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r38/log/dummy.rlg
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2011-09-02 18:13:33
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Tue Apr 15 00:32:36 2008 run on win32 % test of DUMMY package version 1.1 running in REDUCE 3.6 and 3.7 % DATE: 15 September 1998 % Authors: H. Caprasse <hubert.caprasse@ulg.ac.be> % % Case of commuting operator: % operator co1,co2; % declare dummy indices % first syntax : base <name> % dummy_base dv; dv % dummy indices are dv1, dv2, dv3, ... exp := co2(dv2)*co2(dv2)$ c_exp := canonical(exp); 2 c_exp := co2(dv1) exp := dv2*co2(dv2)*co2(dv2)$ c_exp := canonical(exp); 2 c_exp := co2(dv1) *dv1 exp := c_exp * co1(dv3); 2 exp := co1(dv3)*co2(dv1) *dv1 c_exp := canonical(exp); 2 c_exp := co1(dv2)*co2(dv1) *dv1 % operator a,aa,dd,te; clear_dummy_base; t dummy_names a1,a2,b1,b2,mu1,mu2,nu1,nu2; t es1:=a(a1,b1)*a(a2,b2); es1 := a(a1,b1)*a(a2,b2) asn14:=aa(mu1,a1)*aa(nu2,b2)*dd(nu1,b1,mu2,a2) *te(mu1,mu2,nu1,nu2); asn14 := aa(mu1,a1)*aa(nu2,b2)*dd(nu1,b1,mu2,a2)*te(mu1,mu2,nu1,nu2) asn17:=aa(mu1,a1)*aa(mu2,a2)*dd(nu1,b1,nu2,b2) *te(mu1,mu2,nu1,nu2); asn17 := aa(mu1,a1)*aa(mu2,a2)*dd(nu1,b1,nu2,b2)*te(mu1,mu2,nu1,nu2) esn14:=es1*asn14; esn14 := a(a1,b1)*a(a2,b2)*aa(mu1,a1)*aa(nu2,b2)*dd(nu1,b1,mu2,a2)*te(mu1,mu2,nu1,nu2) esn17:=es1*asn17; esn17 := a(a1,b1)*a(a2,b2)*aa(mu1,a1)*aa(mu2,a2)*dd(nu1,b1,nu2,b2)*te(mu1,mu2,nu1,nu2) esn:=es1*(asn14+asn17); esn := a(a1,b1)*a(a2,b2)*aa(mu1,a1)*te(mu1,mu2,nu1,nu2) *(aa(mu2,a2)*dd(nu1,b1,nu2,b2) + aa(nu2,b2)*dd(nu1,b1,mu2,a2)) canonical esn; a(a1,a2)*a(b1,b2)*aa(mu2,b1)*(aa(mu1,a1)*dd(nu1,b2,nu2,a2)*te(mu2,mu1,nu1,nu2) + aa(mu1,a2)*dd(nu1,b2,nu2,a1)*te(mu2,nu2,nu1,mu1)) % that the next result is correct is not trivial % to show. % for esn14 changes of names are % % nu1 -> nu1 % b1 -> b2 -> a2 % mu2 -> nu2 -> mu1 -> mu2 % % for esn17 they are % % nu1 -> nu1 % nu2 -> nu2 % b1 -> b2 -> a2 -> a1 -> b1 % % the last result should be zero canonical esn -(canonical esn14 +canonical esn17); 0 % remove dummy_names and operators. clear_dummy_names; t clear a,aa,dd,te; % % Case of anticommuting operators % operator ao1, ao2; anticom ao1, ao2; t % product of anticommuting operators with FREE indices a_exp := ao1(s1)*ao1(s2) - ao1(s2)*ao1(s1); a_exp := ao1(s1)*ao1(s2) - ao1(s2)*ao1(s1) a_exp := canonical(a_exp); a_exp := 2*ao1(s1)*ao1(s2) % the indices