GEORGIAN MATHEMATICAL JOURNAL: Vol. 2, No. 2, 1995, 189-199 CONSTRUCTION OF ENTIRE MODULAR FORMS OF WEIGHTS 5 AND 6 FOR THE CONGRUENCE GROUP Γ0 (4N ) G. LOMADZE Abstract. Two classes of entire modular forms of weight 5 and two of weight 6 are constructed for the congruence subgroup Γ0 (4N ). The constructed modular forms as well as the modular forms from [1] will be helpful in the theory of representation of numbers by the quadratic forms in 10 and 12 variables. The present paper is a direct continuation of [1] whose notation will be preserved here. 1. Lemma 1. For a given N let Ψ3 (τ ) = Ψ3 (τ ; g1 , . . . , g4 ; h1 , . . . , h4 ; c1 , . . . , c4 ; N1 , . . . , N4 ) = n 1 ϑ00 (τ ; c1 , 2N1 )ϑg2 h2 (τ ; c2 , 2N2 ) − = N1 g1 h1 o 1 − ϑg1 h1 (τ ; c1 , 2N1 )ϑg002 h2 (τ ; c2 , 2N2 ) × N2 ×ϑg0 3 h3 (τ ; c3 , 2N3 )ϑg4 h4 (τ ; c4 , 2N4 ) (1.1) and Ψ4 (τ ) = Ψ4 (τ ; g1 , . . . , g4 ; h1 , . . . , h4 ; c1 , . . . , c4 ; N1 , . . . , N4 ) = = 3 Y ϑ0gk hk (τ ; ck , 2Nk )ϑg4 h4 (τ ; c4 , 2N4 ), (1.2) k=1 1991 Mathematics Subject Classification. 11F11,11F03,11F27. Key words and phrases. Quadratic form, entire modular form, congruence subgroup, theta-series, generalized Gauss’ sum. 189 c 1995 Plenum Publishing Corporation 1072-947X/95/0300-0189$07.50/0 190 G. LOMADZE where 2|gk , Nk |N (k = 1, 2, 3, 4), 4 X hk . 4N Nk (1.3) k=1 For all substitutions from Γ in the neighborhood of each rational point τ = − γδ (γ = 6 0, (γ, δ) = 1), we then have (γτ + δ)5 Ψj (τ ; g1 , . . . , g4 ; h1 , . . . , h4 ; 0, . . . , 0; N1 , . . . , N4 ) = ∞ n ατ + β X = Cn(j) e (j = 3, 4). 4N γτ + δ n=0 (1.4) Proof. I. Taking into account (1.19) from [1], by Lemma 4 from [1], it follows for n = 2 (with g1 , h1 , g10 , h10 , N1 , H1 instead of g, h, g 0 , h0 , N , H) and n = 0 (with g2 , h2 , g20 , h02 , N2 , H2 instead of g, h, g 0 , h0 , N , H) that 1 (γτ + δ)3 ϑ00g1 h1 (τ ; 0, 2N1 )ϑg2 h2 (τ ; 0, 2N2 ) = N1 X 1 3 = − e sgn γ (2|γ|(N1 N2 )1/2 )−1 ϕg10 g1 h1 (0, H1 ; 2N1 ) × N1 4 H1 mod2N1 ατ + β o n ατ + β ; H1 , 2N1 + 2A21 ; H1 , 2N1 × · ϑg10 h01 × ϑg000 h0 1 1 γτ + δ γτ + δ z=0 ατ + β X ϕg20 g2 h2 (0, H2 ; 2N2 )ϑg20 h02 ; H2 , 2N2 = × γτ + δ H2 mod2N2 X −1 3 ϕg10 g1 h1 (0, H1 ; 2N1 ) × = −e sgn γ 2|γ|(N1 N2 )1/2 4 H1 mod2N1 H2 mod2N2 n 1 ατ + β ; H1 , 2N1 × ϑ00g0 h0 N1 1 1 γτ + δ ατ + β ατ + β ; H2 , 2N2 − 4γπi(γτ + δ)ϑg10 h01 ; H1 , 2N1 × ×ϑg20 h02 γτ + δ γτ + δ ατ + β o ×ϑg20 h02 (1.5) ; H2 , 2N2 . γτ + δ ×ϕg20 g2 h2 (0, H2 ; 2N2 ) If in (1.5) N1 , g1 , h1 , H1 , g10 , h10 are replaced by N2 , g2 , h2 , H2 , g20 , h20 , and vice versa, then we have 1 (γτ + δ)3 ϑ00g2 h2 (τ ; 0, 2N2 )ϑg1 h1 (τ ; 0, 2N1 ) = N2 X 3 −1 ϕg20 g2 h2 (0, H2 ; 2N2 ) × = −e sgn γ 2|γ|(N1 N2 )1/2 4 H2 mod2N2 H1 mod2N1 CONSTRUCTION OF ENTIRE MODULAR FORMS ×ϕg10 g1 h1 (τ ; 0, H1 ; 2N1 ) × n 1 ατ + β ατ + β × ; H2 , 2N2 ϑg10 h01 ; H1 , 2N1 − ϑ00g0 h0 N2 2 2 γτ + δ γτ + δ ατ + β −4γπi(γτ + δ)ϑg20 h02 ; H2 , 2N2 × γτ + δ o ατ + β ×ϑg10 h01 ; H1 , 2N1 . γτ + δ 191 (1.6) Subtracting (1.6) from (1.5), we obtain n 1 ϑ00 (τ ; 0, 2N1 )ϑg2 h2 (τ ; 0, 2N2 ) − N1 g1 h1 o 3 1 − ϑg1 h1 (τ ; 0, 2N1 )ϑ00g2 h2 (τ ; 0, 2N2 ) = −e sgn γ × N2 4 X 1/2 −1 ϕg10 g1 h1 (0, H1 ; 2N1 )ϕg20 g2 h2 (0, H2 ; 2N2 ) × × 2|γ|(N1 N2 ) (γτ + δ)3 H1 mod2N1 H2 mod2N2 n 1 ατ + β ατ + β ϑ00g0 h0 ; H1 , 2N1 ϑg20 h02 ; H2 , 2N2 − N1 1 1 γτ + δ γτ + δ o 1 ατ + β ατ + β ; H1 , 2N1 ϑg000 h0 ; H2 , 2N2 . − ϑg10 h01 2 2 N2 γτ + δ γτ + δ × (1.7) Analogously, by Lemma 4 from [1], for n − 1 and n = 0 we obtain × (γτ + δ)2 ϑg0 3 h3 (τ ; 0, 2N3 )ϑg4 h4 (τ ; 0, 2N4 ) = 1 −1 = −e sgn γ 2|γ|(N3 N4 )1/2 i sgn γ × 2 X ϕg30 g3 h3 (0, H3 ; 2N3 )ϕg40 g4 h4 (0, H4 ; 2N4 ) × H3 mod2N3 H4 mod2N4 ατ + β ατ + β ; H3 , 2N3 ϑg40 h04 ; H4 , 2N4 . 3 γτ + δ γτ + δ ×ϑ0g0 h0 3 Multiplying (1.7) by (1.8), on account of (1.1), we obtain (γτ + δ)5 Ψ3 (τ ; g1 , . . . , g4 ; h1 , . . . , h4 ; 0, . . . , 0; N1 , . . . , N4 ) = 4 Y 1/2 −1 5 = e sgn γ 4γ 2 Nk i sgn γ × 4 k=1 × X 4 Y Hk mod2Nk k=1 (k=1,2,3,4) ϕgk0 gk hk (0, Hk ; 2Nk ) × (1.8) 192 G. LOMADZE ×Ψ3 ατ + β ; g10 , . . . , g40 ; h01 , . . . , h04 ; H1 , . . . , H4 ; N1 , . . . , N4 . γτ + δ (1.9) Further, applying the same reasoning as in [1, Lemma 