On Four Dimensional Semi-C-reducible. Landsberg Space
|
|
- Audra Patrick
- 5 years ago
- Views:
Transcription
1 Internatonal Matematcal Forum Vol no On Four Dmensonal Sem--reducble Landsberg Space V. K. aubey and *Rakes Kumar Dwved Department of Matematcs & Statstcs D.D.U. Gorakpur Unversty Gorakpur (U.P.) Inda vkcoct@gmal.com * Pundt Deen Dayal Inter ollege Pprac Gorakpur (U.P.) Inda Abstract. In te present paper we ave work out te -connecton vectors of fourdmensonal Landsberg and Berwald spaces four dmensonal sem -reducble Landsberg spaces and necessary and suffcent condton under wc te fourdmensonal sem--reducble Landsberg space to be a Berwald space. Matematcs Subject lassfcaton: 5B0 560 Keywords: Landsbeg space Berwald space Sem--reducble Fnsler space four-dmensonal Fnsler space 1. Introducton A teory of ntrnsc ortonormal frame feld on n-dmensonal Fnsler space as been studed by Matsumoto and Mron ([2] []) and s called Mron frame by Matsumoto. A four dmensonal Fnsler space wt Mron frame as been studed n [5] [6] and [7]. Let F be a four dmensonal Fnsler space wt fundamental functon L. Te metrc tensor g j and () v-torson tensor jk of F are defned by g L 2 y y j j 2 1 L. y y y jk j k
2 192 V. K. aubey and R. K. Dwved Let {e }; λ 1 2 ; be te Mron frame of F were λ s te normalzed supportng element e2) m p are constructed by ge j λ) eμ) λμ jk jkg e 1) l y L s te normalzed torson vector e) n and e) δ. Hence s te lengt of torson vector. Te greek letters λ μ ν vares from 1 to trougout te capter. Te () v-torson tensor jk of F s wrtten as [7] (1.1) L jk λμνeλ) eμ) j eν )k 222mm jmk 2 (jk)(mn jn k ) 2 (jk)(mp jp k) 22 (jk)(mm jn k) (nnjn k) (jk)(np jpk) (m m p ) (n n p ) (p p p ) 22 (jk) j k (jk) j k j k 2 (jk){(m( np j k nkpj)} were (jk) denote te cyclc permutaton of ndces I j k and summaton for nstance (jk)(ab j k) AB j k AB j k AkB j. If we put 222 H 2 I 2 K J J H I 2 K Ten we ave [7] H I K L 22 - (J J ) 22 - (H I ) And ence (1.1) may be wrtten as (1.2) L jk Hmm jmk Jnn jnk Hppjpk I (jk)(mnjn k ) K (jk)( m pjpk ) J (jk)( npjp k) (J J ) (n mm ) I ( n n p ) (jk) j k (jk) j k (H I ) (m mp ) K {( m (np n p )}. (jk) j k (jk) j k k j Te egt scalars H I J K H I J K are called te man scalars of a four dmensonal Fnsler space. Defnton 1.1. [] A Fnsler space F n s called a Landsberg space f te Berwald connecton BГ s -metrcal. Defnton 1.1. [] In terms of artan s connecton Г a Landsberg space s caracterzed by (1) te (v) v-torson tensor Pjk vanses dentcally namely P ( ) 0 jk jk 0
3 On four dmensonal sem--reducble Landsberg space 19 or (2) te v-curvature tensor P jk vanses dentcally were te suffx 0 ndcates te contracton by supportng element y. Defnton 1.2. [2] In a Fnsler space F n f te connecton coeffcent G jk of Berwald connecton BГ are functon of poston alone ten space s called a Berwald space. Teorem 1.2. [2] In terms of te artan connecton Г a Berwald space s caracterzed by 0. jk 2. Te -connecton vectors and te tensor jk Let us consder te Mron frame {e λ } of F. If a tensor Tj of (1 1) type s gven ten [2] Tj Tλμeλ) eμ)j. Now we denote te -covarant dervatve wt respect to artan * * connecton ( Γjk Γ 0k jk ) by n. Let H λμν ) be scalar components of -covarant dervatve e λ ) j of vector e λ ) belongng to te Mron frame {e λ )} of F.e. (2.1) eλ) j Hλ) μν eμ) eν) j. Te scalar H λ ) μν satsfy te followng condton ([7] [2]) H 1) μν 0 and Hλμν ) Hμ) λν. If we assume (2.2) H2)μ μ H2)μ jμ and H)μ Kμ ten from (.1) we obtan j (2.) l j 0 m j n j p jj n j mj pkj p j m jj n Kj were (2.) j λ e λ ) j j λ e λ ) K K λ e λ ). Defnton 2.1. Te vectors j and K defned n (2.) are called te - connecton vectors of a four dmensonal Fnsler space. Now f we denote te scalar components of T j k by T λμ ν tat s (2.5) Tj k Tλμ νeλ) eμ) j eν)k ten we obtan K (2.6) T ( δ T ) e T H T H were δ Γ &. k k λμ ν K λμ ν) δμ δ) λν λδ δ) μν *j 0k r