are summed upon, i.e. are DUMMY indices clear_dummy_names; t dummy_base dv; dv a_exp := ao1(dv1)*ao1(dv2)$ canonical(a_exp); 0 a_exp := ao1(dv1)*ao1(dv2) - ao1(dv2)*ao1(dv1); a_exp := ao1(dv1)*ao1(dv2) - ao1(dv2)*ao1(dv1) a_exp := canonical(a_exp); a_exp := 0 a_exp := ao1(dv2,dv3)*ao2(dv1,dv2)$ a_exp := canonical(a_exp); a_exp := ao1(dv1,dv2)*ao2(dv3,dv1) a_exp := ao1(dv1)*ao1(dv3)*ao2(dv3)*ao2(dv1)$ a_exp := canonical(a_exp); a_exp := - ao1(dv1)*ao1(dv2)*ao2(dv1)*ao2(dv2) % Case of non commuting operators % operator no1, no2, no3; noncom no1, no2, no3; n_exp := no3(dv2)*no2(dv3)*no1(dv1) + no3(dv3)*no2(dv1)*no1(dv2) + no3(dv1)*no2(dv2)*no1(dv3); n_exp := no3(dv1)*no2(dv2)*no1(dv3) + no3(dv2)*no2(dv3)*no1(dv1) + no3(dv3)*no2(dv1)*no1(dv2) n_exp:=canonical n_exp; n_exp := 3*no3(dv3)*no2(dv2)*no1(dv1) % *** % The example below displays a restriction of the package i.e % The non commuting operators are ASSUMED to COMMUTE with the % anticommuting operators. % *** exp := co1(dv1)*ao1(dv2,dv1,dv4)*no1(dv1,dv5)*co2(dv3)*ao1(dv1,dv3); exp := co1(dv1)*co2(dv3)*(ao1(dv2,dv1,dv4)*no1(dv1,dv5)*ao1(dv1,dv3)) canonical(exp); - co1(dv1)*co2(dv2)*ao1(dv1,dv2)*ao1(dv3,dv1,dv4)*no1(dv1,dv5) exp := c_exp * a_exp * no3(dv2)*no2(dv3)*no1(dv1); 2 exp := - co1(dv2)*co2(dv1) *dv1*ao1(dv1)*ao1(dv2)*ao2(dv1)*ao2(dv2)*no3(dv2) *no2(dv3)*no1(dv1) can_exp := canonical(exp); 2 can_exp := - co1(dv2)*co2(dv1) *dv1*ao1(dv1)*ao1(dv2)*ao2(dv1)*ao2(dv2) *no3(dv2)*no2(dv3)*no1(dv1) % Case where some operators have a symmetry. % operator as1, as2; antisymmetric as1, as2; dummy_base s; s % With commuting and antisymmetric: asc_exp:=as1(s1,s2)*as1(s1,s3)*as1(s3,s4)*co1(s3)*co1(s4)+ 2*as1(s1,s2)*as1(s1,s3)*as1(s3,s4)*co1(s2)*co1(s4)$ canonical asc_exp; as1(s1,s2)*as1(s1,s3)*as1(s3,s4)*co1(s3)*co1(s4) % Indeed: the second term is identically zero as one sees % if the substitutions s2->s4, s4->s2 and % s1->s3, s3->s1 are sucessively done. % % With anticommuting and antisymmetric operators: dummy_base dv; dv exp1 := ao1(dv1)*ao1(dv2)$ canonical(exp1); 0 exp2 := as1(dv1,dv2)$ canonical(exp2); 0 canonical(exp1*exp2); as1(dv1,dv2)*ao1(dv1)*ao1(dv2) canonical(as1(dv1,dv2)*as2(dv2,dv1)); - as1(dv1,dv2)*as2(dv1,dv2) % With symmetric and antisymmetric operators: operator ss1, ss2; symmetric ss1, ss2; exp := ss1(dv1,dv2)*ss2(dv1,dv2) - ss1(dv2,dv3)*ss2(dv2,dv3); exp := ss1(dv1,dv2)*ss2(dv1,dv2) - ss1(dv2,dv3)*ss2(dv2,dv3) canonical(exp); 