POLYNOMIAL FIRST INTEGRALS FOR WEIGHT-HOMOGENEOUS PLANAR POLYNOMIAL DIFFERENTIAL SYSTEMS OF WEIGHT DEGREE 4

Size: px
Start display at page:

Download "POLYNOMIAL FIRST INTEGRALS FOR WEIGHT-HOMOGENEOUS PLANAR POLYNOMIAL DIFFERENTIAL SYSTEMS OF WEIGHT DEGREE 4"

Transcription

1 ROCKY MOUNTAIN JOURNAL OF MATHEMATICS Volume 46, Number 5, 2016 POLYNOMIAL FIRST INTEGRALS FOR WEIGHT-HOMOGENEOUS PLANAR POLYNOMIAL DIFFERENTIAL SYSTEMS OF WEIGHT DEGREE 4 JAUME LLIBRE AND CLAUDIA VALLS ABSTRACT. We classify all of the weight-homogeneous planar polynomial differential systems of weight degree 4 having a polynomial first integral. 1. Introduction and statement of the main result. In this paper, we deal with polynomial differential systems of the form: 1.1) dx dt = ẋ = Px), x = x, y) C2, with Px) = P 1 x), P 2 x)) and P i C[x, y] for i = 1, 2. As usual, Q +, R and C will denote the sets of non-negative rational, real and complex numbers, respectively, and C[x, y] denotes the polynomial ring over C in the variables x, y. Here, t is real or complex. System 1.1) is weight homogeneous or quasi-homogeneous if there exist s = s 1, s 2 ) N 2 and d N such that, for arbitrary α R + = {a R, a > 0}, 1.2) P i α s 1 x, α s 2 y) = α s i 1+d P i x, y), for i = 1, 2. We call s = s 1, s 2 ) the weight exponent of system 1.1) and d the weight degree with respect to the weight exponent s. In the particular case where s = 1, 1), system 1.1) is called a homogeneous polynomial differential system of degree d AMS Mathematics subject classification. Primary 34A05, 34A34, 34C14. Keywords and phrases. Polynomial first integrals, weight-homogeneous polynomial differential systems. The first author is partially supported by MINECO/FEDER, grant Nos. MTM and MTM P, ICREA Academia, grant Nos. FP7- PEOPLE-2012-IRSES and , AGAUR, grant No. 2014SGR-568, and grant No. UNAB13-4E The second author is supported by Portuguese national funds through FCT, Fundação para a Ciência e a Tecnologia, grant No. PEst- OE/EEI/LA0009/2013 CAMGSD). Received by the editors on October 9, 2012, and in revised form on January 9, DOI: /RMJ Copyright c 2016 Rocky Mountain Mathematics Consortium 1619

2 1620 JAUME LLIBRE AND CLAUDIA VALLS Recently, such systems have been investigated by several authors. Labrunie [12] and Ollagnier [15] characterized all polynomial first integrals of the three-dimensional a, b, c) Lotka-Volterra systems. Maciejewski and Strelcyn [14] proved that the so-called Halphen system has no algebraic first integrals. However, some of the best results for general weight homogeneous polynomial differential systems have been provided by Furta [10] and Goriely [11]. For quadratic homogeneous polynomial differential systems, we refer the reader to [13, 16]. Additionally, we refer the reader to [1 5]. A non-constant function Hx, y) is a first integral of system 1.1) if it is constant on all solution curves xt), yt)) of system 1.1), i.e., Hxt), yt))is constant for all values of t for which the solution xt), yt)) is defined. If H is C 1, then H is a first integral of system 1.1) if and only if H 1.3) P 1 x + P H 2 y = 0. The function Hx, y) is weight homogeneous of weight degree m with respect to the weight exponent s if it satisfies Hα s 1 x, α s 2 y) = α m Hx, y), for all α R +. Given H C[x, y], we can split it into the form H = H m + H m H m+l, where H m+i is a weight homogeneous polynomial of weight degree m+i with respect to the weight exponent s, i.e., H m+i α s 1 x, α s 2 y) = α m+i H m+i x, y). The following well-known proposition see [13] for proof) reduces the study of the existence of analytic first integrals of a weighthomogeneous polynomial differential system 1.1) to the study of the existence of a weight-homogeneous polynomial first integral. Proposition 1.1. Let H be an analytic function, and let H = i H i be its decomposition into weight-homogeneous polynomials of weight degree i with respect to the weight exponent s. Then, H is an analytic first

3 WEIGHT-HOMOGENEOUS POLYNOMIAL SYSTEMS 1621 integral of the weight-homogeneous polynomial differential system 1.1) if and only if each weight-homogeneous part H i is a first integral of system 1.1) for all i. The main goal of this paper is to classify all analytic first integrals of the weight-homogenous planar polynomial differential systems of weight degree 4. In view of Proposition 1.1, we only need to classify all polynomial first integrals of the weight-homogenous planar polynomial differential systems of weight degree 4. The classification of all polynomial first integrals and hence, of all analytic first integrals) of the weight-homogenous planar polynomial differential systems of weight degree 1 is straightforward and trivial. The classification of all polynomial first integrals and hence, of all analytic first integrals) of the weighthomogenous planar polynomial differential systems of weight degree 2 was given in [8, 13] and for systems of weight degree 3 in [6, 8]. Kowalevskaya exponents are used in the classification of all polynomial first integrals for weight-homogenous planar polynomial differential systems of weight degrees 2 and 3. However, it was shown in [6, Theorem 4] that these exponents are useless for classifying the polynomial first integrals for weight-homogenous planar polynomial differential systems of weight degrees larger than 3. Proposition 1.2. The systems with weight degree 4 in C 2 and their corresponding values of s can be written as follows: s = 1, 1) : ẋ = a 40 x 4 + a 31 x 3 y + a 22 x 2 y 2 + a 13 xy 3 + a 04 y 4, ẏ = b 40 x 4 + b 31 x 3 y + b 22 x 2 y 2 + b 13 xy 3 + b 04 y 4 ; s = 1, 2) : ẋ = a 40 x 4 + a 21 x 2 y + a 02 y 2, ẏ = b 50 x 5 + b 31 x 3 y + b 12 xy 2 ; s = 1, 3) : ẋ = a 40 x 4 + a 11 xy, ẏ = b 60 x 6 + b 31 x 3 y + b 02 y 2 ; s = 1, 4) : ẋ = a 40 x 4 + a 01 y, ẏ = b 70 x 7 + b 31 x 3 y; s = 2, 3) : ẋ = a 11 xy, ẏ = b 30 x 3 + b 02 y 2 ; s = 2, 5) : ẋ = a 01 y, ẏ = b 40 x 4 ; s = 3, 3) : ẋ = a 20 x 2 + a 11 xy + a 02 y 2, ẏ = b 20 x 2 + b 11 xy + b 02 y 2 ; s = 6, 9) : ẋ = a 01 y, ẏ = b 20 x 2.

4 1622 JAUME LLIBRE AND CLAUDIA VALLS The proof of Proposition 1.2 is provided in Section 2. In what follows, we state our main result, i.e., we classify when the systems of Proposition 1.2 exhibit a polynomial first integral. The systems with weight exponent 1, 1) having a polynomial first integral are given in Section 3. The systems with weight exponent 3, 3) having a polynomial first integral are studied inside the systems with weight exponent 1, 2). The polynomial first integrals for the other systems of Proposition 1.2 are provided in this introduction. We introduce the change X, Y ) = x 2, y) in the planar weight homogeneous polynomial differential systems 1.1) of weight degree 4 with weight exponent 1, 2). With these new variables X, Y ) the system with weight exponent 1, 2) becomes, after introducing the new independent variable dτ = x dt, 1.4) X = 2a 40 X 2 + 2a 21 XY + 2a 02 Y 2, Y = b 50 X 2 + b 31 XY + b 12 Y 2, where the prime denotes the derivative with respect to τ. System 1.4) is a homogeneous quadratic planar polynomial system with s = 1, 1). It is well known see [9]) that, for each quadratic homogeneous system, there exist some linear transformation and a rescaling of time which transform system 1.4) into systems in 1.5). 1.5) ẋ = 2xy xp 1x + p 2 y), ẋ = 2xy xp 1x + p 2 y), ẋ = x xp 1x + p 2 y), ẋ = 2 3 xp 1x + p 2 y), ẋ = 2 3 xp 1x + p 2 y), ẏ = x 2 + y yp 1x + p 2 y), ẏ = x 2 + y yp 1x + p 2 y), ẏ = 2xy yp 1x + p 2 y), ẏ = x yp 1x + p 2 y), ẏ = 2 3 yp 1x + p 2 y). We prove the following theorem which characterizes all polynomial first integrals for the systems in 1.5). Theorem 1.3. The homogeneous polynomial systems in 1.5) have a polynomial first integral H if and only if one of the following conditions hold. a) The first system in 1.5) with p 1 = 0, p 2 = 31 q)/1 + 2q) with q = n/m Q + and, in this case, H = x m 3y 2 x 2 ) n.

5 WEIGHT-HOMOGENEOUS POLYNOMIAL SYSTEMS 1623 b) The second system in 1.5) with p 1 = 0, p 2 = 31 q)/1 + 2q) with q = n/m Q + and, in this case, H = x m 3y 2 + x 2 ) n. c) The third system, in 1.5) with p 1 = 0 and p 2 = 31 2q)/21+q)) with q = n/m Q + and, in this case, H = x m y n. d) The fourth system in 1.5) with p 1 = p 2 = 0 and, in this case, H = x. We note that systems with weight exponent 3, 3) coincide with systems 1.4), and hence, it can be written into systems in 1.5). Therefore, Theorem 1.3 applies to those systems. The proof of Theorem 1.3 is given in Section 4. Theorem 1.4. The weight homogeneous polynomial differential systems with weight exponent 1, 3) and weight degree 4 have a polynomial first integral H if and only if the following conditions hold: a) a 11 = a 40 = 0 with H = x. b) b 60 = b 31 = b 02 = 0 with H = y. c) 3a 11 b 02 )3a 11 2b 02 ) 0, a 40 = a 11 b 31 /3a 11 2b 02 ), 3a 11 /6a 11 2b 02 ) = m/n Q + and m/n < 1 with H = x 3n m) 3a 11 2b 02 )b 60 x a 11 b 02 )b 31 x 3 y 9a a 11 b b 2 02)y 2 ) m. d) b 31 /a 40 = m/n and m/n Q + with H = x 3m b 60 x 3 + b 31 3a 40 )y) 3n. e) b 02 = 0, a 11 0, a 40 = b 31 /3 and b 06 = 3a 40 b 31 ) 2 /12a 11 ) with H = b 31 x 3 3a 11 y. f) 3a 11 b 02 )3a 11 2b 02 ) 0, a 40 = a 11 b 31 /3a 11 2b 02 ), b 06 = 3a 40 b 31 ) 2 /43a 11 b 02 )), b 02 0 and 3a 11 /b 02 = n/m Q +, with H = x 3n b 31 x 3 + 2b 02 3a 11 )y) m. The proof of Theorem 1.4 is given in Section 5. Theorem 1.5. The weight homogeneous polynomial differential systems with weight exponent 1, 4) and weight degree 4 have a polynomial first integral H if and only if the following conditions hold:

