<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">AM</journal-id><journal-title-group><journal-title>Applied Mathematics</journal-title></journal-title-group><issn pub-type="epub">2152-7385</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/am.2013.47A004</article-id><article-id pub-id-type="publisher-id">AM-33983</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Generalized Powers of Substitution with Pre-Function Operators
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>aurent</surname><given-names>Poinsot</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>University Paris 13, Paris Sorbonne Cité, LIPN, CNRS, Villetaneuse, France</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>laurent.poinsot@lipn.univ-paris13.fr</email></corresp></author-notes><pub-date pub-type="epub"><day>04</day><month>07</month><year>2013</year></pub-date><volume>04</volume><issue>07</issue><fpage>12</fpage><lpage>17</lpage><history><date date-type="received"><day>April</day>	<month>13,</month>	<year>2013</year></date><date date-type="rev-recd"><day>May</day>	<month>13,</month>	<year>2013</year>	</date><date date-type="accepted"><day>May</day>	<month>20,</month>	<year>2013</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p><html>
 <head></head>
 
   An operator on formal power series of the form <em>S</em> <img alt="" src="Edit_2e9ead22-c8af-4903-8709-f3231d46573c.bmp" /> <em>μS</em> , where <em>μ</em> is an invertible power series, and  σ is a series of the form t+<img alt="" src="Edit_fce1af4a-6c0e-4c4e-9ef6-17cccbe9abe8.bmp" />（t<sup>2</sup>） is called a unipotent substitution with pre-function. Such operators, denoted by a pair (<em>μ </em>，σ ）  , form a group. The objective of this contribution is to show that it is possible to define a generalized powers for such operators, as for instance fractional powers <img alt="" src="Edit_f46f03a5-0468-44ab-a37e-2c056cb90d92.bmp" />σ for every<img alt="" src="Edit_81b10fa6-109b-429a-ac75-d1923fa40a98.bmp" /> . 
 
</html></p></abstract><kwd-group><kwd>Formal Power Series; Formal Substitution; Riordan Group; Generalized Powers; Sheffer Sequences; Umbral Calculus</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Substitution of Formal Power Series</title><p>In this contribution we let <img src="4-7401480\81e3fc97-5d46-4faa-8b5c-0f220ba6e8dd.jpg" /> denote any field of characteristic zero. We recall some basic definitions from [1,2]. The algebra of formal power series in the variable <img src="4-7401480\0ce9fee1-bba4-4e3a-a81f-c700d200a62b.jpg" /> is denoted by<img src="4-7401480\2691c913-88bf-4082-9009-eb8ea0398fac.jpg" />. In what follows we sometimes use the notation <img src="4-7401480\ea3b8a49-004d-40ae-aa0d-b7a6ab0be06b.jpg" /> for <img src="4-7401480\80b22ec0-059f-4a9c-bfcb-05205411d453.jpg" /> to mean that <img src="4-7401480\b660386b-1e3d-4e7e-82a5-53ede4d0e361.jpg" /></p><p>is a formal power series of the variable t. We recall that any formal power series of the form <img src="4-7401480\e655a505-cb52-4be4-919d-88d42078812c.jpg" /> for</p><p><img src="4-7401480\f208eed2-a803-4d27-aca6-dcec5f95a61c.jpg" />and <img src="4-7401480\e844f4ce-8f8c-492c-abfe-2dcf5d065e75.jpg" /> is invertible with respect to the usual product of series. Its inverse is denoted by <img src="4-7401480\ba09eb8f-3c36-4be6-a173-1babcd021d08.jpg" /> and has the form <img src="4-7401480\9b855a9c-ca77-499d-ae3d-69612bcd41fa.jpg" /> for some<img src="4-7401480\32481b48-53d0-4b6e-8cb0-0e5a437556e7.jpg" />. In particular, the set of all series of the form <img src="4-7401480\a51933a4-33d6-42a4-bef8-17e8e647f44a.jpg" /> forms a group under multiplication, called the group of unipotent series. For a series of the form<img src="4-7401480\3d32a808-404a-47da-a9f9-af9928a737ab.jpg" />we may define for any other series <img src="4-7401480\75bb6b7e-2e6b-49e1-ae9f-7dfd991c8318.jpg" /> an operation of substitution given by<img src="4-7401480\c2a482df-f404-41e4-ad76-2ea38bffe494.jpg" />. A unipotent substitution is a series of the form<img src="4-7401480\963d385d-1d23-4d8d-8fb1-75b33fb6d9cc.jpg" />. Such series form a group under the operation of substitution, called the group of unipotent substitutions (whenever<img src="4-7401480\fe8da266-a6d2-41cc-9ec2-3ccd26917e81.jpg" />, a series <img src="4-7401480\44c1d470-953e-4b42-9a61-c9a9eaa0cc06.jpg" /> is invertible under substitution, and the totality of such series forms a group under the operation of substitution called the group of substutions, and it is clear that the group of unipotent substitutions is a sub-group of this one). The inverse of <img src="4-7401480\589e6807-fef2-4b94-917f-53be6a5b867d.jpg" /> is then denoted by <img src="4-7401480\526ad8ce-2e49-4678-af41-ad63c324b0a6.jpg" /> and satisfies</p><p><img src="4-7401480\1c6c7bb3-e7e0-4e1d-a9cf-bff112d00963.jpg" />. Finally, it is possible to define a semi-direct product of groups by considering pairs <img src="4-7401480\88396643-70d5-462b-97e1-dc2ab72fcb07.jpg" /> where <img src="4-7401480\69dd541f-8010-41f4-ae00-813596168642.jpg" /> is a unipotent series, and <img src="4-7401480\a772f992-81ef-406c-9c02-e58d278411ca.jpg" /> is a unipotent substitution, and the operation <img src="4-7401480\222d4294-04b2-461e-9ada-7d23a982caa2.jpg" /></p><p><img src="4-7401480\4c3e98f4-f946-4ece-b921-3b109bcfd1f8.jpg" />. The identity element is</p><p><img src="4-7401480\58b76794-3295-4369-8748-0b69df82a65d.jpg" />. This group has been previously studied in [3-5], and is called the group of (unipotent) substitutions with pre-function. These substitutions with pre-function act on <img src="4-7401480\e493a8e2-b4f5-45a5-8b18-bee2be9c6c10.jpg" /> as follows: <img src="4-7401480\bf155afb-cac0-406d-ae2a-fabef71d076f.jpg" />for every series<img src="4-7401480\6be6f079-c6f6-4985-90c0-c7161526de09.jpg" />. In [<xref ref-type="bibr" rid="scirp.33983-ref3">3</xref>] is associated a doubly-infinite matrix <img src="4-7401480\8794c0b0-f802-44dc-9c4a-76a386cb38e5.jpg" /> to each such operator which defines a matrix representation of the group of substitutions with prefunction, and it is proved that there exists a oneparameter sub-group<img src="4-7401480\3624f7fe-24da-4a82-a08f-0450563a98c4.jpg" />. Therefore, it satisfies <img src="4-7401480\de0af0c6-e2f0-4194-b494-1a8f238a9244.jpg" /> for every<img src="4-7401480\60ea47f2-f84f-47ac-ab9b-531f396ff506.jpg" />, and</p><p><img src="4-7401480\28b58bf5-6040-482d-98dc-2828a2812a5c.jpg" />is the usual <img src="4-7401480\d06a9440-0f76-4e82-b281-ec4950ca4a1c.jpg" />-th power of <img src="4-7401480\7d3961ca-009e-48cc-8ed0-b14046014209.jpg" /> whenever</p><p><img src="4-7401480\a472d207-bb70-4026-828e-707e43b113ad.jpg" />is an integer. It amounts that for every<img src="4-7401480\77fa579f-a29c-4d1b-bea5-320630e64a03.jpg" />, <img src="4-7401480\62d7aca8-386c-43b6-af8a-accca7d567ff.jpg" />is the matrix representation of a substitution with prefunction say <img src="4-7401480\9927d6e6-79e6-4811-8883-3e099b594ff8.jpg" /> so that<img src="4-7401480\65e8a651-4519-4a31-8692-33b9a31a4b9f.jpg" />. The authors of [<xref ref-type="bibr" rid="scirp.33983-ref3">3</xref>] then define<img src="4-7401480\40531b75-7ec5-4b05-aba7-3a52e9b9f8d7.jpg" />. Actually in [<xref ref-type="bibr" rid="scirp.33983-ref3">3</xref>] no formal proof is given for the existence of such generalized powers for matrices or unipotent substitutions with pre-function.