Magnetic symmetry of the plain domain walls. in ferro- and ferrimagnets

Size: px
Start display at page:

Download "Magnetic symmetry of the plain domain walls. in ferro- and ferrimagnets"

Transcription

1 Magetic syety of the plai doai walls i feo- ad feiagets. M. Taygi ad O. V. Tycho * Kyiv Taas Shevcheo Natioal Uivesity, Radiophysics Faculty, lushov av., build.5, Kyiv, Uaie, 00 E-ail: b..taygi@gail.co E-ail: pasat@uiv.iev.ua Abstact. Magetic syety of all possible plae doai walls i feo- ad feiagets is cosideed. Magetic syety classes of o 80 degee (icludig 0 degee) doai walls ae obtaied. The doai walls degeeacy is ivestigated. The syety classificatio is applied fo eseach of all possible plae doai walls i cystals of the hexoctahedal cystallogaphic class. PACS: 6.50 Ah, Ch Keywods: doai wall type, syety tasfoatio, agetic syety class, degeeacy. Itoductio The ivestigatio of static ad dyaic popeties [,] of doai walls (Ds) i agetically odeed edia is of cosideable iteest fo the physical udestadig of ediu behavio ad it is also ipotat fo applicatios. Fo sequetial exaiatio of these popeties it is ecessay to tae ito accout the agetic syety [3,4] of the edia. Deteiatio of the D agetic syety allows *Coespodig autho. O.V. Tycho. Addess: 64 Vladiisaya st., Taas Shevcheo Kyiv Natioal Uivesity, Radiophysics Faculty Kyiv, Uaie. Tel/fax: E-ail: pasat@uiv.iev.ua, a.tycho@ail.u

2 to chaacteize qualitatively soe eleets of the D stuctue ad thei chage. The coplete syety classificatio of plae 80 degee Ds (80 0 -Ds) i agetically odeed cystals [5] ad siila classificatio of these Ds with loch lies i feoagets ad feites [6] wee caied out ealie. The plae Ds with width δ [,7] exceedig the chaacteistic size a of a uit agetic cell wee cosideed. Popeties of these Ds i feo- ad feiagets ae descibed by the desity of agetic oet M [8]. Thei syety ca be chaacteized by the agetic syety classes (MSCs) [9] of a cystal cotaiig a D [5]. The buildig of a totality of the MSCs of all possible [] plae (i.e. D with 0 >> δ, whee 0 is the cuvatue adius of the D [5]) Ds i feo- ad feiagets is the pupose of this wo.. Doai wall syety i the agetically odeed edia Let be the uit tie-odd axial vecto [9] alog the agetizatio vecto M: = M / M, whee M is the satuatio agetizatio. The ad ae uit tie-odd axial vectos alog agetizatio vectos M ad M i eighboig doais: = M / M, = M / M. The vectos ad coicide with diffeet easy agetizatio axes (EMA) of the ediu. The agle α betwee these vectos deteies the D type ( α -D): = accos( ) α. A uit pola tie-eve vecto idicates the D plae oal. It is diected fo doai with to doai with. I ode to defie the uified co-odiate syste we itoduce the vectos a ad a as well as the paaetes b = [ ] ad = [ ] [ e ~ e~, e~ ] [ a, a, ] b. The uit vectos of the co-odicate syste O ~ xy ~ ~ z ae chose as x, y z =. Hee the uit vecto ( ) (at b 0 ad = 0 b ) o [ ] with the diectio of vecto ( ) (at 0 a coicides with the diectio of the vecto a (at b = 0 o b 0 ). The uit vecto a coicides b ) o [ ] a (at b 0 ad b = 0 ) o else with a abitay diectio i the D plae ( a at b = b = 0 ). The tie-odd axial vectos ad ae deteied by equalities = ad = + espectively.

3 The MSC (hee is a MSC ube) of a α -D is the agetic syety goup icludig all syety tasfoatios (hee ad heeiafte all taslatios ae cosideed as uit opeatios) that do ot chage the spatial distibutio of agetic oets i the cystal with D [5]. The aboveetioed goup is a subgoup of the agetic (Shubiov s) syety goup of the cystal paaagetic phase [0]. These tasfoatios do ot chage D bouday coditios ad ca be classified by two types [5]. The fist type tasfoatios ( ) g do ot chage the diectios of the vectos 3, ad : ( ) g =, ( ) g =, g ( ) =. The secod type tasfoatios ( g ) chage these diectios: ( ) g, = ( ) g =, g ( ) =. I cofoity with the teiology of [6] the MSC of D bouday coditios is the totality of all tasfoatios of the agetic syety goup of the cystal paaagetic phase that satisfy the etioed six coditios. It is the MSC of the axiu possible syety of a α -D i the give cystal fo a paticula utual oietatio of the vectos, ad. The othe possible MSCs of a α -D with fixed diectios of the vectos, ad esult by eueatio of the subgoups of :, whee P is the MSC P of the cystal paaagetic phase. The utual oietatio of the vectos, ad is deteied by the set of paaetes a ( ), a = ( ), a ( ) = C =, b ad C b, whee tie-eve axial vecto is deteied by equality = [ ] C C. The possible MSCs α -Ds with α 80 0 ae peseted i table. ( 4) of Ds wee foud ealie [5]. All possible MSCs of Fo a cetai α -D the diffeet MSCs ae diffeet goups of agetic poit syety tasfoatios. Thei epesetatios [,5] ae witte i the co-odiate syste O ~ xy ~ ~ z. All epeseted MSCs ae ot iteelated by a otatio ove a abitay agle aoud. Also the aboveetioed MSCs ae ot educed with each othe by uit vectos tasfoatio a a. The possible tasfoatios ( ) g o ( ) g (colu Syety eleets of table ) of α -Ds with α 80 0 ae otatios aoud two-fold syety axes, o, o else, that ae

4 colliea with the uit vectos o a o else a, espectively, eflectios i plaes, o o else 4, that ae oal to the above etioed vectos, espectively, otatios aoud thee-, fou-, sixfold syety axes 3, 4, 6 that ae colliea with the vecto, otatios aoud thee-, fou-, sixfold ivesio axes 3, 4, 6 that ae colliea with the vecto, ivesio i the syety cete ad idetity (syety eleet ). Hee a accet at syety eleets eas a siultaeous use of the tie evesal opeatio R [9]. Fo MSCs with 4 39 ad 5 64 oly geeative syety eleets [] ae epeseted i table. Thee is a coespodece betwee MSCs of 80 -Ds (i.e. at = []), 0 -Ds (i.e. at = [3]) ad α -Ds with o-colliea oietatio of vectos ad [] (heeiafte the last Ds will be aed as α -Ds). The above etioed deteiatios of citeios fo tasfoatios ( ) g ad ( ) g ca be epeseted i aothe idetical fo: ( ) g =, ( ) g =, ( ) g = ad ( ) g, = ( ) g =, g ( ) =. These citeios estict a eseble of MSCs syety tasfoatios fo a abitay α -D. e have = 0 ad = 0 fo 0 - ad 80 -Ds, espectively. A pai fo the above etioed citeios does ot estict the MSCs syety tasfoatios of 0 - o 80 -Ds. Theefoe the agetic syety of α -Ds does ot exceed the agetic syety of 0 - ad 80 -Ds geeically. The MSCs of 80 -Ds ae the MSCs of α - Ds if thei tasfoatios do ot bea the syety of the vecto of the α -D (i.e. these MSCs ust be subgoup of the goup /, whee the ifiite-fold syety axis is colliea with the vecto ). Thee is a aalogy betwee MSCs of 80 - ad 0 -Ds: thei tasfoatios ( ) g ae the sae sice they belog to a subgoup of axial tie-odd vecto syety goup (MSC / ), whee the ifiite-fold syety axis is colliea with MSCs cosist of the tasfoatios o fo 80 - o 0 -Ds, espectively. Theefoe if ( ) g oly the these MSCs ae coo fo 80 - ad 0 -Ds. They ae aed with sig - i colu D cete of table. A covesio of MSC of 80 -D ito MSC

5 of 0 -D is siply a chage of the citeio ( ) g = by the citeio g ( ) 5 =. The tasfoatios of coespodig MSCs of these α -Ds ae diffeet by the substitutio g ( ) ( ) g oly. Theefoe, if a pai of MSCs of 80 -Ds ad a pai of MSCs of 0 -Ds is coected by the above-etioed substitutio, the these MSCs ae coo fo 80 - ad 0 -Ds. As a esult the lists of MSCs of 0 -, 80 - ad α -Ds ae itesected i geeal. Total ube of MSCs of a α -D with abitay α value (icludig α =80 0 ) i feo- ad feiagets is equal to 64. eeal eueatio of MSCs of 80 -Ds cotais 4 MSCs: 4 [5]. This eueatio holds also fo MSCs of α -D with α 80 (MSC ubes ae bold type i colu MSC ube of table ). Thee ae 0 MSCs of α -Ds: 7 3 ad 6 8. The geeal list of MSCs of 0 -Ds icludes all 4 MSCs of table : =, 6 3, R, =, 4, 6, 30, 3, 37, 39 ad 3. Doai wall stuctue The α -Ds with δ >> a i feo- ad feiagets ae descibed by the acoscopic desity of agetic oet M( z ~ ) [5]. The tasfoatios ( ) g ad ( ) ( ) g ( g ; ( ) g ) ipose estictios o the id of coodiate depedece of ( z~ ) copoets ( ( ~ z ) ( ~ z ) ( ~ z ) ( ~ ~ + ~ + ~ z ) = ) i the D volue ad allow to fid this depedece [5]. Fo the deteiatio of the id of coodiate depedece of ( z~ ) copoet of 0 - ad α -Ds fo each MSC (colu Coodiate depedeces of ( z~ ) x y z copoets i table ) the ext ules ae used: a) if a axial tie-odd vecto alog uit vectos e ( x ~, y ~ o z ~ ) is ot a ivaiat of the tasfoatio ( ) g the thee is o copoet ( ~ z ) (figue (-) i colu Coodiate depedeces of ( z~ ) copoets of table ); b) if the axial tie-odd vecto alog e is iveted by the tasfoatio ( ) g the the copoet ( ~ z ) is a odd (A) fuctio of coodiate z ~ ; c) if the axial tie-odd vecto alog e is a ivaiat of the tasfoatio ( ) g the ( ~ z ) is a eve (S) fuctio of coodiate ~ z ; d) if the axial tie-odd vecto alog the tasfoatio ( ) g the tasfoatio ( ) g does ot estict the id of fuctio ( ~ z ) e is a ivaiat of (A,S).

6 If the MCS of a α -D icludes tasfoatios that taspose adjacet agetic doais the this D has a cete of syety [5]. These MSCs eclose the syety tasfoatios g aed by coodiate ~ z = 0 i colu D cete of table. ( ) 6. They ae As i the case of Ds [5], the Ds ca be pulsatig (i.e. D with colliea diectios of vectos M ad M cost i its volue [5]) Ds. The MSCs with =, 6, 9-45, descibe syety of pulsatig Ds oly. I cotast with 80 - ad 0 -Ds thee ae o pulsatig Ds aog the α -Ds, sice α -Ds equie the pesece of two ozeo ( z~ ) copoets. The α -Ds ae otay (i.e. D with M =cost i its volue) o sei-otay [5] Ds oly. Aog otay o seiotay Ds thee ae Ds with oly loch (i.e Ds with M =cost) [,4] ( =7, 8 o 46) ad oly Neel (i.e. Ds with otatio i the plae cotaiig ) [,5] ( =9,, 7 o 47) laws of otatio i thei volue. Cystal agetic odeig is accopaied by phase tasitio ad chage of cystal agetic syety [3]. I a agetically odeed cystal q -ultiply degeeate α -Ds with fixed α ca be obtaied [6], whee q = od( )/od( ). Fuctios od ( ) ad ( ) P P od give the ode [] of the agetic poit goup of the cystal paaagetic phase [9,0] ad of a α -D i this cystal, espectively. These α -Ds have the sae eegy but diffeet stuctues (agetizatio distibutio, plae oietatio, etc.). The iiu value of tie evesal opeatio R. q is i accodace with the ivaiace of eegy fo At epesetatio of the P as the totality of (with fixed value ad diffeet syety eleets oietatios) the lost tasfoatios (ebes of adjacet classes) l g [6,] iteelate the above etioed q -ultiply degeeate α -Ds (i.e. ito aothe). l g opeatio covets a oe of such α -Ds The degeeacy q of a α -D ca be witte i the fo q = qq ( q q ), whee ( )/od( ) q = od is the ube of equal-eegy α -Ds with fixed bouday coditios,

7 q = od( )/od( ) is the ube of possible bouday coditios. Hee ( ) P 7 od is the ode of the poit goup of the axiu agetic syety of the α -D i the give cystal. The α -Ds of MSC 6 (MSC ) have the axiu degeeacy q. Fo 80 - ad α -Ds it is equal to 6 (cystallogaphic class ), 48 (cystallogaphic class 6/) ad 96 (cystallogaphic class 3) i cystals of lowe, ediu ad highe syety sigoies (i cofoity with teiology of []), espectively. The 0 -Ds ae foed i spatially ihoogeeous edia [3]. Coditios of occuece ad existece of such Ds dead to tae ito accout ediu peculiaities. 4. Magetic syety classes of doai walls i hexoctahedal cystals As a exaple let's coside MSCs of all possible Ds i agetically odeed cystals of hexoctahedal class (cystallogaphic poit syety goup 3 i the paaagetic phase [3]). This class is assued to exhibit the lagest vaiety of possible Ds. Futheoe it ecopasses widely ivestigated ad used agetic edia (all cubic syety etals, specifically io ad icel [6], agetic oxides, specifically feites with stuctues of spiel [4] ad gaet [6], peovsite, agetite ad othes). The agetic aisotopy (MA) eegy e K is the ivaiat of the iitial paaagetic phase of cystal. Fo the 3 cystal this eegy is give by e K ( α, α, α3 ) = K s + K p + 3 K s + K 4 sp +..., whee K, K, K 3 ad K 4 ae fist, secod, thid ad fouth MA costats, s = α α + α α3 + α α3, p = α α α3, α, α ad α 3 ae the diectio cosies of [6]. The absolute iiu of this eegy coespods to EMAs. Sigs of MA costats ad elatio betwee thei values deteie EMAs diectios. I the faewo of the ( K, K, K 3 ) appoxiatio the EMAs diectios ca coicide with both high-syetic ad low-syetic cystallogaphic diectios [7]. I the faewo of the twocostat ( K, K ) appoxiatio the EMA diectios ca coicide oly with high-syetic <> o <0> o else <00> lie cystallogaphic diectios at K - K 3 o 0 K - K o else K 0 espectively [,8]. At that 7 0 -, ad Ds o , , ad Ds o else ad

