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UDC 530.1; 539.1
RENORMALIZATION OF FIELD MODELS WITH ONE-PARAMETER FERMIONIC SYMMETRY
P. M. Lavrov, O. V. Radchenko
Tomsk State Pedagogical University, Kievskava str., 60, 634061 Tomsk, Russia. E-mail: lavrov@tspu.edu.ru; radchenko@tspu.edu.ru
We prove that the theories invariant under one-parameter fermionic symmetry after renormalization retain invariance. It is shown that the Ward identity for effective action after renormalization has the same form as non-renormalized one.
Keywords: renormalization, supersvmmetric invariance.
1 Introduction
As it is known modern quantum field theory considers many different field models with quantum action invariant under supersymmetric transformations. For example the Faddeev-Popov action for Yang-Mills fields [1]. This action is invariant under remarkable BRST-transformations [2, 3]. The next sample is well-known Curci-Ferrari model of non-abelian massive vector fields [4] possesses supersymmetric invariance connected with the modified BRST and modified anti-BRST transformations, but these supersymmetric transformations are not nilpotent (in contrast with the BRST transformations).
In recent years there is also an interest to similar theories. One of such examples is superextension of the sigma models [5], which leads to actions again invariant under supersymmetric transformations. Recent attempts [6, 7] to formulate Yang-Mills fields in a form being free of the Gribov problem [8-10] give another examples of actions invariant under some nilpotent supersymmetric transformations. Quite recently a new realization of supersymmetry, called scalar supersymmetry, has been proposed in [11] when one meets supersymmetric invariant field models as well. In the paper [12] from general point of view properties of field theories for which an action appearing in the generating functional of Green functions is invariant under supersymmetric transformations were studied. Notice, that here the term "supersymmetry" we use as synonym of fermionic symmetry.
In this paper we continue the study of renormalization of the field theories [13-15] in the case of one-parameter global supersymmetry. Our research of renormalization is mainly based on the method proposed in [16].
We employ the DeWitt's condensed notation [17]. Derivatives with respect to fields are taken from the right and those with respect to antifields, from the left.
The Grassmann parity of a quantity X is denoted as e(X). We use the notation X,j for right derivative of X with respect to 0i.
2 Supersymmetric invariant theories
Our starting point is a theory of fields 0 = {4>1} with Grassmann parities e(0') = £%■ We assume a non-degenerate action S(0) of the theory so that the generating functional of Green functions is given by the standard functional integral
Z (J) = J D0 exp {- [S(0) + J0\} . (1)
We suppose invariance of S(0) under supersymmetric transformations
0i ^ 0i = ¿(0') ,
^(0) = 0' + R'(0)e, e2 = o, (2)
so that
S,i(0)Ri(0) = O . (3)
In (2) e is an odd Grassmann parameter and R^0) are generators of supersymmetric transformations having the Grassmann parities opposite to fields 0': e(Ri) = £i + 1.
It is very useful to use the so-called extended action S(0,0*) instead of the action S(0) by introducing antifields 0* with Grassmann parities opposite to fields
0i £(0i)=£i + 1:
S (0,0*)= S(0) + 0*Ri(0), (4)
and the extended generating functional of Green functions has form
Z(J,0*) = y D0 exp j- [S(0,0*) + J0\}. (5)
Then the condition (3) of invariance of the action can be conveniently represented in the form of classical master-equation written in terms of the antibracket [18]
(S,S) = 0, (6)
P. M. Lavrov, O. V. Radchenko. Re,normalization of Held models with one-parameter fermionic symmetry
where for any functions F, G the antibracket is defined by rule
(F G) = dF_dG _ ( I^F )+1)(e(G) + 1) m
(F,G) 3^34>*( Kn
with Grassmann parity e((F,G)) = e(F)+ e(G) + 1.
Ri(0) = 0 .
¿j)=o.
4 ¿0*
¿W
J u* =0.
¿0*
r(0,0*) = W (J,0* ) - J.04,
0 = ¿W iT = _ t.
0 = ¿J , ¿04 = Ji.
(r, r) = 0.
procedure proposed in [16]. The main points of this approach are: a) the action satisfies the classical master-equation; b) the effective action satisfies the Ward identity; c) there exists regularization, which retains forms of the equation (6) and identity (13).
Let us consider the one - loop approximation for r
(8) r = S + h( rdiV +rf1ii) + O(h2 ),
(1)
Here we will restrict ourselves to a special supersymmetric theory when the generators are
subjected to the restriction [12]
where rdiV Mid rfl) denote the divergent and finite parts of the one-loop approximation for r.
The functional rdiV determines the counterterms of
(1)
(g) the one-loop renormalized action S1R:
Taking into account (9), the Ward identity for the generating functional Z(J,0*) (5) has form
sir=s -
(10)
(S, rdiV ) = 0.
Introducing the generating functional of connected Green functions W(J, 0*) = —ihlnZ, the identity (10) can be rewritten as
(H)
The generating functional of the vertex functions r = r(0,0*) is introduced in a standard way, through the Legendre transformation of W,
(12)
The Ward identity for the generating functional of the vertex functions can be obtained directly from (11) and (12), in the form
(13)
The Ward identity (13) has universal form and plays a very important role in proof of gauge invariant renormalizability of general gauge theories [16].
