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Vol. 22, No. 1 (1999) 91–95 S 0161-17129922091-1

© Electronic Publishing House

ON AZUMAYA GALOIS EXTENSIONS AND SKEW GROUP RINGS

GEORGE SZETO

(Received 6 November 1997 and in revised form 22 December 1997)

Abstract.Two characterizations of an Azumaya Galois extension of a ring are given in terms of the Azumaya skew group ring of the Galois group over the extension and a Galois extension of a ring with a special Galois system is determined by the trace of the Galois group.

Keywords and phrases. Azumaya algebras, Galois extensions, H-separable extensions, skew group rings.

1991 Mathematics Subject Classification. 16S30, 16W20.

1. Introduction. LetSbe a ring with 1,Ga finite automorphism group ofSof order nfor some integerninvertible inS,SGthe subring of the elements fixed under each element inG,Cthe center ofS, andSGthe skew group ring ofGoverS. In [3] and [2], Sis called an Azumaya Galois extension ofSGif it is aG-Galois extension ofSGwhich is an AzumayaCG-algebra. It was shown thatSis an Azumaya Galois extension if and only ifSGis an AzumayaCG-algebra. The purpose of the present paper is to give two more characterizations of an Azumaya Galois extension in terms of the Azumaya skew group ringSG. We show thatS is an AzumayaG-Galois extension if and only ifSGis an Azumaya algebra over its center Z, aG-Galois extension with an inner Galois groupGinduced by the elements ofG, andZGis a finitely generated projective CG-module of rankn. Moreover, for the skew group ringSG, whereSis a separable CG-algebra, an expression of the commutator subring ofCinSGis obtained by using Sand its commutator subring inSG. Furthermore, letHbe a normal subgroup ofG, Kthe commutator subgroup ofHinG, andHthe inner automorphism group ofSG induced by the elements ofH(Kand(G/H)are similarly defined). Then, it is shown that(SG)Kis a(G/K)-Galois extension with a Galois system{m−1gj, g−1j /gjinH}

if and only if TrG(gi)=0 for eachginot inK, wheremis the order ofHfor some integermand TrG(gi)is the trace ofGatgi.

2. Preliminaries. Throughout, letSbe a ring with 1,G= {g1,...,gn}for some in- tegerninvertible inS, C the center ofS,SG the subring of the elements fixed un- der each element inG, andSG the skew group ring ofGover S. LetB be a sub- ring of a ring A. We callA a separable extension of B if there exist {ai,bi} in A, i=1,...,mfor some integer m, such that

aibi=1 and

aai⊗bi =

ai⊗bia for all a in A, where is over B and {ai,bi}is called a separable system for A.

An Azumaya algebra is a separable extension over its center. A ringA is called an H-separable extension ofB ifA⊗A is a direct summand of a finite direct sum of Aas anA-bimodule, where⊗ overB. Denote the commutator subring ofBinAby

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VA(B). An H-separable extensionA over B is equivalent to the existence of anH- separable system{diinVA(B);

(xij⊗yij)inVA⊗A(A)},j=1,...,uandi=1,...,v for some integers u and v such that

di

(xij⊗yij)

= 11, i=1,...,v and j=1,...,u. The ringSis called aG-Galois extension ofSGif there exist{ci,diinS,i= 1,...,kfor some integerk}such that

cidi=1 and

aigj(bi)=0 for eachgj=1, where{ci,di}is called a G-Galois system forS. It is well known that an Azumaya algebra is anH-separable extension and that anH-separable extension is a separa- ble extension. A skew group ringSGis a ring with a free basis{gi}overSsuch that gis=(gi(s))gifor eachgiinGandsinS. We denote the center ofSGbyZ, the inner automorphism group ofSGinduced by the elements of the subgroupHofGbyH (= {g/g(x)=gxg−1forginHand allxinSG}), and the commutator subgroup ofHinGbyVG(H).

3. Skew group rings. In this section, keeping the notations of Section 2, we give two characterizations of an Azumaya Galois extension and an expression of the com- mutator subring ofCinSGwhenSis a separableCG-algebra.

Theorem3.1. The following statements are equivalent:

(i) S is an Azumaya Galois extension,

(ii) SGis an AzumayaZ-algebra andS satisfies the double centralizer property in SG, and

(iii) SGis an AzumayaZ-algebra and aG-Galois extension of(SG)G, and ZG is a finitely generated and projectiveCG-module ofrankn.