</p><p>In this contribution, we provide a combinatorial proof for the existence of these generalized powers for unipotent substitutions with pre-function, and we show that this even forms a one-parameter sub-group. To achieve this objective we use some ingredients well-known in combinatorics such as delta operators, Sheffer sequences and umbral composition which are briefly presented in what follows (Sections 2, 3, 4 and 5). The Section 6 contains the proof of our result.</p></sec><sec id="s2"><title>2. Differential and Delta Operators, and Their Associated Polynomial Sequences</title><p>By operator we mean a linear endomorphism of the <img src="4-7401480\5b7a05c4-8f6c-46c5-9b63-6370e4f7d569.jpg" />-vector space of polynomials <img src="4-7401480\8aaca731-4fde-47ce-a1ab-a8a6e8e0228b.jpg" /> (in one indeterminate<img src="4-7401480\9e1c84d5-1c2e-44e4-bad6-d32dd31e913e.jpg" />). The composition of operators is denoted by a simple juxtaposition. If<img src="4-7401480\f9da988e-0651-4da5-be18-81a9060b99f2.jpg" />, then we sometimes write <img src="4-7401480\a761a1e1-1358-4683-90a9-8de386f60c44.jpg" /> to mean that <img src="4-7401480\be2134b8-647d-4823-9ea5-b9f566a60bd4.jpg" /> is a polynomial in the variable<img src="4-7401480\dab57fac-e8a0-46b7-b421-12812bd97076.jpg" />.</p><p>Let <img src="4-7401480\725e6054-f8f0-4a3e-af78-22aa87a863af.jpg" /> be a sequence of polynomials.</p><p>It is called a polynomial sequence if <img src="4-7401480\fe799aae-2250-4596-8612-2524cc869f09.jpg" /> for every <img src="4-7401480\6b62a472-4c92-43ef-97cf-1c0945515867.jpg" /> (in particular,<img src="4-7401480\8fe8d4b5-6030-4e2d-a763-8205ba499bc9.jpg" />). It is clear that a polynomial sequence is thus a basis for<img src="4-7401480\1673db3f-5c64-47f8-978a-8fd93cd7d8ab.jpg" />.</p><p>An operator <img src="4-7401480\ade17994-6797-4e31-aebf-7078c831b890.jpg" /> is called a differential operator (see [<xref ref-type="bibr" rid="scirp.33983-ref6">6</xref>]) if 1) <img src="4-7401480\0c8c5052-6d79-4d62-b795-994774078152.jpg" />for every<img src="4-7401480\54da7e78-4c00-4430-a39b-643ecd5888fd.jpg" />.</p><p>2) <img src="4-7401480\c7b72f48-8e9d-4e44-9c09-1890d9231667.jpg" />for every non-constant polynomial<img src="4-7401480\7b4284f5-5f80-4524-a304-748caaa25766.jpg" />.</p><p>For instance, the usual derivation <img src="4-7401480\1bff46bf-1819-486c-b0ea-a7f9572d8782.jpg" /> of polynomials is a differential operator. Moreover, let<img src="4-7401480\07c69a84-d54e-47a1-a8d7-14808ac05800.jpg" />, and let us define the shift-invariant operator <img src="4-7401480\68daccd3-26e6-42fd-8e28-c5bda0a71d31.jpg" /> as the unique linear map such that <img src="4-7401480\03090150-2af0-405e-8b0e-014db83b3ced.jpg" /> for every<img src="4-7401480\013f38af-9f26-474f-b135-e7f173bc8b39.jpg" />. Then, <img src="4-7401480\02ab605d-5842-4cdc-81ee-21218af8d1ba.jpg" />is also a differential operator.</p><p>A polynomial sequence <img src="4-7401480\a635e461-2857-4a43-a135-cfeb87424c9c.jpg" /> is said to be a normal family if 1)<img src="4-7401480\c54409cc-cf6c-486c-8c68-a0016a8231c9.jpg" />.</p><p>2) <img src="4-7401480\5e413770-d254-42a4-892f-b2afd637d742.jpg" />for every<img src="4-7401480\eccf040a-b876-4230-9f14-229f209a69df.jpg" />.</p><p>Let <img src="4-7401480\bd25983d-6606-4ce5-a992-e3f855160ead.jpg" /> be a differential operator. A normal family <img src="4-7401480\cae21f68-4967-4c6b-9dbb-71c4e3f9a989.jpg" /> is said to be a basic family for <img src="4-7401480\2d55e3c8-a2c7-470a-8318-dfe8c03d32e8.jpg" /> if</p><p><img src="4-7401480\0a1db03e-f8ca-4ecc-949e-4ac099fa2f01.jpg" /></p><p>for every<img src="4-7401480\43767a8a-602e-4fb3-a39a-9ca45b2f8a3b.jpg" />. It is proved in [<xref ref-type="bibr" rid="scirp.33983-ref6">6</xref>] that for any differential operator admits is one and only one basic family, and, conversely, any normal family is the basic family of a unique differential operator. As an example, the normal family <img src="4-7401480\89583333-cfe3-4239-8c02-1264e5edf92b.jpg" /> is the basic family of<img src="4-7401480\394a258a-58df-4f85-84d5-28992144a8af.jpg" />.</p><p>Let <img src="4-7401480\97452d27-f0a9-4891-ab8b-f5120f5e2799.jpg" /> be an operator such that for every non-zero polynomial<img src="4-7401480\92b598e5-e879-4274-a0b6-9d0cbd81d574.jpg" />, <img src="4-7401480\5a4227cb-601e-48c9-aae1-38431dbbf1c4.jpg" />(in particular, <img src="4-7401480\07840620-7926-4880-8cb8-e54da9e65ff4.jpg" />for every constant<img src="4-7401480\0f8694b6-c869-488a-9888-805cbdd21c89.jpg" />). Such an operator is called a lowering operator (see [<xref ref-type="bibr" rid="scirp.33983-ref7">7</xref>]). For instance any differential operator is a lowering operator. Then given a lowering operator<img src="4-7401480\7baaefea-541f-46c0-9845-e1d22436cac1.jpg" />, we may consider the algebra of formal power series <img src="4-7401480\d7b520eb-776b-4042-9d7a-1f69547e78fb.jpg" /> of operators of the form <img src="4-7401480\0f4a7059-4e66-42f8-adda-28ea4675f637.jpg" /> where <img src="4-7401480\582ce20b-9478-4981-81e2-b3ee90560abb.jpg" /> for every<img src="4-7401480\f4793a1f-3517-4096-b019-44e6f78628b2.jpg" />.