8 80 0 -Ds ae ealized i a 3 cystal, espectively []. The MSCs ad degeeacy q of a α -D bouday coditios with α > 90 ad α 90 ae peseted i tables ad 3 espectively. The ealie obtaied MSCs of eely 80 -Ds (bold type ubes i table ) iclude eleets [5]: = - (,,, ) (, ); =4 - (,,, ); =5 - (,,, ) ; =4 - (,, ), ; =5 - (, ). =3 - (,,, ) (, ); =9 - ( 3, ); =34 - ( 4,, ) 8 ; Oly geeative syety eleets ae peseted fo =9 ad 34. Othe MSCs of tables ad 3 ae peseted i table. I these tables the D plae oietatio is assiged by diffeet Mille idexes h,,l>. A siultaeous chage o egative ad/o cyclic peutatio of all idexes does t chage MSCs. Thee ae o coo MSCs of axiu syetical 80 - ad α -Ds i the 3 cystal. It is coected with the pesece of the tasfoatio ( α -D vecto is chaged by this tasfoatio) i the MSCs of such 80 -D. 5. Coclusios The full agetic syety classificatio of all possible doai walls i feo- ad feiaget cystals icludes 64 agetic syety classes: 4 classes of Ds, 0 classes of α -Ds with 0 0 < α <80 0 ad 4 classes of Ds. Lists of agetic syety classes of all above etioed types of Ds ae itesected i geeal case Ds ca be pulsatig, otay o sei-otay Ds. The α -Ds with 0 0 < α <80 0 ae otay o sei-otay Ds oly. Aog otay o sei-otay Ds thee ae Ds with loch o Neel laws of agetizatio otatio i thei volue. Pulsatig, otay o sei-otay Ds ca have a cete of syety i thei volue. All possible ad α -Ds with 0 0 < α <80 0 have eve degeeacy (its value is betwee ad 96 i geeal case). Magetic syety classes of axiu syetical 80 -Ds do ot eet with such classes of α -Ds with 0 0 < α <80 0 i a 3 cystal.

9 Refeeces 9 [] A. Hubet, Theoie de Doaewade i eodete Mediele (Theoy of Doai alls i Odeed Media), Spige, eli, Heidelbeg, New Yo, 974 A Hubet ad R. Shafe, Magetic Doais. The Aalysis of Magetic Micostuctues, Spige, eli, 998 [] V. oov ad V. Volov, Physics of the Solid State 50 (008)98 [3] L. Shuvalov, Sov. Phys. Cystallog. 4(959)399 [4] L. Shuvalov, Mode Cystallogaphy IV : Physical Popeties of Cystals, Spige, eli, 988 [5] V. ayahta, V. Lvov ad D. Yablosy, JETP 87(984)863 [6] V. ayahta, E. Koteo ad D. Yablosy, JETP 9(986)9 [7]. Lilley, Phil.Mag. 4(950)79 [8] A. Adeev ad V. Macheo, JETP 70(976)5 [9] L. Ladau, E. Lifshitz ad L. Pitaevsii, Couse of Theoetical Physics, vol.8. Electodyaics of Cotiuous Media, Pegao Pess, Lodo, 984 [0] V. A. Kopci, Xubiovsie uppy: Spavoqi po sietii i fiziqesi svostva. istalliqesih stutu [Shubiov s goups: Hadboo o the syety ad physical popeties of cystallie stuctues, i Russia], Izdatel stvo Mosovsogo Uivesiteta, Moscow, 966 A.V. Shubiov ad N.V. elov, Coloed syety, Pegao Pess, Lodo, 964. Tavge ad V. Zaitzev, JETP 3(956)430 []. Vashtei, Mode Cystallogaphy : Syety of Cystals, Methods of Stuctual Cystallogaphy, Spige, eli, 994 [] E. ige, oup Theoy ad its Applicatio to the Quatu Mechaics of Atoic Specta, Acadeic Pess, New Yo, 959 [3] L. Heydea, H. Niedoba, H. upta ad I. Puchalsa, J. Mag. Mag. Mate 96(99)5. R. Vahitov, A Yuaguzi, J. Mag. Mag. Mate. 5-6(000)5 [4] L.Ladau ad E.Lifshitz, Sov.Phys. 8(935)53

10 [5] L. Neel, Copt.ed. 49(955)533 0 [6] A. Paoletti, Physics of Magetic aets, Esevie, Asteda, 978 [7] U. Atzoy ad M. Daiel, Phys. Rev. 3(976)4006 [8] K.P. elov, A.K. Zvezdi, R.Z. Leviti, A.S. Maosya,.V. Mill, A.A. Muhi ad A.P.Peov, JETP 4(975)590

11 Table. Magetic syety classes of the plae α -Ds with α 80. MSC ub. Mutual oietatios of the vectos, ad Syety eleets Coodiate depedeces of ( z~ ) copoets D ( ~ ~ z ) ( ~ ~ z ) ( ~ ~ z ) y x z cete Iteatioal MSC sybol b = a = 0,,, 6 a = a = 0 a = C, (-) (A,S) (-) - (-) (A,S) (-) - 7 a = a = 0,,, (A) (S) (-) ~ z = 0 8 a = a = 0, (A,S) (A,S) (-) - 9 a C = a = b = 0,,, (A) (-) (S) ~ z = 0 0 a = 0, (A) (S) (S) ~ z = 0 a C = a = b = 0, (A) (A) (S) ~ z = 0 a C = 0, (-) (A,S) (A,S) - 3 a = 0, (A) (S) (A) ~ z = 0 6 Abitay (A,S) (A,S) (A,S) - 7 a C = a = b = 0,,, (-) (S) (A) ~ z = 0 8 a C = a = b = 0, (S) (S) (A) ~ z = 0 9 b = b = 0, (-) (-) (A,S) - b = b = 0,,, (-) (-) (A,S) - 4 b = 0 b = 6 b = 0 b = 3, 30 b = 0 b = 3 b = 0 b = 4, 37 b = 0 b = 39 b = 0 b = 6, (,,, ) (, ) 43 b = a = 0 44 b = a = 0,,, 3 (-) (-) (A,S) - 3 (-) (-) (A,S) (-) (-) (A,S) - 4 (-) (-) (A,S) (-) (-) (A,S) - 6 (-) (-) (A,S) - 6 (-) (S) (-) ~ z = 0 (-) (S) (-) ~ z = 0 45 a = b = a = 0,,, (-) (S) (-) ~ z = 0 / 46 a = b = a = 0,,, (S) (S) (-) ~ z = 0 / 47 a = b = 0,,, (-) (S) (S) ~ z = 0 / 48 a b = 0, (S) (S) (S) ~ z = 0 =

