CADE-18 Workshop:
Problems and Problem Sets
Contents:
John Harrison
Invitedtalk: Extracting Test Problems from Real Applications
Jurgen Zimmer, Andreas Franke, Simon Colton, Geo Sutcli e
Integrating HR and tptp2X into MathWeb to Compare Automated The-
orem Provers
Jieh Hsiang, Yuh Pyng Shieh, YaoChinag Chen
The Cyclic Complete Mapppings Counting Problems
John K. Slaney
A Benchmark Template for Substructural Logics
Zack Ernst, Branden Fitelson, Kenneth Harris, William McCune, Ran-
ganathan Padmanabhan, Rob ert Vero , Larry Wos
More First-order Test Problems in Math and Logic
Ko en Claessen, Reiner Hahnle, Johan Martensson
Veri cation of Hardware Systems with First-Order Logic
Johann Schumann
Invitedtalk: TBA
Organizers: Geo Sutcli e, Je Pelletier, Christan Suttner 1 2
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´´eÕÙaдiÒÚeÖ×e´Bµ¸Cµ ² eÕÙaдÑÙÐØiÔÐÝ´B¸Dµ¸Cµ ² eÕÙaдiÒÚeÖ×e´Dµ¸Bµ
² ? [E¸F] : ´eÕÙaдiÒÚeÖ×e´Eµ¸Fµ ² eÕÙaдÑÙÐØiÔÐÝ´E¸Bµ¸Fµµ
² eÕÙaдÑÙÐØiÔÐÝ´D¸Cµ¸Bµµ <=>
´eÕÙaдiÒÚeÖ×e´Dµ¸Cµ ² eÕÙaдiÒÚeÖ×e´Bµ¸Dµ ² eÕÙaдÑÙÐØiÔÐÝ´C¸Dµ¸Bµµµµµº
½ ½ ½
8 b; c; d ´b = c ² b £ d = c ² d = b ² 9 e; f ´e = f ² e £ b = f µ²d £ c = b
½ ½
´µ d = c ² b = d ² c £ d = bµ
FigÙÖe ¾: ÌheÓÖeÑ 49¿ iÒ ×e××iÓÒ ½¸ Ûhich ÇØØeÖ cÓÙÐd ÒÓØ ÔÖÓÚe iÒ ½¾¼ ×ecÓÒd× ½¼ 600 "Bliksem_1.12" "Spass_1.02" "E_0.62"
500
400
300 Average Proof Time (ms) 200
100
0 0 2000 4000 6000 8000 10000 12000
Theorem Number
FigÙÖe ¿: AÚeÖage ØiÑe× ØÓ ÔÖÓÚe ØheÓÖeÑ×
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eÕÙaдÑÙÐØiÔÐÝ´À¸Cµ¸Áµµµµº ½5 The Cyclic Complete Mappings Counting Problems
Jieh Hsiang ∗, YuhPyng Shieh and YaoChiang Chen Dept. of Computer Science and Information Engineering, National Taiwan University, Taipei 106, Taiwan [email protected] {arping,johnjohn}@turing.csie.ntu.edu.tw
Abstract A complete mapping of a group (G, +) is a permutation f(x)ofG with f(0) = 0 such that −x+ f(x) is also a permutation of G.Givena group G,theComplete Mappings Counting Problem is to find, if any, the number of complete mappings of G. Complete mapping problems are ideal for testing the strength of propositional solvers. In this paper we describe various types of complete mapping prob- lems, and their relationship with variations of the n-queen problems. We also present several forms of symmetry operators which, in addition to being theoretically interesting on their own, are crucial for improv- ing the efficiency of the provers. Several classes of challenge problems for propositional provers are given, so are the transformations of these problems into propositional format.
1Overview
A complete mapping of a group (G, +) is a permutation f(x)ofG with f(0)=0where0istheidentityof(G, +) such that −x + f(x)isalsoa permutation. For example, (1, 2, 4)(3, 6, 5) is a complete mapping of (Z7, +).
x 0123456cycle structure f(x) 0246135(1,2,4)(3,6,5) −x + f(x) 0123456
∗Research supported in part by Grant NSC 90-2213-E-002-110 of the National Science Council of the Republic of China.
1 The concept of complete mappings was first introduced by Mann [15], and used to construct orthogonal Latin squares. It was later studied by many people (e.g., [14, 19, 5, 10, 16]) under different names. A strong complete mapping is a complete mapping f(x) such that x+f(x) is also a permutation. The term strong complete mapping was first used by Hsu and Keedwell [12]. They gave a construction for strong complete mappings of odd order abelian groups. Earlier studies also include [2] and [9]. A strong complete mapping can be seen as a solution of the toroidal n-queen problem. The relationship between the complete mapping problems and the n- queen problems is worth investigating. In this paper we present a natural extension of the toroidal n-queen problem (which, in itself, is a natural extension of the n-queen problem), which we call the toroidal-semi n-queen problem. We also establish correspondences between the class of complete mapping problems and the n-queen problems. Both n-queen problems and the complete mapping problems are good challenge problems for propositional provers. They can easily be coded into propositional expressions, but solving them requires more than sophisticated data structures and clever programming. It also needs a good understanding of how search works and how to eliminate redundancy in the search space. Indeed, it would not have been possible for our own prover to produce some impressive results (such as showing that the number of complete mappings in Z23 is 19,686,730,313,955) if not for the symmetry cutting strategies and partition techniques designed [13, 22] to utilize the symmetry operators in search. A symmetry operator Π on complete mappings is a function from GG to GG such that f is a complete mapping if and only if Π(f)isalsoacom- plete mapping. The operators {R, A, Hα,Tc} were described implicitly in Singer(1960) [24] for cyclic groups. In 1991, Hsu [11] used a group of opera- tors spanned by {R, A} to classify the set of complete mappings on a cyclic group Zn. Moreover, Hsiang, Hsu, and Shieh [23] offered the numbers of complete mappings for all abelian groups G with |G|≤19 and the following ones CM(n) for cyclic group Zn.(Remark:CM(n) = 0 for all even numbers n.) n 57 9 1113 CM(n) 3 19 225 3441 79259 n 15 17 19 21 23 CM(n) 2424195 94417089 4613520889 275148653115 19686730313955 The rest of the paper is organized as follows. In Section 2 we give the
2 basic definitions and list known results of various types of n-queen problems and complete mapping problems, including some new ones. Section 3 intro- duces the symmetry operators and their properties. Section 4 defines the challenge problems for propositional provers, and Section 5 transforms the problems into propositional expressions.