</p><p>The series <img src="4-7401480\0236e58e-7588-4743-8a06-9f7f46b8106f.jpg" /> converges to an operator of</p><p><img src="4-7401480\4d1d4452-ada5-438b-8e9e-5f72150658a6.jpg" />in the topology of simple convergence (when <img src="4-7401480\280ddf1a-57d6-4494-8b01-07a04cc71cac.jpg" /> has the discrete topology) since for every<img src="4-7401480\9ab81db4-1f1b-4fef-ae59-13561288246f.jpg" />, there exists <img src="4-7401480\1956617d-21b6-4104-b85f-e43e9452a729.jpg" /> such that for all<img src="4-7401480\4a81ee66-06eb-4ef2-8d79-c7d9950603ab.jpg" />, <img src="4-7401480\b430607a-c7b4-4a26-a881-1b287f61f306.jpg" />, so that we may define</p><p><img src="4-7401480\abb96896-3100-4a08-9354-59549caaee05.jpg" /></p><p>According to [<xref ref-type="bibr" rid="scirp.33983-ref6">6</xref>], if <img src="4-7401480\fa74f04a-c141-442f-8916-429c4650523a.jpg" /> is a differential operator, then</p><p><img src="4-7401480\b3b47e4e-1df6-46c8-ae07-47b74366fb44.jpg" />if, and only if, <img src="4-7401480\48da3650-6403-450e-8ef6-5ac556f0eb0a.jpg" />commutes with<img src="4-7401480\03a8e10c-dcd9-4c0f-b732-15d5310ba8c2.jpg" />, i.e.,</p><p><img src="4-7401480\a3251296-4b56-45f6-be61-b50a1588bb27.jpg" />. Moreover, if<img src="4-7401480\7104c498-b27d-4eb6-92ae-ffd965239fbf.jpg" />, then</p><p><img src="4-7401480\0b90e71e-5ef0-458b-b38b-967fe335d012.jpg" />is also a differential operator if, and only if, <img src="4-7401480\11d9a0b7-8caf-4903-be5f-51ef2fb48b44.jpg" />and<img src="4-7401480\8914fc3c-a4f2-466e-b878-85e169a2c7c9.jpg" />.</p><p>Following [<xref ref-type="bibr" rid="scirp.33983-ref1">1</xref>], let us define a sequence of polynomials</p><p><img src="4-7401480\84ee54a9-a7dc-4f37-8ed5-64891d7df367.jpg" />by <img src="4-7401480\52cc87e0-bc4c-48f1-8447-aff1d915b160.jpg" /> and <img src="4-7401480\a9d68d4c-57f7-4ced-ad7c-96e5a7cb8272.jpg" /></p><p>for every integer<img src="4-7401480\7832ae1b-2aa4-4a4e-bd16-4a555f54443f.jpg" />. For<img src="4-7401480\4f2a8912-1bde-43af-82ac-560172367ec5.jpg" />, we denote by <img src="4-7401480\3a2146ad-cfac-4b1c-b68a-3329b57a575d.jpg" /> the value of the polynomial <img src="4-7401480\015047f9-eb8a-4e1f-8e63-1f256a057a5e.jpg" /> for<img src="4-7401480\bee580aa-714f-4f3e-a431-e8b160b7464a.jpg" />. Let <img src="4-7401480\7a754e75-683b-4338-8caf-6848e984906f.jpg" /> be a lowering operator, and let <img src="4-7401480\631bc15e-5b32-468b-8abb-31545ff88450.jpg" /> be its unipotent part. Then we may consider generalized power</p><p><img src="4-7401480\56c69602-4f48-437e-8f3d-1738eec7e491.jpg" />(in particular, this explains the notation <img src="4-7401480\79a0878d-30d0-4dbe-ae53-bdfe573b69f9.jpg" /> for the shift operator). We observe that for every integer<img src="4-7401480\dd0bdab2-521f-4f9e-b3dd-f97f75ad273d.jpg" />, <img src="4-7401480\35e205f0-10c0-42ee-981b-a3e28c33c774.jpg" />really coincides to the <img src="4-7401480\c8b64211-f900-4a51-9617-18ac27514dda.jpg" />-th power <img src="4-7401480\deaa4e8e-50ef-4b19-acac-9312a4d5e983.jpg" /> of<img src="4-7401480\20175317-ad61-4197-965d-dd758e43c703.jpg" />. Moreover, <img src="4-7401480\51aa738a-0505-4068-8535-42fe1a8cafa8.jpg" />for every<img src="4-7401480\9f577e1b-63e2-45cf-a5f1-7cdce94777ef.jpg" />. We may also form</p><p><img src="4-7401480\b920dc9b-59ed-4f33-815d-2e7a9729ec21.jpg" /></p><p>in such a way that for every<img src="4-7401480\f17cbe81-41a5-4225-ad96-af930810f719.jpg" />,</p><p><img src="4-7401480\dc226665-45aa-4606-8a24-cf36c0f578a0.jpg" /></p><p>where for every <img src="4-7401480\a3a7883b-e41e-4e63-98f2-3e1af7f305c8.jpg" /> with<img src="4-7401480\8830972e-6490-428b-a1f2-ae0d7046bb40.jpg" />, <img src="4-7401480\6cc37ca0-379e-45d0-aada-fa9e2750619f.jpg" />(it is a well-defined operator). This kind of generalized powers may be used to compute fractional power of the form <img src="4-7401480\f72c608f-f07e-426f-a2e8-79d5ccb30a0d.jpg" /> for every<img src="4-7401480\114c990e-4577-4de2-89e2-4bf24522b694.jpg" />, <img src="4-7401480\57e30df9-db81-4273-a44c-b793a1a42730.jpg" />(for instance,<img src="4-7401480\e01cbf72-af38-4cfe-856e-4653f3dd9398.jpg" />). They satisfy the usual properties of powers:<img src="4-7401480\7b038de2-0c17-4211-a1b2-4767169a938d.jpg" />,<img src="4-7401480\f3e9f51d-5e3f-4c90-9d8b-671db127a474.jpg" />. The objective of this contribution is to provide a proof of the existence of such generalized powers for unipotent substitutions with pre-function.</p><p>Following [<xref ref-type="bibr" rid="scirp.33983-ref8">8</xref>], we may consider the following sub-set of differential operators, called delta operators. A polynomial sequence <img src="4-7401480\e88091e1-7cf2-405d-a55a-3a99b4c709db.jpg" /> is said to be of binomial-type if for every<img src="4-7401480\0c294b91-cdd1-4756-a9bd-472d722151ea.jpg" />,</p><p><img src="4-7401480\e5dedafa-3dea-4f88-b495-9e668e333a7b.jpg" /></p><p>An operator <img src="4-7401480\f45beb6c-125b-4b06-8d72-edc9e591c28f.jpg" /> is a shift-invariant operator if for every<img src="4-7401480\e10cbb9f-fe71-4360-8976-c618b38506b4.jpg" />,<img src="4-7401480\c2854f68-819c-440b-ad50-a0d9cfc777d8.jpg" />. Now, a delta operator <img src="4-7401480\a37035ed-4d0f-48d5-817a-9ca17c89104b.jpg" /> is a shift invariant operator such that<img src="4-7401480\f0acbd35-c786-4480-8994-2588f29e6a49.jpg" />. For instance, the usual derivation <img src="4-7401480\152da427-f4b5-454f-bc8c-c7b11cf0b97e.jpg" /> of polynomials is a delta operator. It can be proved that a delta operator is a differential operator. The basic family (uniquely) associated to a delta operator is called its basic set. Moreover, the basic set of a delta operator is of binomial-type, and to any polynomial sequence of binomial-type is uniquely associated a delta operator. If <img src="4-7401480\57926a13-ace0-4fb0-80bd-aef27e6ad626.jpg" /> is a delta operator, then there exists a unique <img src="4-7401480\a1a37f0a-869a-4d67-b1a3-0111702bbad5.jpg" />-algebra isomorphism from <img src="4-7401480\56d992c5-65f7-4dfa-acd2-3dcda1e33d60.jpg" /> to the ring of shift-invariant operators <img src="4-7401480\850c3a5b-f75b-47b5-95c0-e3a3f496f8f8.jpg" /></p><p>that maps <img src="4-7401480\67f88e1a-45ae-4a1b-a810-c3ce9ef43e92.jpg" /> to<img src="4-7401480\713e488a-faec-419d-bc4b-ea90bcafc5f7.jpg" />. In [<xref ref-type="bibr" rid="scirp.33983-ref8">8</xref>]</p><p>is proved that given a delta operator<img src="4-7401480\f1ef653a-d4d9-4985-a3e3-a3912345ad90.jpg" />, and a series <img src="4-7401480\52a0c984-eec4-4ae2-8454-08009acfbf09.jpg" /> <img src="4-7401480\3ac011f8-e5b4-4403-83f5-b27ba0175645.jpg" /> with<img src="4-7401480\efd4c88f-a4b1-4325-b2db-c073aa37f4a5.jpg" />, then <img src="4-7401480\bf5b1e3e-c232-43e6-a532-69fb7ca824db.jpg" /> is also a delta operator. Conversely, if <img src="4-7401480\c56a1602-9fdf-46f3-84e9-e2d9be7c80e0.jpg" /> is a shift-invariant operator (so that<img src="4-7401480\3d6aa51e-aeb3-43e9-9be5-7818f14f463a.jpg" />), then if it is a delta operator, the unique series</p><p><img src="4-7401480\4230c893-d5fd-4875-a8ff-93f05a2f746d.jpg" /></p><p>such that <img src="4-7401480\993dc0bb-a0e6-4013-be7c-30aa42c2e332.jpg" /> satisfies <img src="4-7401480\e1c6870f-44e2-428b-a7e5-4902bcddb1ef.jpg" /> and<img src="4-7401480\33b1170c-7ebf-42f2-8cde-eef01a83cefc.jpg" />.