12 Table. Magetic syety classes of the plae α -Ds with α 80 (cotiue). MSC ub. Mutual oietatios of the vectos, ad Syety eleets Coodiate depedeces of ( z~ ) copoets D ( ~ ~ z ) ( ~ ~ z ) ( ~ ~ z ) y x z cete Iteatioal MSC sybol 49 a = b = b = 0,,, (-) (-) (S) ~ z = 0 / 50 a = b = b = 0,,, (-) (-) (S) ~ z = 0 5 b = b = 0 (,,, ) (, ) 5 b = b = 0 53 b = b = 0, 54 b = b = 0 6, 55 b = b = 0 3, 56 b = b = 0, 57 b = b = 0, 58 b = b = 0,, 59 b = b = 0 60 b = b = 0 4, 6 b = b = 0, 6 b = b = 0, 63 b = b = 0,, 64 b = b = 0 (-) (-) (S) ~ z = 0 6 (-) (-) (S) ~ z = (-) (-) (S) ~ z = 0 3 (-) (-) (S) ~ z = 0 6 (-) (-) (S) ~ z = (-) (-) (S) ~ z = 0 4/ 4 (-) (-) (S) ~ z = (-) (-) (S) ~ z = 0 4 / 4 (-) (-) (S) ~ z = 0 4 (-) (-) (S) ~ z = (-) (-) (S) ~ z = 0 6/ 6 (-) (-) (S) ~ z = (-) (-) (S) ~ z = 0 6 / 3 (-) (-) (S) ~ z = 0 3

13 Table.. Nube (degeeacy q ) of MSC of bouday coditios of abitay oieted plae α -D ( α > 90 ) i the cubic 3 D plae 80 -D [00], [ 00] cystals at selected doai agetizatio diectios. α -D bouday coditios 80 -D [0], [ 0] 80 -D [], [ ] 0 -D [0], [ 0 ] 09 -D [], [ ] (00) 34 (6) 4 (4) 4 (4) 6 (96) 9 (4) (00) () 4 (4) 4 (4) 3 (48) 3 (48) (00) () () 4 (4) 6 (96) 3 (48) () 4 (4) 4 (4) 9 (8) 6 (96) (48) ( ) 4 (4) 4 (4) 4 (4) 3 (48) (48) ( ) 4 (4) 4 (4) 4 (4) 6 (96) 0 (48) ( ) 4 (4) 4 (4) 4 (4) 3 (48) 0 (48) (0) 4 (4) 3 () 4 (4) 6 (96) 6 (96) (0) 4 (4) 5 (48) 4 (4) (48) 6 (96) (0) () 5 (48) 4 (4) 6 (96) 7 (4) ( 0) 4 (4) () 5 (4) 6 (96) 6 (96) ( 0) 4 (4) 5 (48) 5 (4) 3 (48) 6 (96) ( 0 ) () 5 (48) 5 (4) 6 (96) 7 (4) (hhl) 5 (48) 4 (4) 4 (4) 6 (96) 6 (96) (hh) 5 (48) 5 (48) 4 (4) 6 (96) 6 (96) (h) 4 (4) 5 (48) 4 (4) 6 (96) (48) ( h hl) 5 (48) 4 (4) 5 (48) 6 (96) 6 (96) ( h h) 5 (48) 5 (48) 5 (48) 3 (48) 6 (96) ( h ) 4 (4) 5 (48) 5 (48) 6 (96) 0 (48) (h0), ( h 0) 4 (4) 4 (4) 5 (48) 6 (96) 6 (96) (h0l), ( h 0 l) 4 (4) 5 (48) 5 (48) 6 (96) 6 (96) (0l), ( 0 l) 4 (4) 5 (48) 5 (48) 6 (96) 3 (48) (hl), ( h l), ( h l), ( h l ) 5 (48) 5 (48) 5 (48) 6 (96) 6 (96) 3

14 Table.3. Nube (degeeacy q ) of MSC of bouday coditios of abitay oieted plae α -D ( α 90 ) i the cubic 3 D plae cystals at selected doai agetizatio diectios. 90 -D [00], [ 0 0] α -D bouday coditios 90 -D [0], [ 0] 7 -D [], [ ] 60 -D [0], [0] (00) (48) 9 (4) 7 (4) 6 (96) (00) (48) 7 (4) 0 (48) 0 (48) (00) 7 (4) 7 (4) 0 (48) 6 (96) () 3 (48) 6 (96) (48) 0 (48) ( ) 0 (48) 6 (96) (48) 6 (96) ( ) 0 (48) 6 (96) 3 (48) 0 (48) ( ) 3 (48) 6 (96) 3 (48) 6 (96) (0) 7 (4) (48) 6 (96) 6 (96) (0) 6 (96) 0 (48) 6 (96) 0 (48) (0) 6 (96) 3 (48) 9 (4) 6 (96) ( 0) 9 (4) (48) 6 (96) 6 (96) ( 0) 6 (96) 0 (48) 6 (96) 8 (48) ( 0 ) 6 (96) 3 (48) 7 (4) 6 (96) (hhl) 3 (48) 6 (96) 6 (96) 6 (96) (hh) 6 (96) 6 (96) 6 (96) 0 (48) (h) 6 (96) 6 (96) (48) 6 (96) ( h hl) 0 (48) 6 (96) 6 (96) 6 (96) ( h h) 6 (96) 6 (96) 6 (96) 6 (96) ( h ) 6 (96) 6 (96) 3 (48) 6 (96) (h0), ( h 0) (48) (48) 6 (96) 6 (96) (h0l), ( h0 l) 6 (96) 0 (48) 6 (96) 6 (96) (0l), ( 0 l) 6 (96) 3 (48) 0 (48) 6 (96) (hl), ( h l), ( h l), ( h l ) 6 (96) 6 (96) 6 (96) 6 (96) 4

Math 7409 Homework 2 Fall from which we can calculate the cycle index of the action of S 5 on pairs of vertices as

Math 7409 Homework 2 Fall from which we can calculate the cycle index of the action of S 5 on pairs of vertices as Math 7409 Hoewok 2 Fall 2010 1. Eueate the equivalece classes of siple gaphs o 5 vetices by usig the patte ivetoy as a guide. The cycle idex of S 5 actig o 5 vetices is 1 x 5 120 1 10 x 3 1 x 2 15 x 1

More information

Born-Oppenheimer Approximation and Nonadiabatic Effects. Hans Lischka University of Vienna

Born-Oppenheimer Approximation and Nonadiabatic Effects. Hans Lischka University of Vienna Bo-Oppeheie Appoxiatio ad Noadiabatic Effects Has Lischa Uivesity of Viea Typical situatio. Fac-Codo excitatio fo the iiu of the goud state. Covetioal dyaics possibly M* ad TS 3. Coical itesectio fuel

More information

Technical Report: Bessel Filter Analysis

Technical Report: Bessel Filter Analysis Sasa Mahmoodi 1 Techical Repot: Bessel Filte Aalysis 1 School of Electoics ad Compute Sciece, Buildig 1, Southampto Uivesity, Southampto, S17 1BJ, UK, Email: sm3@ecs.soto.ac.uk I this techical epot, we

More information

Strong Result for Level Crossings of Random Polynomials

Strong Result for Level Crossings of Random Polynomials IOSR Joual of haacy ad Biological Scieces (IOSR-JBS) e-issn:78-8, p-issn:19-7676 Volue 11, Issue Ve III (ay - Ju16), 1-18 wwwiosjoualsog Stog Result fo Level Cossigs of Rado olyoials 1 DKisha, AK asigh

More information

Relation (12.1) states that if two points belong to the convex subset Ω then all the points on the connecting line also belong to Ω.