2 Complete mappings and the n-queen problems
The famous n-queen problem [3, 4] can be described as follows: Place n queens on a n by n chessboard, one queen on each square, so that no queen attacks any other. That is, there exists at most one queen on the same row, column and diagonal. There are many different perspectives of the n-queen problem described in Erbas, Sarkeshik, and Tanik [7]. One of the most basic is to view a solution of n-queen problem as a function f(x)fromZn to Zn such that f(x)=y if and only if position (x, y) is occupied by a queen.
f 01234567 x f(x) 0 ✉ 0 1 1 ❅ ✉ 1 7 ✉ 2 ❅ 2 5 3 ✉ ❅ 3 0 ✉ 4 ❅ 4 2 5 ❅✉ 5 4 ✉ 6 ❅ 6 6 7 ✉ ❅ 7 3
Figure 1: A solution of 8-queen problem.
Definition 1 (n-queen problem) Let Zn = {0, 1, 2, ···,n− 1}.Asolu- tion of the n-queen problem is a permutation f(x) from Zn to Zn such that
∀i=j∈Zn i + f(i) = j + f(j) and ∀i=j∈Zn − i + f(i) = −j + f(j) under the natural number addition. We use Q(n) to denote the set of solutions of n-queen problem and Q(n) the cardinality of Q(n).
Consider a modular chessboard, that is, a chessboard where the diagonals continue on the other side as shown in Figure 2. This is a variation of the n- queen problem called the modular n-queen problem. The concept of modular
3 chessboards were introduced by P´olya [20]. There are different names for the modular n-queen problem. We adopt the term toroidal n-queen problem [21] in this paper. Another similar class of problems is the toroidal-semi n- queen problem where the diagonal ”wrapping around” is assumed in only one direction.
Definition 2 (toroidal n-queen problem) A solution of the toroidal n- queen problem is a permutation f(x) from Zn to Zn such that (under the cyclic group (Zn, +)), x + f(x) and −x + f(x) are both permutations. We use TQ(n) to denote the set of solutions of the toroidal n-queen problem and TQ(n) the cardinality of TQ(n).
Definition 3 (toroidal-semi n-queen problem) A solution of the toroidal- semi n-queen problem is a permutation f(x) from Zn to Zn such that (under the cyclic group (Zn, +)), −x + f(x) is a permutation. We use TSQ(n) to denote the set of solutions of toroidal-semi n-queen problem and TSQ(n) the cardinality of TSQ (n).
f −3−2−10 1 2 3 x f(x) f −3−2−10 1 2 3 x f(x) −3 ✉ ❅ −3−3 −3 ❅ ✉ −3 2 ✉ ✉ −2 ❅ −2 1 −2 ❅ −2 0 −1 ✉ ❅ −1−2 −1 ✉ ❅ −1−1 ✉ ✉ 0 ❅ 0 2 0 ❅ 0 3 1 ❅ ✉ 1 −1 1 ✉ ❅ 1 −2 ✉ ✉ 2 ❅ 2 3 2 ❅ 2 1 3 ❅ ✉ 3 0 3 ✉ ❅ 3 −3
Figure 2: The left is one solution of toroidal 7-queen problem and the right is one solution of toroidal-semi 7-queen problem.
Definition 4 (complete mapping problem) A complete mapping of a group (G, +) is a permutation f(x) of G with f(0) = 0 such that −x + f(x) is also a permutation of G. A complete mapping is called strong if x + f(x) is also a permutation of G. Since in this paper we only discuss cyclic groups, we may assume G = Zn.WeuseSCM(n) and CM(n) to denote the set of (strong) complete mappings of Zn and SCM(n),CM(n) the cardinalities of SCM (n) and CM (n), respectively.
4 By the above definitions, if G is a cyclic group Zn,thenasolutionf(x)of the toroidal-semi n-queen problem is also a solution of the complete mapping problem if and only if f(0) = 0. There is a similar correspondence between the toroidal n-queen problem and the strong complete mapping problem. In Figure 3 we list some examples. For example, f1(x) is a solution of the (toroidal)-(semi) 11-queen problem and a (strong) complete mapping of Z11, and f4(x) is a solution of the 11-queen problem and the toroidal-semi 11- queen problem but not a solution of the toroidal 11-queen problem and not a (strong) complete mapping of Z11. x 012345 678910 √√Q TQ √TSQ √SCM √CM f1(x) 024681013579 √√ √ ×× f2(x) 135790 2 46810√ √ √ × × f3(x) 025817 103649 √ √ × ×× f4(x) 136928 0 47510√ ×× × × f5(x) 026971013584 √ √ ×× × f6(x) 021581094376 √ f7(x) 132690 105487 ×× ××
Figure 3: Examples under Z11
Proposition 1 Given a cyclic group Zn,
1. a solution f(x) to the toroidal-semi n-queen problem is a complete mapping if and only if f(0) = 0,
2. a solution f(x) to the toroidal n-queen problem is a strong complete mapping if and only if f(0) = 0,
3. TSQ(n)=n × CM(n) and TQ(n)=n × SCM(n),
4. TQ(n) 5. TQ(n) 2.1 The existence problems Given Zn,theexistence problem asks whether there exists a (toroidal)-(semi) n-queen solution or a (strong) complete mapping. The existence problems of the (toroidal)-(semi) n-queen problem have been completely solved. As 5 a consequence of Proposition 1, the (strong) complete mapping existence problems are also solved. We list the results here. Theorem 2 (The toroidal n-queen existence problem [20]) TQ(n)= 0 if and only if 2 | nor3 | n. Theorem 3 (The complete mapping existence problem [18]) A finite abelian group G admits complete mappings if and only if its Sylow2-subgroup is trivial or non-cyclic. This implies CM(n)=0if and only if 2 n. Theorem 4 (n-queen existence problem [25]) There are solutions to the n-queen problem for all n ≥ 4. 