4 19 V. K. aubey and R. K. Dwved k Furter f S s a scalar feld of F ten S k S λ e λ)k were S λ (δ k S) e λ) and s called -scalar dervatve of S. Dfferentatng equaton (1.2) -covarantly and usng equaton (2.) we ave 1 2 (2.7) L Ammm Annn Appp A (mmn) jk j k j k j k (jk) j k were (2.7) A (mm p ) A (mn n ) A (mp p ) (jk) j k (jk) j k (jk) j k 8 9 A (jk)(nnp j k ) A (jk)(npp j k ) 10 A (jk){(m (n jpk nkp j)} A H (J J ) (H I ) j A J I IK A H Kj JK A (J J ) 2K j (H ) (H I )K A (H I ) 2K (H 2K)j (J J )K. A I (J 2J ) I j 2KK A K J (H )J 2KK A I 2K Ij (J 2J )K A J K 2K j (H 2J )K 10 A K (H ) (J 2J )j (I K)K We denote te scalar components of te vector r A by r A μ ; r e. (2.8) r A r A μ e μ) r for nstant te scalar component of 1 A are gven by (2.8) 1 A H (J J ) (H I )j. μ μ In te vew of equaton (2.6) (2.2) and (2.8) te explct form of αβγ δ can be wrtten as 1 5 A A A (2.9) 222 μ μ 6 2 μ Aμ 7 2 μ Aμ 10 2 μ Aμ. μ 22 μ μ 2 μ Aμ 9 μ Aμ μ 22 μ μ 8 μ Aμ μ Aμ
5 On four dmensonal sem--reducble Landsberg space 195 ontracton of equaton (2.7) by y gves 1 2 (2.10) P A mm m A n n n A pp p jk jk 0 1 j k 1 j k 1 j k A (mm n ) A (mm p ) A (mn n ) (jk) j k 1 (jk) j k 1 (jk) j k (jk) j k 1 (jk) j k 1 (jk) j k 10 A 1 (jk){(m (njpk nkp j)}. A (mp p ) A (n n p ) A (n p p ) Now we consder te four dmensonal Landsberg space. Snce te (v) vtorson tensor P jk of a Landsberg space vanses dentcally terefore we ave r A 1 0 for eac r Moreover jk j k s satsfed n a Landsberg space. So equaton (2.5) mples λμνδ λμδν. In te vew of equaton (2.9) ts can be explctely wrtten as 1 A A 2 1 A 5 A 2 6 A 2 A 6 A 2 A 2 (2.11) A 2 7 A A 9 A A 6 A 2 5 A 7 A 2 2 A 8 A 8 A 9 A A 5 A 10 A 2 6 A 8 A 2 10 A 7 A 9 A 2 10 A. In vew of equatons (2.10) and (2.11) equaton (2.7) gves (2.12) L 1 Ammmm 2 Annnn Appp p jk 2 j k j k j k B (mm mn) B (mmm p) 1 (jk) j k 2 (jk) j k B (m n n n ) B (n n np) (jk) j k (jk) j k B (mp p p ) B (n p p p ) 5 (jk) j k 6 (jk) j k B (m mn n ) B 7 (jk) j k 8 (jk) j k B (n npp ) B (m mp p ) (m mn p ) 9 (jk) j k 10 (jk) j k B (m nn p ) B (m np p ) 11 (jk) j k 12 (jk) j k were B 1 1 A A 2 B 2 1 A 5 A 2 B 6 A 2 A 2 B 2 A 8 A B 5 A 2 7 A B 6 A 9 A B 7 A 6 A 2 B 8 5 A 7 A 2 B 9 8 A 9 A B 10 A 5 A 10 A 2 B 11 6 A 8 A 2 10 A B 12 7 A 9 A 2 10 A. Te notaton (jk) n te expresson (2.12) stands for te possble permutaton of ndces j k and summaton for nstance (m mmn ) mmm n m mm n m mmn m mm n (jk) j k j k j k k j j k (m mn n ) mmn n m m n n m mnn m mn n mmnn m mnn (jk) j k j k j k k j j k k j j k (jk)(m mn j kp) mmn j kp mjmn k p mkmnp j mmnjpk mmn p m m np m m np m mn p j k j k k j k j
6 196 V. K. aubey and R. K. Dwved mmnp k j mmnp k j mjmnp k mjmn kp. Proposton 2.1. Te -covarant dervatve of () v-torson vector jk of a four dmensonal Landsberg space can be wrtten n te form (2.12). Now we consder a four dmensonal Berwald space. From teorem (1.2) suc a space s caracterzed by αβγδ 0. In vew of equaton (2.7) we ave 22 δ δ δ (H I K) δ 0 wc mples δ 0. Smlarly 22 δ δ δ (H I K) j δ 0 wc mples j δ 0. Hence from 222 δ 0 we get H δ 0 and also J δ I K I δ 2K k δ K δ - 2K k δ ' ' ' H δ - J k δ I δ - (J - 2J )k δ J δ (H )k δ K δ (I - K) k δ ' wc gves (H I K) δ (L) δ 0. Summarzng above results we ave: Teorem 2.1. In a four dmensonal Berwald space te -connecton vectors and j vans dentcally. Also man scalar H and te unfed man scalar L are - covarantly constant. Furtermore f -connecton vector K vanses ten all te man scalars are -covarantly constant. To solve te -connecton vectors explctely n terms of man scalar n te next secton we consder a four dmensonal sem--reducble Landsberg space F.. Sem--reducble Landsberg space F Defnton.1. [] A Fnsler space F n (n ) wt te non-zero lengt of te torson vector s called sem--reducble f te () v-torson tensor jk s of te form p q ( ) n 1 jk j k jk k j 2 j k were p and q ( 1 p) do not vans. It as been seen ([6]) tat a four dmensonal Fnsler space F s sem-reducble f and only f (.1) H I K J J 0. Tus for a four dmensonal sem--reducble Landsberg space equaton (2.8) (2.11) and (.1) gves H (H ) 2 H (H 2K) j 2 I 2 (H ) I I 2 (.2) I Ij 2 (I K) K K 2 (H 2K) j K K 2 (I K) K K Kj 2 I Ij (H ) (I K) K 2 (H 2K) j K Ij K Kj.
