By H. Crapo (auth.), H. Crapo, D. Senato (eds.)
This booklet, devoted to the reminiscence of Gian-Carlo Rota, is the results of a collaborative attempt by way of his neighbors, scholars and admirers. Rota was once one of many nice thinkers of our occasions, innovator in either arithmetic and phenomenology. i believe moved, but touched by way of a feeling of disappointment, in offering this quantity of labor, regardless of the phobia that i'll be unworthy of the duty that befalls me. Rota, either the scientist and the fellow, was once marked by way of a generosity that knew no bounds. His principles opened extensive the horizons of fields of study, allowing an striking variety of scholars from all around the globe to turn into enthusiastically concerned. The contagious strength with which he confirmed his great psychological capability continually proved clean and encouraging. past his renown as proficient scientist, what used to be rather outstanding in Gian-Carlo Rota was once his skill to understand the various highbrow capacities of these earlier than him and to conform his communications for that reason. This human experience, complemented by way of his acute appreciation of the significance of the person, acted as a catalyst in bringing forth some of the best in every one of his scholars. Whosoever was once lucky sufficient to get pleasure from Gian-Carlo Rota's longstanding friendship was once such a lot enriched via the event, either mathematically and philosophically, and had celebration to understand son cote de bon vivant. The booklet opens with a heartfelt piece through Henry Crapo within which he meticulously items jointly what Gian-Carlo Rota's premature death has bequeathed to science.
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Additional resources for Algebraic Combinatorics and Computer Science: A Tribute to Gian-Carlo Rota
Again, we say that two polynomials p(x) and q(x) are apolar when A(q(x), p(x» is identically zero, that is, zero for all x. Theorem 1 remains valid as stated. That is, if q(r) = 0, then the polynomial p(x) = (x - r)n is apolar to q(x). Let us consider a special case. Suppose that q(x) is a quadratic polynomial and p(x) is a cubic polynomial: q(x) = x 2 + 2blx + b2 and Then we have, in umbral notation, A(q(x), p(x» ~ (f3 - a)2(x - a) = (f32 - 2af3 + ( 2)x - af32 + 2a 2f3 - a 2. Evaluating the linear functional E, we obtain the following explicit expression for the apolar invariant: + ( 2)x - af32 + 2a 2f3 - ( 2) E (f32) - 2E (af3) + E (a 2)x + E (-af32) + 2E (a 2f3) - E (a 2) E(f32) - 2E(a)E(f3) + E(a 2)x + E(-a)E(f32) + 2E(a 2)E(f3) (b2 - 2albl + a2)x - alb2 + 2a2bl - a3· A(q(x), p(x» = E«f32 - 2af3 E(a 2) What is invariant theory, really?
So I went back to my fantasies and I began to fantasize on the probable topics that other possible candidates on the list of Fubini lectures, past and future, might have chosen. I imagined a brilliant young mathematician, eager to establish himself as a leader in his field, delivering one single dazzling proof beginning with the first Fubini lecture and lasting all the way to the end of the fifth. Or else, some middleaged mathematician, anxious to have his latest theory accepted by the mathematical world, delivering to a thrilled audience a five-hour condensation of material that would normally take an entire term in an advanced graduate course.
Let us consider functions of three variables, such as f(XI, X2, X3). Two wellknown classes of functions of three variables are symmetric functions, defined to satisfy the equations fs(XI,X2,X3) = fs(Xil,Xi2,Xi3) for every permutation sending the indices (l, 2, 3) to (i I, i2, i3), and skew-symmetric functions, defined by the equations fa (XI, X2, X3) = ±fa (Xii' Xi2' Xi3)' where the sign is + 1 or -1 according as the permutation sending the indices (1, 2, 3) to (iI, i2, i3) is even or odd. It is not true that a function of three variables is the sum of a symmetric function and a skew-symmetric function.