2.2 The counting problems The counting problems, on the other hand, are mostly open, due to the tremendous complexity. The best known result for the n-queen problem is n = 23. It was first solved by Pion and Fourre [1] (A000170) using bitwise instructions, depth-first-search and was done in a distributed environment. (The citation [1], a website with an impressive collection of number se- quences, will be used extensively in the rest of this paper. The indicator A000170 refers to the problem number given in that URL.) The best TSQ in- dicated in [1] (A006717) is TSQ(17), done by Wanless. In last year, we ([22]) TSQ(23) extended it to TSQ(23) (by successfully computing CM(23) = 23 ). In order to obtain these results, we used symmetry operators, to be introduced in the next section, and partition strategies based on the symmetry opera- tors to partition the search space. Engelhardt [1] (A007705) used symmetry operators and depth-first-search to compute TQ(29) successfully. The fol- lowings table (Table 1) are the known sequences of Q(n), CM(n), TSQ(n), TQ(n), and SCM(n). 3 Symmetry operators A symmetry operator of the (toroidal)-(semi) n-queen problem or the (strong) complete mapping problem is a bijection Π from the solution space to the solution space such that f(x) is a solution if and only if Π(f)(x)isalsoaso- −1 −1 lution. For example, R(f)=f ,andR90◦ (f)=(−1−f) are two symme- try operators for the n-queen problem. The set of symmetry operators can usually be defined through spanning a set of basic symmetry operators, and we call the set a symmetry operator group. For example, span{R, R90◦ } = 6 n Q(n) CM(n) TSQ(n) TQ(n) SCM(n) 1 11 111 2 00 000 3 01 300 4 20 000 5 103 15102 6 40 000 7 40 19 133 28 4 8 92 0 0 0 0 9 352 225 2025 0 0 10 724 0 0 0 0 11 2680 3441 37851 88 8 12 14200 0 0 0 0 13 73712 79259 1030367 4524 348 14 365596 0 0 0 0 15 2279184 2424195 36362925 0 0 16 14772512 0 0 0 0 17 95815104 94471089 1606008513 140692 8276 18 666090624 0 0 0 0 19 4968057848 4613520889 87656896891 820496 43184 20 39029188884 0 0 0 0 21 314666222712 275148653115 5778121715415 0 0 22 2691008701644 0 0 0 0 23 24233937684440 19686730313955 452794797220965 128850048 5602176 24 ?0 000 25 ? ? ? 1957725000 78309000 26 ?0 000 27 ?? ?00 28 ?0 000 29 ? ? ? 605917055356 20893691564 30 ?0 000 Table 1: The known sequences of Q(n),CM(n),TSQ(n), and TQ(n). 7 2 3 2 3 {Identity, R90◦ ,R90◦ ,R90◦ ,R,R90◦ ◦R, R90◦ ◦R, R90◦ ◦R} is a symmetry operator group spanned from the basic operators R and R90◦ . The symme- try operators generated from the basic operators are also called composite operators. The above 8 symmetry operators are all known ones for the n-queen problem ([17, 6]). Singer (1960) [24] presented 6×n×φ(n) operators spanned by {R, A, Hα,Tc} for complete mappings. Later in this section we will intro- duce an operator R45◦ for the toroidal n-queen problem and strong complete mapping problem that we believe is new. A set of symmetry operators define a notion of equivalence classes. It can reduce the problem of looking for all solutions into one that looks only for the minimal one in each class. Huang [13] designed a symmetry-cutting strategy that utilizes symmetry operators to significantly reduce the search space in his propositional prover. We improved upon his method ([22]) and successfully applied it to the complete mapping counting problems. Without using the symmetry operators and the symmetry-cutting methods, we do not think that computing TSQ(23) is possible. Here we list a summary of symmetry operators, and then describe them in the following propositions and theorems. Problem Basic symmetry operators Number of known operators Q(n) R, R90◦ 8 CM(n) R, A, Tc,Hα 6 × n × φ(n) 2 TSQ(n) R, A, T S(c,d),Hα 6 × n × φ(n) SCM(n) R, R45◦ ,Tc,Hα 8 × n × φ(n) 2 TQ(n) R, R45◦ ,TS(c,d),Hα 8 × n × φ(n) Proposition 5 ([17, 6]) The following are basic symmetry operators for the n-queen problem: reflection R and rotation R90◦ . 1. R(f)(x)=f −1(x). −1 2. R90◦ (f)(x)=(−1 − f) (x). Sometimes we also represent the behavior of R as R(x, y)=(y,x), that is, R(f)(x)=R(x, f(x)) = (f(x),x)=f −1(x). So we rewrite them as follows. 1. R(x, y)=(y,x) and R(f)(x)=f −1(x) −1 2. R90◦ (x, y)=(−1 − y,x) and R90◦ (f)(x)=(−1 − f) (x) Lemma 6 ([17, 6]) The basic symmetry operators (R,andR90◦ )forthe n-queen problem satisfy the following properties. These properties are parts of one proof of Theorem 7. 8 2 4 1. R = R90◦ = id. −1 2. R ◦ R90◦ = R90◦ ◦ R. Zn Here id is the identity. That is, id(f)=f for all f ∈ Zn . Theorem 7 ([17, 6]) There are 8 symmetry operators for n-queen problem spanned by R,andR90◦ . Proposition 8 ([24, 8, 23]) The following are basic symmetry operators for the complete mapping problem of the cyclic group Zn: reflection R, op- erator A, homologies Hα,andtranslations Tc. 1. R(x, y)=(y,x) and R(f)(x)=f −1(x). 2. A(x, y)=(−x + y,−x) and A(f)(x)=−(−id + f)−1(x) where id is the identity function id(x)=x. −1 3. Hα(x, y)=(αx, αy) and Hα(f)(x)=αf(α x) where α ∈ Zn and gcd(α, n)=1. 