</p></sec><sec id="s3"><title>3. Sheffer Sequences</title><p>In this section, we also briefly recall some definitions and results from [<xref ref-type="bibr" rid="scirp.33983-ref8">8</xref>].</p><p>Let <img src="4-7401480\828de58e-db0e-47da-bf63-293fa12b0b9c.jpg" /> be a sequence of polynomials in<img src="4-7401480\09ab7110-0de6-4bbe-8a51-ba66fd1dc2ee.jpg" />. We define the exponential generating function of <img src="4-7401480\2e6409b8-6792-4e94-b8a9-80297a0c9eee.jpg" /> as</p><p><img src="4-7401480\466e43ea-f2e2-4dba-91d9-875ed3c04dbe.jpg" /></p><p>Let <img src="4-7401480\f180356d-6c94-4bac-9d95-4ea2fe2714a2.jpg" /> be a delta operator and <img src="4-7401480\508ad79f-bb5f-4ab2-a570-c07aa23d74c6.jpg" /> be its basic set. Let <img src="4-7401480\ba3cfe33-d15e-4988-94fc-101245d2fbef.jpg" /> with <img src="4-7401480\d8f6e17e-19c3-4bfa-99f4-d8190c3d28e0.jpg" /> and <img src="4-7401480\334a1323-806d-4c02-b8f6-59a2110bd1d1.jpg" /> such that<img src="4-7401480\53715f56-45a4-4d21-a6f1-045bb20e7aa3.jpg" />. Then from [<xref ref-type="bibr" rid="scirp.33983-ref8">8</xref>],</p><p><img src="4-7401480\b3e2ee82-e756-4de0-9b0e-4ff49ebc5b50.jpg" /></p><p>A polynomial sequence <img src="4-7401480\9b5cff3d-cf88-48e4-b895-57a90c8c731f.jpg" /> is said to be a Sheffer sequence (also called a polynomial sequence of type zero in [<xref ref-type="bibr" rid="scirp.33983-ref9">9</xref>] or a poweroid in [<xref ref-type="bibr" rid="scirp.33983-ref10">10</xref>]) if there exists a delta operator <img src="4-7401480\d12882a9-b3a2-4a76-ab55-a1738e9e1879.jpg" /> such that 1)<img src="4-7401480\adb5cda6-c57c-4fb9-9947-2fb1afe165ea.jpg" />2) <img src="4-7401480\8cd841f9-3d39-454a-bf28-6e91b14c7c33.jpg" />for every<img src="4-7401480\c1d1fb3c-d829-44f3-9b8b-1c360271e133.jpg" />.</p><p>Following [<xref ref-type="bibr" rid="scirp.33983-ref9">9</xref>], a polynomial sequence <img src="4-7401480\82c34874-9a9d-437b-8179-f169158c21e6.jpg" /> is a Sheffer sequence if, and only if, there exists a pair <img src="4-7401480\c889018d-d1f8-46ce-ae68-7bbe3f79fd68.jpg" /> of formal power series in <img src="4-7401480\99a41b2c-0e6e-4777-bad0-88206ff3ed7d.jpg" /> with <img src="4-7401480\b694e019-842a-43b1-81a1-b3c75ce695b4.jpg" /> invertible, and<img src="4-7401480\c3b3649c-daa4-47ac-9258-9216ba49529e.jpg" />, <img src="4-7401480\a9d79505-2b23-4af5-be67-d96331c3ad6d.jpg" />, such that</p><p><img src="4-7401480\264a28e8-7162-4b21-b5cd-58c2f1f7e50a.jpg" /></p><p>Remark 1. The basic set of a delta operator <img src="4-7401480\8bb98884-1157-48e5-94d5-70ac455dbe3e.jpg" /> is a Sheffer sequence.</p><p>Let <img src="4-7401480\f79868f4-3de2-4575-9bdd-71c50f3b8195.jpg" /> be a delta-operator with basic set<img src="4-7401480\f877bf41-5dbc-425d-978e-2eafe7cc9c77.jpg" />. Following [<xref ref-type="bibr" rid="scirp.33983-ref8">8</xref>], the following result holds.</p><p>Proposition 1. A polynomial sequence <img src="4-7401480\60b7b0da-c9ac-4416-a779-05dcd8be6e86.jpg" /> is a Sheffer sequence if, and only if, there exists an invertible shift-invariant operator <img src="4-7401480\c4c90451-d433-4310-ba72-ae979fb3b02e.jpg" /> such that <img src="4-7401480\6f56bc27-f706-4e4b-9763-0490885ce6e1.jpg" /> for each<img src="4-7401480\d75b4c05-1fb4-462d-8a4b-e4ce30eb3596.jpg" />. Moreover, let <img src="4-7401480\6a61f1c7-2336-4fd4-b5cc-bb1603862e26.jpg" /> be an invertible shift-invariant operator. Let <img src="4-7401480\9ee86774-d1e5-4f8f-b19d-ae2f7ba9ee08.jpg" /> be the unique formal power series such that<img src="4-7401480\8dcae85f-f486-459a-9018-31018afbb9cd.jpg" />. Then, <img src="4-7401480\b6b9f3e2-9771-42b4-a2e8-04d6842a090c.jpg" />is invertible, and</p><p><img src="4-7401480\811225b9-6119-4c31-8491-56266eb7c0cd.jpg" /></p><p>where <img src="4-7401480\e7ddd44e-247f-4c68-a77a-f64a6f808977.jpg" /> is the Sheffer sequence defined by</p><p><img src="4-7401480\94853b71-4498-4079-ac70-28c460efe449.jpg" />for each<img src="4-7401480\b473175f-57ba-4f79-bb6c-2cd86b8cb0d5.jpg" />, and <img src="4-7401480\0af5973c-1090-4048-a59c-2a01c1af79b1.jpg" /> is the unique formal power series such that<img src="4-7401480\4b350720-a4bf-4d26-9bc1-a980e0a19f73.jpg" />. Finally we also have the following characterization.</p><p>Proposition 2. Let <img src="4-7401480\45c5dbfa-cc53-48ad-beec-9a08336a4619.jpg" /> be a polynomial sequence. It is a Sheffer sequence if, and only if, there exists a delta operator <img src="4-7401480\10da5c90-0e64-4b17-bc7a-a8065e47e589.jpg" /> with basic set <img src="4-7401480\e8cf6777-e0e3-4043-b84f-bdffe2c8e4f5.jpg" /> such that</p><p><img src="4-7401480\f1fd98c4-5e71-4341-82c3-c55a1fe974dd.jpg" /></p></sec><sec id="s4"><title>4. Umbral Composition</title><p>This section is based on [<xref ref-type="bibr" rid="scirp.33983-ref11">11</xref>].</p><p>Let <img src="4-7401480\f60a0246-29fe-4ff7-a636-20c1b6e8b210.jpg" /> be a fixed polynomial sequence. Let us define an operator <img src="4-7401480\75757688-1221-4cdf-a699-f2bba23b8b3b.jpg" /> by <img src="4-7401480\94263bfe-c7a0-46eb-a581-06c1850c5c24.jpg" /> for each<img src="4-7401480\9eec9f9c-203f-4d63-9704-5811d8d2530e.jpg" />.</p><p>Since <img src="4-7401480\e47a8aa4-c31c-4c61-bae7-944acb6f5ed7.jpg" /> is a basis of<img src="4-7401480\e07ff21d-ee8a-4c19-9d95-395f9b90e731.jpg" />, this means that <img src="4-7401480\28b2bdce-e16b-40f7-8cbc-133d00c2143d.jpg" /> is a linear isomorphism of<img src="4-7401480\bf158876-283d-45ac-b2a5-b7bf768b0f04.jpg" />. When <img src="4-7401480\6dcf5235-559c-4948-8e28-38cc776487ff.jpg" /> is the basic set of a delta operator, then <img src="4-7401480\dce33b0d-8864-4373-b355-1dd3da45c646.jpg" /> is referred to as an umbral operator, while if <img src="4-7401480\e0fb4122-a10d-43c5-847d-6680e692bdd4.jpg" /> is a Sheffer sequence, then <img src="4-7401480\8ed9d8a1-b92a-476a-a05d-cdd50b9240b2.jpg" /> is said to be a Sheffer operator. An umbral operator maps basic sets to basic sets, while a Sheffer operator maps Sheffer sequences to Sheffer sequences.