7 On four dmensonal sem--reducble Landsberg space 197 Now we assume tat non of man scalars H I K vans. To solve te connecton vectors we dvde te four dmensonal sem--reducble Fnsler space n followng fve classes (I) H 2K (II) H 2K (III) H 2K (IV) H 2K (V) H 2K. For a sem--reducble Landsberg space equatons (2.10) and (2.8) gve H 1 I 1 K 1 1 j 1 0 and K 1 0 provded K I. Under te restrcton of class (I) usng te fact H I K L t follows from relaton (.2) tat 2 j 2 H I 2 H I I K (L) K L 0 I I K (L) K L and te dentty j 0 j K 2 0 K K 2 2K Ij 2 I K K K 2 I K KI 2 IK 2 2K Holds. Terefore we ave Teorem.1. Te -connecton vectors and -covarant dervatve of () vtorson tensor jk of a four dmensonal sem--reducble Landsberg space of class (I) are gven 2 m I 2 n j 1 j 2 m K 2 2K I K [Ij 2 n K 2 p ] I K II 2 KK 2 and L jk H 2 m m j m k m n n j n k n p p j p k p 2K H (jk)(m m j m k n ) H (jk) (m m j m k p ) I (jk) (m n j n k n ) K (jk)(m p j p k p ) I 2 (jk) (m m j n k n ) K 2 (jk) (m m j p k p ) p
8 198 V. K. aubey and R. K. Dwved A (jk) (n n j p k p ) I (jk) (m n j n k p ) K (jk) (m n j p k p ) were H I K (L) 2 I K L H I K (L) j2 I K L KI 2 IK 2 and A. H H 2K By te smlar process for classes (II) (III) and (IV) of sem--reducble Landsberg space F we obtan Teorem.2. Te -connecton vectors and -covarant dervatve of () vtorson tensor jk of a four dmensonal sem--reducble Landsberg space of class (II) are gven by I 2 n j 1 p K s arbtrary and II 2 L jk H 2 m m j m k m (n n j n k n p p j p k p ) I 2 I 2 (jk)[(m m j (n k n p k p )] II 2 (jk) (n n j p k p ). Teorem.. Te -connecton vectors and -covarant dervatve of () vtorson tensor jk of four dmensonal sem--reducble Landsberg space of class (III) are gven by IK2 K2 n j 1 p 2K(I K) 2( I K) K 0 and 2 II2 K I2 L jk n n j n k n p p j p k p 2(K I) ( K I) KI2 I 2 (jk) m m j n k n (jk) (n n j p k p ). 2( K I) Furter we consder class (V). In ts case equaton (.2) gves I 2 I I 0 2 j 2 j 0 and j. Tus we ave Teorem.. If te () v-torson tensor of a four dmensonal Fnsler space F of class (V) s wrtten n te form L jk m m j m k I (jk)[(m (n j n k p j p k )] ten te man scalar I s -covarant constant. Te -connecton vectors and - covarant dervatve of () v-torson tensor jk for suc space are gven by
9 On four dmensonal sem--reducble Landsberg space 199 Dn j Dp j K s arbtrary vector and L jk DI [n n j n k n p p j p k p (jk) (n n j p k p )] were D s arbtrary scalar. Fnally we sall fnd a condton for a sem--reducble Landsberg space to be Berwald space. From teorem (1.2) equaton (2.7) and (2.8) we ave for a four dmensonal sem--reducble Berwald space (.) H I K 0. Furter f te condton (.) satsfes n a four dmensonal sem-reducble Landsberg space ten usng (.2) and (2.8) n equaton (2.7) we ave jk 0 provded H 2K does not old. Tus we ave Teorem.5. A necessary and suffcent condton for a four dmensonal sem- -reducble Landsberg space to be Berwald space s tat all te non-zero man scalars H I K are -covarant constant provded H 2K does not old. Snce H 1 0 s satsfed n sem--reducble Landsberg space from Rcc dentty t t H j H j - H t j - H t P j we ave H - H 0. Smlarly we obtan I - I 0 and K - K 0. Tus n vew of teorem (.5) we ave Teorem.6. In a four dmensonal sem--reducble Landsberg space F te followng condton are equvalent to eac oter (1) F s a Berwald space. (2) All te man scalar H I K are -covarant constant. () Man scalar H I K satsfy te relatons H 0 I 0 K 0 0 provded H 2K does not old. Acknowledgement: Frst autor s very muc tankful to NBHM-DAE for ter fnancal assstance as a Postdoctoral fellowsp. References [1] Ikeda F.: On some propertes of tree dmensonal Fnsler spaces Tensor N. S. 55 (199) [2] Matsumoto M.: Foundaton of Fnsler geometry and specal Fnsler spaces Kasesa Press Sakawa Otsu 520 Japan [] Matsumoto M. and Mron R.: On an nvarant teory of Fnsler spaces Perod Mat. Hungar 8 (1977) [] Matsumoto M. and Sbata.: On sem--reducblty T- Tensor 0 and S-lkeness of Fnsler spaces J. Mat. Kyoto Unv. 19-2(1979) 01-1.
10 200 V. K. aubey and R. K. Dwved [5] Prasad B. N. Pandey T. N. and Twar B.: On relatons of man scalars between four dmensonal Fnsler space and ts ypersurfaces. ommuncated. [6] Prasad B. N. Pandey T. N. and Jaswal A. K.: P-reducble and P- symmetrc four dmensonal Fnsler spaces accepted J. Nat. Acad. Mat. [7] Pandey T. N. and Dved D. K.: A teory of four dmensonal Fnsler spaces n terms of scalars Nat. Acad. Mat. 11 (1997) Receved: September 2012
Projective change between two Special (α, β)- Finsler Metrics
Internatonal Journal of Trend n Research and Development, Volume 2(6), ISSN 2394-9333 www.jtrd.com Projectve change between two Specal (, β)- Fnsler Metrcs Gayathr.K 1 and Narasmhamurthy.S.K 2 1 Assstant
More informationη-einstein Complex Finsler-Randers Spaces
Open Access Journal of Matematcal and Statstcal Analyss RESEARCH ARTICLE η-ensten Complex Fnsler-Randers Spaces Roopa MK * and Narasmamurty SK Department of PG Studes and Researc n Matematcs Kuvempu Unversty
More informationSome results on a cross-section in the tensor bundle
Hacettepe Journa of Matematcs and Statstcs Voume 43 3 214, 391 397 Some resuts on a cross-secton n te tensor bunde ydın Gezer and Murat tunbas bstract Te present paper s devoted to some resuts concernng
More informationRanders Space with Special Nonlinear Connection