4. Tc(x, f(x)) = (x − c, f(x)− f(c)) and Tc(f)(x)=f(x + c)− f(c) where c ∈ Zn. Lemma 9 ([8, 23]) The basic symmetry operators (R, A, Hα’s, and Tc’s) for the complete mapping problem have the following properties. These prop- erties are parts of one proof of Theorem 10. 2 3 n 1. R = A = T1 = ID. 2. Hα ◦ Hβ = Hα·β. 3. Tc ◦ Td = Tc+d. 4. R ◦ A = A2 ◦ R. 5. R ◦ Hα = Hα ◦ R. 6. (R ◦ Tc)(f)=(Tf(c) ◦ R)(f). 7. A ◦ Hα = Hα ◦ A. 8. (A ◦ Tc)(f)=(T−c+f(c) ◦ A)(f). 9. Hα ◦ Tc = Tc·α ◦ Hα. 9 Theorem 10 ([23]) There are 6×n×φ(n) symmetry operators for complete mapping problem for cyclic group Zn spanned by R, A, Hα’s, and Tc’s where φ(n)=|{x | 0 Proposition 11 The following are basic symmetry operators for the toroidal- semi n-queen problem: reflection R, operator A, homologies Hα and toroidal shiftings TS(c,d). 1. R, A,andHα’s are defined as complete mapping problem (Definition 8). 2. TS(c,d)(x, y)=(x − c, y − d) and TS(c,d)(f)(x)=f(x + c) − d where c, d ∈ Zn. Lemma 12 The basic symmetry operators (R, A, Hα’s and TS(c,d)’s) for the toroidal-semi n-queen problem have the following properties. These prop- erties are parts of one proof of Theorem 13. 1. Relations between R, A,andHα’s are the same as those in the com- plete mapping problem (Lemma 9). 2. TS(c,d) ◦ TS(a,b) = TS(a+c,b+d). 3. R ◦ TS(c,d) = TS(d,c) ◦ R. 4. A ◦ TS(c,d) = TS(d−c,−c) ◦ A. 5. Hα ◦ TS(c,d) = TS(αc,αd) ◦ Hα. Theorem 13 There are 6×n×n×φ(n) symmetry operators for the toroidal- semi n-queen problem spanned by R, A, Hα’s and TS(c,d)’s. Let Sd(x, y)=(x, y − d). We note that span{Tc,Sd | c, d ∈ Zn} = span{TS(c,d) | c, d ∈ Zn} because the only difference between the toroidal- semi n-queen problem and the complete mapping problem is the constraint f(0) = 0. Proposition 14 The following are basic symmetry operators for the strong complete mapping problem: reflection R, translations Tc’s, homologies Hα and rotation R45◦ . 1. R, Hα’s, and Tc’s are as defined in the complete mapping problem (Proposition 8). 10 √ √ x−y x+y −1 −1 ◦ √ √ ◦ − 2. R45 (x, y)=( 2 , 2 ) and R45 (f)(x)= 2 (id+f)(id f) ( 2x). Lemma 15 The basic symmetry operators (R, R45◦ , Hα’s, and Tc’s) for the strong complete mapping problem have following properties. These properties are parts of one proof of Theorem 16. 1. Relations between R, Tc’s, and Hα’s are the same as for complete mappings (Lemma 9). 8 2. R45◦ = ID. −1 3. R ◦ R45◦ = R45◦ ◦ R. 4. Hα ◦ R45◦ = R45◦ ◦ Hα. ◦ ◦ c−f(c) ◦ ◦ 5. (R45 Tc)(f)=(T √ R45 )(f). 2 Theorem 16 There are 8×n×φ(n) symmetry operators for strong complete mapping problem spanned by R, Tc’s, Hα’s and R45◦ . √ 2 ∗ √ In the above statements, 2 is one solution of x =2inZn.Since ∗ 2 does not exist for all Zn, we can also use R45◦ (x, y)=(x − y,x + y) −1 and R45◦ (f)(x)=(id + f) ◦ (id − f) (x) to replace R45◦ .Itiseasyto prove that span{R45◦ ,Hα | α ∈ Zn,gcd(α, n)=1} = span{R45◦ ,Hα | α ∈ Zn,gcd(α, n)=1} when n is an odd number. It is also interesting to observe that the order of reflection R is 2, the order of translation T1 is n,thenumber of homologies Hα is φ(n), and the order of rotation R45◦ is 8. Thus one may tend to think that there are 16 × n × φ(n) symmetry operators. However, 4 note that R180◦ (x, y)=(R45◦ ) (x, y)=(−x, −y)=H−1(x, y). So there are only 8 × n × φ(n) different symmetry operators. We further note that in our 2 discussion here (R45◦ ) (x, y)=R45◦ ◦R45◦ (x, y)=(−y,x), which is different from the R90◦ (x, y)=(−1 − y,x)inthen-queen problem. Definition 5 The following are basic symmetry operators for the toroidal n-queen problem: reflection R, rotation R45◦ , homologies Hα,andtoroidal shifting TS(c,d). 1. R, R45◦ ,andHα’s are defined as in the strong complete mapping prob- lem (Definition 14). 2. TS(c,d)’s are defined as in the toroidal-semi n-queen problem (Propo- sition 11). 11 Lemma 17 The basic symmetry operators (R, R45◦ , Hα’s, and TS(c,d)’s) for the toroidal n-queen problem have following properties. These properties are parts of one proof of Theorem 18. 1. Relations between R, Hα’s, R45◦ are the same as ones in the strong complete mapping problem (Lemma 15). 2. Relations between R, Hα’s, TS(c,d)’s are the same as ones in the toroidal-semi n-queen problem (Lemma 12). ◦ ◦ ◦ ◦ 3. TS(c,d) R45 = R45 TS( −√c−d , −√c+d ). 2 2 Theorem 18 There are 8×n×n×φ(n) symmetry operators for the toroidal n-queen problem spanned by R, R45◦ , Hα’s and TS(c,d)’s. 4 Challenge problems for propositional provers Let P be a symbol in {Q, T SQ, T Q, CM, SCM}, Π be a symmetry operator, and Γ be a symmetry operator group. We are interested in three types of questions. 1. The first one is to evaluate the number of solutions of the original problem. We use P (n) to denote them. For example, Q(n)isthe number of solutions of the n-queen problem. 2. The second one is to evaluate the number of solutions f(x)’s which are fixpoints under the operator Π (Π(f)=f). We use PΠ(n)todenote them. For example, QR90◦ (n) is the number of fixpoint solutions under R90◦ . 