.• field theory: elliptic iterated integrals make an appearance in particular Feynman
diagrams. [Adams, BognerWeinzierl ][Caron-Huot
Larsen ]string theory: one-loop amplitudes are natural for elliptic iterated integrals.• field theory results can be obtained from open string theory in the low-energy
limit.
After all, string theory is a heavily constrained theorywith an amazing degree of symmetry⇒ should produce simple answers.
Johannes Broedel: (Elliptic) multiple zeta values in open superstring amplitudes 3/16
OutlineTree-level
0
z1 z2 zN−2
1
zN−1
zN =∞
· · ·N−2∏i=2
∫ zi+1
0dzi
multiple polylogarithmsG(a1,a2, . . . , an; z)
=∫ z
0dt 1t− a1
G(a2, . . . , an; t)
partial fractionmultiple zeta values ζDrinfeld method - no integrals
One-loop
z1 z2 zN−1 zN
t
1· · ·∫ 1
0dzN
N−1∏i=1
∫ zi+1
0dzi δ(z1)
elliptic iterated integralsΓ ( n1 n2 ... nr
a1 a2 ... ar ; z)
=∫ z
0dt f (n1)(t− a1) Γ ( n2 ... nr
a2 ... ar ; t)
Fay-identitieselliptic multiple zeta values ωelliptic (KZB) associator?
Johannes Broedel: (Elliptic) multiple zeta values in open superstring amplitudes 4/16
Tree-level, basicsN -point tree-level open-string amplitude: [Veneziano]. . . [Mafra, Schlotterer
Stieberger ]
Aopenstring = F .AYM
• dependence on external states in AYM• F = F (sij), sij = α′(ki + kj)2
• coefficients are multiple zeta values (MZVs) 0
z1 z2 zN−2
1
zN−1
zN =∞
· · ·
F 1,2,...,N =N−2∏i=2
∫ zi+1
0dzi
N−1∏i<j
|zij |sij
s12
z12
(s13
z13+ s23
z23
). . .
(s1,N−2
z1,N−2+ . . .+ sN−3,N−2
zN−3,N−2
)
N−2∏i=2
∫ zi+1
0
dzi
zi − ai
N−1∏i<j
|zij |sij︸ ︷︷ ︸expand. . .
⇒N−1∏i<j
∞∑nij=0
(sij)nij(ln |zij |)nij
nij !︸ ︷︷ ︸multiple polylogsMultiple polylogarithms
G(a1, a2, . . . , an; z) =∫ z
0
dtt− a1
G(a2, . . . , an; t), G(; z) = 1, G(~a; 0) = G(; 0) = 0
G(0, 0, . . . , 0︸ ︷︷ ︸w
; z) = 1w! (ln z)w G(1, 1 . . . , 1︸ ︷︷ ︸
w
; z) = 1w! lnw(1− z)
Johannes Broedel: (Elliptic) multiple zeta values in open superstring amplitudes 5/16
N−2∏i=2
∫ zi+1
0
dzizi − ai
N−1∏i<j
∞∑nij=0
(sij)nijG(0, 1, zl, zk)︸ ︷︷ ︸integrate step by step. . .
N−1∏i<j
∞∑nij=0
(sij)nijG(0, 1, 1)
︸ ︷︷ ︸rewrite polylogs as multiple ζ’s
ζn1,...,nr =∑
0<k1<···<kr
1kn1
1 · · · knrr
= (−1)rG(0, 0, . . . , 0, 1︸ ︷︷ ︸nr
, . . . , 0, 0, . . . , 0, 1︸ ︷︷ ︸n1
; 1) = ζ(w)
5-point-example:
F (23) = 1− ζ2(s12s23 + s12s24 + s12s34 + s13s34 + s23s34)+ ζ3(s2
12s23 + s12s223 + s2
12s24 + 2s12s23s24 + s12s224 + · · · ) + · · ·
+ ζ3,5(. . .) + · · ·
Pretty cumbersome - isn’t there an easier way to obtain the result?
Johannes Broedel: (Elliptic) multiple zeta values in open superstring amplitudes 6/16
Drinfeld-method [ Broedel, SchlottererStieberger, Terasoma]
Knizhnik-Zamolodchikov equation [ KnizhnikZamolodchikov]
dF(z0)dz0
=(e0z0− e1z0 − 1
)F(z0) .