0 exp := as1(dv1,dv2)*as1(dv3,dv4)*as1(dv1,dv4); exp := as1(dv1,dv2)*as1(dv1,dv4)*as1(dv3,dv4) canonical(exp); 0 % The last result is equal to half the sum given below: % exp + sub(dv2 = dv3, dv3 = dv2, dv1 = dv4, dv4 = dv1, exp); 0 exp1 := as2(dv3,dv2)*as1(dv3,dv4)*as1(dv1,dv2)*as1(dv1,dv4); exp1 := - as1(dv1,dv2)*as1(dv1,dv4)*as1(dv3,dv4)*as2(dv2,dv3) canonical(exp1); as1(dv1,dv2)*as1(dv1,dv3)*as1(dv3,dv4)*as2(dv2,dv4) exp2 := as2(dv1,dv4)*as1(dv1,dv3)*as1(dv2,dv4)*as1(dv2,dv3); exp2 := as1(dv1,dv3)*as1(dv2,dv3)*as1(dv2,dv4)*as2(dv1,dv4) canonical(exp2); as1(dv1,dv2)*as1(dv1,dv3)*as1(dv3,dv4)*as2(dv2,dv4) canonical(exp1-exp2); 0 % Indeed: % exp2 - sub(dv1 = dv3, dv2 = dv1, dv3 = dv4, dv4 = dv2, exp1); 0 % Case where mixed or incomplete symmetries for operators are declared. % Function 'symtree' can be used to declare an operator symmetric % or antisymmetric: operator om; symtree(om,{!+,1,2,3}); exp:=om(dv1,dv2,dv3)+om(dv2,dv1,dv3)+om(dv3,dv2,dv1); exp := om(dv1,dv2,dv3) + om(dv2,dv1,dv3) + om(dv3,dv2,dv1) canonical exp; 3*om(dv1,dv2,dv3) % Declare om to be antisymmetric in the two last indices ONLY: symtree(om,{!*,{!*,1},{!-,2,3}}); canonical exp; 0 % With an antisymmetric operator m: operator m; dummy_base s; s exp := om(nu,s3,s4)*i*psi*(m(s1,s4)*om(mu,s1,s3) + m(s2,s3)*om(mu,s4,s2) - m(s1,s3)*om(mu,s1,s4) - m(s2,s4)*om(mu,s3,s2))$ canonical exp; - 4*m(s1,s2)*om(mu,s1,s3)*om(nu,s2,s3)*i*psi % Case of the Riemann tensor % operator r; symtree (r, {!+, {!-, 1, 2}, {!-, 3, 4}}); % Without anty dummy indices. clear_dummy_base; t exp := r(dv1, dv2, dv3, dv4) * r(dv2, dv1, dv4, dv3)$ canonical(exp); 2 r(dv1,dv2,dv3,dv4) % With dummy indices: dummy_base dv; dv canonical( r(x,y,z,t) ); - r(t,z,x,y) canonical( r(x,y,t,z) ); r(t,z,x,y) canonical( r(t,z,y,x) ); - r(t,z,x,y) exp := r(dv1, dv2, dv3, dv4) * r(dv2, dv1, dv4, dv3)$ canonical(exp); 2 r(dv1,dv2,dv3,dv4) exp := r(dv1, dv2, dv3, dv4) * r(dv1, dv3, dv2, dv4)$ canonical(exp); r(dv1,dv2,dv3,dv4)*r(dv1,dv3,dv2,dv4) clear_dummy_base; t dummy_names i,j,k,l; t exp := r(i,j,k,l)*ao1(i,j)*ao1(k,l)$ canonical(exp); 0 exp := r(k,i,l,j)*as1(k,i)*as1(k,j)$ canonical(exp); - as1(i,j)*as1(i,k)*r(i,k,j,l) % Cleanup of the previousy declared dummy variables.. clear_dummy_names; t clear_dummy_base; t exp := co1(dv3)$ c_exp := canonical(exp); c_exp := co1(dv3) end; Time for test: 31 ms, plus GC time: 3 ms