5, pp. 62-63], we obtain (1.4) if j = 3. II. As in Subsection I, by Lemma 4 from [1], for n = 1 (with gk , hk , Nk , gk0 , h0k , Hk for all 1 ≤ k ≤ 4 instead of g, h, N , g 0 , h0 , H) and n = 0 (with g4 , h4 , N4 , g40 , h04 , H4 instead of g, h, N , g 0 , h0 , H), we obtain (γτ + δ) 5 3 Y ϑ0gk hk (τ ; 0, 2Nk )ϑg4 h4 (τ ; 0, 2N4 ) = k=1 4 1/2 −1 Y 5 Nk i sgn γ × = e sgn γ 4γ 2 4 k=1 × × 3 Y X 4 Y Hk mod2Nk k=1 (k=1,2,3,4) ϕgk0 gk hk (0, Hk ; 2Nk ) × ατ + β ατ + β ; Hk , 2Nk ϑg40 h04 ; H4 , 2N4 . k γτ + δ γτ + δ ϑ0g0 h0 k k=1 Hence, according to (1.2), it follows that (γτ + δ)5 Ψ4 (τ ; g1 , . . . , g4 ; h1 , . . . , h4 ; 0, . . . , 0; N1 , . . . , N4 ) = =e 4 Y 1/2 −1 5 sgn γ 4γ 2 Nk i sgn γ × 4 k=1 × ×Ψ4 X 4 Y Hk mod2Nk k=1 (k=1,2,3,4) ϕgk0 gk hk (0, Hk ; 2Nk ) × ατ + β ; g10 , . . . , g40 ; h01 , . . . , h04 ; H1 , . . . , H4 ; N1 , . . . , N4 . (1.10) γτ + δ Further, applying the same reasoning as in [1, Lemma 5], we obtain (1.4) if j = 4. Theorem 1. For a given N the functions Ψ3 (τ ) and Ψ4 (τ ) with c1 = c2 = c3 = c4 = 0 are entire modular forms of weight 5 and character χ(δ) = sgn γ( −∆ |δ| ) (∆ is the determinant of an arbitrary positive quadratic form in 10 variables) for the group Γ0 (4N ) if the following conditions hold: 1) 2|gk , Nk |N (k = 1, 2, 3, 4), (1.11) CONSTRUCTION OF ENTIRE MODULAR FORMS 2) 4 4 X h2k X gk2 ,4 4N , Nk 4Nk k=1 3) 193 (1.12) k=1 for all α and δ with αδ ≡ 1 (mod 4N ) Q4 N k=1 k Ψj (τ ; αg1 , . . . , αg4 ; h1 , . . . , h4 ; 0, . . . , 0; N1 , . . . , N4 ) = |δ| −∆ (1.13) = sgn δ Ψj (τ ; g1 , ..., g4 ; h1 , ..., h4 ; 0, ..., 0;N1 , ..., N4 ) |δ| (j = 3, 4). Proof. I. As in the case of Theorem 1 from [1], the functions Ψ3 (τ ) and Ψ4 (τ ) with c1 = c2 = c3 = c4 = 0 satisfy the condition 1) and, by Lemma 1, also the condition 4) of the definition from [1, p. 53–54]. II. From (1.12), since 2 - δ, it follows that 4 4 X X h2k gk2 2ϕ(2Nk )−2 δ 4N δ 2 , 4 . Nk 4Nk k=1 (1.14) k=1 Taking into account (1.11), by Lemma 3 from [1], for n = 2 and n = 0 (with gr , hr , Nr and gs , hs , Ns instead of g, h, N ), we obtain