Proof. (i)⇒(ii). SinceS is an Azumaya Galois extension,SGis an AzumayaCG- algebra (that is, Z= CG) and SG is an H-separable extension of S [3, Thm. 3.1].

Noting that S is a direct summand of SG as a left S-module, we conclude that VSG(VSG(S))=S[6, Prop. 1.2].

(ii)⇒(i). SinceVSG(VSG(S))=S,Zis contained inS; and soZis contained inC. But thenZ=CG. This implies that SG is an AzumayaCG-algebra by (ii). Thus,S is an Azumaya Galois extension [3, Thm. 3.1].

(i)⇒(iii). Since the restriction ofGtoSisG,SGis aG-Galois extension of(SG)G with the same Galois system as S (for S is G-Galois). Also, by hypothesis, S is an Azumaya Galois extension, soSGis an AzumayaCG-algebra [3, Thm. 3.1]. Moreover, sinceZ=CG,ZGis a freeZ-module of rankn.

(iii)⇒(i). SinceSGis a G-Galois extension of(SG)G with an inner Galois group G, it is an H-separable extension of (SG)G [7, Cor. 3]. But n is a unit in S, so VSG((SG)G)is a separable Z-algebra and a finitely generated and projectiveZ- module of rankn[7, Prop. 4]. Moreover,SGis aG-Galois extension of(SG)G, so it is finitely generated and projective(SG)G-module. Sincenis a unit inS,ZGis a sep- arableZ-algebra. But thenVSG((SG)G)=VSG(VSG(ZG))=ZGby the commutator theorem for Azumaya algebras [4, Thm. 4.3]. Therefore, ZG is a finitely generated and projectiveZ-module of rankn[1, Prop. 4]. From the fact that there aren ele- ments{gi}ofGas generators ofZG, it is not difficult to show that{gi}are free over Z. Hence,Z is a finitely generated and projective CG-module. Thus, the rank ofZG over CG is a product of the rank of ZG overZ and the rank ofZ overCG; that is,

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n=n(rank ofZoverCG). This implies thatZ=CG. Therefore,SGis an Azumaya CG-algebra; and soSis an Azumaya Galois extension [3, Thm. 3.1].

Corollary3.2. LetS be a separableCG-algebra. IfVSG(S)is aG-Galois exten- sion, whereGis the inner automorphism group ofVSG(S)induced by and isomorphic withG, thenSis an Azumaya Galois algebra.

Proof. SinceVSG(S) is aG-Galois extension, there exists a G-Galois system {ci,diinVSG(S)|i=1,...,k}forVSG(S). Then, it is straightforward to check that {cj;

gjdi⊗g−1j , i=1,...,kandj=1,...,mfor some integerskandm}is anH-sep- arable system forSG over S [1, Thm. 1]. Hence, S satisfies the double centralizer property inSG[7, Prop. 1.2]. Moreover,nis a unit inS, soSGis a separable exten- sion ofS. By hypothesis,Sis a separableCG-algebra, soSGis a separableCG-algebra by the transitivity of separable extensions. But thenSG is an AzumayaZ-algebra.

Therefore,Sis an Azumaya Galois extension by Theorem 3.1.

For the skew group ringSGofGover a separableCG-algebraS, we next give an expression ofVSG(C)in terms ofS andVSG(S)(for more aboutVSG(S), see [1]).

Theorem3.3. IfSis a separableCG-algebra, then (i) CZ is a commutative separable subalgebra ofSGand

(ii) SZ,VSG(S), andVSG(C)are Azumaya CZ-algebras contained inSG, such that VSG(C)SZ⊗VSG(S), where⊗is over CZ.

Proof. (i) Since S is a separable CG-algebra, C is also a separableCG-algebra.

Hence,C⊗Zis a separableZ-algebra, where⊗is overCG; and so the homomorphic imageCZ ofC⊗Zis also a separableZ-algebra. Clearly,CZ is commutative.

(ii) Sincenis a unit inS,SGis a separableS-extension. Hence,SGis a separable CG- algebra by the transitivity of separable extensions; and soSGis an AzumayaZ- algebra. But thenVSG(CZ)is a separable subalgebra ofSGsuch thatVSG(VSG(CZ))

=CZ [4, Thm. 4.3] (forCZ is a separable subalgebra ofSGby (i)). This implies that the center ofVSG(CZ)isCZ. Thus,VSG(CZ)is an AzumayaCZ-algebra. By hypothe- sis again,Sis a separableCG-algebra, so it is an AzumayaC-algebra. Hence,S⊗CZis an AzumayaCZ-algebra, where⊗is overC. Thus,SZ is also an AzumayaCZ-algebra.