</p><p>Let <img src="4-7401480\d30fcc41-2a7b-4e88-a077-fc99311a5192.jpg" /> be a polynomial sequence. For every<img src="4-7401480\b799dbae-b880-4c23-9fd4-ac3d9a48ecf4.jpg" />,</p><p><img src="4-7401480\cad0b253-5c67-44ca-a052-e0120150eba4.jpg" />where <img src="4-7401480\abeb1a56-aa04-483c-8a60-11f841e28ffb.jpg" /> is the coefficient of <img src="4-7401480\879f7dbb-5cb4-4fad-a91e-901ac348e5fa.jpg" /> in the polynomial<img src="4-7401480\945daa5f-c2f6-4b09-a65c-bde2632022f2.jpg" />. Let <img src="4-7401480\cf388514-ef03-40be-86bd-9b5f6e46db85.jpg" /> and <img src="4-7401480\854fe0da-4bdf-416f-9280-2b876f865f26.jpg" /> be two polynomial sequences. Their umbral composition is defined as the polynomial sequence <img src="4-7401480\c51933a5-d4c6-4bf0-92df-ffe26e43ca54.jpg" /> <img src="4-7401480\71f12974-125d-4bf6-877e-679574ef7221.jpg" /> defined by</p><p><img src="4-7401480\238a394d-3685-455c-ae26-de1ca18f3579.jpg" /></p><p>for each<img src="4-7401480\1aa57b7e-9784-4dac-9cd1-b36795497a44.jpg" />. By simple computations, it may be proved that<img src="4-7401480\6b9e5cf8-38dc-4be6-819e-bd9a0310185f.jpg" />. The set of all polynomial sequences becomes a (non-commutative) monoid under <img src="4-7401480\798def13-bbcc-48c4-8804-ff98aa6ea9c2.jpg" /> with <img src="4-7401480\88980935-190d-4465-89a2-e88c430612d6.jpg" /> as identity. We observe that if <img src="4-7401480\f8f4f128-66fb-4ebf-a9d9-e32422cfd51f.jpg" /> is the operator defined by <img src="4-7401480\18bad688-3472-413a-a99b-b97f593d627d.jpg" /> for each</p><p><img src="4-7401480\9ef388ff-be90-44c3-a7a6-0338461e8ba8.jpg" />, then<img src="4-7401480\ac443316-c8f4-440a-a0aa-87dc0a7bf189.jpg" />. More generally, we have <img src="4-7401480\a3a758c1-d6f1-42bd-93dd-df804fe364e0.jpg" /> where <img src="4-7401480\67fe1a86-d38a-4ed4-916e-a729f88c602c.jpg" /> is the</p><p><img src="4-7401480\421b9247-c336-47ee-a519-0217029afd13.jpg" />-th power of <img src="4-7401480\52a2f5ac-80b9-47ea-944f-79676d314b31.jpg" /> for the umbral composition (it is equal to a sequence say <img src="4-7401480\b8a7a765-7c6b-4fbd-8b25-0d38c09051d8.jpg" /> and we denote <img src="4-7401480\4531a2ab-2420-4ce1-9b86-9f533c5fcd83.jpg" /></p><p>by<img src="4-7401480\03cf582d-5e91-4768-9cf0-7fd22be6fcdf.jpg" />). Under umbral composition, the set of all Sheffer sequences is a (non-commutative) group, called the Sheffer group ([<xref ref-type="bibr" rid="scirp.33983-ref12">12</xref>]), and the set of all basic sequences is a sub-group of the Sheffer group.</p><p>From [<xref ref-type="bibr" rid="scirp.33983-ref8">8</xref>] we have the following result that combines delta operators, basis sets, Sheffer sequences and umbral composition.</p><p>Theorem 1. Let <img src="4-7401480\d93cd11c-f0a0-44e3-a5a6-b31c08fd4eb3.jpg" /> and <img src="4-7401480\a300fc79-8673-411b-8475-91f4d24cd706.jpg" /> be two delta operators with respective basic sets <img src="4-7401480\29ce4193-4f3a-4f39-b3cb-ae9b9d50de47.jpg" /> and<img src="4-7401480\90911284-25a8-4ba9-b64f-b0a0ff37f72e.jpg" />. Let <img src="4-7401480\140b3cf7-30cd-43bd-b85e-cf73de509191.jpg" /> and <img src="4-7401480\589c0baf-dd3f-4039-9a52-3883a20fa044.jpg" /> be two invertible shift-invariant operators. Let <img src="4-7401480\cc71c98b-dbc6-4e54-ad65-d879d7fb829a.jpg" /> and <img src="4-7401480\84e7c131-68d6-4999-84c9-a1a8c0ee868d.jpg" /> be the Sheffer sequences defined by <img src="4-7401480\c5fa5178-4a10-4b3c-851d-36807209709c.jpg" /> and <img src="4-7401480\1b476806-f143-46ad-bb14-9155976d3780.jpg" /> for each<img src="4-7401480\2fba96dc-f8cd-418c-8edd-813c561eb9a5.jpg" />. Let <img src="4-7401480\8ecfa819-d055-4cdd-8e3c-508d81d7ac00.jpg" /> be two invertible series such that<img src="4-7401480\e692f525-e80c-4652-8a29-681bb8984477.jpg" />,<img src="4-7401480\9821e6ce-6c89-4dc9-ac9f-e3f20f307080.jpg" />. Let <img src="4-7401480\ac30b832-b5f7-461a-85d8-49e16c8fcc63.jpg" /> be two formal power series with<img src="4-7401480\5cc6ef62-b4bc-4733-9440-00216ad590e5.jpg" />, <img src="4-7401480\9f629cc0-1ec2-4174-8b88-17a4e77c96dd.jpg" />such that <img src="4-7401480\b2fbc1ab-b4a9-4e7b-979a-209cf3d412ca.jpg" /> and<img src="4-7401480\3fc13558-c64e-4b27-be52-e88f5f9d1f16.jpg" />. Then,</p><p><img src="4-7401480\bfde6849-d36d-4021-afa1-b380a068cfed.jpg" />is a shift-invariant operator, <img src="4-7401480\9d5df030-31f5-4347-b85a-96fff3c5ee5c.jpg" />is a delta operator with basic sequence</p><p><img src="4-7401480\6de3fd31-d512-4a02-90fd-969dd9e169a2.jpg" />. Finally, let <img src="4-7401480\31b7fc4b-ebe0-4e87-877b-c7384d2d11e9.jpg" /> be the Sheffer sequence given by<img src="4-7401480\fee450ab-feaa-4a17-9c05-5d67621a6110.jpg" />. Then, <img src="4-7401480\20de3b23-7f74-4ddf-8cd4-5bb81ed9db9d.jpg" /></p><p>for each<img src="4-7401480\266ec3d4-34a0-4ec5-83f0-2d576470c46c.jpg" />.</p><p>It may be proved that if <img src="4-7401480\e5d554b8-f972-423c-bbe2-a12d0e3877ea.jpg" /> is the Sheffer sequence obtained from the delta operator <img src="4-7401480\e2bd9561-9f3c-4af7-a91b-88f7892eaf5c.jpg" /> with basic set <img src="4-7401480\8449c94c-0441-46b5-9b87-ee106d04edc7.jpg" /> and the invertible shift-invariant operator<img src="4-7401480\71b99195-c83a-4e2b-8e1d-d029130ce5e7.jpg" />, i.e., <img src="4-7401480\0cd2c993-843f-4bce-bb9a-06698910906e.jpg" />for each<img src="4-7401480\cee5be6f-cbef-4623-a3bf-99979c54083a.jpg" />, then the inverse</p><p><img src="4-7401480\2cca5147-ae51-40da-b6bd-d12bd7854b8f.jpg" />of <img src="4-7401480\e0824491-279b-47d6-89e1-0dcbb475847d.jpg" /> with respect to the umbral composition is the basic set of the delta operator<img src="4-7401480\a9f88429-bc87-4962-8dd1-b41e6c703211.jpg" />, the inverse</p><p><img src="4-7401480\e219a63f-377b-4161-b06e-b02422e146dd.jpg" />of <img src="4-7401480\033b2779-2f19-463e-90ba-2236725b1015.jpg" /> with respect to the umbral composition is the Sheffer sequence<img src="4-7401480\c258d42b-efcf-4a76-9531-6a90fd063b8a.jpg" />.</p></sec><sec id="s5"><title>5. Unipotent Sequences</title><p>The basic set <img src="4-7401480\f9bd08ae-7ad4-498c-9d71-ea121b4e0021.jpg" /> of a delta operator <img src="4-7401480\5028e374-2a9d-4e83-884e-37ad37e35e26.jpg" /> is said to be unipotent if the unique series <img src="4-7401480\5de6ca0c-f549-4291-873e-843e1c01db1d.jpg" /> such that <img src="4-7401480\a0af1e14-de5d-4cb5-9046-6ac7fb152a40.jpg" /> satisfies <img src="4-7401480\b71f63b0-5f56-4634-be40-7f9a48dd1c87.jpg" /> (and, obviously,<img src="4-7401480\649f238e-9895-456b-b2a8-ca8fd20470ca.jpg" />), i.e., <img src="4-7401480\3d59650e-412b-4272-bc92-888c29091fc5.jpg" />is a unipotent substitution. A Sheffer sequence <img src="4-7401480\642b95d9-31d1-49ee-9275-a3498af73b1d.jpg" /> associated to a delta operator <img src="4-7401480\bf56b1ce-0e0e-4a89-97a4-f06e47330a9b.jpg" /> (with<img src="4-7401480\4ab4e14c-80db-4624-a9e9-3bdab339d747.jpg" />,<img src="4-7401480\30551fe7-74df-46af-b003-bbbfad63ffcf.jpg" />) and an invertible shift-invariant operator <img src="4-7401480\2a6ae045-f5fa-4bee-99db-9289a75d0143.jpg" /> (with <img src="4-7401480\1f85f9bf-f7f0-4dea-8285-430d0954980e.jpg" /> invertible), i.e., <img src="4-7401480\432d1443-d7c5-4718-9a6f-64d8194c5e23.jpg" />for every <img src="4-7401480\7ab95eed-9c8c-41ce-8577-26baec5b448e.jpg" /> where <img src="4-7401480\216638f8-230d-44c1-8665-5b066ee22a8c.jpg" /> is the basic set of<img src="4-7401480\25723f41-86d0-4ea9-8dc6-434729b8d623.jpg" />, is said to be unipotent if <img src="4-7401480\ccecf94e-4774-46ae-9511-839916897793.jpg" /> is unipotent, and if <img src="4-7401480\d11355ad-a5c6-46ca-97ae-28ee45ecc66a.jpg" /> is unipotent, i.e.,<img src="4-7401480\d656024e-7772-445f-985d-b1c0533175b4.jpg" />. It is also clear from the previous section (theorem 4) that the (umbral) inverse of a unipotent basic set is unipotent, and the (umbral) inverse of a Sheffer sequence is also unipotent.