3. The last one is to evaluate the number of equivalence classes up to a symmetry operator group Γ. (Since Γ defines an equivalence rela- tion on solution space , we are interested in the number of equivalence classes.) We use P Γ(n) to denote them. For example, Qspan{R,R90◦ }(n) is the number of equivalence classes of n-queen problem for the sym- metry operator group span{R, R90◦ }. Definition 6 We define the symbols for the fixpoints of the symmetry op- erators. 1. QΠ(n)=|{f ∈ Q(n) | Π(f)=f}| for Π ∈ span{R, R90◦ } 2. TQΠ(n)=|{f ∈ TQ(n) | Π(f)=f}| for Π ∈ span{R, R45◦ ,TS(c,d),Hα} 12 3. TSQΠ(n)=|{f ∈ TSQ(n) | Π(f)=f}| for Π ∈ span{R, A, T S(c,d),Hα} 4. CMΠ(n)=|{f ∈ CM(n) | Π(f)=f}| for Π ∈ span{R, A, Tc,Hα} 5. SCMΠ(n)=|{f ∈ SCM(n) | Π(f)=f}| for Π ∈ span{R, R45◦ ,Tc,Hα} We are interested in the fixpoints defined by the basic symmetry oper- ators. Shieh et al. [23] (2000) gave a solution for Tc by reducing CMTc (n) and SCMTc (n)toCM(c)andSCM(c),asshowninthefollowingtheorem. c−1 Theorem 19 ([23]) We have CMTc (c × a)=φ2(a) × a × CM(c) and c−1 SCMTc (c × a)=φ3(a) × a × SCM(c) where φ2(a)=|{x ∈ Za | (x, a)= (x − 1,a)=1}| and φ3(a)=|{x ∈ Za | (x +1,a)=(x, a)=(x − 1,a)=1}|. We calculate CMR(n), CMA(n), CMHα (n) and obtained the following results. For complete mappings fixed under reflection R (CMR), Horton calls them starters and calculates CMR(n)forn ≤ 28 in [1](A006204) and [9]. n 7 9 11 13 15 17 CMR(n) 3 9 25 133 631 3857 n 19 21 23 25 27 29 CMR(n) 25905 188181 1515283 13376125 128102625 1317606101 (Remark: CMA(n)=0if2| n or n ≡ 2(mod3).) n 17131925 31 37 43 49 CMA(n) n−1 1 1 5 52 1055 31814 1403925 83999589 6567620752 2 3 n 3915212733 39 45 CMA(n) n−3 1 0 3 30 513 15996718404 43148682 2 3 (Remark: We note that CMH−1 (n)=CMR180◦ (n).) n 3 5 7 9 11 13 15 17 19 21 CMR180◦ (n) 1 3 5 21 69 319 1957 12513 85445 656771 n 23 25 27 29 31 CMR180◦ (n) 5591277 51531405 509874417 5438826975 62000480093 13 n 33 35 37 CMR180◦ (n) 752464463029 9685138399785 131777883431119 ··· Szabo [1](A032522)(A033148) produced QR180◦ (n)forn =1, 2, 3, , 32 ··· and QR90◦ (n)forn =1, 2, 3, , 47. In the following we also list some new results of QR90◦ (n). The details will be described in forthcoming papers. ≡ (Remark: QR90◦ (n)=0ifn 2, 3(mod4).) n 48 49 52 53 Q (n) R90◦ n 5253278 8551800 49667373 79595269 2 4 n 56 57 60 61 Q (n) R90◦ n 525731268 764804085 5932910966 8905825760 2 4 Definition 7 (equivalence classes counting problem) Let P be the prob- lem Q,TQ,TSQ,CM or SCM,andletΓ be a symmetry operator group. 1. Γ define an equivalence relation ∼ on solution set: f ∼ g if and only if there exists a Π ∈ Γ such that f =Π(g). 2. We define P Γ(n) be the number of equivalence classes. For example, Qspan{R,R90◦ }(n) is the number of equivalence classes of the n-queen problem up to symmetry operator group span{R, R90◦ }.Forsim- plicity, we may drop the word ”span”, and simply use Q{R,R90◦ }(n)for Qspan{R,R90◦ }(n). Engelhardt computed Q{R,R90◦ }(23) [1](A002562) and TQ{R,R90◦ ,T S(c,d)}(29) [1](A053994) successfully. To summarize all the above, we suggest the following challenge prob- lems to the propositional provers in the CADE community. They are good test problems for incorporating symmetry elimination, an often encountered technique, in propositional problem solving. In the following we give the problems as well as the best known results, which are presented in the boxes. Problem 1 Compute Q(n), TQ(n)(= n × SCM(n)), and TSQ(n)(= n × CM(n)). 14 Q(23) = 24233937684440 in [1] (A000170) TQ(29) = 605917055356 in [1] (A007705) TSQ(17) = 1606008513 in [1] (A006717) CM(23) = 19686730313955 in [22] Problem 2 Compute QR90◦ (n), and QR180◦ (n). QR90◦ (45) = 1795233792 in [1] (A033148) QR90◦ (61) = 291826098503680 in this paper QR180◦ (32) = 181254386312 in [1] (A032522) Problem 3 Compute TQR45◦ (n)(= SCMR45◦ (n)), TQR90◦ (n)(= SCMR90◦ (n)), and TQR180◦ (n)(= SCMR180◦ (n)). Problem 4 Compute TSQR(n)(= n × CMR(n)), CMA(n), TSQA(n)and TSQR180◦ (n)(= CMR180◦ (n)). CMR(27) = 128102625 in [1] (A006204) CMR(29) = 1317606101 in this paper CMA(49) = 430415593603072 in this paper CMR180◦ (37) = 131777883431119 in [22] Problem 5 Compute Q{R,R90◦ }(n). Q{R,R90◦ }(23) = 3029242658210 in [1] (A002562) Problem 6Compute TQ{R,R90◦ ,T S(c,d)}(n). TQ{R,R90◦ ,T S(c,d)}(29) = 90120677 in [1] (A054500) Problem 7 Compute TQ{R,R45◦ }(n), {R,R ,T S ,H } TQ 45◦ (c,d) α (n)(= SCM{R,R45◦ ,Tc,Hα}(n)), and TSQ{R,A,T S(c,d),Hα}(n)(= CM{R,A,Tc,Hα}(n)). 5 Presenting the problems in propositional logic In this section we give a translation of the problems proposed in Section 4 into propositional logic. We use the propositional symbols xi,j to denote positions. That is, xi,j = true if and only if the place (i,j) is occupied by a queen. Let P be a symbol in {Q, T SQ, T Q, CM, SCM}, Π be a symmetry 15 operator, and Γ be a symmetry operator group. We use φ[P, n], φ[PΠ,n], and φ[P Γ,n] to denote the propositional expressions corresponding to the Γ counting problems P (n), PΠ(n), and P (n), respectively. In other words, Γ computing the numbers P (n), PΠ(n), and P (n) is the same as comput- Γ ing the numbers of assignments that satisfy φ[P, n], φ[PΠ,n], and φ[P ,n], respectively. Proposition 20 The number of satisfiable assignments for the propositional expression φ[Q, n] is the same as Q(n). 