6 1624 JAUME LLIBRE AND CLAUDIA VALLS a) a 40 = a 01 = 0 and H = x. b) b 70 = b 31 = 0 and H = y. c) b 31 = 4a 40, and 4a a 01 b 70 0 with H = b 70 x 8 + 8a 40 x 4 y + 4a 01 y 2. d) b 31 = 4a 40, a 40 b 70 0 and 4a a 01 b 70 = 0 with H = b 70 x 4 4a 40 y. The proof of Theorem 1.5 is given in Section 6. Theorem 1.6. The weight homogeneous polynomial differential systems with weight exponent 2, 3) and weight degree 4 have a polynomial first integral H if and only if a 11 = 0, in which case H = x, or b 30 = b 02 = 0, in which case, H = y, or a 11 3a 11 2b 02 ) 0 and 2b 02 /a 11 = n/m Q +, in which case, H = x n 2b 30 x 3 3a 11 y 2 + 2b 02 y 2 ) m. The proof of Theorem 1.6 is given in Section 7. Theorem 1.7. The weight homogeneous polynomial differential systems with weight exponent 2, 5) and weight degree 4 have the polynomial first integral H = 2b 40 x 5 5a 01 y 2. The proof of Theorem 1.7 is given in Section 8. Theorem 1.8. The weight homogeneous polynomial differential systems with weight exponent 6, 9) and weight degree 4 have the polynomial first integral H = 2b 20 x 3 3a 01 y 2. The proof of Theorem 1.8 is given in Section Proof of Proposition 1.2. From the definition of weight homogeneous polynomial differential systems 1.1) with weight degree 4, the exponents u i and v i of any monomial x u i y v i of P i for i = 1, 2, are such that they satisfy respectively the relations 2.1) s 1 u 1 + s 2 v 1 = s and s 1 u 2 + s 2 v 2 = s 2 + 3,

7 WEIGHT-HOMOGENEOUS POLYNOMIAL SYSTEMS 1625 respectively. Moreover, we can assume that P 1 and P 2 are coprime, and, without loss of generality, we can also assume that s 1 s 2. We consider different values of s 1. Case s 1 = 1. If s 2 = 1, then in view of 2.1), we must have u 1 + v 1 = 4 and u 2 + v 2 = 4, that is, u i, v i ) = 0, 4), u i, v i ) = 1, 3), u i, v i ) = 2, 2), u i, v i ) = 3, 1) and u i, v i ) = 4, 0), for i = 1, 2. If s 2 = 2, then, in view of 2.1), we must have u 1 + 2v 1 = 4 and u 2 + 2v 2 = 5, that is, u 1, v 1 ) = 0, 2), u 1, v 1 ) = 2, 1) and u 1, v 1 ) = 4, 0), while u 2, v 2 ) = 1, 2), u 2, v 2 ) = 3, 1), and finally, u 2, v 2 ) = 5, 0). If s 2 = 3, then, in view of 2.1), we must have u 1 + 3v 1 = 4 and u 2 + 3v 2 = 6, that is, u 1, v 1 ) = 1, 1), u 1, v 1 ) = 4, 0), while u 2, v 2 ) = 0, 2), u 2, v 2 ) = 3, 1), and finally, u 2, v 2 ) = 6, 0). If s 2 = 4, then, in view of 2.1), we must have u 1 + 4v 1 = 4 and u 2 + 4v 2 = 7, that is, u 1, v 1 ) = 0, 1), u 1, v 1 ) = 4, 0), while u 2, v 2 ) = 3, 1), and finally, u 2, v 2 ) = 7, 0). If s 2 = 4 + l with l 1, then equation 2.1) becomes 2.2) u l)v 1 = 4 and u l)v 2 = 7 + l. From the first equation of 2.2), we obtain v 1 = 0 and u 1 = 4. By the second equation of 2.2), it follows that v 2 {0, 1}. If v 2 = 0, then u 2 = 7 + l; if v 2 = 1, then u 2 = 3. In both cases, P 1 and P 2 are not coprime. Thus, this case is not considered. Case s 1 = 2. Now, we have s 2 2. If s 2 = 2, then in view of 2.1), we must have 2u 1 + 2v 1 = 5 and 2u 2 + 2v 2 = 5, which is not possible because 5 is not an even number. If s 2 = 3, then, in view of 2.1), we must have 2u 1 + 3v 1 = 5 and 2u 2 + 3v 2 = 6, that is, u 1, v 1 ) = 1, 1), while u 2, v 2 ) = 0, 2) and u 2, v 2 ) = 3, 0). If s 2 = 4, then, in view of 2.1), we must have 2u 1 + 4v 1 = 5 and 2u 2 + 4v 2 = 7, which is not possible because 5 is not even. If s 2 = 5, then, in view of 2.1), we must have 2u 1 + 5v 1 = 5 and 2u 2 + 5v 2 = 8, that is, u 1, v 1 ) = 0, 1) and u 2, v 2 ) = 4, 0). If s 2 = 5 + l with l 1, then equation 2.1) becomes 2.3) 2u l)v 1 = 5 and 2u l)v 2 = 8 + l.

8 1626 JAUME LLIBRE AND CLAUDIA VALLS The first equation of 2.3) is not possible because 5 is not an even number, 5 + l 6 and u 1 and v 1 are non-negative integers. Case s 1 = 3. Now, we have s 2 3. If s 2 = 3, then in view of 2.1), we must have 3u 1 + 3v 1 = 6 and 3u 2 + 3v 2 = 6, that is, u i, v i ) = 0, 2), u i, v i ) = 1, 1) and u i, v i ) = 2, 0), for i = 1, 2. If s 2 = 3 + l with l 1, then in view of 2.1), we must have 2.4) 3u l)v 1 = 6 and 3u l)v 2 = 6 + l. From the first equation of 2.4) we have that v 1 = 6 3u l and, using l 1, then v 1 {0, 1} l, When v 1 = 0, then 3u 1 = 6; thus, u 1 = 2. Then, from the second equation of 2.4) we obtain that v 2 {0, 1}. If v 2 = 0, then u 2 1, and, if v 2 = 1, then u 2 = 1. In both cases, we have that P 1 and P 2 are not coprime. When v 1 = 1, then 3u 1 = 3 l, which is not possible since u 1 is an integer and l 1. Case s 1 = 3 + l with l 1. Now, we have s l with l 1, and equation 2.1) becomes 2.5) and 3 + l)u 1 + s 2 v 1 = 6 + l = 3 + l) l)u 2 + s 2 v 2 = 3 + s 2. From the first equation of 2.5), and taking into account that l 1, we obtain that u 1 {0, 1}. When u 1 = 0, we must have s 2 v 1 = 6 + l, and since s l, we obtain v 1 = 6 + l 3 + l) + 3 = s l 3 + l. Since v 1 0 and l 1, we must have v 1 = 1. Then s 2 = 6 + l. Now, the second equation of 2.5) becomes 2.6) 3 + l)u l)v 2 = 6 + l) + 3.

9 WEIGHT-HOMOGENEOUS POLYNOMIAL SYSTEMS 1627 Then v 2 = 0. From equation 2.6), we have u 2 = 1 + 6/l + 3). Thus, l = 3 and u 2 = 2, and we obtain the systems with weight exponent 6, 9). When u 1 = 1, we must have s 2 v 1 = 3, and, since s 2 3+l, we obtain 3 + l)v 2 3, which is not possible because l 1. This concludes the proof of the proposition. 3. Weight exponent s = 1, 1). A weight homogeneous polynomial system, ẋ = P 1 x, y); ẏ = P 2 x, y), with weight exponent 1, 1) and weight degree d is integrable, and its inverse integrating factor is V x, y) = xp 2 x, y) yp 1 x, y). See [7] for more details. As P 1 x, y), P 2 x, y) and V x, y) are homogeneous polynomials, if the degree of P 1 x, y) and P 2 x, y) is d, then, of course, the degree of V x, y) is d + 1. Thus, for d = 4, we can write the homogeneous polynomials as follows: 3.1) and P 1 x, y) = p 1 a 1 )x 4 + p 2 4a 2 )x 3 y + p 3 6a 3 )x 2 y 2 + p 4 4a 4 )xy 3 a 5 y 4, P 2 x, y) = a 0 x 4 + 4a 1 + p 1 )x 3 y + 6a 2 + p 2 )x 2 y 2 + 4a 3 + p 3 )xy 3 + a 4 + p 4 )y 4, V x, y) = a 0 x 5 + 5a 1 x 4 y + 10a 2 x 3 y a 3 x 2 y 3 + 5a 4 xy 4 + a 5 y 5. Thus, the first integral is Hx, y) = P1 x, y) dy + gx), V x, y) satisfying H/ x = P 2 /V. The canonical forms appear in the factorization of V. Assume that V x, y) factorizes as: i) five simple real roots: a 0 x r 1 y)x r 2 y)x r 3 y)x r 4 y)x r 5 y), ii) one double and three simple real roots: a 0 x r 1 y) 2 x r 2 y)x r 3 y)x r 4 y),

10 1628 JAUME LLIBRE AND CLAUDIA VALLS iii) two double roots and one simple real root: a 0 x r 1 y) 2 x r 2 y) 2 x r 3 y), iv) one triple and two simple real roots: a 0 x r 1 y) 3 x r 2 y)x r 3 y), v) one triple and one double real roots: a 0 x r 1 y) 3 x r 2 y) 2, vi) one quadruple and one simple real roots: a 0 x r 1 y) 4 x r 2 y), vii) one quintuple real root: a 0 x ry) 5, viii) three real and one couple of conjugate complex roots: a 0 x r 1 y)x r 2 y)x r 3 y)x 2 + bxy + cy 2 ) with b 2 4c < 0, ix) one double, one simple real and one couple of conjugate complex roots: a 0 x r 1 y) 2 x r 2 y)x 2 + bxy + cy 2 ) with b 2 4c < 0, x) one triple real and one couple of conjugate complex roots: a 0 x r 1 y) 3 x 2 + bxy + cy 2 ) with b 2 4c < 0, xi) one simple real and two couples of conjugate complex roots: a 0 x ry)x 2 + b 1 xy + c 1 y 2 )x 2 + b 2 xy + c 2 y 2 ) with b 2 1 4c 1 < 0, b 2 2 4c 2 < 0, xii) one simple real and one double couple of conjugate complex roots: a 0 x ry)x 2 + bxy + cy 2 ) 2 with b 2 4c < 0. Now, we shall compute the first integral for each case and obtain the conditions in order to show that it is a polynomial. We define the function: fr) = 5p 4 + p 3 r + p 2 r 2 + p 1 r 3 ). Case i). A first integral H is x r 1 y) γ 1 x r 2 y) γ 2 x r 3 y) γ 3 x r 4 y) γ 4 x r 5 y) γ 5, where γ i = fr i ) + a 0 5 r i r j ) j=1 j i 5 r i r j ) j=1 j i. We note that an integer power of H is a polynomial if and only if γ i Q for i = 1, 2, 3, 4, 5, if they all have the same sign.