• z0 ∈ C\0, 1, Lie-algebra generators e0, e1 0
z1 z2 zN−2 z0
1
zN−1
zN =∞
· · ·Regularized boundary values
C0 ≡ limz0→0
z−e00 F(z0)
(N− 1)-point
0
z1z2
z0 z0
1
zN−1
zN =∞
C1 ≡ limz0→1
(1− z0)e1F(z0)
N-point
0
z1 z2 zN−2 z0 z0
1
zN−1
zN =∞
· · ·
are related by the Drinfeld associator Φ: [Drinfeld][ LeMurakami][Furusho][Drummond
Ragoucy ]
C1 = Φ(e0, e1)C0, Φ(e0, e1) =∑
w∈0,1w[e0, e1]ζ(w)
Johannes Broedel: (Elliptic) multiple zeta values in open superstring amplitudes 7/16
Collect tree-level resultsTree-level
0
z1 z2 zN−2
1
zN−1
zN =∞
· · ·N−2∏i=2
∫ zi+1
0dzi
multiple polylogarithmsG(a1,a2, . . . , an; z)
=∫ z
0dt 1t− a1
G(a2, . . . , an; t)
partial fractionmultiple zeta values ζDrinfeld method - no integrals
One-loop
z1 z2 zN−1 zN
t
1· · ·∫ 1
0dzN
N−1∏i=1
∫ zi+1
0dzi δ(z1)
elliptic iterated integralsΓ ( n1 n2 ... nr
a1 a2 ... ar ; z)
=∫ z
0dt f (n1)(t− a1) Γ ( n2 ... nr
a2 ... ar ; t)
Fay-identitieselliptic multiple zeta values ωelliptic (KZB) associator?
Johannes Broedel: (Elliptic) multiple zeta values in open superstring amplitudes 8/16
z1 z2 zN−1 zN
t
1· · ·
One-loop open string• topologies: all genus-one worldsheets
with boundaries.• here: cylinder with insertions on
one boundary only: Im(z) = 0• one imaginary parameter: τ
General form of the integral:
A1-loopstring (1, 2, 3, 4) = s12s23A
treeYM(1, 2, 3, 4)
∫ ∞0
dτ I4pt(1, 2, 3, 4)(τ)
I4pt(1, 2, 3, 4)(τ) ≡∫ 1
0dz4
∫ z4
0dz3
∫ z3
0dz2
∫ z2
0dz1 δ(z1)
4∏j<k
[χjk(τ)
]sjk
︸ ︷︷ ︸Koba-Nielsen
Green’s function of the free boson on a genus-one surface with modulus τ :
lnχij(τ)∣∣∣zij=τxij
Johannes Broedel: (Elliptic) multiple zeta values in open superstring amplitudes 9/16
Compare tree-level
N−2∏i=2
∫ zi+1
0
dzizi − ai
N−1∏i<j
∞∑nij=0
1nij !
(sij)nij (ln |zij |)nij︸ ︷︷ ︸multiple polylogs
with one-loop situation:
∫ 1
0dzN
N−1∏i=1
∫ zi+1
0dzi δ(z1)
N∏i<j
∞∑nij=0
1nij !
(sij)nij (lnχij(τ))nij︸ ︷︷ ︸???
Suitable (iterated) object:
lnχij(τ) =∫ zi
zj
dw f (1)(w − zj , τ)
Johannes Broedel: (Elliptic) multiple zeta values in open superstring amplitudes 10/16
Natural weights for differentials on an elliptic curve: [Enriquez][BrownLevin ]
f (n)(z, τ) = f (n)(z + 1, τ) and f (n)(z, τ) = f (n)(z + τ, τ) .
Explicitly: (simplification in our situation because Im(z) = 0)
f (0)(z, τ) ≡ 1 f (1)(z, τ) ≡ ∂ ln θ1(z, τ) + 2πi ImzImτ
f (2)(z, τ) ≡ 12[(∂ ln θ1(z, τ) + 2πi ImzImτ
)2+ ∂2 ln θ1(z, τ)− 1
3θ′′′1 (0, τ)θ′1(0, τ)
]Parity: f (n)(−z, τ) = (−1)nf (n)(z, τ)
Relation to Eisenstein–Kronecker-series: [Kronecker][BrownLevin ]
F (z, α, τ) ≡ θ′1(0, τ)θ1(z + α, τ)θ1(z, τ)θ1(α, τ) ,
αΩ(z, α, τ) ≡ α exp(
2πiα Im(z)Im(τ)
)F (z, α, τ) =
∞∑n=0
f (n)(z, τ)αn
Johannes Broedel: (Elliptic) multiple zeta values in open superstring amplitudes 11/16
Elliptic iterated integrals (suppress τ -dependence from here. . . )
Γ ( n1 n2 ... nra1 a2 ... ar ; z) ≡
∫ z
0dw f (n1)(w − a1) Γ ( n2 ... nr
a2 ... ar ;w)
⇒ can rewrite any integral∫
1234 . . . into an elliptic iterated integral .