1. φ[F, n]= i∈Zn ( j∈Zn xi,j). ⇒ ¬ 2. φ[Horizontal,n]= i,j∈Zn (xi,j j=k∈Zn xi,k). ⇒ ¬ 3. φ[Vertical,n]= i,j∈Zn (xi,j i=k∈Zn xk,j). 1 4. φ[Diagonal,n]= i∈Zn i+j,j∈Zn ⇒ ¬ ⇒ ¬ ((xi+j,j j=k,i+k∈Zn xi+k,k) (xj,i+j j=k,i+k∈Zn xk,i+k)). 2 i−j,j ⇒ ¬ i−k,k 5. φ[Diagonal ,n]= i∈Zn i−j,j∈Zn ((x j=k,i−k∈Zn x ) ⇒ ¬ (xn−1−j,i+j j=k,i+k∈Zn xn−1−k,i+k)). 6. φ[Q, n]=φ[F, n] φ[Horizontal,n] φ[Vertical,n] φ[Diagonal1,n] φ[Diagonal2,n]. Example 1 Take Q(3) as an example. φ[Q, 3] = (x0,0 ∨ x0,1 ∨ x0,2) ∧ (x1,0 ∨ x1,1 ∨ x1,2) ∧ (x2,0 ∨ x2,1 ∨ x2,2) φ[F, 3] ∧(¬x0,0 ∨¬x0,1) ∧ (¬x0,0 ∨¬x0,2) ∧ (¬x0,1 ∨¬x0,2) φ[Horizontal,3] ∧(¬x1,0 ∨¬x1,1) ∧ (¬x1,0 ∨¬x1,2) ∧ (¬x1,1 ∨¬x1,2) φ[Horizontal,3] ∧(¬x2,0 ∨¬x2,1) ∧ (¬x2,0 ∨¬x2,2) ∧ (¬x2,1 ∨¬x2,2) φ[Horizontal,3] ∧(¬x0,0 ∨¬x1,0) ∧ (¬x0,0 ∨¬x2,0) ∧ (¬x1,0 ∨¬x2,0) φ[Vertical,3] ∧(¬x0,1 ∨¬x1,1) ∧ (¬x0,1 ∨¬x2,1) ∧ (¬x1,1 ∨¬x2,1) φ[Vertical,3] ∧(¬x0,2 ∨¬x1,2) ∧ (¬x0,2 ∨¬x2,2) ∧ (¬x1,2 ∨¬x2,2) φ[Vertical,3] ∧(¬x0,0 ∨¬x1,1) ∧ (¬x0,0 ∨¬x2,2) ∧ (¬x1,1 ∨¬x2,2) φ[Diagonal1, 3] ∧(¬x0,1 ∨¬x1,2) ∧ (¬x1,0 ∨¬x2,1) φ[Diagonal1, 3] ∧(¬x0,2 ∨¬x1,1) ∧ (¬x0,2 ∨¬x2,0) ∧ (¬x1,1 ∨¬x2,0) φ[Diagonal2, 3] ∧(¬x0,1 ∨¬x1,0) ∧ (¬x1,2 ∨¬x2,1) φ[Diagonal2, 3] The main difference between the transformations of φ[Q, n]andφ[TQ,n] or φ[TSQ,n] is the way the addition operator in the variable indices i and j is defined. For the n-queen problem the addition ia natural addition. For the others it is the cyclic group addition (Zn, +). 16 Proposition 21 The number of satisfiable assignments in the expressions φ[TQ,n], φ[TSQ,n], φ[CM,n] and φ[SCM,n] isthesameasTQ(n), TSQ(n), CM(n),andSCM(n), respectively. ⇒ ¬ 1. φ[TDiagonal1,n]= i∈Zn j∈Zn (xi+j,j j=k∈Zn xi+k,k). ⇒ ¬ 2. φ[TDiagonal2,n]= i∈Zn j∈Zn (xi−j,j j=k∈Zn xi−k,k). 3. φ[TQ,n]=φ[F, n] φ[Horizontal,n] φ[Vertical,n] φ[TDiagonal1,n] φ[TDiagonal2,n]. 4. φ[TSQ,n]=φ[F, n] φ[Horizontal,n] φ[Vertical,n] φ[TDiagonal1,n]. 5. φ[CM,n]=φ[TSQ,n] x0,0. 6. φ[SCM,n]=φ[TQ,n] x0,0. The basic symmetry operators R, R90◦ , R45◦ , TSc,d, Tc, Hα,andA, can be regarded as functions from Zn × Zn to Zn × Zn.(Forexample, R(x, y)=(y,x)). We remark that the operators Tc’s depend on the solution f(x)since Tc(x, y)=(x − c, y − f(c)). Thus they cannot be used directly in the formulation of the fixpoint sets that we are going to formulate. This problem can be circumvented by using Theorem19, which reduced the computation of CMTc and SCMTc to that of CM(c)andSCM(c), respectively. We now give the transforation for the fixpoint counting problems. Proposition 22 Let Π denote a basic symmetry operator mentioned above other than Π = Tc,wherec ∈ Zn.LetP be a symbol in {Q, T SQ, T Q, CM, SCM}. ⇔ 1. φ[f =Π(f),n]= i,j∈Zn (xi,j xΠ(i,j)). ⇒ ⇔ 2. φ[f = Tc(f),n]= v∈Zn (xc,v ( i,j∈Zn (xi,j xi−c,j−v))). 3. φ[PΠ,n]=φ[P, n] φ[f =Π(f),n]. 4. φ[PTc ,n]=φ[P, n] φ[f = Tc(f),n]. In order to solve the equivalence classes counting problems, we use a lexicographical ordering on the solutions: f 17 Proposition 23 Let P be a symbol in {Q, T SQ, T Q, CM, SCM} and Γ be a symmetry operator group. For any composite symmetry operator Π (not including those defined using Tc), we have φ[f ≤ Π(f),n], and finally we define φ[P Γ,n]. u,v ⇔ −1 1. φ[f<Π(f),k,n]=( u 2. φ[f<Π(f),n]= k∈Zn φ[f<Π(f),k,n]. 3. φ[f ≤ Π(f),n]=φ[f<Π(f),n] φ[f =Π(f),n]. Γ 4. φ[P ,n]=φ[P, n] ( Π∈Γ φ[f ≤ Π(f),n]). 6 Discussion In this paper we proposed seven series of challenge problems for propositional provers. The series involve variations of the complete mapping problems and the n-queen problems. We also established, in this paper, the relationship between the complete mapping problems and the n-queen problems. These proposed challenges are interesting in several aspects. First, they are counting problems, not existence problems. Thus a straightforward im- plementation of Davis-Putnam like procedures may not be sufficient. Sec- ond, they require sophisticated search techniques, such as symmetry elimi- nation and partitioning, in order to trim the search space effectively. Third, the computational cost grows almost exponentially with every increment of n. Of the three better known series, Q, CM,andTQ, the current magic numbers are Q(24), CM(25), and TQ(31). In the following we provide some data of our experiments. For the n- queen problem, it took our program 20 days on a Pentium IV 1.8GHz PC to compute Q(22) successfully. We estimate that we can get Q(24) in 1266 days using the same machine. Another way of making estimations is via the number of computing cycles. We ran the program of Pion and Fourre on the same machine, and made the following comparisons. Note that for the n-queen problems (Q), our program uses about 1/10 of the cycles as theirs. The saving is even more significant for the complete mapping prob- lems (CM) due to the symmetry elimination and partition strategies that we employed. (In our estimation the cycle-difference between our program and Pion/Fourre will increase from 100 times to 1000 when n is 23.) 