11 WEIGHT-HOMOGENEOUS POLYNOMIAL SYSTEMS 1629 Case ii). A first integral H is x r 1 y) γ 1 x r 2 y) γ 2 x r 3 y) γ 3 x r 4 y) γ 4 ) fr 1 )x exp, r 1 r 1 r 2 )r 1 r 3 )r 1 r 4 )x r 1 y) with γ 1 = A 1 /B 1 = A 1 /[r 1 r 2 ) 2 r 1 r 3 ) 2 r 1 r 4 ) 2 ], A 1 = 5p 1 r 2 + r 3 + r 4 )r 2 1 2r 3 r 4 + r 2 r 3 + r 4 ))r 1 + 3r 2 r 3 r 4 )r p 2 r 3 1 r 3 r 4 + r 2 r 3 + r 4 ))r 1 + 2r 2 r 3 r 4 )r 1 + 5p 3 2r 3 1 r 2 + r 3 + r 4 )r r 2 r 3 r 4 ) + 5p 4 3r 2 1 2r 2 + r 3 + r 4 )r 1 + r 3 r 4 + r 2 r 3 + r 4 )) 2a 0 B 1, for i = 2,..., 4 and γ i = A i B i = fr i ) + a 0 B i ). 4 r 1 r i ) 2 r i r j ) We note that an integer power of H is a polynomial if and only if fr 1 ) = 0 and γ i Q for i = 1, 2, 3, 4, if they all have the same sign. Case iii). A first integral H is x r 1 y) γ 1 x r 2 y) γ 2 x r 3 y) γ 3 exp j=2 j i 2 i=1 ) fr i )x r i r 1 r 2 ) 2, r i r 3 )r i y x) with γ i = A i /B i = A i /[r 1 r 2 ) 3 r i r 3 ) 2 ] for i = 1, 2, γ 3 = A 3 /B 3 = fr 3 ) + a 0 B 3 )/[r 1 r 3 ) 2 r 2 r 3 ) 2 ], A i = 2a 0 B i + 1) i+1 5p 4 3r i r j 2r 3 ) 5p 3 r 1 + r 2 )r 3 2r 2 i ) + 5p 2 r i r i r 1 + r 2 ) 2r j r 3 ) + 5p 1 r 2 i 3r j r 3 + r i 2r j + r 3 ))), for i, j = 1, 2 and i j. We note that an integer power of H is a polynomial if and only if fr i ) = 0 for i = 1, 2 and γ i Q for i = 1, 2, 3, if they all have the same sign. Case iv). A first integral H is ) 5βx x r 1 y) γ1 x r 2 y) γ2 x r 3 y) γ3 exp 2r1 2r 1 r 2 ) 2 r 1 r 3 ) 2 r 1 y x) 2,

12 1630 JAUME LLIBRE AND CLAUDIA VALLS with β = p 1 r 2 1 3r 2 r 1 3r 3 r 1 +5r 2 r 3 )r 3 1 p 2 r 2 1 +r 2 r 1 +r 3 r 1 3r 2 r 3 )r 2 1 p 3 3r 2 1 r 2 r 1 r 3 r 1 r 2 r 3 )r 1 +p 4 5r r 2 r 1 +3r 3 r 1 r 2 r 3 ))x + 2r 1 p 1 r 1 r 2 2r 3 r 2 + r 1 r 3 )r p 3 2r 1 r 2 r 3 )r p 2 r 2 1 r 2 r 3 )r p 4 3r 2 1 2r 2 r 1 2r 3 r 1 + r 2 r 3 ))y, γ 1 = A 1 /B 1 = A 1 /[r 1 r 2 ) 3 r 1 r 3 ) 3 ], A 1 = 3a 0 B 1 5r 2 p 2 + p 1 r 2 )r r 1 3r 2 )p 2 + p 1 r 2 )r 3 r p 2 r p 1 r 1 r 2 1 3r 2 r 1 + 3r 2 2))r 2 3) + 5p 3 r 3 1 3r 2 r 3 r 1 + r 2 r 3 r 2 + r 3 )) + 5p 4 3r 2 1 3r 2 + r 3 )r 1 + r r r 2 r 3 ), γ i = A i /B i = 1) i fr i ) + a 0 B i )/[r 1 r i ) 3 r 2 r 3 )] for i = 2, 3. We note that an integer power of H is a polynomial if and only if β = 0 and γ i Q for i = 1, 2, 3, if they all have the same sign. Case v). A first integral H is where β = 2r 1 r 2 )xfr 2 )r 2 1 r 2 r 2 y x) and x r 1 y) γ 1 x r 2 y) γ 2 expβ), + r 1 r 2 ) 2 x 2 fr 1 ) x r 1 y) r 1 r 2 )2p 3 + 2p 1 r 1 r 2 + p 2 r 1 + r 2 ))r1 2 + p 4 3r 1 r 2 ))x, r 1 y x γ 1 = 2r 2 1 3a0 r 1 r 2 ) p 4 + 5p 3 r 1 + 2r 2 ) + 5r 2 3p 1 r 1 r 2 + p 2 2r 1 + r 2 )) ), γ 2 = 2r 2 1 2a0 r 1 r 2 ) 4 15p 4 5p 3 r 1 + 2r 2 ) 5r 2 3p 1 r 1 r 2 + p 2 2r 1 + r 2 )) ). We note that an integer power of H is a polynomial if and only if β = 0 and γ i Q for i = 1, 2, if they all have the same sign. Case vi). A first integral H is x r 1 y) γ 1 x r 2 y) γ 2 expβ),

13 WEIGHT-HOMOGENEOUS POLYNOMIAL SYSTEMS 1631 where β = 2r 1 r 2 ) 3 fr 1 )x 3 r 3 1 r 1y x) 3 and + 30r 1 r 2 )p 3 +r 2 p 2 + p 1 r 2 ))r p 4 3r 2 1 3r 2 r 1 + r 2 2))x r 3 1 r 1y x) + 15r 1 r 2 ) 2 p 4 3r 1 2r 2 )+r 1 p 2 +p 1 r 2 )r p 3 2r 1 r 2 )))x 2 r 3 1 x r 1y) 2, γ 1 = 6 4a 0 r 1 r 2 ) 4 + 5p 4 + 5r 2 p 3 + r 2 p 2 + p 1 r 2 ))), γ 2 = 6a 0 r 1 r 2 ) 4 + 5p 4 + 5r 2 p 3 + r 2 p 2 + p 1 r 2 ))). We note that an integer power of H is a polynomial if and only if β = 0 and γ i Q for i = 1, 2, if they all have the same sign. Case vii). A first integral H is x ry) γ 1 exp where βx x ry) 4 β = rxrx p 2 x + 3p 1 rx + 4p 2 ry) + p 3 x 2 4ryx + 6r 2 y 2 )) 3p 4 x 2ry)x 2 2ryx + 2r 2 y 2 ), and γ 1 = 12a 0 r 4. We note that x ry is a polynomial first integral if and only if β = 0. Case viii). A first integral H is x r 1 y) γ 1 x r 2 y) γ 2 x r 3 y) γ 3 x 2 + bxy + cy 2 ) γ 4 βx bx + 2cy exp 3 i=1 c + b r i + ri 2) 4c b 2 )x arctan )), 2 4c b2 )x 2 where β = 52p 1 c 3 bp 2 p 1 r 1 + r 2 + r 3 )) + 2p 3 + p 2 r 1 + r 2 + r 3 ) + p 1 r 2 r 3 + r 1 r 2 + r 3 ))))c 2 + p 3 + p 1 r 1 r 2 + p 1 r 1 + r 2 )r 3 )b 2 + 3p 4 3p 1 r 1 r 2 r 3 + p 3 r 1 + r 2 + r 3 ) p 2 r 2 r 3 + r 1 r 2 + r 3 )))b + 2p 2 r 1 r 2 r 3 + p 4 r 1 + r 2 + r 3 ) + p 3 r 2 r 3 + r 1 r 2 + r 3 ))))c ),

14 1632 JAUME LLIBRE AND CLAUDIA VALLS bp 4 b + r 1 )b + r 2 )+p 1 r 1 b 3 p 2 r 1 b 2 p 4 b + p 3 r 1 b 2p 4 r 1 )r 2 bp 4 b + r 1 ))r 3 ), and γ i = A i /B i = fr i ) + a 0 B i )/[c + br i + r 2 i ) 3 j=1, j i r i r j )] for i = 1, 2, 3, γ 4 = A 4 /B 4 = A 4 /[2 3 i=1 c + b r i + r 2 i )] A 4 = a 0 B 4 + 5p 2 + p 1 r 1 + r 2 + r 3 ))c 2 p 4 + p 1 r 1 r 2 r 3 + p 3 r 1 + r 2 + r 3 ) + p 2 r 2 r 3 + r 1 r 2 + r 3 )) + bp 3 p 1 r 2 r 3 + r 1 r 2 + r 3 ))))c + p 4 b + r 1 )b + r 2 ) + p 4 b + r 1 ) + p 4 + p 1 b 2 p 2 b + p 3 )r 1 )r 2 )r 3 ). We note that an integer power of H is a polynomial if and only if β = 0 and γ i Q for i = 1, 2, 3, 4, if they all have the same sign. Case ix). A first integral H is x r 1 y) γ1 x r 2 y) γ2 x 2 +bxy+cy 2 ) γ3 fr 1 )x exp r 1 r 1 r 2 )c+r 1 b+r1 2)r 1y x) βx bx + 2cy + 2 i=1 c + b r i + ri 2)3 i 4c b 2 )x arctan )), 2 4c b2 )x 2 where β = 52p 1 c 3 bp 2 p 1 2r 1 + r 2 )) + 2p 3 + p 2 2r 1 + r 2 ) + p 1 r 1 r 1 + 2r 2 )))c 2 + p 3 + p 1 r 1 r 1 + 2r 2 ))b 2 + 3p 4 + p 3 2r 1 + r 2 ) r 1 3p 1 r 1 r 2 + p 2 r 1 + 2r 2 )))b + 2p 4 2r 1 + r 2 ) + r 1 p 2 r 1 r 2 + p 3 r 1 + 2r 2 ))))c bp 4 b + r 1 ) 2 + p 4 b 2 2p 4 r 1 b+bp 1 b 2 p 2 b + p 3 ) 2p 4 )r 2 1)r 2 ), A 1 γ 1 = A 1 = B 1 r 1 r 2 ) 2 c + b r 1 + r1 2, )2 A 1 = 2a 0 c 2 r 1 r 2 ) 2 + 2a 0 b 2 r 2 1r 1 r 2 ) 2 + c 5p 4 + r 1 4a 0 b + r 1 )r 1 r 2 ) 2 + 5p 1 r 1 2r 1 3r 2 ) + 5p 2 r 1 2r 2 )) 5p 3 r 2 ) + b4a 0 r 1 r 1 r 2 ) 2 5p 3 + 5p 1 r 1 r 1 2r 2 ) 5p 2 r 2 )r p 4 r 2 2r 1 ))+r 1 5p 4 2r 2 3r 1 ) + r 1 2a 0 r 1 r 2 ) 2 5p 2 5p 1 r 2 )r p 3 r 2 2r 1 ))),

15 WEIGHT-HOMOGENEOUS POLYNOMIAL SYSTEMS 1633 γ 2 = A 2 B 2 = fr 2 ) + a 0 B 2 r 1 r 2 ) 2 c + b r 2 + r2 2), γ 3 = A 3 A 3 = B 3 2c + b r 1 + r1 2)2 c + b r 2 + r2 2), A 3 = a 0 B 3 + 5p 2 + p 1 2r 1 + r 2 ))c 2 p 4 + p 3 2r 1 + r 2 ) + r 1 p 1 r 1 r 2 + p 2 r 1 + 2r 2 )) + bp 3 p 1 r 1 r 1 + 2r 2 )))c + p 4 b + r 1 ) 2 + p 1 b 2 p 2 b + p 3 )r p 4 r 1 + bp 4 )r 2 ). We note that an integer power of H is a polynomial if and only if fr 1 ) = 0, β = 0 and γ i Q for i = 1, 2, 3, if they all have the same sign. Case x). A first integral H is x r 1 y) γ 1 x 2 + bxy + cy 2 ) γ fr1 2 )c + b r 1 + r 2 exp 1) 2 x 2 r1 2x r 1y) 2 β 1c + b r 1 + r1)x 2 β 2 x bx + 2cy r1 2x r + 1y) 4c b2 )x arctan )), 2 4c b2 )x 2 where and β 1 = 10p 2 bp 1 )r p 3 cp 1 )r cp 2 + bp 3 + 3p 4 )r bp 4 r 1 + cp 4 ), β 2 = 10p 1 r 3 1 p 4 )b 3 r 1 p 2 r p 4 )b 2 + r 2 1p 3 r 1 3p 4 )b 2p 4 r c 3 p 1 c 2 2p 3 + bp 2 3p 1 r 1 ) + 6r 1 p 2 + p 1 r 1 )) + c3p 1 r p 3 )b 2 + 3p 4 + r 1 p 3 r 1 p 2 + p 1 r 1 )))b + 2r 1 3p 4 + r 1 3p 3 + p 2 r 1 )))), γ 1 = 23a 0 c + r 1 b + r 1 )) 3 + 5p 1 b 2 p 2 b + p 3 )r p 4 r bp 4 r 1 + b 2 p 4 + c 2 p 2 + 3p 1 r 1 ) cp 4 + bp 3 3p 1 r 2 1) + r 1 3p 3 + r 1 3p 2 + p 1 r 1 ))))), γ 2 = 5p 1 b 2 p 2 b + p 3 )r p 4 r bp 4 r 1 + b 2 p 4 + c 2 p 2 + 3p 1 r 1 ) cp 4 + bp 3 3p 1 r 2 1) + r 1 3p 3 + r 1 3p 2 + p 1 r 1 )))) 2a 0 c + r 1 b + r 1 )) 3.