Relation (12.1) states that if two points belong to the convex subset Ω then all the points on the connecting line also belong to Ω. Lectue 6. Poectio Opeato Deiitio A.: Subset Ω R is cove i [ y Ω R ] λ + λ [ y = z Ω], λ,. Relatio. states that i two poits belog to the cove subset Ω the all the poits o the coectig lie also belog to Ω.

More information

MATH Midterm Solutions

MATH Midterm Solutions MATH 2113 - Midtem Solutios Febuay 18 1. A bag of mables cotais 4 which ae ed, 4 which ae blue ad 4 which ae gee. a How may mables must be chose fom the bag to guaatee that thee ae the same colou? We ca

More information

THE GRAVITATIONAL POTENTIAL OF A MULTIDIMENSIONAL SHELL

THE GRAVITATIONAL POTENTIAL OF A MULTIDIMENSIONAL SHELL THE GRAVITATIONAL POTENTIAL OF A MULTIDIMENSIONAL SHELL BY MUGUR B. RĂUŢ Abstact. This pape is a attept to geealize the well-kow expessio of the gavitatioal potetial fo oe tha thee diesios. We used the

More information

MATH /19: problems for supervision in week 08 SOLUTIONS

MATH /19: problems for supervision in week 08 SOLUTIONS MATH10101 2018/19: poblems fo supevisio i week 08 Q1. Let A be a set. SOLUTIONS (i Pove that the fuctio c: P(A P(A, defied by c(x A \ X, is bijective. (ii Let ow A be fiite, A. Use (i to show that fo each

More information

Lacunary Almost Summability in Certain Linear Topological Spaces

Lacunary Almost Summability in Certain Linear Topological Spaces BULLETIN of te MLYSİN MTHEMTİCL SCİENCES SOCİETY Bull. Malays. Mat. Sci. Soc. (2) 27 (2004), 27 223 Lacuay lost Suability i Cetai Liea Topological Spaces BÜNYMIN YDIN Cuuiyet Uivesity, Facutly of Educatio,

More information

Mapping Radius of Regular Function and Center of Convex Region. Duan Wenxi

Mapping Radius of Regular Function and Center of Convex Region. Duan Wenxi d Iteatioal Cofeece o Electical Compute Egieeig ad Electoics (ICECEE 5 Mappig adius of egula Fuctio ad Cete of Covex egio Dua Wexi School of Applied Mathematics Beijig Nomal Uivesity Zhuhai Chia 363463@qqcom

More information

Strong Result for Level Crossings of Random Polynomials. Dipty Rani Dhal, Dr. P. K. Mishra. Department of Mathematics, CET, BPUT, BBSR, ODISHA, INDIA

Strong Result for Level Crossings of Random Polynomials. Dipty Rani Dhal, Dr. P. K. Mishra. Department of Mathematics, CET, BPUT, BBSR, ODISHA, INDIA Iteatioal Joual of Reseach i Egieeig ad aageet Techology (IJRET) olue Issue July 5 Available at http://wwwijetco/ Stog Result fo Level Cossigs of Rado olyoials Dipty Rai Dhal D K isha Depatet of atheatics

More information

Cylindrical quantum well of finite depth in external magnetic field.

Cylindrical quantum well of finite depth in external magnetic field. Cylidical quatu well of fiite depth i eteal agetic field Lobaova OR a Ivaov AI b ab Kaliigad State Uivesity Theoetical Physics Depatet Kaliigad Russia Abstact egy spectu of a electo cofied by fiite had-wall

More information

International Journal of Mathematical Archive-3(5), 2012, Available online through ISSN

International Journal of Mathematical Archive-3(5), 2012, Available online through   ISSN Iteatioal Joual of Matheatical Achive-3(5,, 8-8 Available olie though www.ija.ifo ISSN 9 546 CERTAIN NEW CONTINUED FRACTIONS FOR THE RATIO OF TWO 3 ψ 3 SERIES Maheshwa Pathak* & Pakaj Sivastava** *Depatet

More information

EVALUATION OF SUMS INVOLVING GAUSSIAN q-binomial COEFFICIENTS WITH RATIONAL WEIGHT FUNCTIONS

EVALUATION OF SUMS INVOLVING GAUSSIAN q-binomial COEFFICIENTS WITH RATIONAL WEIGHT FUNCTIONS EVALUATION OF SUMS INVOLVING GAUSSIAN -BINOMIAL COEFFICIENTS WITH RATIONAL WEIGHT FUNCTIONS EMRAH KILIÇ AND HELMUT PRODINGER Abstact We coside sums of the Gaussia -biomial coefficiets with a paametic atioal

More information

a) The average (mean) of the two fractions is halfway between them: b) The answer is yes. Assume without loss of generality that p < r.

a) The average (mean) of the two fractions is halfway between them: b) The answer is yes. Assume without loss of generality that p < r. Solutios to MAML Olympiad Level 00. Factioated a) The aveage (mea) of the two factios is halfway betwee them: p ps+ q ps+ q + q s qs qs b) The aswe is yes. Assume without loss of geeality that p

More information

Supplementary materials. Suzuki reaction: mechanistic multiplicity versus exclusive homogeneous or exclusive heterogeneous catalysis

Supplementary materials. Suzuki reaction: mechanistic multiplicity versus exclusive homogeneous or exclusive heterogeneous catalysis Geeal Pape ARKIVOC 009 (xi 85-03 Supplemetay mateials Suzui eactio: mechaistic multiplicity vesus exclusive homogeeous o exclusive heteogeeous catalysis Aa A. Kuohtia, Alexade F. Schmidt* Depatmet of Chemisty

More information

CHAPTER 5 : SERIES. 5.2 The Sum of a Series Sum of Power of n Positive Integers Sum of Series of Partial Fraction Difference Method

CHAPTER 5 : SERIES. 5.2 The Sum of a Series Sum of Power of n Positive Integers Sum of Series of Partial Fraction Difference Method CHAPTER 5 : SERIES 5.1 Seies 5. The Sum of a Seies 5..1 Sum of Powe of Positive Iteges 5.. Sum of Seies of Patial Factio 5..3 Diffeece Method 5.3 Test of covegece 5.3.1 Divegece Test 5.3. Itegal Test 5.3.3

More information

Multivector Functions

Multivector Functions I: J. Math. Aal. ad Appl., ol. 24, No. 3, c Academic Pess (968) 467 473. Multivecto Fuctios David Hestees I a pevious pape [], the fudametals of diffeetial ad itegal calculus o Euclidea -space wee expessed

More information

On Some Fractional Integral Operators Involving Generalized Gauss Hypergeometric Functions

On Some Fractional Integral Operators Involving Generalized Gauss Hypergeometric Functions Available at http://pvamu.edu/aam Appl. Appl. Math. ISSN: 93-9466 Vol. 5, Issue (Decembe ), pp. 3 33 (Peviously, Vol. 5, Issue, pp. 48 47) Applicatios ad Applied Mathematics: A Iteatioal Joual (AAM) O