</p><p>It is clear from theorem 4 that the group of basic sets under umbral composition is isomorphic to the group of substitutions. Moreover, the group of unipotent basic sets also is isomorphic to the group of unipotent substitutions. Likewise, the group of (unipotent) Sheffer sequences is isomorphic to the group of (unipotent) substitutions with pre-function (see also [<xref ref-type="bibr" rid="scirp.33983-ref12">12</xref>]).</p><p>Lemma 1. Let <img src="4-7401480\56687019-e698-4a7a-97e6-effc4c0374ae.jpg" /> be a substitution with prefunction, and let <img src="4-7401480\a10d53f5-3a0b-4c15-9100-167e8c4cda56.jpg" /> be the Sheffer sequence and the basic set associated to the delta operator <img src="4-7401480\79925d88-c5f5-4945-857c-639aa93f1d3d.jpg" /> and the invertible shift-invariant operator <img src="4-7401480\0255805c-f734-4667-b631-2b9fb7c510e0.jpg" /> (this means that <img src="4-7401480\750fb8e6-3a7a-4487-a17c-642aff8bb8fa.jpg" /> is the basic set of<img src="4-7401480\6c7c2441-8561-4fe9-bb3f-70ad9d8dafd6.jpg" />, and</p><p><img src="4-7401480\69abe5c5-de35-4fe9-86fd-7cc94393f8e0.jpg" />for each<img src="4-7401480\808c907d-2eb5-4cb3-84b4-9bdbf13e70eb.jpg" />). Then, <img src="4-7401480\98a82e06-16df-467a-a645-6b3b6a922b2f.jpg" />is a unipotent substitution with pre-function if, and only if, <img src="4-7401480\02568233-3a7e-4bde-be7a-12e3b348ce52.jpg" />for every<img src="4-7401480\2d49eb54-a612-4147-af6a-8b03e9883d25.jpg" />.</p><p>Proof. Let us first assume that <img src="4-7401480\b2f7f898-f384-453e-ad4b-d82ec42f6b87.jpg" /> is a unipotent substitution with prefunction. We have <img src="4-7401480\df99b75b-e896-4b31-be4c-2c3348e4cd60.jpg" /> for every basic set, so that<img src="4-7401480\8a4c035e-e829-4a41-9d47-82d220b5724d.jpg" />. Let<img src="4-7401480\a75bc3c7-e31d-484f-8659-43dbfadf8f29.jpg" />. We have</p><p><img src="4-7401480\7928f000-86c8-4866-ba3e-bafa6fdcc78d.jpg" />. Then, <img src="4-7401480\d3dcf882-e327-470c-92ce-7655947f3951.jpg" />is equivalent to</p><p><img src="4-7401480\9401ecce-770d-4505-a50e-b75564117124.jpg" />.</p><p>By identification of the coefficient of <img src="4-7401480\a9e8c7bb-d44b-4ff8-a2d5-35e66d33f671.jpg" /> on both sideswe obtain <img src="4-7401480\e02155d0-1900-4b22-a4b6-435540b03575.jpg" /></p><p>(since <img src="4-7401480\8fb587b4-d823-488a-8a02-0f95dd4680b6.jpg" /> is assumed to be a unipotent substitution), and, by induction,<img src="4-7401480\cc013b4c-9a9a-4261-b9e4-898ce2eadffb.jpg" />. Besides, we have</p><p><img src="4-7401480\9119f6be-8e29-41c6-bbe0-750e84db442b.jpg" />for each<img src="4-7401480\f7e074d1-4ca8-4f04-a58a-e3bb77dc2d06.jpg" />. But <img src="4-7401480\3415b41b-138e-4dd1-a212-71274509de29.jpg" /></p><p>(because there is a ring isomorphism between <img src="4-7401480\436995fb-2cfd-493a-9231-3df733c96041.jpg" /></p><p>and<img src="4-7401480\200364a4-e70b-4c1d-a8ac-cab9503eb24c.jpg" />), and<img src="4-7401480\73e546f2-c632-4066-be7d-dbb091723599.jpg" />, where<img src="4-7401480\c02d9e8f-1047-4c54-84d0-e127206f393c.jpg" />.</p><p>Then, by identification of the coefficient of<img src="4-7401480\3e53d78b-f184-4978-b54b-4888c8827a1f.jpg" />, we have</p><p><img src="4-7401480\f4877271-e086-4c1d-8df8-eaed96587b8b.jpg" />for every<img src="4-7401480\3076a311-4634-4b24-b717-7223e8e2ab37.jpg" />. Conversely, let us assume that <img src="4-7401480\828ac3d4-5bae-49ca-9d85-26af8212e8d5.jpg" /> is the Sheffer sequence and the basic set associated to the delta operator <img src="4-7401480\6d831828-886a-4b84-b3f0-f1a04d0b4a7f.jpg" /> and the invertible shift-invariant operator <img src="4-7401480\17e7492b-23dd-4166-817f-e3f42d7755bb.jpg" /> with</p><p><img src="4-7401480\d6f98054-1565-48a2-bc63-37f28c42e4a2.jpg" />for every<img src="4-7401480\351b70cb-8547-4dae-84db-a9d17e60eda5.jpg" />. By construction we have <img src="4-7401480\e5fea1bb-6783-425e-99bb-01b7defea7b2.jpg" /> so that<img src="4-7401480\9ae64d3e-9dd9-4b7c-a5b3-8b61dc35528e.jpg" />. Likewise, <img src="4-7401480\643e32d5-e959-42f2-81ec-92b6d07674c0.jpg" />, so that<img src="4-7401480\aa688ef8-8426-4c5d-9ae8-ed5abf3318fb.jpg" />. □</p></sec><sec id="s6"><title>6. Generalized Powers of Unipotent Substitutions with Pre-Function</title><p>The purpose of this section is to define <img src="4-7401480\c88e1930-5d39-4c7e-95b9-af933bc6dc00.jpg" /> for any <img src="4-7401480\544d27a7-2900-4284-86e9-3fbecadc9fc7.jpg" /> and any unipotent substitution with pre-function<img src="4-7401480\0e10ad40-ad2c-4c1a-995e-146f81fdde1a.jpg" />, and to prove that it is also a unipotent substitution with pre-function. Moreover we show that</p><p><img src="4-7401480\1354aebe-4175-44ad-80e6-d4faa08da305.jpg" />is a one-parameter sub-group, i.e.,</p><p><img src="4-7401480\930fe744-dcb0-4da0-9ec7-11ec11870654.jpg" />for every<img src="4-7401480\04da8483-c28a-49e5-8df0-a9b4c506b3a3.jpg" />, and<img src="4-7401480\63756ed0-d226-49e4-8e6d-1a37acbb2124.jpg" />.