Noting thatSZ⊂VSG(CZ), we conclude thatVSG(CZ)SZ⊗VSG(SZ), where⊗is overCZ [7, Thm. 4.3]. Moreover, sinceVSG(CZ)=VSG(C)andVSG(SZ)=VSG(S), we conclude thatVSG(C)SZ⊗VSG(S), where⊗is overCZ.

By [3, Thm. 3.1], ifS is an Azumaya Galois extension, thenSGis an AzumayaCG- algebra (that is,Z=CG) andS is a separableCG-algebra. Thus, we have the following result.

Corollary3.4. IfS is an Azumaya Galois extension, thenVSG(C)S⊗VSG(S) as AzumayaC-algebras, where⊗is overCsuch thatVSG(C)is aG-Galois extension ofVSG(CG).

Proof. By the above remark, it suffices to show thatVSG(C)is aG-Galois exten- sion ofVSG(CG). In fact, sinceS is aG-Galois extension andS⊂VSG(C),VSG(C) is aG-Galois extension with the same Galois system asS by noting thatVSG(C)is

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G-invariant (forGis the restriction ofGtoS). Moreover, it is clear that(VSG(C))G= VSG(CG).

4. A Galois system. It is well known that{n−1gi,gi−1|giinG}is a separable system for a separable group ringRGover a ringR with 1, whereG= {gi|i=1,...,n}for some integerninvertible inR, for a separable skew group ringSGoverSand for a separable projective group ringRGfoverRas defined in [9]. In this section, we give an equivalent condition for(SG)K to have a(G/K)-Galois system similar to the above separable system for a normal subgroupKofG.

Theorem4.1. LetHbe a normal subgroupofGandVG(H)=K. Then (i) Kis a normal subgroupofGand

(ii) TrH(gi)=0for eachgi not inK if and only if(SG)K is a(G/K)-Galois ex- tension of(SG)Gwith a Galois system{m−1gj, g−1j |gjinH}, wheremis the order ofH.

Proof. (i) We want to show that giKgi−1⊂K for eachgi in G. For anyx in K and y in H, gixg−1i y=gixgi−1ygigi−1=gixzgi−1, where z=g−1i ygi. SinceH is normal inG,zis inH. Hence,xz=zx. But thengixg−1i y=gixzg−1i =gizxgi−1= gigi−1ygixgi−1=ygixg−1i . This implies thatgixgi−1is inK. Thus,Kis normal inG.

(ii) Assume that TrH(gi)=0 for eachginot inK. Then

gjgigj−1=0, whereH= {gj|j=1,...,mfor some integerm}; that is,

gjgigj−1gi−1gi= gj

(gi)(g−1j ) gi

=0,j=1,...,m. Hence,(m−1) gj

(gi)(g−1j )

=0 for eachginot inK. Clearly, for eachgi inK,(m−1)

gj

(gi)(g−1j )

=1. Thus,{m−1gj, gj−1|gjinH}is a (G/K)- Galois system for(SG)K(forH⊂(SG)K), wheremis the order ofH.

Conversely,(m−1) gj

(gi)(gj−1)

=0 for eachginot inK, so

gjgigj−1gi−1=0.

Hence,

gjgig−1j =0; that is, TrH(gi)=0 for eachginot inK.

We derive the following corollaries.

Corollary4.2. SGhas a(G/K)-Galois system{n−1gi,g−1i |giinG}, whereKis the center ofG, if and only ifTrG(gi)=0for eachginot inK.

Proof. LetHbeG. ThenK=the center ofG; and so the corollary follows imme- diately from the theorem.

Corollary4.3. SG has aG-Galois system{n−1gi,g−1i |giinG}if and only if TrG(gi)=0for eachgi=1.

Proof. This is the case of the theorem that the center ofGis trivial.

We derive an equivalent condition for a Galois subring ofSG arising from aG- invariant subring.

Corollary4.4. LetAbe aG-invariant subring ofSGandH= {giinG|gi(a)= afor eachainA}. Then

(i) His normal inGand

(ii) Denoting (SG)HbyB andVG(H)byK,TrK(gi)=0for each gi not in H if and only if {m−1gj,g−1j |gjinK}is a(G/H)-Galois system for B, where m is the

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order ofK.

Proof. Part (i) is straightforward and part (ii) follows immediately from Theo- rem 4.1.