ISSN 1995-0802, obachevsk Journal of Mathematcs, 2008, Vol. 29, No. 1, pp. 27 31. c Pleades Publshng, td., 2008. Rers Space wth Specal Nonlnear Connecton H. G. Nagaraja * (submtted by M.A. Malakhaltsev)
More informationTR/95 February Splines G. H. BEHFOROOZ* & N. PAPAMICHAEL
TR/9 February 980 End Condtons for Interpolatory Quntc Splnes by G. H. BEHFOROOZ* & N. PAPAMICHAEL *Present address: Dept of Matematcs Unversty of Tabrz Tabrz Iran. W9609 A B S T R A C T Accurate end condtons
More informationAbout Three Important Transformations Groups
About Tree Important Transformatons Groups MONICA A.P. PURCARU Translvana Unversty of Braşov Department of Matematcs Iulu Manu Street 5 591 Braşov ROMANIA m.purcaru@yaoo.com MIRELA TÂRNOVEANU Translvana
More informationABOUT THE GROUP OF TRANSFORMATIONS OF METRICAL SEMISYMMETRIC N LINEAR CONNECTIONS ON A GENERALIZED HAMILTON SPACE OF ORDER TWO
Bulletn of the Translvana Unversty of Braşov Vol 554 No. 2-202 Seres III: Mathematcs Informatcs Physcs 75-88 ABOUT THE GROUP OF TRANSFORMATIONS OF METRICAL SEMISYMMETRIC N LINEAR CONNECTIONS ON A GENERALIZED
More informationThe Order Relation and Trace Inequalities for. Hermitian Operators
Internatonal Mathematcal Forum, Vol 3, 08, no, 507-57 HIKARI Ltd, wwwm-hkarcom https://doorg/0988/mf088055 The Order Relaton and Trace Inequaltes for Hermtan Operators Y Huang School of Informaton Scence
More informationOn Pfaff s solution of the Pfaff problem
Zur Pfaff scen Lösung des Pfaff scen Probles Mat. Ann. 7 (880) 53-530. On Pfaff s soluton of te Pfaff proble By A. MAYER n Lepzg Translated by D. H. Delpenc Te way tat Pfaff adopted for te ntegraton of
More information2-π STRUCTURES ASSOCIATED TO THE LAGRANGIAN MECHANICAL SYSTEMS UDC 531.3: (045)=111. Victor Blãnuţã, Manuela Gîrţu
FACTA UNIVERSITATIS Seres: Mechancs Automatc Control and Robotcs Vol. 6 N o 1 007 pp. 89-95 -π STRUCTURES ASSOCIATED TO THE LAGRANGIAN MECHANICAL SYSTEMS UDC 531.3:53.511(045)=111 Vctor Blãnuţã Manuela
More informationStanford University CS254: Computational Complexity Notes 7 Luca Trevisan January 29, Notes for Lecture 7
Stanford Unversty CS54: Computatonal Complexty Notes 7 Luca Trevsan January 9, 014 Notes for Lecture 7 1 Approxmate Countng wt an N oracle We complete te proof of te followng result: Teorem 1 For every
More informationBernoulli Numbers and Polynomials
Bernoull Numbers and Polynomals T. Muthukumar tmk@tk.ac.n 17 Jun 2014 The sum of frst n natural numbers 1, 2, 3,..., n s n n(n + 1 S 1 (n := m = = n2 2 2 + n 2. Ths formula can be derved by notng that
More informationSL n (F ) Equals its Own Derived Group
Internatonal Journal of Algebra, Vol. 2, 2008, no. 12, 585-594 SL n (F ) Equals ts Own Derved Group Jorge Macel BMCC-The Cty Unversty of New York, CUNY 199 Chambers street, New York, NY 10007, USA macel@cms.nyu.edu
More information5 The Laplace Equation in a convex polygon
5 Te Laplace Equaton n a convex polygon Te most mportant ellptc PDEs are te Laplace, te modfed Helmoltz and te Helmoltz equatons. Te Laplace equaton s u xx + u yy =. (5.) Te real and magnary parts of an
More informationFinslerian Nonholonomic Frame For Matsumoto (α,β)-metric
Internatonal Journal of Mathematcs and Statstcs Inventon (IJMSI) E-ISSN: 2321 4767 P-ISSN: 2321-4759 ǁ Volume 2 ǁ Issue 3 ǁ March 2014 ǁ PP-73-77 Fnsleran Nonholonomc Frame For Matsumoto (α,)-metrc Mallkarjuna
More informationLecture 6/7 (February 10/12, 2014) DIRAC EQUATION. The non-relativistic Schrödinger equation was obtained by noting that the Hamiltonian 2
P470 Lecture 6/7 (February 10/1, 014) DIRAC EQUATION The non-relatvstc Schrödnger equaton was obtaned by notng that the Hamltonan H = P (1) m can be transformed nto an operator form wth the substtutons
More informationMathematical Preparations
1 Introducton Mathematcal Preparatons The theory of relatvty was developed to explan experments whch studed the propagaton of electromagnetc radaton n movng coordnate systems. Wthn expermental error the
More informationThe Finite Element Method: A Short Introduction
Te Fnte Element Metod: A Sort ntroducton Wat s FEM? Te Fnte Element Metod (FEM) ntroduced by engneers n late 50 s and 60 s s a numercal tecnque for solvng problems wc are descrbed by Ordnary Dfferental
More informationBallot Paths Avoiding Depth Zero Patterns
Ballot Paths Avodng Depth Zero Patterns Henrch Nederhausen and Shaun Sullvan Florda Atlantc Unversty, Boca Raton, Florda nederha@fauedu, ssull21@fauedu 1 Introducton In a paper by Sapounaks, Tasoulas,
More informationBOUNDEDNESS OF THE RIESZ TRANSFORM WITH MATRIX A 2 WEIGHTS
BOUNDEDNESS OF THE IESZ TANSFOM WITH MATIX A WEIGHTS Introducton Let L = L ( n, be the functon space wth norm (ˆ f L = f(x C dx d < For a d d matrx valued functon W : wth W (x postve sem-defnte for all
More informationThe finite element method explicit scheme for a solution of one problem of surface and ground water combined movement
IOP Conference Seres: Materals Scence and Engneerng PAPER OPEN ACCESS e fnte element metod explct sceme for a soluton of one problem of surface and ground water combned movement o cte ts artcle: L L Glazyrna
More informationSolution for singularly perturbed problems via cubic spline in tension
ISSN 76-769 England UK Journal of Informaton and Computng Scence Vol. No. 06 pp.6-69 Soluton for sngularly perturbed problems va cubc splne n tenson K. Aruna A. S. V. Rav Kant Flud Dynamcs Dvson Scool
More informationSOME RESULTS ON TRANSFORMATIONS GROUPS OF N-LINEAR CONNECTIONS IN THE 2-TANGENT BUNDLE
STUDIA UNIV. BABEŞ BOLYAI MATHEMATICA Volume LIII Number March 008 SOME RESULTS ON TRANSFORMATIONS GROUPS OF N-LINEAR CONNECTIONS IN THE -TANGENT BUNDLE GHEORGHE ATANASIU AND MONICA PURCARU Abstract. In
More informationGames of Threats. Elon Kohlberg Abraham Neyman. Working Paper
Games of Threats Elon Kohlberg Abraham Neyman Workng Paper 18-023 Games of Threats Elon Kohlberg Harvard Busness School Abraham Neyman The Hebrew Unversty of Jerusalem Workng Paper 18-023 Copyrght 2017
More informationENERGY-DEPENDENT MINKOWSKI METRIC IN SPACE-TIME
ENERGY-DEPENDENT MINKOWSKI METRIC IN SPACE-TIME R. Mron, A. Jannusss and G. Zet Abstract The geometrcal propertes of the space-tme endowed wth a metrc dependng on the energy E of the consdered process
More informationLectures - Week 4 Matrix norms, Conditioning, Vector Spaces, Linear Independence, Spanning sets and Basis, Null space and Range of a Matrix
Lectures - Week 4 Matrx norms, Condtonng, Vector Spaces, Lnear Independence, Spannng sets and Bass, Null space and Range of a Matrx Matrx Norms Now we turn to assocatng a number to each matrx. We could
More informationELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM
ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM An elastc wave s a deformaton of the body that travels throughout the body n all drectons. We can examne the deformaton over a perod of tme by fxng our look
More informationVanishing S-curvature of Randers spaces
Vanshng S-curvature of Randers spaces Shn-ch OHTA Department of Mathematcs, Faculty of Scence, Kyoto Unversty, Kyoto 606-850, JAPAN (e-mal: sohta@math.kyoto-u.ac.jp) December 31, 010 Abstract We gve a
More informationA Global Approach to Absolute Parallelism Geometry
A Global Approac to Absolute Parallelsm Geometry Nabl L. Youssef 1,2 and Waleed A. Elsayed 1,2 arxv:1209.1379v4 [gr-qc] 15 Jul 2013 1 Department of Matematcs, Faculty of Scence, Caro Unversty, Gza, Egypt
More informationAffine and Riemannian Connections
Affne and Remannan Connectons Semnar Remannan Geometry Summer Term 2015 Prof Dr Anna Wenhard and Dr Gye-Seon Lee Jakob Ullmann Notaton: X(M) space of smooth vector felds on M D(M) space of smooth functons
More informationON THE JACOBIAN CONJECTURE
v v v Far East Journal of Mathematcal Scences (FJMS) 17 Pushpa Publshng House, Allahabad, Inda http://www.pphm.com http://dx.do.org/1.17654/ms1111565 Volume 11, Number 11, 17, Pages 565-574 ISSN: 97-871
More informationAppendix for Causal Interaction in Factorial Experiments: Application to Conjoint Analysis
A Appendx for Causal Interacton n Factoral Experments: Applcaton to Conjont Analyss Mathematcal Appendx: Proofs of Theorems A. Lemmas Below, we descrbe all the lemmas, whch are used to prove the man theorems
More informationFoundations of Arithmetic
Foundatons of Arthmetc Notaton We shall denote the sum and product of numbers n the usual notaton as a 2 + a 2 + a 3 + + a = a, a 1 a 2 a 3 a = a The notaton a b means a dvdes b,.e. ac = b where c s an
More information8.4 COMPLEX VECTOR SPACES AND INNER PRODUCTS
SECTION 8.4 COMPLEX VECTOR SPACES AND INNER PRODUCTS 493 8.4 COMPLEX VECTOR SPACES AND INNER PRODUCTS All the vector spaces you have studed thus far n the text are real vector spaces because the scalars
More informationFINITELY-GENERATED MODULES OVER A PRINCIPAL IDEAL DOMAIN
FINITELY-GENERTED MODULES OVER PRINCIPL IDEL DOMIN EMMNUEL KOWLSKI Throughout ths note, s a prncpal deal doman. We recall the classfcaton theorem: Theorem 1. Let M be a fntely-generated -module. (1) There
More informationSalmon: Lectures on partial differential equations. Consider the general linear, second-order PDE in the form. ,x 2
Salmon: Lectures on partal dfferental equatons 5. Classfcaton of second-order equatons There are general methods for classfyng hgher-order partal dfferental equatons. One s very general (applyng even to
More informationDeterminants Containing Powers of Generalized Fibonacci Numbers
1 2 3 47 6 23 11 Journal of Integer Sequences, Vol 19 (2016), Artcle 1671 Determnants Contanng Powers of Generalzed Fbonacc Numbers Aram Tangboonduangjt and Thotsaporn Thanatpanonda Mahdol Unversty Internatonal
More informationLagrangian Field Theory
Lagrangan Feld Theory Adam Lott PHY 391 Aprl 6, 017 1 Introducton Ths paper s a summary of Chapter of Mandl and Shaw s Quantum Feld Theory [1]. The frst thng to do s to fx the notaton. For the most part,
More informationFedosov s approach to deformation quantization
Fedosov s approac to deformaton quantzaton Sean Poorence Introducton In classcal mecancs te order of measurements does not affect te results of te measurements. However, trougout te 19t and early 20t centures,
More information338 A^VÇÚO 1n ò Lke n Mancn (211), we make te followng assumpton to control te beavour of small jumps. Assumpton 1.1 L s symmetrc α-stable, were α (,
A^VÇÚO 1n ò 1oÏ 215c8 Cnese Journal of Appled Probablty and Statstcs Vol.31 No.4 Aug. 215 Te Speed of Convergence of te Tresold Verson of Bpower Varaton for Semmartngales Xao Xaoyong Yn Hongwe (Department
More informationare called the contravariant components of the vector a and the a i are called the covariant components of the vector a.