18 Problem Pion and Fourre [1](A000170) Partition Strategies Q(16) 4.7 × 105megacycles/1 min 4.7 × 104megacycles/26sec Q(18) 5.7 × 106/53min 1.4 × 106/13 min Q(20) 3.5 × 108/2days 5.2 × 107/8 hours Q(22) —— 3.2 × 109/20 days Q(24) 1.9 × 1012/12104 days(estimate) 1.9 × 1011/1266 days(estimate) CM(17) 4.2 × 106/237 sec 9.0 × 103/5 sec CM(19) 2.3 × 107/220 min 2.4 × 105/134 sec CM(21) —— 8.5 × 106/80min CM(23) —— 2.8 × 108/43hours CM(25) —— 9.8 × 109/ 63 days (estimate) A number of results reported in this paper are new. While the num- bers have already been given elsewhere in the paper, we now give a table summarizing these results. Problem Set Our results Note 1. CM(n) n =19∼ 23 CM(n)=0forn ≡ 0(mod2) ∼ ≡ 2. QR90◦ (n) n =49 61 QR90◦ (n)=0forn 2, 3(mod4) 4. CMR(n) n =29 CMR(n)=0forn ≡ 0(mod2) 4. CMA(n) n =1∼ 49 CMA(n)=0forn ≡ 0, 2, 4, 5(mod6) ∼ ≡ 4. CMR180◦ (n) n =1 37 CMR180◦ (n)=0forn 0(mod2) As another table, we list the largest number that we achieved in each series, together with the computing time. Problem Value Megacycles P4 1.8G CM(23) 19686730313955 2.8 × 108 43 hours 8 CMR(29) 1317606101 1.1 × 10 17 hours 8 CMA(49) 6567620752 1.9 × 10 30 hours × 9 CMR180◦ (37) 131777883431119 1.5 10 10 days × 8 QR90◦ (61) 291826098503680 2.1 10 33 hours The binary of our program is publically available at http://turing.csie.ntu.edu.tw/arping/cm, together with a program that transforms the problems indicated in this paper to propositional expressions so that other researchers can test their own ATP systems. 19 References [1] http://www.research.att.com/∼njas/sequences/. [2] B. A. Anderson, Sequencings and houses, Congr. Numer., 43 (1984), pp. 23–43. [3] Anonymous, Unknown, Berliner Schachgesellschaft, 3 (1848), p. 363. [4] W. W. R. Ball., Mathematical Recreations and Essays, MacMillan and Co., 1926, p. 113. [5] R. C. Bose, I. M. 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Keedwell, Generalized complete mappings, neofields, sequenceable groups and block designs II,PacificJ.ofMath., 117 (1985), pp. 291–312. [13] G. S. Huang, Search Reduction Techniques and Applications to Prob- lems in Combinatorics, PhD thesis, National Taiwan University, 1999. 20 [14] D. M. Johnson, A. L. Dulmage, and N. S. Mendelsohn, Ortho- morphisms of groups and orthogonal Latin squares I, Canad. J. Math., 13 (1961), pp. 356–372. [15] H. B. Mann, The construction of orthogonal Latin squares, Ann. Math. Statistics, 13 (1942), pp. 418–423. [16] H. Niederreiter and K. H. Robinson, Complete mappings of finite fields, J. Austral. Math. Soc. Ser. A, 33 (1982), pp. 197–212. [17] A. T. Olson., The eight queens problem, Journal of Computers in Mathematics and Science Teaching, 12, pp. 93–102. [18] L. J. Paige, A note on finite abelian groups, Bull. Amer. Math. Soc., 53 (1947), pp. 590–593. [19] , Complete mappings of finite groups, Pacific J. Math., 1 (1951), pp. 111–116. [20] G. Polya´ , Uber die ’doppelt-periodischen’ Losungen des n-Damen- Problems, Mathematische Unterhaltungen und Spiele., (1918), pp. 364– 374. [21] I. Rivin, I. Vardi, and P. Zimmermann, The n-queens problem, vol. 101 of Amer. Math. Monthly, 1994, pp. 629–639. [22] Y. Shieh, Partition Strategies for #P-Complete Problem with Appli- cations to Enumerative Combinatorics, PhD thesis, National Taiwan University, 2001. [23] Y. P. Shieh, J. Hsiang, and D. F. Hsu, On the enumeration of abelian k-complete mappings, vol. 144 of Congressus Numerantium, 2000, pp. 67–88. [24] J. Singer, A class of groups associated with Latin squares,Amer. Math. Monthly, 67 (1960), pp. 235–240. [25] A. Yaglom and I. Yaglom, Challenging Mathematical Problems with Elementary Solutions, Holden-Day, 1964, pp. 76–101. 21 A Benchmark Template for Substructural Logics John Slaney Computer Sciences Laboratory The Australian National University Canberra, ACT, Australia [email protected] June 4, 2002 Abstract This paper suggests a benchmark template for non-classical proposi- tional reasoning systems, based on work done some twenty years ago in the investigation of relevant logic. The idea is simple: generate non-equivalent binary operations in the language of the logic and use an automated rea- soning system to decide which ones satisfy given algebraic properties. Of course, problem classes generated in this way are not in any sense uni- formly distributed: indeed, they are highly structured and have special features such as a low ratio of variables to length. Nonetheless, they have the character of theorem proving “in the field”, and should be part of the evaluation equipment for systems dealing with a wide range of nonclassical logics. 