for each substitution from Γ0 (4N ) ατ + β ατ + β ; 0, 2Nr ϑgs hs ; 0, 2Ns = i3η(γ)(sgnδ−1) i1−|δ| × γτ + δ γτ + δ N N βδ g 2 g2 r s r × (γτ + δ)3 e δ 2ϕ(2Nr )−2 + s δ 2ϕ(2Ns )−2 × |δ| 4 4Nr 4Ns αγδ 2 h2 2 h r + s × ×e − 4 4Nr 4Ns 00 (τ ; 0, 2Nr )ϑ0αgs ,hs (τ ; 0, 2Ns ) ×ϑαg (1.15) r ,hr ϑg00r hr for r = 1, s = 2 and r = 2, s = 1. Analogously, by Lemma 3 from [1], for n = 1 and n = 0, we have ατ + β ατ + β ; 0, 2N3 ϑg4 h4 ; 0, 2N4 = sgn δ i2η(γ)(sgnδ−1) × γτ + δ γτ + δ βδ g 2 N N g2 3 4 3 ×i1−|δ| (γτ + δ)2 e δ 2ϕ(2N3 )−2 + 4 δ 2ϕ(2N4 )−2 × |δ| 4 4N3 4N4 αγδ 2 h2 2 h 3 × ×e − + 4 4 4N3 4N4 (1.16) ×ϑ0αg3 ,h3 (τ ; 0, 2N3 )ϑαg4 ,h4 (τ ; 0, 2Ns ). ϑ0g3 h3 194 G. LOMADZE Hence, by (1.1), (1.15), (1.16), and (1.14), we obtain ατ + β ; g1 , . . . , g4 ; h1 , . . . , h4 ; 0, . . . , 0; N1 , . . . , N4 = γτ + δ Q4 N k=1 k (γτ + δ)5 × = sgn δ iη(γ)(sgn δ−1) (−1)1−|δ| |δ| ×Ψ3 (τ ; αg 1 , . . . , αg 4 ; h1 , . . . , h4 ; 0, . . . , 0; N1 , . . . , N4 ), Ψ3 from which according to (1.13) it follows for all α and δ with αδ ≡ 1 (mod 4N ) that ατ + β ; g1 , . . . , g4 ; h1 , . . . , h4 ; 0, . . . , 0; N1 , . . . , N4 = γτ + δ −∆ = sgn δ (γτ + δ)5 Ψ3 (τ ; g1 , . . . , g4 ; h1 , . . . , h4 ; 0, . . . , 0; N1 , . . . , N4 ). |δ| Ψ3 Analogously, by the just mentioned Lemma 3, for n = 1 and n = 0 (with gk , hk , Nk (k = 1, 2, 3, 4) instead of g, h, N ), according to (1.11) and (1.14), we find for all substitutions from Γ0 (4N ) that ατ + β ατ + β ; 0, 2Nk ϑg4 h4 ; 0, 2N4 = γτ + δ γτ + δ k=1 Q4 N k=1 k = sgn δ iη(γ)(sgn δ−1) (−1)1−|δ| (γτ + δ)5 × |δ| 3 Y ϑ0gk hk × 3 Y ϑ0αgk ,hk (τ ; 0, 2Nk )ϑ0αg4 ,h4 (τ ; 0, 2N4 ). (1.17) k=1 Hence, by (1.2), (1.17), and (1.13), for all α and δ with αδ ≡ 1 (mod 4N ) we have ατ + β Ψ4 ; g1 , . . . , g4 ; h1 , . . . , h4 ; 0, . . . , 0; N1 , . . . , N4 = γτ + δ −∆ (γτ + δ)5 Ψ4 (τ ; g1 , . . . , g4 ; h1 , . . . , h4 ; 0, . . . , 0; N1 , . . . , N4 ). = sgn δ |δ| Thus the functions Ψ3 (τ ) and Ψ4 (τ ) with c1 = c2 = c3 = c4 = 0 satisfy the condition 2) of the definition from [1]. III. According to (13) from [1] we have 1) ϑ00gr