3 Supersymmetric invariant renormalization
Let us consider functional integro-differential equation for the generating functionals of vertex Green's functions (effective action)
expj - r(0,0*)J (14)
= J exp { - [S(0 + ,0*) - /
Solutions of this equation are studied within -
Our study of the renormalization of a given supersymmetric invariant theory is based on the
and satisfies the equation
div ) = 0. (15)
Then we find that S1R satisfies the basic equation (Sir, SIR) = -2E2 up to certain terms E2
E = (r(i) r(i)) E2 = (r div, 1 div )
-
Let us construct the effective action r1R with the help of the action S1R. This functional is finite in the one-loop approximation and satisfies the equation
(r 1R, T1R) = -2E2 + O(-3).
Represent r1R in the form
r1R = S + tr% + +-2(r12div + rgi„) + O(-3).
The divergent part r1^diV °f the two - loop approximation for r1R determines the two - loop renormalization for S2R
S2R = S1R - -2 r12,div and satisfies the equation
(S r12div ) = E2.
Let us now consider (S2R, S2R) = -3E + O(-4).
We find that S2R satisfies the master-equation up to terms E3
E3 = 2(rdlV, r12<)iv) -
action r2R generated by S2R is finite in the two - loop approximation
r
2R = S + h/ + h2r12)f. + h3(r23 )
2R 1 /in 1 1,fin 1 v 2,
div
+ r2/ J + O (h4)
and satisfies the equation
(r2fl) T2r) = h3E3 + O(h4)
up to certain terms E3 of the third order in h.
Applying the induction method we establish that the totally renormalized action SR
w
SR = S - Y h-r^iv (16)
n=1
satisfies the basic equation exactly:
(SR, SR) = 0, (17)
while the renormalized effective action rR is finite in h
w
rfl = S+y hnr:\Jm, (is)
n=1
and satisfies the identity
(rfl, rfl)=0. (19)
Here, we have denoted by r— div and T— fin the divergent and finite parts, respectively, of the n - loop approximation for the effective action which is finite in (n-l)th approximation and is constructed from the action S(n_1)R.
Thus, the identity (19) means that after renormalization the effective action has the same symmetry properties as non-renormalized one.
Acknowledgement
The work is supported by Ministry of Education and Science of Russian Federation, project No. 867.
References
[1] Faddeev L. D. and Popov V. N. Phys. Lett. B25 29.
[2] Becchi C., Rouet A. and Stora R. 1975 Gommun. Math. Phys. 42 127.
[3] Tyutin I. V. 1975 Gauge invarianee infield theory and statistical physics in operator formalism, Lebedev Inst, preprint N 39 arXiv:0812.0580 [hep-th],
[4] Curci G. and Ferrari R. 1976 Nuovo Cim. A32 151.
[5] Catterall S. and Chadab S. 2004 JEEP 0405 044.
[6] Slavnov A. A. Gauge fields beyond perturbation theory arXiv: 1310.8164 [hep-th],
[7] Quagri A. and Slavnov A. A. 2010 JEEP 1007 087.
[8] Gribov V. N.. 1978 Nucl. Phys. B139 1.
[9] Zwanziger D. 1989 Nucl. Phys. B321 591.
[10] Zwanziger D. 1989 Nucl. Phys. B 323 513.
[11] Jourjine A. 2013 Phys. Lett. B727 211.
[12] Esipova S. R„ Lavrov P. M. and Radchenko O. V. 2014 Int. J. Mod. Phys. A29 1450065.
[13] Lavrov P. M. and Shapiro I. L. 2010 Phys. Rew. D81 044026.
[14] Lavrov P. M. 2011 Nucl. Phys. B849 503.
[15] Lavrov P. M. 2012 TSPU Bulletin 13 98.
[16] Lavrov P. M., Tyutin I. V. and Voronov B. L. 1982 Sov. J. Nucl. Phys. 36 292.
[17] DeWitt B. S. 1965 Dynamical Theory of Groups and Fields (Gordon and Breach, New York) 288 p.
[18] Batalin I. A. and Vilkovisky G. A. 1981 Phys. Lett. B102 27.
Received H.11.2014
P. M. Lavrov, О. V. Radchenko. Re,normalization of field models with one-parameter fermionic symmetry
П. M. Лавров, О. В. Радченко
ПЕРЕНОРМИРОВКА ПОЛЕВЫХ МОДЕЛЕЙ С ОДТТОПАРАМАТРИЧЕСКОЙ
ФЕРМИОННОЙ СИММЕТРИЕЙ
Доказано, что теории, инвариантные относительно однонараметрической фермионной симметрии, после перенормировки сохраняют это свойство инвариантности. Показано, что тождество Уорда для эффективного действия после перенормировки имеют ту же форму, что и до нее.
Ключевые слова: перенормировка, суперсимметричная инвариантность.
Лавров П. М., доктор физико-математических наук, профессор. Томский государственный педагогический университет.
Ул. Киевская, 60, 634061 Томск, Россия. E-mail: lavrov@tspu.edu.ru
Радченко О.В., кандидат физико-математических наук. Томский государственный педагогический университет.
Ул. Киевская, 60, 634061 Томск, Россия. E-mail: radchenko@tspu.edu.ru