</p><p>Let <img src="4-7401480\0ab0d357-2906-4981-abd0-5950d815ae4c.jpg" /> be a unipotent substitution with prefunction of<img src="4-7401480\bbdda1ec-1ee6-4dce-bf18-d50402c85179.jpg" />. Let <img src="4-7401480\44857a2f-2c50-49aa-abdc-0610cc62d2cd.jpg" /> be the unipotent basic set of the (unipotent) delta operator<img src="4-7401480\f77040ac-d112-4d0a-8dfa-c802b2a71a45.jpg" />. Let <img src="4-7401480\95c49c29-70d5-4dce-b64b-41d3e2e6daa9.jpg" /></p><p>be the unipotent Sheffer sequence associated to <img src="4-7401480\81b30ee7-7d25-4afa-b32d-c075ce1d7464.jpg" /></p><p>and the (unipotent) invertible shift-invariant operator<img src="4-7401480\fca6fd57-ef3d-48b7-9bb2-985fd37a2a65.jpg" />. Let <img src="4-7401480\01222eec-422b-4083-81f2-17a30079ba14.jpg" /> be the umbral operator given by <img src="4-7401480\1fb33fee-5b26-43d4-9867-005ea55e3467.jpg" /> for all<img src="4-7401480\1a7b8a40-e2fc-451b-bfb3-5d00523c9a5e.jpg" />, and let <img src="4-7401480\c48cbc4b-24db-4218-8b32-7e390af6ffcb.jpg" /> be the Sheffer operator defined by <img src="4-7401480\8023e0d1-7a00-467a-aa20-3af5a5105126.jpg" /> for all<img src="4-7401480\db064b0a-05ad-47f1-9b63-4381baa1b23a.jpg" />. It is easily checked that for every integer<img src="4-7401480\c213ea05-3c67-46bf-954f-d88aba2da6a6.jpg" />, <img src="4-7401480\db3679d2-9a3f-4713-8d05-52b324c5791e.jpg" />and<img src="4-7401480\389f9cba-a634-4e68-904e-088d206f1e80.jpg" />. In particular, for each<img src="4-7401480\8d2f02b4-c7a5-4307-8245-ca614d24ee47.jpg" />, <img src="4-7401480\48e73ae1-191f-4932-bd02-3a394fc94acc.jpg" /></p><p>(by Lemma 5). Therefore, <img src="4-7401480\8ca563d7-667c-41da-83aa-1d63e5433539.jpg" />, where</p><p><img src="4-7401480\a357ee93-d93b-4b1f-90f1-5ab9fee9a80c.jpg" />for each<img src="4-7401480\ae0b9f38-3da7-4734-bd70-f5c98d1cd7d4.jpg" />. The operator <img src="4-7401480\c777f982-c71e-4164-bfd0-5bce56058fa4.jpg" /> is actually a lowering operator. Then according to section 2it is possible to define <img src="4-7401480\0281969e-4074-47e9-aa5d-91f854fa64e7.jpg" /> for every<img src="4-7401480\e02b56c3-42b4-4588-bda8-f378312a207e.jpg" />. Moreover, we have<img src="4-7401480\cbefc090-2fc7-4d09-a7a2-7383cf0eadd3.jpg" />.</p><p>For each<img src="4-7401480\f41deaf7-71eb-44ba-a701-7a82146884b7.jpg" />, let us define <img src="4-7401480\e32b6cfc-635f-4697-80d9-cf895c95eabd.jpg" /> for every<img src="4-7401480\87ac25df-81ab-445b-93e4-3964512fed2b.jpg" />. When<img src="4-7401480\e2d6f3b0-b8ad-41c1-b0a3-98d5cf230650.jpg" />, we have <img src="4-7401480\919f3692-25ca-4a08-9965-d3edd3a35ce7.jpg" /> <img src="4-7401480\0e968b17-7ab4-46d2-a347-28fad8f286af.jpg" />. So that in this case, <img src="4-7401480\f739140d-fcef-4a42-89c3-cc9320be0727.jpg" />is the unipotent Sheffer sequence associated to<img src="4-7401480\e73f1172-d0e3-46e2-810a-debf388d5766.jpg" />. This means that if<img src="4-7401480\53734133-d164-48b5-b04a-49e2897302dd.jpg" />, and <img src="4-7401480\4c611d80-c80e-407f-ae2c-9afea45009ab.jpg" /> is the unipotent basic set of the (unipotent) delta operator<img src="4-7401480\580928b6-6c5c-498d-afa8-3a6cd185bec4.jpg" />then <img src="4-7401480\1635dba5-1de7-4341-85cf-9cc5e5486252.jpg" /> for each<img src="4-7401480\ba016d24-e655-45bc-9be2-6d45935ed057.jpg" />. Similarly, let</p><p><img src="4-7401480\028f5d0e-1eef-4695-9799-1029895b7f4c.jpg" />for every<img src="4-7401480\22495432-c659-44ae-8bfb-deea7bcf8e91.jpg" />. Therefore, <img src="4-7401480\ac39c70f-722f-4419-8a8e-d1bae49e2cff.jpg" />, where <img src="4-7401480\92c4c14c-2789-41f2-b353-b44faeb6754d.jpg" /> is a lowering operator. Again for every<img src="4-7401480\0f039d07-99fc-4783-9f26-fc1c342245a8.jpg" />, we define</p><p><img src="4-7401480\4b0ef268-c0f1-44ae-aaff-c97a97ec7312.jpg" />. For each</p><p><img src="4-7401480\5128caa6-3694-42fe-9716-aacf588f74e4.jpg" />, we define <img src="4-7401480\7bda1132-5740-43bf-b181-11716dd1dadc.jpg" /> for each<img src="4-7401480\1de892ea-adbd-4175-b5ed-9049dd2a18c2.jpg" />. In particular for<img src="4-7401480\e3772f89-c8b2-4784-82fd-45cc57e67b3f.jpg" />, <img src="4-7401480\52f112b6-71ab-4bdd-97c7-53c909c682ba.jpg" />, so that it is the basic set of the unipotent delta operator<img src="4-7401480\88dea8d8-574b-4f1c-825e-805bcecddf47.jpg" />. Clearly, <img src="4-7401480\dfbca0a1-f123-4d12-924b-a7467be40c7b.jpg" />for each<img src="4-7401480\7e4bad00-87b6-4700-8f74-a5c5c07ec14d.jpg" />. Thus for every<img src="4-7401480\505ec07b-26ff-4ec2-be9d-59fa2bae4671.jpg" />, we have</p><disp-formula id="scirp.33983-formula98892"><label>(1)</label><graphic position="anchor" xlink:href="4-7401480\4e55d818-de20-49e7-8a0e-a67367a52f48.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.33983-formula98893"><label>(2)</label><graphic position="anchor" xlink:href="4-7401480\97be9d76-d4a5-4f7d-95ef-127959a21b6f.jpg"  xlink:type="simple"/></disp-formula><p>Now, let <img src="4-7401480\654e17c2-c92f-4982-86e5-895693ae21c5.jpg" /> be a variable commuting with <img src="4-7401480\94ee242f-80ca-49bb-86f6-8db3483b401b.jpg" /> and<img src="4-7401480\4c2bc9ac-1f85-4a5a-90d8-160a5fbdb4af.jpg" />, and let us define</p><p><img src="4-7401480\56972c01-8d34-425d-a5d0-fd69454ac292.jpg" /></p><p>and similarly,</p><p><img src="4-7401480\6404094d-6277-42b0-96de-cc611e9e5c0a.jpg" />for each<img src="4-7401480\701cec46-c6c3-4286-bf92-df49b13058ca.jpg" />. As polynomials in the variable<img src="4-7401480\19763ddd-91a1-4c4d-95eb-e83bb0d31ed8.jpg" />, their degrees are at most<img src="4-7401480\5125f47e-6e6a-4694-86b8-a908e01c239c.jpg" />. As polynomials in the variable<img src="4-7401480\a2709450-2d2a-401e-a787-cb0f8b0d4e8a.jpg" />, <img src="4-7401480\16c13d45-58c8-41db-8791-6a78e779668f.jpg" />, <img src="4-7401480\b6c77c81-7d60-492e-bde1-c4216c6dc126.jpg" />,</p><p><img src="4-7401480\4aed2fbd-5188-4046-81f7-8675ebfa6199.jpg" /></p><p>and</p><p><img src="4-7401480\d845d475-6993-45e0-a4bc-a0474d2931ec.jpg" /></p><p>have also a degree at most<img src="4-7401480\b3481ea4-ce7b-4374-9e22-a1cdf26d03bd.jpg" />. Because the equations (1) and (2) hold for every integer<img src="4-7401480\b3abb8b0-5937-43ed-9757-7a17dec7f66b.jpg" />, the polynomials (in the variable<img src="4-7401480\d90cf846-daeb-460c-9d65-f4b58847f3f7.jpg" />)</p><p><img src="4-7401480\7d9c9111-c471-464a-a3ca-efca02e0bb51.jpg" /></p><p>and</p><p><img src="4-7401480\b5499d6c-fe16-4bd1-a6ed-dfa65760dc5f.jpg" /></p><p>are identically zero, and the above equations hold for every<img src="4-7401480\45e9a725-2906-48b9-b673-d2e98b9585e3.jpg" />. Therefore, <img src="4-7401480\0a3903e2-f66d-4f2c-8861-e36ebd46b3f0.jpg" />is a polynomial sequence of binomial-type, and <img src="4-7401480\ff6060f2-6b3f-4d10-8dce-cdeea8804fe6.jpg" /> is a Sheffer sequence for every<img src="4-7401480\e9194b66-06f0-44db-a5a3-365f8a098e13.jpg" />. Moreover, for every<img src="4-7401480\3e2145fe-a15a-4d45-a836-b0419534047d.jpg" />, we have</p><p><img src="4-7401480\d6e55121-ec79-490d-b22a-5fdc1976941c.jpg" /></p><p>so that<img src="4-7401480\95db6c72-a036-461e-aafb-44a5f3793850.jpg" />. Similarly,</p><p><img src="4-7401480\2f71010c-a254-4ff3-b9fe-126caa7f9cfd.jpg" />for every<img src="4-7401480\84e806f0-d051-416c-8857-2409c5ea45ca.jpg" />. Moreover,</p><p><img src="4-7401480\02467c38-cb44-4f47-b52f-99adeb54f3ce.jpg" />.