Products of differential weights (tree-level) ⇒ partial fraction:∫ z
0dw 1
w − a1
1w − a2
· · · ⇒ 1(w−a1)(w − a2) = 1
(w−a1)(a1−a2)+ 1(w−a2)(a2−a1)
Products of differential weights (one-loop) ⇒ Fay identities∫ z
0dw f (n1)(w − x)f (n2)(w) · · · ⇒ f (1)(w−x)f (1)(w) =f (1)(w−x)f (1)(x)−f (1)(w)f (1)(x)
+ f (2)(w) + f (2)(x) + f (2)(w − x)
The Fay identity is a form of the trisecant equation for Eisenstein–Kronecker series:
F (z1, α1)F (z2, α2) = F (z1, α1 + α2)F (z2 − z1, α2)+ F (z2, α1 + α2)F (z1 − z2, α1)
Johannes Broedel: (Elliptic) multiple zeta values in open superstring amplitudes 12/16
Elliptic multiple zeta values (eMZV’s)
ω(n1, n2, . . . , nr) ≡∫
0≤zi≤zi+1≤1
f (n1)(z1)dz1 f(n2)(z2)dz2 . . . f
(nr)(zr)dzr
= Γ(nr, . . . , n2, n1; 1) = Γ ( nr nr−1 ... n10 0 ... 0 ; 1)
Four-point result
I4pt(1, 2, 3, 4)(τ) =ω(0, 0, 0) − 2ω(0, 1, 0, 0) (s12 + s23)+ 2ω(0, 1, 1, 0, 0)
(s2
12 + s223)− 2ω(0, 1, 0, 1, 0) s12s23
+ β5 (s312 + 2s2
12s23 + 2s12s223 + s3
23)+ β2,3 s12s23(s12 + s23) + O(α′4)
with
β5 = 43[ω(0, 0, 1, 0, 0, 2) + ω(0, 1, 1, 0, 1, 0)− ω(2, 0, 1, 0, 0, 0)− ζ2 ω(0, 1, 0, 0)
]β2,3 = 1
3 ω(0, 0, 1, 0, 2, 0)− 32 ω(0, 1, 0, 0, 0, 2)− 1
2 ω(0, 1, 1, 1, 0, 0)
− 2 ω(2, 0, 1, 0, 0, 0)− 43 ω(0, 0, 1, 0, 0, 2)− 10
3 ζ2 ω(0, 1, 0, 0)
Johannes Broedel: (Elliptic) multiple zeta values in open superstring amplitudes 13/16
ComparisonTree-level
0
z1 z2 zN−2
1
zN−1
zN =∞
· · ·N−2∏i=2
∫ zi+1
0dzi
multiple polylogarithmsG(a1,a2, . . . , an; z)
=∫ z
0dt 1t− a1
G(a2, . . . , an; t)
partial fractionmultiple zeta values ζDrinfeld method - no integrals
One-loop
z1 z2 zN−1 zN
t
1· · ·∫ 1
0dzN
N−1∏i=1
∫ zi+1
0dzi δ(z1)
elliptic iterated integralsΓ ( n1 n2 ... nr
a1 a2 ... ar ; z)
=∫ z
0dt f (n1)(t− a1) Γ ( n2 ... nr
a2 ... ar ; t)
Fay-identitieselliptic multiple zeta values ωelliptic associator? [Knizhnik, Bernard
Zamolodchikov ]Johannes Broedel: (Elliptic) multiple zeta values in open superstring amplitudes 14/16
Summary• eMZVs are natural language for one-loop amplitudes in open string theory• full amplitude only after τ -integration and consideration of other topologies
eMZVs might not be the only ingredient: Euler sums?• open-string result does not contain divergent eMZVs
xWhat else?• eMZVs: can be represented as iterated Eisenstein integrals• iterated Eisenstein integrals nicely related to special derivation algebra, [Pollack]
available cusp forms on the elliptic curve ⇔ number of ”basis” eMZVs [Brown]• number of ”basis” eMZVs + canonical choice known [Hain][Broedel, Matthes
Schlotterer ]• using our formalism, one can derive new relations in the derivation algebra u,
which match the known pattern of cusp forms• numerous relations for eMZVs: https://tools.aei.mpg.de/emzv
xGoal• closed/recursive form of the integrand for the one-loop open-string amplitude
in terms of iterated Eisenstein integrals (analogue of Drinfeld-method)• relation to functions ELi occurring in [Adams, Bogner
Weinzierl ]Johannes Broedel: (Elliptic) multiple zeta values in open superstring amplitudes 15/16
Thanks!
Johannes Broedel: (Elliptic) multiple zeta values in open superstring amplitudes 16/16