16 1634 JAUME LLIBRE AND CLAUDIA VALLS We note that an integer power H is a polynomial if and only if fr 1 ) = 0, β 1 = β 2 = 0 and γ i Q for i = 1, 2, if they all have the same sign. Case xi). A first integral H is x 2 + b 1 xy + c 1 y 2 ) γ 1 x 2 + b 2 xy + c 2 y 2 ) γ 2 x r 1 y) γ 3 2 β i x exp 4ci b arctan bi x + 2c i y )), 2 i )x2 4ci b 2 i )x2 i=1 with β i = α i /δ i for i = 1, 2, where α i = 5 b i c 2 i p 2 + c i c j p 2 + b j c i c i p 1 + p 3 ) 3c i p 4 + c j p 4 ) + b i c 2 i p 1 + c j p 3 + c i 3c j p 1 + b j p 2 + p 3 ) + b j p 4 )r 1 + b 3 i p 4 +c j p 1 r 1 )+b 2 i c i c j p 1 +c i p 3 +b j p 4 b j c i p 1 +c j p 2 +p 4 )r 1 ) + 2c 3 i p 1 c j p 4 r 1 c 2 i c j p 1 + p 3 + p 2 r 1 b j p 2 + p 1 r 1 )) + c i p 4 r 1 + c j p 3 + p 2 r 1 ) b j p 4 + p 3 r 1 )))), δ i = b 2 2c 1 + c 1 c 2 ) 2 + b 2 1c 2 b 1 b 2 c 1 + c 2 ))c i + b i r 1 + r 2 1), for i, j = 1, 2 and i j, γ i = 2a 0 b 2 jc i + c i c j ) 2 + b 2 i c j b i b j c i + c j ))c i + r 1 b i + r 1 )) + 5b 2 i p 4 + c j p 1 r 1 ) + b i c i c j p 1 c i p 3 c j p 2 r 1 + p 4 r 1 ) + c i c j ) p 4 p 3 r 1 + c i p 2 + p 1 r 1 )) b j c 2 i p 1 + p 4 b i + r 1 ) c i p 3 + b i p 1 + p 2 )r 1 ))), for i, j = 1, 2 and i j. Finally, γ 3 = A 3 = fr 1) + a 0 B 3 ). B 3 2 c i + b i r 1 + r1) 2 i=1 We note that an integer power of H is a polynomial if and only if β 1 = β 2 = 0 and γ i Q for i = 1, 2, 3, if they all have the same sign. Case xii). A first integral H is x ry) γ 1 x 2 +bxy+cy 2 ) γ 2 exp β 1 x 3 arctan [4c b 2 )x 2 ] 3/2 ) bx + 2cy 4c b2 )x 2

17 WEIGHT-HOMOGENEOUS POLYNOMIAL SYSTEMS β 2 c + b r + r 2 ) )x b 2 4c)cx 2 + bxy + cy 2, ) where β 1 = 10p 4 + rp 3 rp 2 + p 1 r)))b 3 + 4p 3 r 2 b 2 + 2r 2 p 3 r 3p 4 )b 4p 4 r 3 + 4c 3 p 1 + c 2 4p 3 + rp 2 + 3p 1 r)) 2bp 2 3p 1 r)) 2c2p 2 rb 2 + 3p 4 rp 3 + r3p 1 r p 2 )))b + 2r3p 4 + rp 3 + p 2 r)))), β 2 = p 4 yb 3 + cp 1 rx + p 3 y) p 4 x + ry))b 2 + p 1 x + ry) p 2 y)c 2 + p 2 rx + 3p 4 y + p 3 x + ry))c p 4 rx)b + 2cp 1 yc 2 p 1 rx + p 3 y + p 2 x + ry))c + p 3 rx + p 4 x + ry)), γ 1 = 2a 0 c + br + r 2 ) 2 + fr)), γ 2 = 4a 0 c + br + r 2 ) 2 fr). We note that an integer power of H is a polynomial if and only if β 1 = β 2 = 0 and γ i Q for i = 1, 2, if they all have the same sign. 4. Weight exponent s = 1, 2). In this section, we prove Theorem 1.3. Since systems in equation 1.5) are homogeneous, we know that they are integrable because they have the inverse integrating factor V = xẏ yẋ. The strategy will be to obtain such first integrals and to determine which of them are polynomials. Denoting systems in equation 1.5) by ẋ = P x, y) and ẏ = Qx, y), the first integral is Hx, y) = satisfying H/ x = Qx, y)/v x, y). P x, y) dy + gx), V x, y) The first system in equation 1.5) has the first integral H = x 3 2p 2 3y 2 x 2 ) 3+p 2 exp 2 x 3p 1 arctanh )). 3y Note that an integer power of H is a polynomial if and only if p 1 = 0 and p 2 = 31 q)/1 + 2q) with q Q +.

18 1636 JAUME LLIBRE AND CLAUDIA VALLS The second system in equation 1.5) has the first integral H = x 3 2p 2 3y 2 + x 2 ) 3+p 2 exp 2 x 3p 1 arctan )). 3y Note that an integer power of H is a polynomial if and only if p 1 = 0 and p 2 = 31 q)/1 + 2q) with q Q +. The third system in equation 1.5) has the first integral H = x 23+p1) y 3+2p1 exp 2p 2y x. Note that an integer power of H is a polynomial if and only if p 2 = 0 and p 1 = 31 2q)/21 + q)) with q Q +. The fourth system in equation 1.5) has the first integral H = x exp y 2p ) 1x + p 2 y 3x 2. Note that an integer power of H is a polynomial if and only if p 1 = p 2 = 0. The fifth system in equation 1.5) has the first integral x/y which is never a polynomial. 5. Weight exponent s = 1, 3). Performing a change of variables X, Y ) = x 3, y), the planar weight homogeneous systems of weight degree 4 and weight exponent 1, 3) become 5.1) Ẋ = 3a 40 X 2 + 3a 11 XY, Ẏ = b 60 X 2 + b 31 XY + b 02 Y 2. Again, we shall use the inverse integrating factor V = XẎ Y Ẋ for computing the first integrals of system 5.1). It is clear that, if a 11 = a 40 = 0, then a polynomial first integral is X, and, if b 60 = b 31 = b 02 = 0, then a polynomial first integral is Y. Now, we consider the other cases. Case i). 3a 11 b 02 0 and R = 3a 40 b 31 ) a 11 + b 02 )b In this case, system 5.1) has the first integral ) 6 3a40 X b 31 X +6a 11 Y 2b 02 Y a 11 3a 40 + b 31 ) 2a 40 b 02 ) arctan R RX

19 WEIGHT-HOMOGENEOUS POLYNOMIAL SYSTEMS 1637 ) Y 3a40 X b 31 X +3a 11 Y b 02 Y ) +23a 11 b 02 ) log X +3a 11 log X 2 b 60. Here, log A always means log A and, as usual, log is the logarithm in base e. Since this first integral must be a polynomial, we must have 5.2) a 11 3a 40 + b 31 ) 2a 40 b 02 = 0. Now, we consider different subcases. If 3a 11 2b 02 0, then from equation 5.2), we obtain a 40 = a 11b 31 3a 11 2b 02. Therefore, using the exponential of the previous first integral, we obtain that the first integral is where H = X 1 3a11/6a11 2b02) px, Y ) 3a11/6a11 2b02), px, Y ) = 3a 11 2b 02 )b 60 X a 11 b 02 )b 31 XY 9a a 11 b b 2 02)Y 2. Note that, since a 11 b 02 0 and 3a 11 2b 02 0, we have 9a a 11 b b Therefore, an integer power of H is a polynomial first integral if and only if 3a 11 /6a 11 2b 02 ) = m/n Q +, and m/n < 1. In this case, the first integral H is X n m 3a 11 2b 02 )b 60 X a 11 b 02 )b 31 XY 9a a 11 b b 2 02)Y 2 ) m. If 3a 11 2b 02 = 0, that is, b 02 = 3a 11 /2. In this case, from equation 5.2), we obtain a 11 b 31 = 0. Hence, either a 11 = 0 or b 31 = 0. However, if a 11 = 0, then b 02 = 0, which contradicts the fact that 3a 11 2b Therefore, this case is not possible and we must have b 31 = 0. Then, the first integral is which is never a polynomial. H = 2b 60X 2 + 6a 40 XY + 3a 11 Y 2, X

20 1638 JAUME LLIBRE AND CLAUDIA VALLS Case ii). b 02 = 3a 11 and b 31 3a In this case, system 5.1) has the first integral b 31 3a 40 ) 2 log X + 3a 113a 40 b 31 )Y X + 3 3a b 31 a 40 a 11 b 60 ) log b ) 60X 3a 40 Y + b 31 Y. X In order for the first integral to be a polynomial, we must have a 11 3a 40 b 31 ) = 0, that is, a 11 = 0 and hence, b 02 = 0). Then, using the exponential of the previous first integral, we obtain the following first integral X 1/3 b60 X 3a 40 Y + b 31 Y X ) a40/3a 40 b 31). Then, we must have b 31 /a 40 = m/n with m/n Q +. In this case, the previous first integral becomes H = X m b 60 X 3a 40 Y + b 31 Y ) 3n. Case iii). b 02 = 3a 11 and b 31 = 3a 40. System 5.1) has the first integral 2b 60 X 2 log X + 6a 40 Y X + 3a 11 Y 2 6X 2. Since the case a 40 = a 11 = 0 has been studied, we have that in this case the first integral is never a polynomial. Case iv). 3a 11 b 02 0 and R = 0. Then, b 06 = 3a 40 b 31 ) 2 43a 11 b 02 ), and system 5.1) has the first integral 3 3a 11 a 40 +2b 02 a 40 a 11 b 31 )X 3a 40 X b 31 X +6a 11 Y 2b 02 Y +3a 11 b 02 ) log36a 11 X 12b 02 X) + 3a 11 log 3a ) 40X b 31 X + 6a 11 Y 2b 02 Y. X In order to show that it is a polynomial, we must have 5.3) 2a 40 b 02 a 11 3a 40 + b 31 ) = 0. We will now consider two different subcases.

21 WEIGHT-HOMOGENEOUS POLYNOMIAL SYSTEMS 1639 If 3a 11 2b 02, then condition 5.3) becomes a 40 = a 11b 31 3a 11 2b 02. Using the exponential of the previous first integral, we obtain the following first integral: X 1/36a11 12b02) b31 X 3a 11 Y + 2b 02 Y X From this first integral, we obtain the first integral: Xb 31 X 3a 11 Y + 2b 02 Y ) 3a11/b02. ) a11 /4b 02 3a 11 ) 2. So, if b 02 0, then 3a 11 /b 02 = m/n with m/n Q +, and the polynomial first integral is X n b 31 X 3a 11 Y + 2b 02 Y ) m. If b 02 = 0, then H = b 31 X 3a 11 Y is a polynomial first integral. This concludes the proof of Theorem Weight exponent s = 1, 4). We introduce the change X, Y ) = x 4, y) in the planar weight homogeneous polynomial differential systems 1.1) of weight degree 4 with weight exponent 1, 4). In these new variables X, Y ), the systems with weight exponent 1, 4) become, after introducing the new independent variable dτ = x 3 dt, as follows: 6.1) X = 4a 40 X + a 01 Y ), Y = b 70 X + b 31 Y, where the prime denotes the derivative with respect to τ. If a 40 = a 01 = 0, then a polynomial first integral is X, and, if b 70 = b 31 = 0, then a polynomial first integral is Y. Now, we consider the other cases. Case i). R = 4a 40 b 31 ) 2 16a 01 b Now, a first integral of system 6.1) is: ) 24a 40 + b 31 ) 4a40 b 31 )X + 8a 01 Y arctan R RX + log b 70 X 2 + 4a 40 b 31 )XY + 4a 01 Y 2 ).