1 Substructural reasoning: the impossible takes a little longer This paper is a response to an implicit challenge in the description of this work- shop: ‘As the use of ATP systems expands to harder problems and new domains, it is important to place new problems and problem types in public view. . . ‘There will be no limitation to classical logics { problems and prob- lem sets in other logics, e.g., modal and relevance logics, are of in- terest. . . ’ PaPS 2002 CFP My rst recommendation to the automated reasoning community, addressed especially to those of its members with interests in non-classical logics, is to work on automating inference in a family of substructural logics which includes 1 linear logic, the relevant logics, Lambek’s associative calculus, a ne logic and others. This is not merely a wish that more logicians and more system builders would share my enthusiasm for these logics. They are of independent interest for their applications (well-rehearsed in the case of linear logic, but also present in other cases|see [7] for an account and many entry points into the literature) and call for a community e ort similar to that which has gone into SAT solving for classical logic, and more recently into modal and temporal logics. Automated theorem proving for some such substructural systems is enor- mously hard [13, 5]|indeed, some of the propositional systems such as linear logic and the original Anderson-Belnap relevant logics are undecidable|and proof search in those logics is quite di erent from what is classically familiar, so directing some of the e ort of system developers into the deduction and deci- sion problems for these logics is itself a goal in line with the sentiment expressed above. I also believe that the step up in richness as we move from classical to substructural reasoning will lead us to devise new algorithms and heuristics which will ultimately feed back into the rest of what we do. Certainly, it leads us to think di erently in some respects: while boolean 3-SAT problems with several hundred variables are routine fare for modern solvers, there are tough decision questions for formulae of relevant logic which t on one line of a page and contain only 3 variables. So the change of perspective is good for us, and anyway climbing fresh mountains is excellent exercise. However, the literature lacks good benchmarks for automated reasoning of this type. A major reason for this is that there is little uniformity across the canvassed range of non-classical systems: what is trivial given the proof mechanisms of one logic may be a severe test for those of another. The challenge raised by the Call for Papers, therefore, is to devise a benchmark template which can deliver worthwhile problem sets for a vast range of propositional logics, with various sets of connectives and no uniform features such as normal forms either for formulae or for inferences. 2 Logics In order to sharpen the goal a little, it is necessary to delineate the class of logics for which the technique is intended to work. Therefore, let logic L be a formal system built up as follows. There is a denumerable set P of basic propositions (or \propositional variables") and a nite set C of nitary connectives. The basic propositions and nullary connectives (\constants") make up the set A of atoms. For c ∈ C, let A(c) be the adicity (or \arity") of c. The set F of formulae is de ned as usual: F = P | c(F A(c)), c ∈ C To sharpen still further, we are especially interested in a class of substructural logics in the vicinity of linear logic. Their connectives include the constants t, f, > and ⊥, negation ¬, conjunction and disjunction ∧ and ∨ , their intensional counterparts fusion and ssion ◦ and +, and implication operators → and ←. Other connectives such as modalities (the \exponentials" of linear logic) may 2 be added, as is done for the example in Section 6 below, but for the purposes of this introduction we omit them. So the language of these systems is A = P | t | f | > | ⊥ F = A | ¬F | F ∧ F | F ∨ F | F ◦ F | F +F | F →F | F ←F Next, since L is supposed to be a propositional logic, it should be a theory about what follows from what in virtue of properties of the connectives. Hence there is some notion of implication intended to capture the validity of inferences in L. That is, there are structures of some kind built up out of the formulae|the structures may be simply sets as in classical and intuitionist logic, or multisets as in linear logic, or sequences as in the Lambek associative calculus, or more exotic objects such as trees with several di erent labelled branching operations, as in display logic for instance. Then there is a relation ` between structures, satisfying some conditions related to deducibility|classically, enough conditions to make it a consequence relation in the Gentzen-Tarski sense, but in the general setting perhaps some weaker analogue of those. In the particularly intended logics, the structures are binary trees. and the implication relation is that given in Appendix A. For linear logic, the trees can be \ attened" into multisets by adding structural rules of associativity and commutativity. One e ect of this is identify the two implication connectives. For the relevant logic LR, add to linear logic the left and right rules of contraction: