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IJMMS 2003:37, 2345–2347 PII. S0161171203203045 http://ijmms.hindawi.com

© Hindawi Publishing Corp.

THE CONJUGATION OPERATOR ONAq(G)

SANJIV KUMAR GUPTA Received 5 March 2002

Letq >2. We prove that the conjugation operatorHdoes not extend to a bounded operator on the space of integrable functions defined on any compact abelian group with the Fourier transform inlq.

2000 Mathematics Subject Classification: 42A50, 43A17.

LetGbe a compact abelian group with dualΓ. For 1q <, the spaceAq

is defined as

Aq(G)=f:fL1(G),fˆlq(Γ)

(1) with the normfAq= fL1+fˆlq. ThenAq(G)is a commutative semisim- ple Banach algebra with maximal ideal spaceΓ, in which the set of trigonomet- ric polynomials is dense [4]. TheAp-spaces have been studied in [1,6].

IfGis, in addition, a connected group, then its dual can be ordered; there exists a semigroupPΓsuch thatP∩−P= {0},P∪−P=Γ (see [5]), and we say thatγΓis positive ifγP. Iff=

γ∈Ff (γ)γˆ is a trigonometric polynomial, the conjugation operatorHis defined as

Hf=

γ∈F

sgn(γ)f (γ)γ,ˆ (2)

where sgn(γ)= +1 ifγP,1 ifγ∈ −P, and 0 ifγ=0.

If 1q2, thenAq(G)L2(G), and it is easy to see thatHextends to a bounded operator onAq(G). It was mentioned in [5] that the corresponding result forq >2 is not known. Note thatHextends to a bounded operator on Aq(G)if and only ifHextends to a bounded operator fromAq(G)toL1(G). In [5], the following theorem was proved.

Theorem1. LetGbe a compact, connected abelian group andPany fixed order onΓ. Ifq >2andφis a Young’s function, then the conjugation operator Hdoes not extend to a bounded operator fromAq(G)toLφ(G).

We prove inTheorem 2thatH does not extend to a bounded operator on Aq(G),q >2, thus answering the problem mentioned in [5]. Also,Theorem 1 follows from our theorem (Theorem 2).Theorem 2was proved for the circle group in [2] but for the completeness sake, we give it below.

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2346 SANJIV KUMAR GUPTA

Theorem2. LetGbe a compact, connected abelian group andPany fixed order on Γ. If q >2, then the conjugation operator H does not extend to a bounded operator onAq(G).

Proof. We will show thatHdoes not extend to a bounded operator from Aq(G)toL1(G). The proof is divided into three steps.

Step1. LetG=T, the circle group. Suppose thatHextends as a bounded operator fromAq toL1. Chooseµ0M(T), ˆµ0lq such thatµ0is not abso- lutely continuous. DefineT:L1L1by

T f=H fµ0

, (3)

whereTis well defined asfµ0AqandHmapsAqintoL1by our assump- tion onH. Hence,T is a multiplier fromL1toL1, and therefore is given by a measureµM(T)(see [3]). Hence

sgn(n)ˆµ0(n)=µ(n).ˆ (4)

Observe that

µˆ0=µˆ0+µˆ

2 +µˆ0µˆ

2 . (5)

Now,µ0+µ)/2 andˆ µ0µ)/2 are absolutely continuous by F. and M. Rieszˆ theorem. Hence, ˆµ0is absolutely continuous, which contradicts the choice of µ0. Hence,His unbounded onAq,q >2.

Step2. LetI be a closed subgroup ofGsuch thatHdoes not extend as a bounded operator onAq(G/I). ThenHdoes not extend as a bounded operator onAq(G).

Proof. Let(fn)be a sequence of trigonometric polynomials onG/I such that

HfnL1(G/I) → ∞, fnA

q(G/I) 0, asn → ∞. (6) Letgn=fnq, whereq:GG/Iis the quotient map. Then it is easily seen that Hgn=(Hfn)q,HgnL1(G)= HfnL1(G/I), andfnqAq(G)= fnAq(G/I). Hence

HgnL1(G) → ∞, gnA

q(G) 0, asn → ∞, (7)

andStep 2follows.

Step3. SinceG is connected,Γ contains an element of infinite order, say γ0(see [3]). Let S denote the subgroup generated byγ0and letI=S. Then G/His isomorphic to the circle groupT. Now, the proof of the theorem follows from Steps1and2.

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THE CONJUGATION OPERATOR ONAq(G) 2347 Acknowledgment. This research was supported by Sultan Qaboos Uni- versity, Oman.

References

[1] L. M. Bloom and W. R. Bloom,Multipliers on spaces of functions withp-summable Fourier transforms, Harmonic Analysis (Luxembourg, 1987), Lecture Notes in Math., vol. 1359, Springer, Berlin, 1988, pp. 100–112.

[2] J. T. Burnham, H. E. Krogstad, and R. Larsen,Multipliers and the Hilbert distribution, Nanta Math.8(1975), no. 2, 95–103.

[3] E. Hewitt and K. A. Ross,Abstract Harmonic Analysis. Vol. I: Structure of Topolog- ical Groups. Integration Theory, Group Representations, Die Grundlehren der Mathematischen Wissenschaften, vol. 115, Academic Press, New York, 1963.

[4] ,Abstract Harmonic Analysis. Vol. II: Structure and Analysis for Compact Groups. Analysis on Locally Compact Abelian Groups, Die Grundlehren der Mathematischen Wissenschaften, vol. 152, Springer-Verlag, New York, 1970.

[5] W. Rudin,Fourier Analysis on Groups, Interscience Tracts in Pure and Applied Mathematics, no. 12, Interscience Publishers, New York, 1962.

[6] U. B. Tewari and A. K. Gupta,The algebra of functions with Fourier transforms in a given function space, Bull. Austral. Math. Soc.9(1973), 73–82.

Sanjiv Kumar Gupta: Department of Mathematics and Statistics, College of Science, Sultan Qaboos University, P.O. Box 36, Al-Khaud 123, Sultanate of Oman

E-mail address:[email protected]

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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.

Authors should follow the Mathematical Problems in Engineering manuscript format described at http://www .hindawi.com/journals/mpe/. Prospective authors should submit an electronic copy of their complete manuscript through the journal Manuscript Tracking System athttp://

mts.hindawi.com/according to the following timetable:

Manuscript Due December 1, 2008 First Round of Reviews March 1, 2009 Publication Date June 1, 2009

Guest Editors

Edson Denis Leonel,Departamento de Estatística, Matemática Aplicada e Computação, Instituto de Geociências e Ciências Exatas, Universidade Estadual Paulista, Avenida 24A, 1515 Bela Vista, 13506-700 Rio Claro, SP, Brazil ; [email protected]

Alexander Loskutov,Physics Faculty, Moscow State University, Vorob’evy Gory, Moscow 119992, Russia;

[email protected]

Hindawi Publishing Corporation http://www.hindawi.com

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