22 1640 JAUME LLIBRE AND CLAUDIA VALLS Since it must be a polynomial, we must have b 31 = 4a 40 such that the polynomial first integral is H = b 70 X 2 + 8a 40 XY + 4a 01 Y 2. Case ii). R = 0. We consider different subcases. First, we study when b Then, from R = 0, we obtain 6.2) a 01 = 4a 40 b 31 ) 2 16b 70. If b 31 4a 40 0, then the first integral is: 24a 40 + b 31 )b 70 X 2b 70 X + 4a 40 b 31 )Y + 4a 40 b 31 ) log2b 70 X + 4a 40 + b 31 )Y ), which is a polynomial if and only if b 31 = 4a 40. The polynomial first integral is b 70 X 4a 40 Y. If b 31 = 4a 40, then a 40 0 otherwise, b 31 = 0 and, from equation 6.2), we also have a 01 = 0, which has already been considered), and the first integral of equation 6.1) is which is never a polynomial. H = Y X b 70 log X 4a 40, If b 70 = 0, then from R = 0, we obtain b 31 = 4a 40. We only consider the case a 40 0, where the first integral of equation 6.1) is: a 40X Y This completes the proof of Theo- which is never a polynomial. rem a 01 log Y, 7. Weight exponent s = 2, 3). We prove Theorem 1.6. The planar weight homogeneous polynomial differential systems 1.1) with weight degree 4 and weight-exponent 2, 3) are: 7.1) ẋ = a 11 xy, ẏ = b 30 x 3 + b 02 y 2. If a 11 3a 11 2b 02 ) 0, then the first integral of system 7.1) is: H = x 2b 02/a 11 2b 30 x 3 3a 11 y 2 + 2b 02 y 2).

23 WEIGHT-HOMOGENEOUS POLYNOMIAL SYSTEMS 1641 Then, an integer power of H is a polynomial first integral if and only if 2b 02 /a 11 Q +. If a 11 = 0, then H = x is a polynomial first integral of system 7.1). If b 30 = b 02 = 0, then H = y is a polynomial first integral of system 7.1). If a 11 0 and 3a 11 = 2b 02, then the first integral of system 7.1) is: This completes the proof of Theo- which is never a polynomial. rem 1.6. H = y4 x 3 2b 30 a 11 log x, 8. Weight exponent s = 2, 5). Here, we prove Theorem 1.7. The planar weight homogeneous polynomial differential systems 1.1) of weight degree 4 with weight exponent 2, 5) are: ẋ = a 01 y, ẏ = b 40 x 4. It is straightforward to prove that H = 2b 40 x 5 5a 01 y 2 is a polynomial first integral. 9. Weight exponent s = 6, 9). Now, we prove Theorem 1.8. The planar weight homogeneous polynomial differential systems 1.1) of weight degree 4 with weight exponent 6, 9) are: ẋ = a 01 y, ẏ = b 20 x 2. It is straightforward to prove that H = 2b 20 x 3 3a 01 y 2 is a polynomial first integral. This completes the proof of Theorem 1.8. REFERENCES 1. A. Algaba, E. Freire, E. Gamero and C. García, Monodromy, center-focus and integrability problems for quasi-homogeneous polynomial systems, Nonlin. Anal ), A. Algaba, N. Fuentes and C. García, Centers of quasi-homogeneous polynomial planar systems, Nonlin. Anal. Real World Appl ), A. Algaba, C. García and M. Reyes, Integrability of two dimensional quasihomogeneous polynomial differential systems, Rocky Mountain J. Math ), , Rational integrability of two-dimensional quasi-homogeneous polynomial differential systems, Nonlin. Anal ),

24 1642 JAUME LLIBRE AND CLAUDIA VALLS 5. A. Algaba, C. García and M.A. Teixeira, Reversibility and quasi-homogeneous normal forms of vector fields, Nonlin. Anal ), C. Cairó and J. Llibre, Polynomial first integrals for weight-homogeneous planar polynomial differential systems of weight degree 3, J. Math. Anal. Appl ), J. Chavarriga, H. Giacomini, J. Giné and J. Llibre, Darboux integrability and the inverse integrating factor, J. Diff. Eq ), A. Cima and J. Llibre, Algebraic and topological classification of the homogeneous cubic vector fields in the plane, J. Math. Anal. Appl ), T. Date and M. Lai, Canonical forms of real homogeneous quadratic transformations, J. Math. Anal. Appl ), S.D. Furta, On non-integrability of general systems of differential equations, Z. Angew. Math. Phys ), A. Goriely, Integrability, partial integrability, and nonintegrability for systems of ordinary differential equations, J. Math. Phys ), S. Labrunie, On the polynomial first integrals of the a, b, c) Lotka-Volterra system, J. Math. Phys ), J. Llibre and X. Zhang, Polynomial first integrals for quasi-homogeneous polynomial differential systems, Nonlinearity ), A.J. Maciejewski and J.M. Strelcyn, On algebraic non-integrability of the Halphen system, Phys. Lett ), J. Moulin-Ollagnier, Polynomial first integrals of the Lotka-Volterra system, Bull. Sci. Math ), A. Tsygvintsev, On the existence of polynomial first integrals of quadratic homogeneous systems of ordinary differential equations, J. Phys. Math. Gen ), Departament de Matemàtiques, Universitat Autònoma de Barcelona, Bellaterra, Barcelona, Catalonia, Spain address: Departamento de Matemática, Instituto Superior Técnico, Lisboa, Portugal address:

arxiv: v1 [math.ds] 27 Jul 2017

arxiv: v1 [math.ds] 27 Jul 2017 POLYNOMIAL VECTOR FIELDS ON THE CLIFFORD TORUS arxiv:1707.08859v1 [math.ds] 27 Jul 2017 JAUME LLIBRE AND ADRIAN C. MURZA Abstract. First we characterize all the polynomial vector fields in R 4 which have

More information

ISOCHRONICITY FOR TRIVIAL QUINTIC AND SEPTIC PLANAR POLYNOMIAL HAMILTONIAN SYSTEMS

ISOCHRONICITY FOR TRIVIAL QUINTIC AND SEPTIC PLANAR POLYNOMIAL HAMILTONIAN SYSTEMS ISOCHRONICITY FOR TRIVIAL QUINTIC AND SEPTIC PLANAR POLYNOMIAL HAMILTONIAN SYSTEMS FRANCISCO BRAUN JAUME LLIBRE AND ANA C. MEREU Abstract. In this paper we completely characterize trivial polynomial Hamiltonian

More information

LIOUVILLIAN FIRST INTEGRALS FOR QUADRATIC SYSTEMS WITH AN INTEGRABLE SADDLE

LIOUVILLIAN FIRST INTEGRALS FOR QUADRATIC SYSTEMS WITH AN INTEGRABLE SADDLE This is a preprint of: Liouvillian first integrals for quadratic systems with an integrable saddle, Yudi Marcela Bolan os Rivera, Jaume Llibre, Cla udia Valls, Rocky Mountain J. Math., vol. 45(6), 765

More information

ZERO-HOPF BIFURCATION FOR A CLASS OF LORENZ-TYPE SYSTEMS

ZERO-HOPF BIFURCATION FOR A CLASS OF LORENZ-TYPE SYSTEMS This is a preprint of: Zero-Hopf bifurcation for a class of Lorenz-type systems, Jaume Llibre, Ernesto Pérez-Chavela, Discrete Contin. Dyn. Syst. Ser. B, vol. 19(6), 1731 1736, 214. DOI: [doi:1.3934/dcdsb.214.19.1731]

More information

Preprint Preprint Preprint Preprint

Preprint Preprint Preprint Preprint CADERNOS DE MATEMÁTICA 15, 179 193 October 2014) ARTIGO NÚMERO SMA#398 On the integrability and the zero Hopf bifurcation of a Chen Wang differential system Jaume Llibre Departament de Matemàtiques, Universitat

More information

AVERAGING THEORY AT ANY ORDER FOR COMPUTING PERIODIC ORBITS

AVERAGING THEORY AT ANY ORDER FOR COMPUTING PERIODIC ORBITS This is a preprint of: Averaging theory at any order for computing periodic orbits, Jaume Giné, Maite Grau, Jaume Llibre, Phys. D, vol. 25, 58 65, 213. DOI: [1.116/j.physd.213.1.15] AVERAGING THEORY AT

More information

Stability and bifurcation in a two species predator-prey model with quintic interactions

Stability and bifurcation in a two species predator-prey model with quintic interactions Chaotic Modeling and Simulation (CMSIM) 4: 631 635, 2013 Stability and bifurcation in a two species predator-prey model with quintic interactions I. Kusbeyzi Aybar 1 and I. acinliyan 2 1 Department of

More information

Characterizing planar polynomial vector fields with an elementary first integral

Characterizing planar polynomial vector fields with an elementary first integral Characterizing planar polynomial vector fields with an elementary first integral Sebastian Walcher (Joint work with Jaume Llibre and Chara Pantazi) Lleida, September 2016 The topic Ultimate goal: Understand

More information

1. Introduction and statement of the main results

1. Introduction and statement of the main results Publ. Mat. (214), 297 38 Proceedings of New Trends in Dynamical Systems. Salou, 212. DOI: 1.5565/PUBLMAT Extra14 16 CUBIC HOMOGENEOUS POLYNOMIAL CENTERS Chengzhi Li and Jaume Llibre Abstract: First, doing

More information

GENERALIZED RATIONAL FIRST INTEGRALS OF ANALYTIC DIFFERENTIAL SYSTEMS

GENERALIZED RATIONAL FIRST INTEGRALS OF ANALYTIC DIFFERENTIAL SYSTEMS This is a preprint of: Generalized rational first integrals of analytic differential systems, Wang Cong, Jaume Llibre, Xiang Zhang, J. Differential Equations, vol. 251, 2770 2788, 2011. DOI: [10.1016/j.jde.2011.05.016]

More information

Spatial bi stacked central configurations formed by two dual regular polyhedra

Spatial bi stacked central configurations formed by two dual regular polyhedra This is a preprint of: Spatial bi-stacked central configurations formed by two dual regular polyhedra, Montserrat Corbera, Jaume Llibre, Ernesto Pérez-Chavela, J. Math. Anal. Appl., vol. 43), 648 659,

More information

On the polynomial differential systems having polynomial first integrals

On the polynomial differential systems having polynomial first integrals Bull. Sci. math. 136 (2012) 309 316 www.elsevier.com/locate/bulsci On the olynomial differential systems having olynomial first integrals Belén García a,, Jaume Llibre b, Jesús S. Pérez del Río a a Deartamento

More information

LIMIT CYCLES COMING FROM THE PERTURBATION OF 2-DIMENSIONAL CENTERS OF VECTOR FIELDS IN R 3

LIMIT CYCLES COMING FROM THE PERTURBATION OF 2-DIMENSIONAL CENTERS OF VECTOR FIELDS IN R 3 Dynamic Systems and Applications 17 (28 625-636 LIMIT CYCLES COMING FROM THE PERTURBATION OF 2-DIMENSIONAL CENTERS OF VECTOR FIELDS IN R 3 JAUME LLIBRE, JIANG YU, AND XIANG ZHANG Departament de Matemàtiques,

More information

Centers of projective vector fields of spatial quasi-homogeneous systems with weight (m, m, n) and degree 2 on the sphere

Centers of projective vector fields of spatial quasi-homogeneous systems with weight (m, m, n) and degree 2 on the sphere Electronic Journal of Qualitative Theory of Differential Equations 2016 No. 103 1 26; doi: 10.14232/ejqtde.2016.1.103 http://www.math.u-szeged.hu/ejqtde/ Centers of projective vector fields of spatial

More information

PLANAR ANALYTIC NILPOTENT GERMS VIA ANALYTIC FIRST INTEGRALS

PLANAR ANALYTIC NILPOTENT GERMS VIA ANALYTIC FIRST INTEGRALS PLANAR ANALYTIC NILPOTENT GERMS VIA ANALYTIC FIRST INTEGRALS YINGFEI YI AND XIANG ZHANG Abstract. We generalize the results of [6] by giving necessary and sufficient conditions for the planar analytic

