On the associativity anomaly in open string field theory

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  • Volume 197, number 3 PHYSICS LETTERS B 29 October 1987

    ON THE ASSOCIATIVITY ANOMALY IN OPEN STRING FIELD THEORY

    Mark RAKOWSKI and George THOMPSON International Centre for Theoretical Physics, 1-34100 Trieste, Italy

    Received 8 July 1987

    The associativity anomaly in the star algebra of the open bosonic string is demonstrated by a simple oscillator calculation. In an associative algebra, formal arguments require that the "half string" BRST operator QL be nilpotent; however, we show that associativity is actually violated by computing Q~ in an explicit operator representation of the star algebra.

    I. Introduction. The purely cubic form of the string field theory action [ 1,2] was introduced in an effort to eliminate the background field dependence in Witten's approach to string field theory [3,4]. The cubic action takes the form

    S= ~ q~,q~,q~, (1)

    where is a functional on the space of string con- figurations, and the ,-product and f-integral were formulated in ref. [ 3 ]. Formally, the star algebra for open strings is associative, but a more careful anal- ysis [ 5 ], where the star algebra is realized in the Fock space of the first quantized string [6,7 ], revealed an anomaly in associativity. Moreover, this violation in associativity was shown to be related to the gener- ation of closed string intermediate states [ 5 ]. Their calculation used an explicit operator expression for the three-string vertex in a manner which was essen- tially independent of the ghost oscillators. It is the purpose of this letter to demonstrate the anomaly in associativity in a simple way - one which does not explicitly employ the three string vertex - and which in contrast to ref. [ 5 ], reduces to a calculation solely with the ghost oscillators.

    2. Formal properties of the star algebra. Let us now quickly review those properties of the star algebra which will be crucial in our subsequent analysis. In the formulation of the purely cubic action [1 ], a major role is played by the "half string" BRST oper- ators QL and QR defined by

    n/2

    QL= I j (a) &r, QR=Q-QL, (2) 0

    where j (a) is the BRST current and Q is the total nilpotent BRST charge. One also assumes that there exists an identity string functional I with the property

    I ,A=A,I=A, (3)

    holding for all string functionals A. In ref. [ 1 ], the following identities were formally established which relate these objects:

    (i) QRI= --aLl, (4)

    (ii) QRA*B= --(--)AA*QLB, (5)

    (iii) {Q, QL}=O. (6)

    Somewhat later, a careful analysis confirmed these properties [ 7 ] within the context of an explicit oper- ator formalism. Using (5), the authors of ref. [ 1 ] also showed that 00---QLI is an extremum of the action S:

    o *o =0. (7)

    Our problem begins by first noticing that if we set A=I in (5):

    Oo*B=QLB, (8)

    and then taking B= QLC, one obtains

    0o,(0o,C)=Q2C. (9)

    0370-2693/87/$ 03.50 Elsevier Science Publishers B.V. (North-Holland Physics Publishing Division)

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  • Volume 197, number 3 PHYSICS LETTERS B 29 October 1987

    Now, if the star algebra is associative, (7) then implies that Q2L = 0 (and similarly for QR). Although the total BRST charge Q was constructed to be nil- potent in the critical dimension, one does not expect this of the "half string" BRST operators QL and QR. In the following section, we undertake a careful anal- ysis of Q,2, and show explicitly that it does not vanish.

    3. The associativity anomaly. An analysis of Witten's string field theory and the purely cubic action, where the star algebra is realized in a first- quantized Fock space of the string, has been given [ 6,7 ]. In this formulation, a string functional A [x(a), b(tr), coy)] is represented by a state IA) in the Fock space, and the star product is realized through the three-string vertex I V3) via the relation

    IA*B) I =2 (A[3 (BI V3 ) 123- (10)

    The three-string vertex lives in a tensor product of three single-string Fock spaces labeled by the indices 1, 2, 3. An explicit form for this vertex can be found in refs. [6,7].