More information

On composite conformal mapping of an annulus to a plane with two holes

On composite conformal mapping of an annulus to a plane with two holes O composite cofomal mappig of a aulus to a plae with two holes Mila Batista (July 07) Abstact I the aticle we coside the composite cofomal map which maps aulus to ifiite egio with symmetic hole ad ealy

More information

Consider unordered sample of size r. This sample can be used to make r! Ordered samples (r! permutations). unordered sample

Consider unordered sample of size r. This sample can be used to make r! Ordered samples (r! permutations). unordered sample Uodeed Samples without Replacemet oside populatio of elemets a a... a. y uodeed aagemet of elemets is called a uodeed sample of size. Two uodeed samples ae diffeet oly if oe cotais a elemet ot cotaied

More information

DANIEL YAQUBI, MADJID MIRZAVAZIRI AND YASIN SAEEDNEZHAD

DANIEL YAQUBI, MADJID MIRZAVAZIRI AND YASIN SAEEDNEZHAD MIXED -STIRLING NUMERS OF THE SEOND KIND DANIEL YAQUI, MADJID MIRZAVAZIRI AND YASIN SAEEDNEZHAD Abstact The Stilig umbe of the secod id { } couts the umbe of ways to patitio a set of labeled balls ito

More information

RELIABILITY ASSESSMENT OF SYSTEMS WITH PERIODIC MAINTENANCE UNDER RARE FAILURES OF ITS ELEMENTS

RELIABILITY ASSESSMENT OF SYSTEMS WITH PERIODIC MAINTENANCE UNDER RARE FAILURES OF ITS ELEMENTS Y Geis ELIABILITY ASSESSMENT OF SYSTEMS WITH PEIODIC MAINTENANCE UNDE AE FAILUES OF ITS ELEMENTS T&A # (6) (Vol) 2, Mach ELIABILITY ASSESSMENT OF SYSTEMS WITH PEIODIC MAINTENANCE UNDE AE FAILUES OF ITS

More information

Quantum Mechanics Lecture Notes 10 April 2007 Meg Noah

Quantum Mechanics Lecture Notes 10 April 2007 Meg Noah The -Patice syste: ˆ H V This is difficut to sove. y V 1 ˆ H V 1 1 1 1 ˆ = ad with 1 1 Hˆ Cete of Mass ˆ fo Patice i fee space He Reative Haitoia eative coodiate of the tota oetu Pˆ the tota oetu tota

More information

Auchmuty High School Mathematics Department Sequences & Series Notes Teacher Version

Auchmuty High School Mathematics Department Sequences & Series Notes Teacher Version equeces ad eies Auchmuty High chool Mathematics Depatmet equeces & eies Notes Teache Vesio A sequece takes the fom,,7,0,, while 7 0 is a seies. Thee ae two types of sequece/seies aithmetic ad geometic.

More information

Generalized Fibonacci-Lucas Sequence

Generalized Fibonacci-Lucas Sequence Tuish Joual of Aalysis ad Numbe Theoy, 4, Vol, No 6, -7 Available olie at http://pubssciepubcom/tjat//6/ Sciece ad Educatio Publishig DOI:6/tjat--6- Geealized Fiboacci-Lucas Sequece Bijeda Sigh, Ompaash

More information

Complementary Dual Subfield Linear Codes Over Finite Fields

Complementary Dual Subfield Linear Codes Over Finite Fields 1 Complemetay Dual Subfield Liea Codes Ove Fiite Fields Kiagai Booiyoma ad Somphog Jitma,1 Depatmet of Mathematics, Faculty of Sciece, Silpao Uivesity, Naho Pathom 73000, hailad e-mail : ai_b_555@hotmail.com

More information

Conditional Convergence of Infinite Products

Conditional Convergence of Infinite Products Coditioal Covegece of Ifiite Poducts William F. Tech Ameica Mathematical Mothly 106 1999), 646-651 I this aticle we evisit the classical subject of ifiite poducts. Fo stadad defiitios ad theoems o this

More information

1. Using Einstein Summation notation, prove the identity: = A

1. Using Einstein Summation notation, prove the identity: = A 1. Usig Eistei Suatio otatio, pove the idetity: ( B ( B B( + ( B ( B [1 poits] We begi by witig the coss poduct of ad B as: So the ou idetity, C B C ( B C, i ε ik B k We coside ( C ε i ε ik ε iε ik ( ε

More information

A NOTE ON DOMINATION PARAMETERS IN RANDOM GRAPHS

A NOTE ON DOMINATION PARAMETERS IN RANDOM GRAPHS Discussioes Mathematicae Gaph Theoy 28 (2008 335 343 A NOTE ON DOMINATION PARAMETERS IN RANDOM GRAPHS Athoy Boato Depatmet of Mathematics Wilfid Lauie Uivesity Wateloo, ON, Caada, N2L 3C5 e-mail: aboato@oges.com

More information

LOCUS OF THE CENTERS OF MEUSNIER SPHERES IN EUCLIDEAN 3-SPACE. 1. Introduction

LOCUS OF THE CENTERS OF MEUSNIER SPHERES IN EUCLIDEAN 3-SPACE. 1. Introduction LOCUS OF THE CENTERS OF MEUSNIER SPHERES IN EUCLIDEAN -SPACE Beyha UZUNOGLU, Yusuf YAYLI ad Ismail GOK Abstact I this study, we ivestigate the locus of the cetes of the Meusie sphees Just as focal cuve

More information

INTERACTION OF E-POLARIZED WAVE WITH PREFRACTAL WEAKLY FILLED DIFFRACTION GRATING (AN ASYMPTOTICAL MODEL)

INTERACTION OF E-POLARIZED WAVE WITH PREFRACTAL WEAKLY FILLED DIFFRACTION GRATING (AN ASYMPTOTICAL MODEL) J. Nao- Electo. Phys. 3 (20) No2, P. 9-25 Ó 20 SuDU (Suy State Uivesity) PACS ubes: 07.57. c, 02.30.Rz INTERACTION OF E-POLARIZED WAVE WITH PREFRACTAL WEAKLY FILLED DIFFRACTION GRATING (AN ASYMPTOTICAL

More information

Module II: Part A. Optical Fibers

Module II: Part A. Optical Fibers Module II: Pat A Optical Fibes Optical Fibes as Tasissio Mediu Mai Liitatio: Atteuatio Although fibes have bee kow sice the 8 s as ediu fo light tasissio, thei pactical use becae evidet whe losses whee

More information

FERMAT S THEOREM ON BINARY POWERS

FERMAT S THEOREM ON BINARY POWERS NNTDM (00), - ERMAT S THEOREM ON BINARY POWERS J. V. Leyedekkes The Uivesity of Sydey, 00, Austalia A. G. Shao Waae College, The Uivesity of New South Wales, Kesigto,, & KvB Istitute of Techology, Noth

More information

On ARMA(1,q) models with bounded and periodically correlated solutions

On ARMA(1,q) models with bounded and periodically correlated solutions Reseach Repot HSC/03/3 O ARMA(,q) models with bouded ad peiodically coelated solutios Aleksade Weo,2 ad Agieszka Wy oma ska,2 Hugo Steihaus Cete, Woc aw Uivesity of Techology 2 Istitute of Mathematics,

More information

= 5! 3! 2! = 5! 3! (5 3)!. In general, the number of different groups of r items out of n items (when the order is ignored) is given by n!