More information

LIMIT CYCLES OF POLYNOMIAL DIFFERENTIAL EQUATIONS WITH QUINTIC HOMOGENOUS NONLINEARITIES

LIMIT CYCLES OF POLYNOMIAL DIFFERENTIAL EQUATIONS WITH QUINTIC HOMOGENOUS NONLINEARITIES This is a preprint of: Limit cycles of polynomial differential equations with quintic homogenous nonlinearities, Rebiha Benterki, Jaume Llibre, J. Math. Anal. Appl., vol. 47(), 6 22, 23. DOI: [.6/j.jmaa.23.4.76]

More information

A NON-AUTONOMOUS KIND OF DUFFING EQUATION JAUME LLIBRE AND ANA RODRIGUES

A NON-AUTONOMOUS KIND OF DUFFING EQUATION JAUME LLIBRE AND ANA RODRIGUES This is a preprint of: A non-autonomous kind of Duffing equation, Jaume Llibre, Ana Rodrigues, Appl. Math. Comput., vol. 25, 669 674, 25. DOI: [.6/j.amc.24..7] A NON-AUTONOMOUS KIND OF DUFFING EQUATION

More information

DARBOUX INTEGRABILITY OF A GENERALIZED FRIEDMANN-ROBERTSON-WALKER HAMILTONIAN SYSTEM

DARBOUX INTEGRABILITY OF A GENERALIZED FRIEDMANN-ROBERTSON-WALKER HAMILTONIAN SYSTEM This is a preprint of: Daroux integrailit of a generalized Friedmann-Roertson-Walker Hamiltonian sstem, Jaume Llire, Clàudia Valls, J. Nonlinear Math. Phs., vol. 203, 394 406, 2013. DOI: [10.1080/14029251.2013.854482]

More information

PERIODIC SOLUTIONS OF EL NIÑO MODEL THROUGH THE VALLIS DIFFERENTIAL SYSTEM

PERIODIC SOLUTIONS OF EL NIÑO MODEL THROUGH THE VALLIS DIFFERENTIAL SYSTEM This is a preprint of: Periodic solutios of El niño model thorugh the Vallis differential system, Rodrigo D. Euzébio, Jaume Llibre, Discrete Contin. Dyn. Syst., vol. 34(9), 3455 3469, 214. DOI: [1.3934/dcds.214.34.3455]

More information

Rational constants of monomial derivations

Rational constants of monomial derivations Rational constants of monomial derivations Andrzej Nowicki and Janusz Zieliński N. Copernicus University, Faculty of Mathematics and Computer Science Toruń, Poland Abstract We present some general properties

More information

The center problem for a 2 : 3 resonant cubic Lotka Volterra system

The center problem for a 2 : 3 resonant cubic Lotka Volterra system The center problem for a 2 : 3 resonant cubic Lotka Volterra system Diana Dolićanin a, Jaume Giné b, Regilene Oliveira c, Valery G. Romanovski d,e a State University of Novi Pazar, Department of Mathematics,

More information

Qualitative Classification of Singular Points

Qualitative Classification of Singular Points QUALITATIVE THEORY OF DYNAMICAL SYSTEMS 6, 87 167 (2005) ARTICLE NO. 94 Qualitative Classification of Singular Points Qibao Jiang Department of Mathematics and Mechanics, Southeast University, Nanjing

More information

HIGHER ORDER CRITERION FOR THE NONEXISTENCE OF FORMAL FIRST INTEGRAL FOR NONLINEAR SYSTEMS. 1. Introduction

HIGHER ORDER CRITERION FOR THE NONEXISTENCE OF FORMAL FIRST INTEGRAL FOR NONLINEAR SYSTEMS. 1. Introduction Electronic Journal of Differential Equations, Vol. 217 (217), No. 274, pp. 1 11. ISSN: 172-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu HIGHER ORDER CRITERION FOR THE NONEXISTENCE

More information

Infinitely many periodic orbits for the rhomboidal five-body problem

Infinitely many periodic orbits for the rhomboidal five-body problem Infinitely many periodic orbits for the rhomboidal five-body problem Montserrat Corbera and Jaume Llibre Citation: J. Math. Phys. 47 1701 (006); doi:.63/1.378617 View online: http://dx.doi.org/.63/1.378617

More information

RATIONAL FIRST INTEGRALS FOR POLYNOMIAL VECTOR FIELDS ON ALGEBRAIC HYPERSURFACES OF R N+1

RATIONAL FIRST INTEGRALS FOR POLYNOMIAL VECTOR FIELDS ON ALGEBRAIC HYPERSURFACES OF R N+1 This is a preprint of: Rational first integrals for polynomial vector fields on algebraic hypersurfaces of R N+1, Jaume Llibre, Yudi Marcela Bolaños Rivera, Internat J Bifur Chaos Appl Sci Engrg, vol 22(11,

More information

COEXISTENCE OF ALGEBRAIC AND NON-ALGEBRAIC LIMIT CYCLES FOR QUINTIC POLYNOMIAL DIFFERENTIAL SYSTEMS

COEXISTENCE OF ALGEBRAIC AND NON-ALGEBRAIC LIMIT CYCLES FOR QUINTIC POLYNOMIAL DIFFERENTIAL SYSTEMS Electronic Journal of Differential Equations, Vol. 217 (217), No. 71, pp. 1 7. ISSN: 172-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu COEXISTENCE OF ALGEBRAIC AND NON-ALGEBRAIC LIMIT

More information

A NOTE ON THE DZIOBECK CENTRAL CONFIGURATIONS JAUME LLIBRE

A NOTE ON THE DZIOBECK CENTRAL CONFIGURATIONS JAUME LLIBRE This is a preprint of: A note on the Dziobek central configurations, Jaume Llibre, Proc. Amer. Math. Soc., vol. 43(8), 3587 359, 205. DOI: [http://dx.doi.org/0.090/s0002-9939-205-2502-6] A NOTE ON THE

More information

arxiv: v1 [math.ac] 24 Mar 2015

arxiv: v1 [math.ac] 24 Mar 2015 A Note on Darboux Polynomials of Monomial Derivations arxiv:1503.07011v1 [math.ac] 24 Mar 2015 Abstract Jiantao Li School of Mathematics, Liaoning University, Shenyang, 110031, China We study a monomial

More information

PHASE PORTRAITS OF PLANAR SEMI HOMOGENEOUS VECTOR FIELDS (III)

PHASE PORTRAITS OF PLANAR SEMI HOMOGENEOUS VECTOR FIELDS (III) This is a preprint of: Phase portraits of planar semi-homogeneous systems III, Laurent Cairó, Jaume Llibre, Qual. Theory Dyn. Syst., vol. 10, 203 246, 2011. DOI: [10.1007/s12346-011-0052-y] PHASE PORTRAITS

More information

THE NUMBER OF POLYNOMIAL SOLUTIONS OF POLYNOMIAL RICCATI EQUATIONS

THE NUMBER OF POLYNOMIAL SOLUTIONS OF POLYNOMIAL RICCATI EQUATIONS This is a preprint of: The number of polynomial solutions of polynomial Riccati equations, Armengol Gasull, Joan Torregrosa, Xiang Zhang, J. Differential Equations, vol. 261, 5071 5093, 2016. DOI: [10.1016/j.jde.2016.07.019]

More information

PERIODIC ORBITS FOR REAL PLANAR POLYNOMIAL VECTOR FIELDS OF DEGREE n HAVING n INVARIANT STRAIGHT LINES TAKING INTO ACCOUNT THEIR MULTIPLICITIES

PERIODIC ORBITS FOR REAL PLANAR POLYNOMIAL VECTOR FIELDS OF DEGREE n HAVING n INVARIANT STRAIGHT LINES TAKING INTO ACCOUNT THEIR MULTIPLICITIES PERIODIC ORBITS FOR REAL PLANAR POLYNOMIAL VECTOR FIELDS OF DEGREE n HAVING n INVARIANT STRAIGHT LINES TAKING INTO ACCOUNT THEIR MULTIPLICITIES JAUME LLIBRE 1 AND ANA RODRIGUES 2 Abstract. We study the

More information

GEOMETRIC CLASSIFICATION OF CONFIGURATIONS OF SINGULARITIES WITH TOTAL FINITE MULTIPLICITY FOUR FOR A CLASS OF QUADRATIC SYSTEMS

GEOMETRIC CLASSIFICATION OF CONFIGURATIONS OF SINGULARITIES WITH TOTAL FINITE MULTIPLICITY FOUR FOR A CLASS OF QUADRATIC SYSTEMS This is a preprint of: Global configurations of singularities for quadratic differential systems with exactly two finite singularities of total multiplicity four, Joan Carles Artés, Jaume Llibre, Alex

More information

PIECEWISE LINEAR DIFFERENTIAL SYSTEMS WITH TWO REAL SADDLES. 1. Introduction

PIECEWISE LINEAR DIFFERENTIAL SYSTEMS WITH TWO REAL SADDLES. 1. Introduction PIECEWISE LINEAR DIFFERENTIAL SYSTEMS WITH TWO REAL SADDLES JOAN C. ARTÉS1, JAUME LLIBRE 1, JOAO C. MEDRADO 2 AND MARCO A. TEIXEIRA 3 Abstract. In this paper we study piecewise linear differential systems

More information

Darboux theory of integrability for polynomial vector fields in R n taking into account the multiplicity at infinity

Darboux theory of integrability for polynomial vector fields in R n taking into account the multiplicity at infinity Bull. Sci. math. 33 (2009 765 778 www.elsevier.com/locate/bulsci Darboux theory of integrability for polynomial vector fields in R n taking into account the multiplicity at infinity Jaume Llibre a,, Xiang

More information

Preprint Preprint Preprint Preprint

Preprint Preprint Preprint Preprint CADERNOS DE MATEMÁTICA 14, 19 30 May (2013) ARTIGO NÚMERO SMA#374 The center problem for a 2 : 3 resonant cubic Lotka Volterra system Diana Dolićanin State University of Novi Pazar, Department of Mathematics,

More information

arxiv: v1 [math.ds] 11 Aug 2017

arxiv: v1 [math.ds] 11 Aug 2017 GLOBAL DYNAMICS OF PLANAR QUASI HOMOGENEOUS DIFFERENTIAL SYSTEMS arxiv:1708.03437v1 [math.ds] 11 Aug 2017 YILEI TANG 1 AND XIANG ZHANG 2 Abstract. In this paper we provide a new method to study global

More information

Integrability and dynamical degree of periodic non-autonomous Lyness recurrences. Anna Cima

Integrability and dynamical degree of periodic non-autonomous Lyness recurrences. Anna Cima Proceedings of the International Workshop Future Directions in Difference Equations. June 13-17, 2011, Vigo, Spain. PAGES 77 84 Integrability and dynamical degree of periodic non-autonomous Lyness recurrences.