Non-Cartesan Coordnates The poston of an arbtrary pont P n space may be expressed n terms of the three curvlnear coordnates u 1,u,u 3. If r(u 1,u,u 3 ) s the poston vector of the pont P, at every such
More information3.1 Expectation of Functions of Several Random Variables. )' be a k-dimensional discrete or continuous random vector, with joint PMF p (, E X E X1 E X
Statstcs 1: Probablty Theory II 37 3 EPECTATION OF SEVERAL RANDOM VARIABLES As n Probablty Theory I, the nterest n most stuatons les not on the actual dstrbuton of a random vector, but rather on a number
More informationCONDITIONS FOR INVARIANT SUBMANIFOLD OF A MANIFOLD WITH THE (ϕ, ξ, η, G)-STRUCTURE. Jovanka Nikić
147 Kragujevac J. Math. 25 (2003) 147 154. CONDITIONS FOR INVARIANT SUBMANIFOLD OF A MANIFOLD WITH THE (ϕ, ξ, η, G)-STRUCTURE Jovanka Nkć Faculty of Techncal Scences, Unversty of Nov Sad, Trg Dosteja Obradovća
More information9 Characteristic classes
THEODORE VORONOV DIFFERENTIAL GEOMETRY. Sprng 2009 [under constructon] 9 Characterstc classes 9.1 The frst Chern class of a lne bundle Consder a complex vector bundle E B of rank p. We shall construct
More informationPerron Vectors of an Irreducible Nonnegative Interval Matrix
Perron Vectors of an Irreducble Nonnegatve Interval Matrx Jr Rohn August 4 2005 Abstract As s well known an rreducble nonnegatve matrx possesses a unquely determned Perron vector. As the man result of
More informationBezier curves. Michael S. Floater. August 25, These notes provide an introduction to Bezier curves. i=0
Bezer curves Mchael S. Floater August 25, 211 These notes provde an ntroducton to Bezer curves. 1 Bernsten polynomals Recall that a real polynomal of a real varable x R, wth degree n, s a functon of the
More informationSrednicki Chapter 34
Srednck Chapter 3 QFT Problems & Solutons A. George January 0, 203 Srednck 3.. Verfy that equaton 3.6 follows from equaton 3.. We take Λ = + δω: U + δω ψu + δω = + δωψ[ + δω] x Next we use equaton 3.3,
More information5 The Rational Canonical Form
5 The Ratonal Canoncal Form Here p s a monc rreducble factor of the mnmum polynomal m T and s not necessarly of degree one Let F p denote the feld constructed earler n the course, consstng of all matrces
More informationA Discrete Approach to Continuous Second-Order Boundary Value Problems via Monotone Iterative Techniques
Internatonal Journal of Dfference Equatons ISSN 0973-6069, Volume 12, Number 1, pp. 145 160 2017) ttp://campus.mst.edu/jde A Dscrete Approac to Contnuous Second-Order Boundary Value Problems va Monotone
More informationCausal Diamonds. M. Aghili, L. Bombelli, B. Pilgrim
Causal Damonds M. Aghl, L. Bombell, B. Plgrm Introducton The correcton to volume of a causal nterval due to curvature of spacetme has been done by Myrhem [] and recently by Gbbons & Solodukhn [] and later
More informationThe Parity of the Number of Irreducible Factors for Some Pentanomials
The Party of the Nuber of Irreducble Factors for Soe Pentanoals Wolfra Koepf 1, Ryul K 1 Departent of Matheatcs Unversty of Kassel, Kassel, F. R. Gerany Faculty of Matheatcs and Mechancs K Il Sung Unversty,
More information7. Products and matrix elements
7. Products and matrx elements 1 7. Products and matrx elements Based on the propertes of group representatons, a number of useful results can be derved. Consder a vector space V wth an nner product ψ
More informationSpecial Relativity and Riemannian Geometry. Department of Mathematical Sciences
Tutoral Letter 06//018 Specal Relatvty and Reannan Geoetry APM3713 Seester Departent of Matheatcal Scences IMPORTANT INFORMATION: Ths tutoral letter contans the solutons to Assgnent 06. BAR CODE Learn
More informationSolving Singularly Perturbed Differential Difference Equations via Fitted Method
Avalable at ttp://pvamu.edu/aam Appl. Appl. Mat. ISSN: 193-9466 Vol. 8, Issue 1 (June 013), pp. 318-33 Applcatons and Appled Matematcs: An Internatonal Journal (AAM) Solvng Sngularly Perturbed Dfferental
More informationNot-for-Publication Appendix to Optimal Asymptotic Least Aquares Estimation in a Singular Set-up
Not-for-Publcaton Aendx to Otmal Asymtotc Least Aquares Estmaton n a Sngular Set-u Antono Dez de los Ros Bank of Canada dezbankofcanada.ca December 214 A Proof of Proostons A.1 Proof of Prooston 1 Ts roof
More informationGELFAND-TSETLIN BASIS FOR THE REPRESENTATIONS OF gl n
GELFAND-TSETLIN BASIS FOR THE REPRESENTATIONS OF gl n KANG LU FINITE DIMENSIONAL REPRESENTATIONS OF gl n Let e j,, j =,, n denote the standard bass of the general lnear Le algebra gl n over the feld of
More informationCHAPTER 5: Lie Differentiation and Angular Momentum
CHAPTER 5: Le Dfferentaton and Angular Momentum Jose G. Vargas 1 Le dfferentaton Kähler s theory of angular momentum s a specalzaton of hs approach to Le dfferentaton. We could deal wth the former drectly,
More informationFACTORIZATION IN KRULL MONOIDS WITH INFINITE CLASS GROUP
C O L L O Q U I U M M A T H E M A T I C U M VOL. 80 1999 NO. 1 FACTORIZATION IN KRULL MONOIDS WITH INFINITE CLASS GROUP BY FLORIAN K A I N R A T H (GRAZ) Abstract. Let H be a Krull monod wth nfnte class
More informationA CHARACTERIZATION OF ADDITIVE DERIVATIONS ON VON NEUMANN ALGEBRAS
Journal of Mathematcal Scences: Advances and Applcatons Volume 25, 2014, Pages 1-12 A CHARACTERIZATION OF ADDITIVE DERIVATIONS ON VON NEUMANN ALGEBRAS JIA JI, WEN ZHANG and XIAOFEI QI Department of Mathematcs
More informationn α j x j = 0 j=1 has a nontrivial solution. Here A is the n k matrix whose jth column is the vector for all t j=0
MODULE 2 Topcs: Lnear ndependence, bass and dmenson We have seen that f n a set of vectors one vector s a lnear combnaton of the remanng vectors n the set then the span of the set s unchanged f that vector
More informationAdaptive Kernel Estimation of the Conditional Quantiles
Internatonal Journal of Statstcs and Probablty; Vol. 5, No. ; 206 ISSN 927-7032 E-ISSN 927-7040 Publsed by Canadan Center of Scence and Educaton Adaptve Kernel Estmaton of te Condtonal Quantles Rad B.
