{"docId":1317,"paperId":1317,"url":"https:\/\/hrj.episciences.org\/1317","doi":"10.46298\/hrj.2014.1317","journalName":"Hardy-Ramanujan Journal","issn":"","eissn":"2804-7370","volume":[{"vid":50,"name":"Volume 37 - 2014"}],"section":[],"repositoryName":"Hal","repositoryIdentifier":"hal-01220303","repositoryVersion":1,"repositoryLink":"https:\/\/hal.archives-ouvertes.fr\/hal-01220303v1","dateSubmitted":"2015-10-30 09:41:00","dateAccepted":"2015-10-30 09:41:00","datePublished":"2014-01-01 08:00:00","titles":{"en":"On the Galois groups of generalized Laguerre Polynomials"},"authors":["Laishram, Shanta"],"abstracts":{"en":"For a positive integer n and a real number \u03b1, the generalized Laguerre polynomials are defined by L (\u03b1) n (x) = n j=0 (n + \u03b1)(n \u2212 1 + \u03b1) \u00b7 \u00b7 \u00b7 (j + 1 + \u03b1)(\u2212x) j j!(n \u2212 j)!. These orthogonal polynomials are solutions to Laguerre's Differential Equation which arises in the treatment of the harmonic oscillator in quantum mechanics. Schur studied these Laguerre polynomials for their interesting algebraic properties. In this short article, it is shown that the Galois groups of Laguerre polynomials L(\u03b1)(x) is Sn with \u03b1 \u2208 {\u00b11,\u00b11,\u00b12,\u00b11,\u00b13} except when (\u03b1,n) \u2208 {(1,2),(\u22122,11),(2,7)}. The proof is based on ideas of p\u2212adic Newton polygons."},"keywords":[{"en":" Laguerre Polynomials"},{"en":" Primes"},{"en":" Arithmetic Progressions"},{"en":" Newton Polygons"},{"en":"Irreducibility"},"[MATH] Mathematics [math]","[MATH.MATH-NT] Mathematics [math]\/Number Theory [math.NT]"]}