= 5! 3! 2! = 5! 3! (5 3)!. In general, the number of different groups of r items out of n items (when the order is ignored) is given by n! 0 Combiatoial Aalysis Copyight by Deiz Kalı 4 Combiatios Questio 4 What is the diffeece betwee the followig questio i How may 3-lette wods ca you wite usig the lettes A, B, C, D, E ii How may 3-elemet

More information

The Pigeonhole Principle 3.4 Binomial Coefficients

The Pigeonhole Principle 3.4 Binomial Coefficients Discete M athematic Chapte 3: Coutig 3. The Pigeohole Piciple 3.4 Biomial Coefficiets D Patic Cha School of Compute Sciece ad Egieeig South Chia Uivesity of Techology Ageda Ch 3. The Pigeohole Piciple

More information

THE ANALYSIS OF SOME MODELS FOR CLAIM PROCESSING IN INSURANCE COMPANIES

THE ANALYSIS OF SOME MODELS FOR CLAIM PROCESSING IN INSURANCE COMPANIES Please cite this atle as: Mhal Matalyck Tacaa Romaiuk The aalysis of some models fo claim pocessig i isuace compaies Scietif Reseach of the Istitute of Mathemats ad Compute Sciece 004 Volume 3 Issue pages

More information

Modular Spaces Topology

Modular Spaces Topology Applied Matheatics 23 4 296-3 http://ddoiog/4236/a234975 Published Olie Septebe 23 (http://wwwscipog/joual/a) Modula Spaces Topology Ahed Hajji Laboatoy of Matheatics Coputig ad Applicatio Depatet of Matheatics

More information

Structure and Some Geometric Properties of Nakano Difference Sequence Space

Structure and Some Geometric Properties of Nakano Difference Sequence Space Stuctue ad Soe Geoetic Poeties of Naao Diffeece Sequece Sace N Faied ad AA Baey Deatet of Matheatics, Faculty of Sciece, Ai Shas Uivesity, Caio, Egyt awad_baey@yahooco Abstact: I this ae, we exted the

More information

Progression. CATsyllabus.com. CATsyllabus.com. Sequence & Series. Arithmetic Progression (A.P.) n th term of an A.P.

Progression. CATsyllabus.com. CATsyllabus.com. Sequence & Series. Arithmetic Progression (A.P.) n th term of an A.P. Pogessio Sequece & Seies A set of umbes whose domai is a eal umbe is called a SEQUENCE ad sum of the sequece is called a SERIES. If a, a, a, a 4,., a, is a sequece, the the expessio a + a + a + a 4 + a

More information

Advanced Physical Geodesy

Advanced Physical Geodesy Supplemetal Notes Review of g Tems i Moitz s Aalytic Cotiuatio Method. Advaced hysical Geodesy GS887 Chistophe Jekeli Geodetic Sciece The Ohio State Uivesity 5 South Oval Mall Columbus, OH 4 7 The followig

More information

International Journal of Mathematics Trends and Technology (IJMTT) Volume 47 Number 1 July 2017

International Journal of Mathematics Trends and Technology (IJMTT) Volume 47 Number 1 July 2017 Iteatioal Joual of Matheatics Teds ad Techology (IJMTT) Volue 47 Nube July 07 Coe Metic Saces, Coe Rectagula Metic Saces ad Coo Fixed Poit Theoes M. Sivastava; S.C. Ghosh Deatet of Matheatics, D.A.V. College

More information

On the Circulant Matrices with. Arithmetic Sequence

On the Circulant Matrices with. Arithmetic Sequence It J Cotep Math Scieces Vol 5 o 5 3 - O the Ciculat Matices with Aithetic Sequece Mustafa Bahsi ad Süleya Solak * Depatet of Matheatics Educatio Selçuk Uivesity Mea Yeiyol 499 Koya-Tukey Ftly we have defied

More information

Applications of the Dirac Sequences in Electrodynamics

Applications of the Dirac Sequences in Electrodynamics Poc of the 8th WSEAS It Cof o Mathematical Methods ad Computatioal Techiques i Electical Egieeig Buchaest Octobe 6-7 6 45 Applicatios of the Diac Sequeces i Electodyamics WILHELM W KECS Depatmet of Mathematics

More information

Global asymptotic stability in a rational dynamic equation on discrete time scales

Global asymptotic stability in a rational dynamic equation on discrete time scales Iteatioal Joual of Egieeig Reseach & Sciece (IJOER) ISSN: [395-699] [Vol-, Issue-, Decebe- 6] Global asyptotic stability i a atioal dyaic euatio o discete tie scales a( t) b( ( t)) ( ( t)), t T c ( ( (

More information

Using Counting Techniques to Determine Probabilities

Using Counting Techniques to Determine Probabilities Kowledge ticle: obability ad Statistics Usig outig Techiques to Detemie obabilities Tee Diagams ad the Fudametal outig iciple impotat aspect of pobability theoy is the ability to detemie the total umbe

More information

Some Topics on Weighted Generalized Inverse and Kronecker Product of Matrices

Some Topics on Weighted Generalized Inverse and Kronecker Product of Matrices Malaysia Soe Joual Topics of Matheatical o Weighted Scieces Geealized (): Ivese 9-22 ad Koece (27) Poduct of Matices Soe Topics o Weighted Geealized Ivese ad Koece Poduct of Matices Zeyad Abdel Aziz Al

More information

Asymptotic Expansions of Legendre Wavelet

Asymptotic Expansions of Legendre Wavelet Asptotic Expasios of Legede Wavelet C.P. Pade M.M. Dixit * Depatet of Matheatics NERIST Nijuli Itaaga Idia. Depatet of Matheatics NERIST Nijuli Itaaga Idia. Astact A e costuctio of avelet o the ouded iteval

More information

Range Symmetric Matrices in Minkowski Space

Range Symmetric Matrices in Minkowski Space BULLETIN of the Bull. alaysia ath. Sc. Soc. (Secod Seies) 3 (000) 45-5 LYSIN THETICL SCIENCES SOCIETY Rae Symmetic atices i ikowski Space.R. EENKSHI Depatmet of athematics, amalai Uivesity, amalaiaa 608

More information

Minimal order perfect functional observers for singular linear systems

Minimal order perfect functional observers for singular linear systems Miimal ode efect fuctioal obseves fo sigula liea systems Tadeusz aczoek Istitute of Cotol Idustial lectoics Wasaw Uivesity of Techology, -66 Waszawa, oszykowa 75, POLAND Abstact. A ew method fo desigig

More information

Sums of Involving the Harmonic Numbers and the Binomial Coefficients

Sums of Involving the Harmonic Numbers and the Binomial Coefficients Ameica Joual of Computatioal Mathematics 5 5 96-5 Published Olie Jue 5 i SciRes. http://www.scip.og/oual/acm http://dx.doi.og/.46/acm.5.58 Sums of Ivolvig the amoic Numbes ad the Biomial Coefficiets Wuyugaowa

More information

ON CERTAIN CLASS OF ANALYTIC FUNCTIONS

ON CERTAIN CLASS OF ANALYTIC FUNCTIONS ON CERTAIN CLASS OF ANALYTIC FUNCTIONS Nailah Abdul Rahma Al Diha Mathematics Depatmet Gils College of Educatio PO Box 60 Riyadh 567 Saudi Aabia Received Febuay 005 accepted Septembe 005 Commuicated by