More informationProblem Set 4: Sketch of Solutions
Problem Set 4: Sketc of Solutons Informaton Economcs (Ec 55) George Georgads Due n class or by e-mal to quel@bu.edu at :30, Monday, December 8 Problem. Screenng A monopolst can produce a good n dfferent
More informationCOMPARISON OF SOME RELIABILITY CHARACTERISTICS BETWEEN REDUNDANT SYSTEMS REQUIRING SUPPORTING UNITS FOR THEIR OPERATIONS
Avalable onlne at http://sck.org J. Math. Comput. Sc. 3 (3), No., 6-3 ISSN: 97-537 COMPARISON OF SOME RELIABILITY CHARACTERISTICS BETWEEN REDUNDANT SYSTEMS REQUIRING SUPPORTING UNITS FOR THEIR OPERATIONS
More informationCS 468 Lecture 16: Isometry Invariance and Spectral Techniques
CS 468 Lecture 16: Isometry Invarance and Spectral Technques Justn Solomon Scrbe: Evan Gawlk Introducton. In geometry processng, t s often desrable to characterze the shape of an object n a manner that
More informationBézier curves. Michael S. Floater. September 10, These notes provide an introduction to Bézier curves. i=0
Bézer curves Mchael S. Floater September 1, 215 These notes provde an ntroducton to Bézer curves. 1 Bernsten polynomals Recall that a real polynomal of a real varable x R, wth degree n, s a functon of
More informationThe Jacobsthal and Jacobsthal-Lucas Numbers via Square Roots of Matrices
Internatonal Mathematcal Forum, Vol 11, 2016, no 11, 513-520 HIKARI Ltd, wwwm-hkarcom http://dxdoorg/1012988/mf20166442 The Jacobsthal and Jacobsthal-Lucas Numbers va Square Roots of Matrces Saadet Arslan
More informationThe Multiple Classical Linear Regression Model (CLRM): Specification and Assumptions. 1. Introduction
ECONOMICS 5* -- NOTE (Summary) ECON 5* -- NOTE The Multple Classcal Lnear Regresson Model (CLRM): Specfcaton and Assumptons. Introducton CLRM stands for the Classcal Lnear Regresson Model. The CLRM s also
More informationOn quasiperfect numbers
Notes on Number Theory and Dscrete Mathematcs Prnt ISSN 1310 5132, Onlne ISSN 2367 8275 Vol. 23, 2017, No. 3, 73 78 On quasperfect numbers V. Sva Rama Prasad 1 and C. Suntha 2 1 Nalla Malla Reddy Engneerng
More informationAPPENDIX A Some Linear Algebra
APPENDIX A Some Lnear Algebra The collecton of m, n matrces A.1 Matrces a 1,1,..., a 1,n A = a m,1,..., a m,n wth real elements a,j s denoted by R m,n. If n = 1 then A s called a column vector. Smlarly,
More informationTHEORY OF FINSLER SUBMANIFOLDS VIA BERWALD CONNECTION
Internatonal Electronc Journal of Geometry Volume 7 No. 1 pp. 108 125 (2014) c IEJG THEORY OF FINSLER SUBMANIFOLDS VIA BERWALD CONNECTION AUREL BEJANCU AND HANI REDA FARRAN Dedcated to memory of Proffessor
More informationHila Etzion. Min-Seok Pang
RESERCH RTICLE COPLEENTRY ONLINE SERVICES IN COPETITIVE RKETS: INTINING PROFITILITY IN THE PRESENCE OF NETWORK EFFECTS Hla Etzon Department of Technology and Operatons, Stephen. Ross School of usness,
More information763622S ADVANCED QUANTUM MECHANICS Solution Set 1 Spring c n a n. c n 2 = 1.
7636S ADVANCED QUANTUM MECHANICS Soluton Set 1 Sprng 013 1 Warm-up Show that the egenvalues of a Hermtan operator  are real and that the egenkets correspondng to dfferent egenvalues are orthogonal (b)
More informationKey Words: Hamiltonian systems, canonical integrators, symplectic integrators, Runge-Kutta-Nyström methods.
CANONICAL RUNGE-KUTTA-NYSTRÖM METHODS OF ORDERS 5 AND 6 DANIEL I. OKUNBOR AND ROBERT D. SKEEL DEPARTMENT OF COMPUTER SCIENCE UNIVERSITY OF ILLINOIS AT URBANA-CHAMPAIGN 304 W. SPRINGFIELD AVE. URBANA, ILLINOIS
More informationVARIATION OF CONSTANT SUM CONSTRAINT FOR INTEGER MODEL WITH NON UNIFORM VARIABLES
VARIATION OF CONSTANT SUM CONSTRAINT FOR INTEGER MODEL WITH NON UNIFORM VARIABLES BÂRZĂ, Slvu Faculty of Mathematcs-Informatcs Spru Haret Unversty barza_slvu@yahoo.com Abstract Ths paper wants to contnue
More informationCENTROID (AĞIRLIK MERKEZİ )
CENTOD (ĞLK MEKEZİ ) centrod s a geometrcal concept arsng from parallel forces. Tus, onl parallel forces possess a centrod. Centrod s tougt of as te pont were te wole wegt of a pscal od or sstem of partcles
More informationIranian Journal of Mathematical Chemistry, Vol. 5, No.2, November 2014, pp
Iranan Journal of Matematcal Cemstry, Vol. 5, No.2, November 204, pp. 85 90 IJMC Altan dervatves of a grap I. GUTMAN (COMMUNICATED BY ALI REZA ASHRAFI) Faculty of Scence, Unversty of Kragujevac, P. O.