More information

UNIVERSIDADE DE SÃO PAULO

UNIVERSIDADE DE SÃO PAULO UNIVERSIDADE DE SÃO PAULO Instituto de Ciências Matemáticas e de Computação ISSN 010-577 GLOBAL DYNAMICAL ASPECTS OF A GENERALIZED SPROTT E DIFFERENTIAL SYSTEM REGILENE OLIVEIRA CLAUDIA VALLS N o 41 NOTAS

More information

First integrals and phase portraits of planar polynomial differential cubic systems with invariant straight lines of total multiplicity eight

First integrals and phase portraits of planar polynomial differential cubic systems with invariant straight lines of total multiplicity eight Electronic Journal of Qualitative Theory of Differential Equations 2017, No. 85, 1 35; https://doi.org/10.14232/ejqtde.2017.1.85 www.math.u-szeged.hu/ejqtde/ First integrals and phase portraits of planar

More information

POLYNOMIALS. x + 1 x x 4 + x 3. x x 3 x 2. x x 2 + x. x + 1 x 1

POLYNOMIALS. x + 1 x x 4 + x 3. x x 3 x 2. x x 2 + x. x + 1 x 1 POLYNOMIALS A polynomial in x is an expression of the form p(x) = a 0 + a 1 x + a x +. + a n x n Where a 0, a 1, a. a n are real numbers and n is a non-negative integer and a n 0. A polynomial having only

More information

ADDITIVE DECOMPOSITION SCHEMES FOR POLYNOMIAL FUNCTIONS OVER FIELDS

ADDITIVE DECOMPOSITION SCHEMES FOR POLYNOMIAL FUNCTIONS OVER FIELDS Novi Sad J. Math. Vol. 44, No. 2, 2014, 89-105 ADDITIVE DECOMPOSITION SCHEMES FOR POLYNOMIAL FUNCTIONS OVER FIELDS Miguel Couceiro 1, Erkko Lehtonen 2 and Tamás Waldhauser 3 Abstract. The authors previous

More information

UNIVERSIDADE DE SÃO PAULO

UNIVERSIDADE DE SÃO PAULO UNIVERSIDADE DE SÃO PAULO Instituto de Ciências Matemáticas e de Computação ISSN 0103-2577 GLOBAL DYNAMICAL ASPECTS OF A GENERALIZED CHEN-WANG DIFFERENTIAL SYSTEM REGILENE D. S. OLIVEIRA CLAUDIA VALLS

More information

GEOMETRIC CONFIGURATIONS OF SINGULARITIES FOR QUADRATIC DIFFERENTIAL SYSTEMS WITH TOTAL FINITE MULTIPLICITY m f = 2

GEOMETRIC CONFIGURATIONS OF SINGULARITIES FOR QUADRATIC DIFFERENTIAL SYSTEMS WITH TOTAL FINITE MULTIPLICITY m f = 2 This is a preprint of: Geometric configurations of singularities for quadratic differential systems with total finite multiplicity m f = 2, Joan Carles Artés, Jaume Llibre, Dana Schlomiuk, Nicolae Vulpe,

More information

CUBIC SYSTEMS WITH INVARIANT AFFINE STRAIGHT LINES OF TOTAL PARALLEL MULTIPLICITY SEVEN

CUBIC SYSTEMS WITH INVARIANT AFFINE STRAIGHT LINES OF TOTAL PARALLEL MULTIPLICITY SEVEN Electronic Journal of Differential Equations, Vol. 2013 (2013), No. 274, pp. 1 22. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu CUBIC SYSTEMS

More information

Explicit expression for a first integral for some classes of polynomial differential systems

Explicit expression for a first integral for some classes of polynomial differential systems Int. J. Adv. Appl. Math. and Mech. 31 015 110 115 ISSN: 347-59 Journal homepage: www.ijaamm.com International Journal of Advances in Applied Mathematics and Mechanics Eplicit epression for a first integral

More information

Algebra I. Book 2. Powered by...

Algebra I. Book 2. Powered by... Algebra I Book 2 Powered by... ALGEBRA I Units 4-7 by The Algebra I Development Team ALGEBRA I UNIT 4 POWERS AND POLYNOMIALS......... 1 4.0 Review................ 2 4.1 Properties of Exponents..........

More information

REMARKS ON THE CLASSIFICATION OF REVERSIBLE CUBIC SYSTEMS WITH CENTER. Henryk Żołądek

REMARKS ON THE CLASSIFICATION OF REVERSIBLE CUBIC SYSTEMS WITH CENTER. Henryk Żołądek Topological Methods in Nonlinear Analysis Journal of the Juliusz Schauder Center Volume 8, 1996, 5 4 REMARKS ON THE CLASSIFICATION OF REVERSIBLE CUBIC SYSTEMS WITH CENTER Henryk Żołądek The paper [8] from

More information

The rolling ball problem on the sphere

The rolling ball problem on the sphere São Paulo Journal of Mathematical Sciences 6, 2 (2012), 145 154 The rolling ball problem on the sphere Laura M. O. Biscolla Universidade Paulista Rua Dr. Bacelar, 1212, CEP 04026 002 São Paulo, Brasil

More information

2. Second-order Linear Ordinary Differential Equations

2. Second-order Linear Ordinary Differential Equations Advanced Engineering Mathematics 2. Second-order Linear ODEs 1 2. Second-order Linear Ordinary Differential Equations 2.1 Homogeneous linear ODEs 2.2 Homogeneous linear ODEs with constant coefficients

More information

The Period Function for Second-Order Quadratic ODEs is Monotone *

The Period Function for Second-Order Quadratic ODEs is Monotone * QUALITATIVE THEORY OF DYNAMICAL SYSTEMS 4, 329 32 (2004) ARTICLE NO. 66 The Period Function for Second-Order Quadratic ODEs is Monotone * Armengol Gasull Dept. de Matemàtiques, Edifici Cc, Universitat

More information

1. Introduction and statement of main results. dy dt. = p(x, y),

1. Introduction and statement of main results. dy dt. = p(x, y), ALGORITHM FOR DETERMINING THE GLOBAL GEOMETRIC CONFIGURATIONS OF SINGULARITIES OF QUADRATIC DIFFERENTIAL SYSTEMS WITH THREE DISTINCT REAL SIMPLE FINITE SINGULARITIES JOAN C. ARTÉS1, JAUME LLIBRE 1, DANA

More information

On a Hamiltonian version of a 3D Lotka-Volterra system

On a Hamiltonian version of a 3D Lotka-Volterra system On a Hamiltonian version of a 3D Lotka-Volterra system Răzvan M. Tudoran and Anania Gîrban arxiv:1106.1377v1 [math-ph] 7 Jun 2011 Abstract In this paper we present some relevant dynamical properties of

More information

Algebra Homework, Edition 2 9 September 2010

Algebra Homework, Edition 2 9 September 2010 Algebra Homework, Edition 2 9 September 2010 Problem 6. (1) Let I and J be ideals of a commutative ring R with I + J = R. Prove that IJ = I J. (2) Let I, J, and K be ideals of a principal ideal domain.

More information

arxiv: v1 [math.ra] 24 Aug 2016

arxiv: v1 [math.ra] 24 Aug 2016 Characterizations and representations of core and dual core inverses arxiv:1608.06779v1 [math.ra] 24 Aug 2016 Jianlong Chen [1], Huihui Zhu [1,2], Pedro Patrício [2,3], Yulin Zhang [2,3] Abstract: In this

More information

Pacific Journal of Mathematics

Pacific Journal of Mathematics Pacific Journal of Mathematics CHEBYSHEV PROPERTY OF COMPLETE ELLIPTIC INTEGRALS AND ITS APPLICATION TO ABELIAN INTEGRALS Armengol Gasull, Weigu Li, Jaume Llibre, and Zhifen Zhang Volume No. February PACIFIC

More information

7 Planar systems of linear ODE

7 Planar systems of linear ODE 7 Planar systems of linear ODE Here I restrict my attention to a very special class of autonomous ODE: linear ODE with constant coefficients This is arguably the only class of ODE for which explicit solution

More information

LIOUVILLIAN FIRST INTEGRALS OF SECOND ORDER POLYNOMIAL DIFFERENTIAL EQUATIONS Colin Christopher. 1. Introduction

LIOUVILLIAN FIRST INTEGRALS OF SECOND ORDER POLYNOMIAL DIFFERENTIAL EQUATIONS Colin Christopher. 1. Introduction Electronic Journal of Differential Equations, Vol. 1999(1999) No. 49, pp. 1 7. ISSN: 1072-6691. URL: http://ejde.math.swt.edu or http://ejde.math.unt.edu ftp ejde.math.swt.edu ftp ejde.math.unt.edu (login:

More information

GOLOMB S ARITHMETICAL SEMIGROUP TOPOLOGY AND A SEMIPRIME SUFFICIENCY CONDITION FOR DIRICHLET S THEOREM

GOLOMB S ARITHMETICAL SEMIGROUP TOPOLOGY AND A SEMIPRIME SUFFICIENCY CONDITION FOR DIRICHLET S THEOREM ROCKY MOUNTAIN JOURNAL OF MATHEMATICS Volume 46, Number 3, 2016 GOLOMB S ARITHMETICAL SEMIGROUP TOPOLOGY AND A SEMIPRIME SUFFICIENCY CONDITION FOR DIRICHLET S THEOREM CHRIS ORUM ABSTRACT. Dirichlet s theorem

More information

SQUARE ROOTS OF 2x2 MATRICES 1. Sam Northshield SUNY-Plattsburgh

SQUARE ROOTS OF 2x2 MATRICES 1. Sam Northshield SUNY-Plattsburgh SQUARE ROOTS OF x MATRICES Sam Northshield SUNY-Plattsburgh INTRODUCTION A B What is the square root of a matrix such as? It is not, in general, A B C D C D This is easy to see since the upper left entry

More information

The Moore-Penrose inverse of differences and products of projectors in a ring with involution

The Moore-Penrose inverse of differences and products of projectors in a ring with involution The Moore-Penrose inverse of differences and products of projectors in a ring with involution Huihui ZHU [1], Jianlong CHEN [1], Pedro PATRÍCIO [2] Abstract: In this paper, we study the Moore-Penrose inverses

More information

27 Wyner Math 2 Spring 2019

27 Wyner Math 2 Spring 2019 27 Wyner Math 2 Spring 2019 CHAPTER SIX: POLYNOMIALS Review January 25 Test February 8 Thorough understanding and fluency of the concepts and methods in this chapter is a cornerstone to success in the

More information

Mathematics Notes for Class 12 chapter 7. Integrals

Mathematics Notes for Class 12 chapter 7. Integrals 1 P a g e Mathematics Notes for Class 12 chapter 7. Integrals Let f(x) be a function. Then, the collection of all its primitives is called the indefinite integral of f(x) and is denoted by f(x)dx. Integration

More information

Elementary ODE Review

Elementary ODE Review Elementary ODE Review First Order ODEs First Order Equations Ordinary differential equations of the fm y F(x, y) () are called first der dinary differential equations. There are a variety of techniques

More information

ENGI 4430 PDEs - d Alembert Solutions Page 11.01

ENGI 4430 PDEs - d Alembert Solutions Page 11.01 ENGI 4430 PDEs - d Alembert Solutions Page 11.01 11. Partial Differential Equations Partial differential equations (PDEs) are equations involving functions of more than one variable and their partial derivatives

More information

A note on Derivations of Commutative Rings

A note on Derivations of Commutative Rings A note on Derivations of Commutative Rings MICHAEL GR. VOSKOGLOU School of Technological Applications Graduate Technological Educational Institute (T. E. I.) Meg. Alexandrou 1, 26334 Patras GREECE e-mail:

More information

Roots and Coefficients Polynomials Preliminary Maths Extension 1

Roots and Coefficients Polynomials Preliminary Maths Extension 1 Preliminary Maths Extension Question If, and are the roots of x 5x x 0, find the following. (d) (e) Question If p, q and r are the roots of x x x 4 0, evaluate the following. pq r pq qr rp p q q r r p

More information

b n x n + b n 1 x n b 1 x + b 0

b n x n + b n 1 x n b 1 x + b 0 Math Partial Fractions Stewart 7.4 Integrating basic rational functions. For a function f(x), we have examined several algebraic methods for finding its indefinite integral (antiderivative) F (x) = f(x)

More information

Mathematical Olympiad Training Polynomials

Mathematical Olympiad Training Polynomials Mathematical Olympiad Training Polynomials Definition A polynomial over a ring R(Z, Q, R, C) in x is an expression of the form p(x) = a n x n + a n 1 x n 1 + + a 1 x + a 0, a i R, for 0 i n. If a n 0,

More information

Math 141: Lecture 11

Math 141: Lecture 11 Math 141: Lecture 11 The Fundamental Theorem of Calculus and integration methods Bob Hough October 12, 2016 Bob Hough Math 141: Lecture 11 October 12, 2016 1 / 36 First Fundamental Theorem of Calculus