</p><p>Therefore, <img src="4-7401480\7e3be1d8-78d2-4515-b94a-79292886210e.jpg" />and <img src="4-7401480\ebc0cf5d-3d3c-4585-8cf6-0de8ed736bca.jpg" /> are one-parameter sub-groups. It follows that</p><p><img src="4-7401480\2b26e523-f19a-4e57-a3cc-d85fb625ba24.jpg" /></p><p>and</p><p><img src="4-7401480\91f95fb6-9c3a-4746-962b-6ba955e8632c.jpg" /></p><p>(inverses under umbral operation).</p><p>We define <img src="4-7401480\e26d1f2a-1575-4ac7-bc12-03ffc5d71815.jpg" /> as the pair of formal power series <img src="4-7401480\63a2d001-b033-4d02-955c-8526d05c9f9a.jpg" /> such that <img src="4-7401480\6149e213-5d61-478f-928c-30c1685fbbf7.jpg" /> is the substitution that defines the delta operator <img src="4-7401480\01d7f31a-a2a5-4b73-abb0-e37423c1e4a8.jpg" /> with basic sequence<img src="4-7401480\967778e6-ec67-473f-a83f-8eee4d11ad09.jpg" />, and <img src="4-7401480\ddea1124-2caf-4a83-90b3-1ea06a4c212c.jpg" /> is the invertible series such that</p><p><img src="4-7401480\b0b2728b-e146-4507-ae63-06b47524e0e3.jpg" /></p><p>for each<img src="4-7401480\290157c9-8bb9-4388-a2d0-50ecb2546165.jpg" />. Since <img src="4-7401480\99da7d31-fb4e-473e-937e-737ecd99e723.jpg" /> and <img src="4-7401480\b181ed97-886a-476f-9876-076c95d5e3f7.jpg" /> are unipotent sequences, it is clear that <img src="4-7401480\69b39c17-4aad-4704-ab3d-d2f2c5b946ce.jpg" /> is unipotent, and <img src="4-7401480\7404d9e4-a9e3-4e75-b5e3-7d80414bfd92.jpg" /> is a unipotent substitution. It is also clear that whenever<img src="4-7401480\ebece5dc-9f8b-4a27-8eab-82cb9943b9ed.jpg" />, then<img src="4-7401480\9318820d-d468-44aa-9497-56e3e81b3624.jpg" />. Let us check that <img src="4-7401480\c3d241b7-8d67-4129-9b5e-7ea7afff22e7.jpg" /> is a one-parameter subgroup of the group of unipotent substitutions with prefunction. This means that for every<img src="4-7401480\9658a6f8-69eb-410a-8f2a-952fb3380121.jpg" />,</p><p><img src="4-7401480\86ad5150-2e49-47f4-9d2b-f1a8e976773f.jpg" /></p><p>First of all, by definition, <img src="4-7401480\04ee8094-27c1-4d06-a037-a29b6a1ef3a8.jpg" />is the unipotent substitution associated to the basic set</p><p><img src="4-7401480\96ab31a5-fe52-4fb3-90f6-71cec7ebec46.jpg" />and therefore<img src="4-7401480\c1aede8e-6a3e-4ec6-ad63-72f96c9266fd.jpg" />. In a similar way, the series <img src="4-7401480\c8cd50d7-9421-4ef5-af0a-80171982c9bb.jpg" /> is uniquely associated to the Sheffer sequence</p><p><img src="4-7401480\40e9a1fa-ee19-4918-a8c1-3924af570c3c.jpg" />and to the basic set</p><p><img src="4-7401480\0093a8ce-5fe2-4489-bb6a-377517de5499.jpg" />. Again this means that<img src="4-7401480\8ccb64b3-480d-404f-aafc-432f068eba52.jpg" />. Therefore, we obtain the expected result. It is also clear that<img src="4-7401480\f6b0a895-94ca-484a-8c13-c6c078efb02b.jpg" />.</p><p>Remark 2. In particular, since <img src="4-7401480\c8213c2b-7d43-41ac-960b-4dca82647a35.jpg" /> is a field of characteristic zero, for every<img src="4-7401480\390989d4-4dc8-444a-b37e-3d209d857a13.jpg" />, we may define fractional powers <img src="4-7401480\b06092c3-601b-4d3e-90c3-3276f272114d.jpg" /> such as for instance<img src="4-7401480\d65a0321-b890-4f53-a5da-ce93fa4de501.jpg" /></p><p>for each integer<img src="4-7401480\44a81911-b2d4-416b-8b72-55fb0f99b1a6.jpg" />.</p></sec><sec id="s7"><title>REFERENCES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.33983-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">A. Benhissi, “Rings of Formal Power Series,” Queen’s Papers in Pure and Applied Mathematics, Queen’s University, Kingsone, 2003.</mixed-citation></ref><ref id="scirp.33983-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">R. P. Stanley, “Enumerative Combinatorics—Volume 1, Volume 49 of Cambridge Studies in Advanced Mathematics,” Cambridge University Press, Cambridge, 2000.</mixed-citation></ref><ref id="scirp.33983-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">G. H. E. Duchamp, K. A. Penson, A. I. Solomon, A. Horzeal and P. Blasiak, “One-Parameter Groups and Combinatorial Physics,” Proceedings of the Symposium COPROMAPH3: Contemporary Problems in Mathematical Physics, Cotonou, 2004, pp. 436-449.</mixed-citation></ref><ref id="scirp.33983-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">L. Poinsot and G. H. E. Duchamp, “A Formal Calculus on the Riordan near Algebra,” Advances and Applications in Discrete Mathematics, Vol. 6, No. 1, 2010, pp. 11-44.</mixed-citation></ref><ref id="scirp.33983-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">L. W. Shapiro, S. Getu, W.-J. Woan and L. C. Woodson, “The Riordan Group,” Discrete Applied Mathematics, Vol. 34, No. 1-3, 1991, pp. 229-239. 
doi:10.1016/0166-218X(91)90088-E</mixed-citation></ref><ref id="scirp.33983-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">G. Markowsky, “Differential Operators and the Theory of Binomial Enumeration,” Journal of Mathematical Analysis and Application, Vol. 63, No. 1, 1978, pp. 145-155.  
doi:10.1016/0022-247X(78)90111-7</mixed-citation></ref><ref id="scirp.33983-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">G. H. E. Duchamp, L. Poinsot, A. I. Solomon, K. A. Penson, P. Blasiak and A. Horzela, “Ladder Operators and Endomorphisms in Combinatorial Physics,” Discrete Mathematics and Theoretical Computer Science, Vol. 12, No. 2, 2010, pp. 23-46.</mixed-citation></ref><ref id="scirp.33983-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">G.-C. Rota, D. Kahaner and A. Odlyzko, “Finite Operator Calculus,” Journal of Mathematical Analysis and Its Applications, Vol. 42, No. 3, 1973, pp. 684-760.</mixed-citation></ref><ref id="scirp.33983-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">I. M. Sheffer, “Some Properties of Polynomial Sets of Type Zero,” Duke Mathematical Journal, Vol. 5, No. 3, 1939, pp. 590-622. doi:10.1215/S0012-7094-39-00549-1</mixed-citation></ref><ref id="scirp.33983-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">J. F. Steffensen, “The Poweroid, an Extension of the Mathematical Notion of Power,” Acta Mathematica, Vol. 73, No. 1, 1941, pp. 333-366. doi:10.1007/BF02392231</mixed-citation></ref><ref id="scirp.33983-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">S. Roman, “The Umbral Calculus,” Dover Publications, New York, 1984.</mixed-citation></ref><ref id="scirp.33983-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">T.-X. He, L.C. Hsu and P.J.-S. Shiue, “The Sheffer Group and the Riordan Group,” Discrete Applied Mathematics, Vol. 155, No. 15, 2007, pp. 1895-1909. 
doi:10.1016/j.dam.2007.04.006</mixed-citation></ref></ref-list></back></article>