More informationThe Pseudoblocks of Endomorphism Algebras
Internatonal Mathematcal Forum, 4, 009, no. 48, 363-368 The Pseudoblocks of Endomorphsm Algebras Ahmed A. Khammash Department of Mathematcal Scences, Umm Al-Qura Unversty P.O.Box 796, Makkah, Saud Araba
More informationCanonical transformations
Canoncal transformatons November 23, 2014 Recall that we have defned a symplectc transformaton to be any lnear transformaton M A B leavng the symplectc form nvarant, Ω AB M A CM B DΩ CD Coordnate transformatons,
More informationMATH 241B FUNCTIONAL ANALYSIS - NOTES EXAMPLES OF C ALGEBRAS
MATH 241B FUNCTIONAL ANALYSIS - NOTES EXAMPLES OF C ALGEBRAS These are nformal notes whch cover some of the materal whch s not n the course book. The man purpose s to gve a number of nontrval examples
More informationON A DETERMINATION OF THE INITIAL FUNCTIONS FROM THE OBSERVED VALUES OF THE BOUNDARY FUNCTIONS FOR THE SECOND-ORDER HYPERBOLIC EQUATION
Advanced Mathematcal Models & Applcatons Vol.3, No.3, 2018, pp.215-222 ON A DETERMINATION OF THE INITIAL FUNCTIONS FROM THE OBSERVED VALUES OF THE BOUNDARY FUNCTIONS FOR THE SECOND-ORDER HYPERBOLIC EUATION
More informationTAIL BOUNDS FOR SUMS OF GEOMETRIC AND EXPONENTIAL VARIABLES
TAIL BOUNDS FOR SUMS OF GEOMETRIC AND EXPONENTIAL VARIABLES SVANTE JANSON Abstract. We gve explct bounds for the tal probabltes for sums of ndependent geometrc or exponental varables, possbly wth dfferent
More informationMULTIPLICATIVE FUNCTIONS: A REWRITE OF ANDREWS CHAPTER 6
MULTIPLICATIVE FUNCTIONS: A REWRITE OF ANDREWS CHAPTER 6 In these notes we offer a rewrte of Andrews Chapter 6. Our am s to replace some of the messer arguments n Andrews. To acheve ths, we need to change
More informationNATURAL 2-π STRUCTURES IN LAGRANGE SPACES
AALELE ŞTIIŢIFICE ALE UIVERSITĂŢII AL.I. CUZA DI IAŞI (S.. MATEMATICĂ, Tomul LIII, 2007, Suplment ATURAL 2-π STRUCTURES I LAGRAGE SPACES Y VICTOR LĂUŢA AD VALER IMIEŢ Dedcated to Academcan Radu Mron at
More informationAppendix B. Criterion of Riemann-Stieltjes Integrability
Appendx B. Crteron of Remann-Steltes Integrablty Ths note s complementary to [R, Ch. 6] and [T, Sec. 3.5]. The man result of ths note s Theorem B.3, whch provdes the necessary and suffcent condtons for
More informationA Spline based computational simulations for solving selfadjoint singularly perturbed two-point boundary value problems
ISSN 746-769 England UK Journal of Informaton and Computng Scence Vol. 7 No. 4 pp. 33-34 A Splne based computatonal smulatons for solvng selfadjont sngularly perturbed two-pont boundary value problems
More informationScreen transversal conformal half-lightlike submanifolds
Annals of the Unversty of Craova, Mathematcs and Computer Scence Seres Volume 40(2), 2013, Pages 140 147 ISSN: 1223-6934 Screen transversal conformal half-lghtlke submanfolds Wenje Wang, Yanng Wang, and
More informationM-LINEAR CONNECTION ON THE SECOND ORDER REONOM BUNDLE
STUDIA UNIV. AEŞ OLYAI, MATHEMATICA, Volume XLVI, Number 3, September 001 M-LINEAR CONNECTION ON THE SECOND ORDER REONOM UNDLE VASILE LAZAR Abstract. The T M R bundle represents the total space of a tme
More informationSmarandache-Zero Divisors in Group Rings
Smarandache-Zero Dvsors n Group Rngs W.B. Vasantha and Moon K. Chetry Department of Mathematcs I.I.T Madras, Chenna The study of zero-dvsors n group rngs had become nterestng problem snce 1940 wth the
More informationCENTROID (AĞIRLIK MERKEZİ )
CENTOD (ĞLK MEKEZİ ) centrod s a geometrcal concept arsng from parallel forces. Tus, onl parallel forces possess a centrod. Centrod s tougt of as te pont were te wole wegt of a pscal od or sstem of partcles
More informationApplied Mathematics Letters. On equitorsion geodesic mappings of general affine connection spaces onto generalized Riemannian spaces
Appled Mathematcs Letters (0) 665 67 Contents lsts avalable at ScenceDrect Appled Mathematcs Letters journal homepage: www.elsever.com/locate/aml On equtorson geodesc mappngs of general affne connecton
More informationA note on almost sure behavior of randomly weighted sums of φ-mixing random variables with φ-mixing weights
ACTA ET COMMENTATIONES UNIVERSITATIS TARTUENSIS DE MATHEMATICA Volume 7, Number 2, December 203 Avalable onlne at http://acutm.math.ut.ee A note on almost sure behavor of randomly weghted sums of φ-mxng
More informationStructure and Drive Paul A. Jensen Copyright July 20, 2003
Structure and Drve Paul A. Jensen Copyrght July 20, 2003 A system s made up of several operatons wth flow passng between them. The structure of the system descrbes the flow paths from nputs to outputs.
More informationOpen Systems: Chemical Potential and Partial Molar Quantities Chemical Potential
Open Systems: Chemcal Potental and Partal Molar Quanttes Chemcal Potental For closed systems, we have derved the followng relatonshps: du = TdS pdv dh = TdS + Vdp da = SdT pdv dg = VdP SdT For open systems,
More informationPoisson brackets and canonical transformations
rof O B Wrght Mechancs Notes osson brackets and canoncal transformatons osson Brackets Consder an arbtrary functon f f ( qp t) df f f f q p q p t But q p p where ( qp ) pq q df f f f p q q p t In order
More informationPHYS 705: Classical Mechanics. Calculus of Variations II
1 PHYS 705: Classcal Mechancs Calculus of Varatons II 2 Calculus of Varatons: Generalzaton (no constrant yet) Suppose now that F depends on several dependent varables : We need to fnd such that has a statonary
More informationh-analogue of Fibonacci Numbers
h-analogue of Fbonacc Numbers arxv:090.0038v [math-ph 30 Sep 009 H.B. Benaoum Prnce Mohammad Unversty, Al-Khobar 395, Saud Araba Abstract In ths paper, we ntroduce the h-analogue of Fbonacc numbers for
More informationAn efficient algorithm for multivariate Maclaurin Newton transformation
Annales UMCS Informatca AI VIII, 2 2008) 5 14 DOI: 10.2478/v10065-008-0020-6 An effcent algorthm for multvarate Maclaurn Newton transformaton Joanna Kapusta Insttute of Mathematcs and Computer Scence,
More informationDIFFERENTIAL FORMS BRIAN OSSERMAN
DIFFERENTIAL FORMS BRIAN OSSERMAN Dfferentals are an mportant topc n algebrac geometry, allowng the use of some classcal geometrc arguments n the context of varetes over any feld. We wll use them to defne
More informationMore metrics on cartesian products
More metrcs on cartesan products If (X, d ) are metrc spaces for 1 n, then n Secton II4 of the lecture notes we defned three metrcs on X whose underlyng topologes are the product topology The purpose of
More informationOn a nonlinear compactness lemma in L p (0, T ; B).
On a nonlnear compactness lemma n L p (, T ; B). Emmanuel Matre Laboratore de Matématques et Applcatons Unversté de Haute-Alsace 4, rue des Frères Lumère 6893 Mulouse E.Matre@ua.fr 3t February 22 Abstract
More information