More information

MathB65 Ch 4 VII, VIII, IX.notebook. November 06, 2017

MathB65 Ch 4 VII, VIII, IX.notebook. November 06, 2017 Chapter 4: Polynomials I. Exponents & Their Properties II. Negative Exponents III. Scientific Notation IV. Polynomials V. Addition & Subtraction of Polynomials VI. Multiplication of Polynomials VII. Greatest

More information

Topics from Algebra and Pre-Calculus. (Key contains solved problems)

Topics from Algebra and Pre-Calculus. (Key contains solved problems) Topics from Algebra and Pre-Calculus (Key contains solved problems) Note: The purpose of this packet is to give you a review of basic skills. You are asked not to use the calculator, except on p. (8) and

More information

Homework 8 Solutions to Selected Problems

Homework 8 Solutions to Selected Problems Homework 8 Solutions to Selected Problems June 7, 01 1 Chapter 17, Problem Let f(x D[x] and suppose f(x is reducible in D[x]. That is, there exist polynomials g(x and h(x in D[x] such that g(x and h(x

More information

QUADRATIC EQUATIONS AND MONODROMY EVOLVING DEFORMATIONS

QUADRATIC EQUATIONS AND MONODROMY EVOLVING DEFORMATIONS QUADRATIC EQUATIONS AND MONODROMY EVOLVING DEFORMATIONS YOUSUKE OHYAMA 1. Introduction In this paper we study a special class of monodromy evolving deformations (MED). Chakravarty and Ablowitz [4] showed

More information

Permutations and Polynomials Sarah Kitchen February 7, 2006

Permutations and Polynomials Sarah Kitchen February 7, 2006 Permutations and Polynomials Sarah Kitchen February 7, 2006 Suppose you are given the equations x + y + z = a and 1 x + 1 y + 1 z = 1 a, and are asked to prove that one of x,y, and z is equal to a. We

More information

Progress in Mathematics 313. Jaume Llibre Rafael Ramírez. Inverse Problems in Ordinary Differential Equations and Applications

Progress in Mathematics 313. Jaume Llibre Rafael Ramírez. Inverse Problems in Ordinary Differential Equations and Applications Progress in Mathematics 313 Jaume Llibre Rafael Ramírez Inverse Problems in Ordinary Differential Equations and Applications Progress in Mathematics Volume 313 Series Editors Hyman Bass, University of

More information

arxiv: v1 [math.ds] 18 Mar 2010

arxiv: v1 [math.ds] 18 Mar 2010 arxiv:1003.3589v1 [math.ds] 18 Mar 2010 An integrating factor matrix method to find first integrals 1. Introduction K V I Saputra 1, G R W Quispel 2, L van Veen 3 1 Faculty of Science and Mathematics,

More information

Global phase portraits of a SIS model

Global phase portraits of a SIS model Global phase portraits of a SIS model Regilene D. S. Oliveira and Alex C. Rezende Abstract In the qualitative theory of ordinary differential equations, we can find many papers whose objective is the classification

More information

ON POSITIVE, LINEAR AND QUADRATIC BOOLEAN FUNCTIONS

ON POSITIVE, LINEAR AND QUADRATIC BOOLEAN FUNCTIONS Kragujevac Journal of Mathematics Volume 36 Number 2 (2012), Pages 177 187. ON POSITIVE, LINEAR AND QUADRATIC BOOLEAN FUNCTIONS SERGIU RUDEANU Abstract. In [1], [2] it was proved that a function f : {0,

More information

Absence of limit cycles for Kukles-type systems

Absence of limit cycles for Kukles-type systems AVANZA. Vol. iv. Fm - Iit, Uacj (014) 5 13. Isbn: 978-607-94-5-3 Absence of limit cycles for Kukles-type systems Osuna, Osvaldo, Rodríguez-Ceballos, Joel, Villaseñor, Gabriel Abstract In this note, we

More information

Unit 2-1: Factoring and Solving Quadratics. 0. I can add, subtract and multiply polynomial expressions

Unit 2-1: Factoring and Solving Quadratics. 0. I can add, subtract and multiply polynomial expressions CP Algebra Unit -1: Factoring and Solving Quadratics NOTE PACKET Name: Period Learning Targets: 0. I can add, subtract and multiply polynomial expressions 1. I can factor using GCF.. I can factor by grouping.

More information

Period function for Perturbed Isochronous Centres

Period function for Perturbed Isochronous Centres QUALITATIE THEORY OF DYNAMICAL SYSTEMS 3, 275?? (22) ARTICLE NO. 39 Period function for Perturbed Isochronous Centres Emilio Freire * E. S. Ingenieros, Universidad de Sevilla, Camino de los Descubrimientos

More information

A note on linear differential equations with periodic coefficients.

A note on linear differential equations with periodic coefficients. A note on linear differential equations with periodic coefficients. Maite Grau (1) and Daniel Peralta-Salas (2) (1) Departament de Matemàtica. Universitat de Lleida. Avda. Jaume II, 69. 251 Lleida, Spain.

More information

MATH 431 PART 2: POLYNOMIAL RINGS AND FACTORIZATION

MATH 431 PART 2: POLYNOMIAL RINGS AND FACTORIZATION MATH 431 PART 2: POLYNOMIAL RINGS AND FACTORIZATION 1. Polynomial rings (review) Definition 1. A polynomial f(x) with coefficients in a ring R is n f(x) = a i x i = a 0 + a 1 x + a 2 x 2 + + a n x n i=0

More information

Operational method for the solution of ordinary differential equations using Hermite series

Operational method for the solution of ordinary differential equations using Hermite series MATHEMATICAL COMMUNICATIONS 79 Math. Commun. 3(018, 79 93 Operational method for the solution of ordinary differential equations using Hermite series Gabriel Bengochea 1,, Luis Verde Star 1 and Manuel

More information

Polynomials. Chapter 4

Polynomials. Chapter 4 Chapter 4 Polynomials In this Chapter we shall see that everything we did with integers in the last Chapter we can also do with polynomials. Fix a field F (e.g. F = Q, R, C or Z/(p) for a prime p). Notation

More information

Math 0320 Final Exam Review

Math 0320 Final Exam Review Math 0320 Final Exam Review SHORT ANSWER. Write the word or phrase that best completes each statement or answers the question. Factor out the GCF using the Distributive Property. 1) 6x 3 + 9x 1) Objective:

More information

BIFURCATION PHENOMENA Lecture 1: Qualitative theory of planar ODEs

BIFURCATION PHENOMENA Lecture 1: Qualitative theory of planar ODEs BIFURCATION PHENOMENA Lecture 1: Qualitative theory of planar ODEs Yuri A. Kuznetsov August, 2010 Contents 1. Solutions and orbits. 2. Equilibria. 3. Periodic orbits and limit cycles. 4. Homoclinic orbits.

More information

Operations w/polynomials 4.0 Class:

Operations w/polynomials 4.0 Class: Exponential LAWS Review NO CALCULATORS Name: Operations w/polynomials 4.0 Class: Topic: Operations with Polynomials Date: Main Ideas: Assignment: Given: f(x) = x 2 6x 9 a) Find the y-intercept, the equation

More information

ON SEMINORMAL SUBGROUPS OF FINITE GROUPS

ON SEMINORMAL SUBGROUPS OF FINITE GROUPS ROCKY MOUNTAIN JOURNAL OF MATHEMATICS Volume 47, Number 2, 2017 ON SEMINORMAL SUBGROUPS OF FINITE GROUPS A. BALLESTER-BOLINCHES, J.C. BEIDLEMAN, V. PÉREZ-CALABUIG AND M.F. RAGLAND ABSTRACT. All groups

More information

On the fixed points set of differential systems reversibilities arxiv: v1 [math.ds] 6 Oct 2015

On the fixed points set of differential systems reversibilities arxiv: v1 [math.ds] 6 Oct 2015 On the fixed points set of differential systems reversibilities arxiv:1510.01464v1 [math.ds] 6 Oct 2015 Marco Sabatini October 5, 2015 Abstract We extend a result proved in [7] for mirror symmetries of

More information

Uniqueness of Limit Cycles For Liénard Differential Equations of Degree Four

Uniqueness of Limit Cycles For Liénard Differential Equations of Degree Four Uniqueness of Limit Cycles For Liénard Differential Equations of Degree Four Chengzhi Li and Jaume Llibre (Peking University and Universitat Autònoma de Barcelona) Salou, Spain, October 1-5, 2012 Congratulations

More information

Basic Theory of Linear Differential Equations

Basic Theory of Linear Differential Equations Basic Theory of Linear Differential Equations Picard-Lindelöf Existence-Uniqueness Vector nth Order Theorem Second Order Linear Theorem Higher Order Linear Theorem Homogeneous Structure Recipe for Constant-Coefficient

More information

Review session Midterm 1

Review session Midterm 1 AS.110.109: Calculus II (Eng) Review session Midterm 1 Yi Wang, Johns Hopkins University Fall 2018 7.1: Integration by parts Basic integration method: u-sub, integration table Integration By Parts formula

More information

A new qualitative proof of a result on the real jacobian conjecture

A new qualitative proof of a result on the real jacobian conjecture Anais da Academia Brasileira de Ciências (2015) (Annals of the Brazilian Academy of Sciences) Printed version ISSN 0001-3765 / Online version ISSN 1678-2690 http://dx.doi.org/10.1590/0001-3765201520130408

More information

LINEAR DIFFERENTIAL EQUATIONS. Theorem 1 (Existence and Uniqueness). [1, NSS, Section 6.1, Theorem 1] 1 Suppose. y(x)

LINEAR DIFFERENTIAL EQUATIONS. Theorem 1 (Existence and Uniqueness). [1, NSS, Section 6.1, Theorem 1] 1 Suppose. y(x) LINEAR DIFFERENTIAL EQUATIONS MINSEON SHIN 1. Existence and Uniqueness Theorem 1 (Existence and Uniqueness). [1, NSS, Section 6.1, Theorem 1] 1 Suppose p 1 (x),..., p n (x) and g(x) are continuous real-valued

More information

Unit 2 Rational Functionals Exercises MHF 4UI Page 1

Unit 2 Rational Functionals Exercises MHF 4UI Page 1 Unit 2 Rational Functionals Exercises MHF 4UI Page Exercises 2.: Division of Polynomials. Divide, assuming the divisor is not equal to zero. a) x 3 + 2x 2 7x + 4 ) x + ) b) 3x 4 4x 2 2x + 3 ) x 4) 7. *)

More information

ON THE DYNAMICS OF THE RIGID BODY WITH A FIXED POINT: PERIODIC ORBITS AND INTEGRABILITY

ON THE DYNAMICS OF THE RIGID BODY WITH A FIXED POINT: PERIODIC ORBITS AND INTEGRABILITY ON THE DYNAMICS OF THE RIID BODY WITH A FIXED POINT: PERIODIC ORBITS AND INTERABILITY JUAN L.. UIRAO 1, JAUME LLIBRE 2 AND JUAN A. VERA 3 Abstract. The aim of the present paper is to study the periodic

More information

PERIODIC ORBITS OF A COLLINEAR RESTRICTED THREE BODY PROBLEM

PERIODIC ORBITS OF A COLLINEAR RESTRICTED THREE BODY PROBLEM PERIODIC ORBITS OF A COLLINEAR RESTRICTED THREE BODY PROBLEM MONTSERRAT CORBERA Departament d Informàtica i Matemàtica, Escola Politècnica Superior, Universitat de Vic, C/ Laura 13, 85 Vic, Barcelona,

More information

arxiv: v1 [math.ra] 24 Feb 2018

arxiv: v1 [math.ra] 24 Feb 2018 THE LATTICE OF CHARACTERISTIC SUBSPACES OF AN ENDOMORPHISM WITH JORDAN-CHEVALLEY DECOMPOSITION DAVID MINGUEZA, M EULÀLIA MONTORO, AND ALICIA ROCA arxiv:180208832v1 [mathra] 24 Feb 2018 Abstract Given an

More information