We conclude the present paper with an example of an Azumaya skew group ring SG which is aG-Galois extension such that the rank of ZG overCG is notn(see Theorem 3.1(iii)). Hence,S is not an Azumaya Galois extension by Theorem 3.1.

LetR be the real field,S=R[i,j,k]the quaternion algebra overR, andG= {1,g| g(x)=ix(i)−1for eachxinS}. Then

(1)S is aG-Galois extension with a Galois system{2−1,2−1j;1,−j}. Hence,SGis a G-Galois extension with the same Galois system.

(2) SinceSGis a separable extension ofS andSis an AzumayaR-algebra,SGis a separableR-algebra. Hence,SGis an AzumayaZ-algebra.

(3) The centerZofSGis(R+Ri)by direct computation.

(4)ZGis free overZby direct verification.

(5)C=RandCG=C=R.

(6)Zis a freeR-module of rank 2 andZGis a freeCG-module of rank 4 (=2=the order ofG), so one of the three conditions in Theorem 3.1(iii) does not hold.

Acknowledgement. This work was supported by the Caterpillar Fellowship at Bradley University during the author’s sabbatical leave in Fall, 1997. The present paper was revised according to the suggestions of the referee. The author would like to thank the referee for his valuable suggestions.

References

[1] R. Alfaro and G. Szeto,The centralizer onH-separable skew group rings, Rings, extensions, and cohomology (New York), Lecture Notes in Pure and Appl. Math., vol. 159, Marcel Dekker, Inc., 1994, Basal Hong Kong, pp. 1–7. MR 95g:16027. Zbl 812.16038.

[2] ,Skew grouprings which are Azumaya, Comm. Algebra23(1995), no. 6, 2255–2261.

MR 96b:16027. Zbl 828.16030.

[3] ,On Galois extensions of an Azumaya algebra, Comm. Algebra25 (1997), no. 6, 1873–1882. CMP 97 11. Zbl 890.16017.

[4] F. DeMeyer and E. Ingraham, Separable algebras over commutative rings, Lecture Notes in Mathematics, vol. 181, Springer-Verlag, New York, 1971. MR 43#6199.

Zbl 215.36602.

[5] F. R. DeMeyer,Some notes on the general Galois theory of rings, Osaka J. Math.2(1965), 117–127. MR 32#128. Zbl 143.05602.

[6] K. Sugano,Note on semisimple extensions and separable extensions, Osaka J. Math.4(1967), 265–270. MR 37#1412. Zbl 199.07901.

[7] ,On a special type of Galois extensions, Hokkaido Math. J.9(1980), no. 2, 123–128.

MR 82c:16036. Zbl 467.16005.

[8] G. Szeto,Separable Subalgebras of a Class of Azumaya Algebras, to appear in Internat. J.

Math. Math. Sci.

[9] G. Szeto and Y. F. Wong,On Azumaya projective group rings, Azumaya algebras, ac- tions, and modules, Contemp. Math., vol. 124, Amer. Math. Soc., 1992, pp. 251–256.

MR 92m:16024. Zbl 749.16013.

Szeto: Department of Mathematics, Bradley University, Peoria, Illinois61625, USA

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Mathematical Problems in Engineering

Special Issue on

Time-Dependent Billiards

Call for Papers

This subject has been extensively studied in the past years for one-, two-, and three-dimensional space. Additionally, such dynamical systems can exhibit a very important and still unexplained phenomenon, called as the Fermi acceleration phenomenon. Basically, the phenomenon of Fermi accelera- tion (FA) is a process in which a classical particle can acquire unbounded energy from collisions with a heavy moving wall.

This phenomenon was originally proposed by Enrico Fermi in 1949 as a possible explanation of the origin of the large energies of the cosmic particles. His original model was then modified and considered under different approaches and using many versions. Moreover, applications of FA have been of a large broad interest in many different fields of science including plasma physics, astrophysics, atomic physics, optics, and time-dependent billiard problems and they are useful for controlling chaos in Engineering and dynamical systems exhibiting chaos (both conservative and dissipative chaos).

We intend to publish in this special issue papers reporting research on time-dependent billiards. The topic includes both conservative and dissipative dynamics. Papers dis- cussing dynamical properties, statistical and mathematical results, stability investigation of the phase space structure, the phenomenon of Fermi acceleration, conditions for having suppression of Fermi acceleration, and computational and numerical methods for exploring these structures and applications are welcome.

To be acceptable for publication in the special issue of Mathematical Problems in Engineering, papers must make significant, original, and correct contributions to one or more of the topics above mentioned. Mathematical papers regarding the topics above are also welcome.

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