hr (τ ; 0, 2Nr )ϑgs hs (τ ; 0, 2Ns ) = = −π 2 ∞ X (−1)hr mr+hs ms (4Nr mr +gr )2 e(Λ1 τ ) mr ,ms=−∞ (1.18) CONSTRUCTION OF ENTIRE MODULAR FORMS 195 for r = 1, s = 2 and r = 2, s = 1, where Λ1 = 2 X 1 (2Nk mk + gk /2)2 = 4Nk k=1 = 2 X k=1 2 1X 2 1 Nk m2k + mk gk + gk /4Nk ; 2 4 (1.19) k=1 2) ϑ0g3 h3 (τ ; 0, 2N3 )ϑg4 h4 (τ ; 0, 2N4 ) = ∞ X = πi (−1)h3 m3 +h4 m4 (4N3 m3 + g3 )e(Λ2 τ ), (1.20) m3 ,m4 =−∞ where Λ2 = 4 X 1 (2Nk mk + gk /2)2 = 4Nk k=3 = 4 X k=3 3) 3 Y 4 1X 2 1 Nk m2k + mk gk + gk /4Nk ; 2 4 (1.21) k=3 ϑg0 k hk (τ ; 0, 2Nk )ϑg4 h4 (τ ; 0, 2N4 ) = k=1 = −π 3 i ∞ X 3 P4 Y (−1) k=1 hk mk (4Nk mk + gk )e(Λτ ), m1 ,...,m4 =−∞ k=1 where Λ= = 4 X 1 (2Nk mk + gk /2)2 = 4Nk k=1 4 X k=1 4 1X 2 1 Nk m2k + mk gk + gk /4Nk . 2 4 (1.22) k=1 Λ1 + Λ2 and Λ are integers by virtue of (1.11) and (1.12). Therefore the functions Ψ3 (τ ) and Ψ4 (τ ) satisfy the condition 3) of the definition from [1]. 196 G. LOMADZE 2. Lemma 2. For a given N let Φ3 (τ ) = Φ3 (τ ; g1 , . . . , g4 ; h1 , . . . , h4 ; c1 , . . . , c4 ; N1 , . . . , N4 ) = n 1 ϑ00 (τ ; c1 , 2N1 )ϑg2 h2 (τ ; c2 , 2N2 ) − = N1 g1 h1 4 oY 1 ϑ0gk hk (τ ; ck , 2Nk ) (2.1) − ϑg1 h1 (τ ; c1 , 2N1 ))ϑ00g2 h2 (τ ; c2 , 2N2 ) N2 k=3 and Φ4 (τ ) = Φ4 (τ ; g1 , . . . , g4 ; h1 , . . . , h4 ; c1 , . . . , c4 ; N1 , . . . , N4 ) = = 4 Y ϑ0gk hk (τ ; ck , 2Nk ), (2.2) k=1 where 4 X hk . 2gk , Nk N (k = 1, 2, 3, 4), 4N Nk (2.3) k=1 For all substitutions from Γ in the neighborhood of each rational point τ = − γδ (γ = 6 0, (γ, δ) = 1), we then have (γτ + δ)6 Φj (τ ) = ∞ X n=0 Dn(j) e n ατ + β 4N γτ + δ (j = 3, 4). (2.4) Proof. I. As in the proof of Lemma 1, by Lemma 4 from [1], it follows for n = 1 that × (γτ + δ)3 ϑg0 3 h3 (τ ; 0, 2N3 )ϑ0g4 h4 (τ ; 0, 2N4 ) = 3 1/2 −1 = −e sgn γ 2|γ|(N3 N4 ) × 4 4 X Y ϕg30 g3 h3 (0, H3 ; 2N3 )ϕg40 g4 h4 (τ ; 0, H4 ; 2N4 ) × H3 mod2N3 k=1 H4 mod2N4 ατ + β ατ + β ; H3 , 2N3 ϑ0g0 h0 ; H4 , 2N4 . 3 4 4 γτ + δ γτ + δ ×ϑ0g0 h0 3 Multiplying (1.7) by (2.5), by virtue of (2.1), we obtain (γτ + δ)6 Φ3 (τ ; g1 , . . . , g4 ; h1 , . . . , h4 ; 0, . . . , 0; N1 , . . . , N4 ) = (2.5) CONSTRUCTION OF ENTIRE MODULAR FORMS 4 1/2 −1 2 Y 3 Nk = e sgn γ 4γ 2 k=1 ×Φ3 X Hk mod2Nk (k=1,2,3,4) 197 ϕgk0 gk hk (0, Hk ; 2Nk ) × ατ + β ; g 0 1 , . . . , g 0 4 ; h0 1 , . . . , h0 4 ; H1 , . . . , H4 ; N1 , . . . , N4 . (2.6) γτ + δ Further, applying the same reasoning as in [1, Lemma 5], we obtain (2.4) if j = 3. II. By Lemma 4 from [1], for n = 1 we have (γτ + δ)6 4 Y k=1 × X 4 1/2 −1 Y 3 ϑ0gk hk (τ ; 0, 2Nk ) = e sgn γ 4γ 2 Nk × 2 k=1 4 Y ϕgk0 gk hk (0, Hk ; 2Nk ) 4 Y k=1 Hk mod2Nk k=1 (k=1,2,3,4) ατ + β ϑ0g0 h0 ; Hk , 2Nk . k k γτ + δ Hence, according to (2.2), it follows that (γτ + δ)6 Φ4 (τ ; g1 , . . . , g4 ; h1 , . . . , h4 ; 0, . . . , 0; N1 , . . . , N4 ) = =e 4 Y 1/2 −1 3 Nk sgn γ 4γ 2 2 k=1 ×Φ4 X 4 Y Hk mod2Nk k=1 (k=1,2,3,4) ϕgk0 gk hk (0, Hk ; 2Nk ) × ατ + β ; g 0 1 , . . . , g 0 4 ; h0 1 , . . . , h0 4 ; H1 , . . . , H4 ; N1 , . . . , N4 . γτ + δ Further, applying the same reasoning as in [1, Lemma 5], we obtain (2.4) if j = 4. Theorem 2. For a given N the functions Φ3 (τ ) and Φ4 (τ ) with c1 = c2 = c3 = c4 = 0 are entire modular forms of weight 6 and character ∆ ) (∆ is the determinant of an arbitrary positive quadratic form χ(δ) = ( |δ| in 12 variables) for the group Γ0 (4N ) provided that the following conditions hold: 1) 2) 2|gk , Nk |N 4 4 X h2k X gk2 4 N , ,4 Nk 4Nk k=1 3) (k = 1, 2, 3, 4), (2.7) (2.8) k=1 for all α and δ with αδ ≡ 1 (mod 4N ) Q4 N k=1 k Φj (τ ; αg1 , . . . , αg4 ; h1 , . . . , h4 ; 0, . . . , 0; N1 , . . . , N4 ) = |δ| 198 G. LOMADZE = ∆ |δ| Φj (τ ; g1 , . . . , g4 ; h1 , . . . , h4 ; 0, . . . , 0; N1 , . . . , N4 ) (2.9) (j = 3, 4). Proof. I. As in the case of Theorem 1, the functions Φ3 (τ ) and Φ4 (τ ) with c1 = c2 = c3 = c4 = 0 satisfy the condition 1) and, on account of Lemma 2, also the condition 4) of the definition from [1]. II. Since 2 - δ, from (2.8) it follows that 4 4 2 X hk2 X gk2 2ϕ(2Nk )−2 4N δ . , 4 δ Nk 4Nk k=1 (2.10) k=1 Taking into account (2.7), by Lemma 3 from [1], for n = 1 we find that for all substitutions from Γ0 (4N ) we have ατ + β N N 3 4 ; 0, 2Nk = i3η(γ)(sgnδ−1) i1−|δ| × γτ + δ |δ| k=3 βδ g 2 g2 3 ×(γτ + δ)3 e δ 2ϕ(2N3 )−2 + 4 δ 2ϕ(2N4 )−2 × 4 4N3 4N4 4 αγδ 2 h2 2 Y h 3 0 + 4 ϑαg (τ ; 0, 2Nk ). (2.11) ×e − k ,hk 4 4N3 4N4 4 Y ϑ0gk hk k=3 Taking into account (2.10) and (2.9), by (2.1), (1.15), and (2.11), for all α and δ with αδ ≡ 1 (mod 4N ) we obtain ατ + β Φ3 ; g1 , . . . , g4 ; h1 , . . . , h4 ; 0, . . . , 0; N1 , . . . , N4 = γτ + δ Q4 N 1−|δ| 2η(γ)(sgn δ−1) k=1 k (γτ + δ)6 × =i (−1) |δ| ×Φ3 (τ ; αg 1 , . . . , αg 4 ; h1 , . . . , h4 ; 0, . . . , 0; N1 , . . . , N4 ) = ∆ = (γτ + δ)6 Φ3 (τ ; g1 , . . . , g4 ; h1 , . . . , h4 ; 0, . . . , 0; N1 , . . . , N4 ). |δ| Analogously, taking into account (2.7) and (2.10), by Lemma 3 from [1], for n = 1, we have = Q4 4 Y ϑ0gk hk k=1 k=1 |δ| Nk ατ + β ; 0, 2Nk = γτ + δ 6 (γτ + δ) for all substitutions from Γ0 (4N ). 4 Y k=1 ϑαgk ,hk (τ ; 0, 2Nk ) (2.12) CONSTRUCTION OF ENTIRE MODULAR FORMS 199 Hence, by (2.2), (2.12), and (2.9), for all α and δ with αδ ≡ 1 (mod 4N ), we have ατ + β Φ4 ; g1 , . . . , g4 ; h1 , . . . , h4 ; 0, . . . , 0; N1 , . . . , N4 = γτ + δ ∆ (γτ + δ)6 Φ4 (τ ; g1 , . . . , g4 ; h1 , . . . , h4 ; 0, . . . , 0; N1 , . . . , N4 ). = |δ| Thus the functions Φ3 (τ ) and Φ4 (τ ) with c1 = c2 = c3 = c4 = 0 satisfy the condition 2) of the definition from [1]. III. According to (13) from [1], we have 1) (1.18) with Λ1 defined by (1.19); 2) 4 Y ϑ0gk hk (τ ; 0, 2Nk ) = k=3 = −π 2 ∞ X (−1)h3 m3 +h4 m4 m3 ,m4 =−∞ 4 Y (4Nk mk + gk )e(Λ2 τ ), k=3 where Λ2 is defined by (1.20); 3) 4 Y ϑ0gk hk (τ ; 0, 2Nk ) = k=1 = π4 ∞ X m1 ,...,m4 =−∞ 4 P4 Y (−1) k=1 hk mk (4Nk mk + gk )e(Λτ ), k=3 where Λ2 is defined by (1.21). Thus the functions Φ3 (τ ) and Φ4 (τ ) with c1 = c2 = c3 = c4 = 0 satisfy the condition 3) of the definition from [1]. References 1. G. Lomadze, On some entire modular forms of weights 5 and 6 for the congruence group Γ0 (4N ). Georgian Math. J. 1(1994), No. 1, 53-76. (Received 28.06.1993) Author’s address: Faculty of Mechanics and Mathematics I. Javakhishvili Tbilisi State University 2, University St., Tbilisi 380043 Republic of Georgia