Volume 212, number 2 PHYSICS LETTERS B 22 September 1988
THE TOPOLOGICAL SUSCEPTIBILITY ON THE LATTICE ~"
M. CAMPOSTRINI, A. DI GIACOMO and H. PANAGOPOULOS
INF]V;Sezionedi Pisa, and Dipartimento di Fisica, UniversRd di Pisa,2-56 ! O0 Pisa, Italy
Received 5 July 1988
w~ s*.udy the multiNicative renormaIization of the topologicalcharge operator on the iat.zicewkh respect tc the continuum.
Apgarent discrepanciesbetween different methods of determination &the topologica!charge on ~he lattice are exNained by our
result.
I. Introduction
The existence of a nonzero topological susceptibil-
ity of the QCD vacuum was proposed some years ago
[I~3] to solve the so-ca'led U(I ) problem, i.e. the
exp!icit breaking of the U ( 1 ) axial symmet~.
The topological susceptibility is defined by the
equation
A= ( d"x(OiT(Q(x)Q(O))!O) , (d)
j
where
Q(x) =: ~ Eu~'%FG(x~ F ~ ( x ) (2)
0~+%2 U ~ pa,
is the topological charge density. O is the divergence
of the topoiogical current K v [ 11
O(x) = GK,,
K~,= .g2,e ~/jAg(~A~-}ga~a~A~A~) (3)
the prescription defining the product of the operators
ineq. (!) is [41
(Oi T(Q(x) Q(O) )tO)
=- a. ( Oi T(KU(x) O(O ) ) iO ). (4)
Chira! Ward identities lead to the prediction [ 3 ]
Partly sappor.'.ed by M.P,I. (kalian Minis'..ry for PuNic
Education ).
206
2Ny. .
~ A=m~ + m~, -- 2m~. (5)
or, with three Iight flavours,
A= (180MeV)4 ~ (6)
The lattice is a unique too! to determine quant;.ties
like A, which have nontrivial dimension in mass, and
therefore cannot be computed by pegurbation theory.
Three different methods have been used to extract
.4 from iattice QCD.
(i) The "naive" method [5-7] consists in the
measurement (by Monte Carlo simulation) of the
vacuun-_.- two-point correlation at zero momentum of
an operator QL (x) which coincides with the topolog-
ical charge Q(x) in the limit of zero lattice spacing
(a-.0).
A possibie choice of QL is
(7)
where//_"~ (x) is the parallel transport matrix aiong a
! × i Wilson loop; in the usual notation
~""(x) = u,(x) G,(x+¢) U;(x+~) g;(x) o (8)
By this method either
is measured [5,71, or the value Q,~=Z~Q:.(x) is
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