    We will be interested in the specific form of QL which is given by [ 7 ]

    1 ( _ )k +Q- 1)), (11) QL = Qo + rc k=o - ~ (Qzk+l (2k+

    Q,,= ~ (c_iff,.+i+ff,._ici)+ff,.co-a.c., (12) i=1

    QR = Qo - QL, (13)

    x + _lrg. (14) /~,, =L~ - 2~n ,

    x -1 L,, - ~ a_i'an+i, n~O, i~ -oo

    L~=p2 + ~ ot_i.oti, (15) i=1

    L~h= ~ (2n+i)b_~G+~, n~0, i~ --oo

    L~h= ~ i(b_ici+c_ibi), (16) i= l

    where the vacuum is required to satisfy Col0)=0, and is an eigenstate of ot~=p u. The somewhat unconventional normal-ordering coefficients a, are chosen such that {Q, Q,}=0, and are given by [7]

    a,, 1 - 1"- 3..2 (17)

    The square of QL is straightforward to compute, and we find

    1

    k,l=O p= --o:,

    - -C2k_2 l_2+ p q-2C_2k+Zl+p). (18)

    This is a complicated triple sum, and as we will shortly see, needs to be regularized. For our pur- poses, it suffices to find a state which is not anni- hilated by Q2. It is simplest to look at terms in (18) which are proportional to CoC_2m, m>~ 1. The terms of this type are

    ---T ( - )'~CoC_2,~m 2-m+2 ~ 1 . (19)

    Using the usual (-function regularization, we obtain

    -2 re-----7- coc_2m ( - )" m(1 -m) , (20)

    and hence it is possible to find states on which Q[ 0. It is noteworthy that one can also write a completely regularized expression for all of Q~. Again, using (-function regularization we obtain

    a2= -~'~r=~--oo rC--r m= ~ --oo ( - ) re ( l - Jml)c2m+"

    (21)

    4. Conclusion. In this letter, we have demonstrated the existence of an anomaly in the associativity of the star algebra in purely cubic open string field the- ory. Coupled with the observation that in an asso- ciative star algebra the "half string" BRST operators aL and QR are separately nilpotent, this simply amounted to showing that Q~ ~ 0. This analysis was then carried out within the context of an explicit operator realization of the star algebra. As observed in ref. [ 5 ], this anomaly is connected to the fact that one generates infinite sums over oscillator modes which are not absolutely convergent. This formula- tion of classical string field theory therefore requires regularization.

    The non-associativity as demonstrated here, is purely in the ghost sector of the Fock space, unlike the original derivation given in ref. [ 5 ]. It is also

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  • Volume 197, number 3 PHYSICS LETTERS B 29 October 1987

    worth noting that this violation of associativity is not an obstruction to obtaining Witten's action [ 3 ] from the purely cubic theory,

    Recently, a more geometric approach [ 8 ] to string field theory has been advanced which does not break world sheet reparametrization invariance by singling out a preferred midpoint on the string. It would be of interest to analyze the possible breakdown of asso- ciativity in this new algebra.

    The authors would like to thank Professor Abdus Salam, the International Atomic Energy Agency and UNESCO for hospitality at the International Centre for Theoretical Physics, Trieste.

    References

    [ 1 ] G. Horowitz, J. Lykken, R. Rohm and A. Strominger, Phys. Rev. Lett. 57 (1986) 283.

    [ 2 ] H. Hata, K. Itoh, T. Kugo, H. Kunitomo and K. Ogawa, Phys. Left. B 175 (1986) 138.

    [3] E. Witten, Nucl. Phys. B 268 (1986) 253, [4] E. Witten, Nucl. Phys. B 276 (1986) 291. [5] G. Horowitz and A. Strominger, Phys. Lett. B 185 (1987)

    45. [6] D. Gross and A. Jevicki, Nucl. Phys. B 283 (1987) 1. [ 7 ] L.J. Romans, Operator approach to purely cubic string field

    theory, Santa Barbara preprint (1987). [ 8 ] M. Kaku, Geometric derivation of string field theory from

    first principles I: curvature tensors and the tensor calculus preprint HEP-CCNY- 14 (1986).

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