More information

FAR FIELD SOLUTION OF SH-WAVE BY CIRCULAR INCLUSION AND LINEAR CRACK

FAR FIELD SOLUTION OF SH-WAVE BY CIRCULAR INCLUSION AND LINEAR CRACK The 4 th Wold Cofeece o Eathquake Egieeig Octobe -7, 8, Beijig, Chia FAR FIELD SOLUTION OF SH-WAVE BY CIRCULAR INCLUSION AND LINEAR CRACK HogLiag Li,GuoHui Wu, Associate Pofesso, Depatmet of Egieeig Mechaics,

More information

Combinatorial Interpretation of Raney Numbers and Tree Enumerations

Combinatorial Interpretation of Raney Numbers and Tree Enumerations Ope Joual of Discete Matheatics, 2015, 5, 1-9 Published Olie Jauay 2015 i SciRes. http://www.scip.og/joual/ojd http://dx.doi.og/10.4236/ojd.2015.51001 Cobiatoial Itepetatio of Raey Nubes ad Tee Eueatios

More information

Effect of Material Gradient on Stresses of Thick FGM Spherical Pressure Vessels with Exponentially-Varying Properties

Effect of Material Gradient on Stresses of Thick FGM Spherical Pressure Vessels with Exponentially-Varying Properties M. Zamai Nejad et al, Joual of Advaced Mateials ad Pocessig, Vol.2, No. 3, 204, 39-46 39 Effect of Mateial Gadiet o Stesses of Thick FGM Spheical Pessue Vessels with Expoetially-Vayig Popeties M. Zamai

More information

Finite q-identities related to well-known theorems of Euler and Gauss. Johann Cigler

Finite q-identities related to well-known theorems of Euler and Gauss. Johann Cigler Fiite -idetities elated to well-ow theoems of Eule ad Gauss Joha Cigle Faultät fü Mathemati Uivesität Wie A-9 Wie, Nodbegstaße 5 email: oha.cigle@uivie.ac.at Abstact We give geealizatios of a fiite vesio

More information

COUNTING SUBSET SUMS OF FINITE ABELIAN GROUPS

COUNTING SUBSET SUMS OF FINITE ABELIAN GROUPS COUNTING SUBSET SUMS OF FINITE ABELIAN GROUPS JIYOU LI AND DAQING WAN Abstact I this pape, we obtai a explicit fomula fo the umbe of zeo-sum -elemet subsets i ay fiite abelia goup 1 Itoductio Let A be

More information

SOME ARITHMETIC PROPERTIES OF OVERPARTITION K -TUPLES

SOME ARITHMETIC PROPERTIES OF OVERPARTITION K -TUPLES #A17 INTEGERS 9 2009), 181-190 SOME ARITHMETIC PROPERTIES OF OVERPARTITION K -TUPLES Deick M. Keiste Depatmet of Mathematics, Pe State Uivesity, Uivesity Pak, PA 16802 dmk5075@psu.edu James A. Selles Depatmet

More information

Generalization of Horadam s Sequence

Generalization of Horadam s Sequence Tuish Joual of Aalysis ad Nube Theoy 6 Vol No 3-7 Available olie at http://pubssciepubco/tjat///5 Sciece ad Educatio Publishig DOI:69/tjat---5 Geealizatio of Hoada s Sequece CN Phadte * YS Valaulia Depatet

More information

SVD ( ) Linear Algebra for. A bit of repetition. Lecture: 8. Let s try the factorization. Is there a generalization? = Q2Λ2Q (spectral theorem!

SVD ( ) Linear Algebra for. A bit of repetition. Lecture: 8. Let s try the factorization. Is there a generalization? = Q2Λ2Q (spectral theorem! Liea Algeba fo Wieless Commuicatios Lectue: 8 Sigula Value Decompositio SVD Ove Edfos Depatmet of Electical ad Ifomatio echology Lud Uivesity it 00-04-06 Ove Edfos A bit of epetitio A vey useful matix

More information

BINOMIAL THEOREM An expression consisting of two terms, connected by + or sign is called a

BINOMIAL THEOREM An expression consisting of two terms, connected by + or sign is called a BINOMIAL THEOREM hapte 8 8. Oveview: 8.. A epessio cosistig of two tems, coected by + o sig is called a biomial epessio. Fo eample, + a, y,,7 4 5y, etc., ae all biomial epessios. 8.. Biomial theoem If

More information

( ) 1 Comparison Functions. α is strictly increasing since ( r) ( r ) α = for any positive real number c. = 0. It is said to belong to

( ) 1 Comparison Functions. α is strictly increasing since ( r) ( r ) α = for any positive real number c. = 0. It is said to belong to Compaiso Fuctios I this lesso, we study stability popeties of the oautoomous system = f t, x The difficulty is that ay solutio of this system statig at x( t ) depeds o both t ad t = x Thee ae thee special

More information

BINOMIAL THEOREM NCERT An expression consisting of two terms, connected by + or sign is called a

BINOMIAL THEOREM NCERT An expression consisting of two terms, connected by + or sign is called a 8. Oveview: 8.. A epessio cosistig of two tems, coected by + o sig is called a biomial epessio. Fo eample, + a, y,,7 4, etc., ae all biomial 5y epessios. 8.. Biomial theoem BINOMIAL THEOREM If a ad b ae

More information

Rotational symmetry applied to boundary element computation for nuclear fusion plasma

Rotational symmetry applied to boundary element computation for nuclear fusion plasma Bouda Elemets ad Othe Mesh Reductio Methods XXXII 33 Rotatioal smmet applied to bouda elemet computatio fo uclea fusio plasma M. Itagaki, T. Ishimau & K. Wataabe 2 Facult of Egieeig, Hokkaido Uivesit,

More information

KEY. Math 334 Midterm II Fall 2007 section 004 Instructor: Scott Glasgow

KEY. Math 334 Midterm II Fall 2007 section 004 Instructor: Scott Glasgow KEY Math 334 Midtem II Fall 7 sectio 4 Istucto: Scott Glasgow Please do NOT wite o this exam. No cedit will be give fo such wok. Rathe wite i a blue book, o o you ow pape, pefeably egieeig pape. Wite you

More information

Dynamic Programming for Estimating Acceptance Probability of Credit Card Products

Dynamic Programming for Estimating Acceptance Probability of Credit Card Products Joual of Copute ad Couicatios, 07, 5, 56-75 http://wwwscipog/joual/jcc ISSN Olie: 7-57 ISSN Pit: 7-59 Dyaic Pogaig fo Estiatig Acceptace Pobability of Cedit Cad Poducts Lai Soo Lee,, Ya Mei Tee, Hsi Vo

More information

Lecture 24: Observability and Constructibility

Lecture 24: Observability and Constructibility ectue 24: Obsevability ad Costuctibility 7 Obsevability ad Costuctibility Motivatio: State feedback laws deped o a kowledge of the cuet state. I some systems, xt () ca be measued diectly, e.g., positio

More information

Ch 3.4 Binomial Coefficients. Pascal's Identit y and Triangle. Chapter 3.2 & 3.4. South China University of Technology

Ch 3.4 Binomial Coefficients. Pascal's Identit y and Triangle. Chapter 3.2 & 3.4. South China University of Technology Disc ete Mathem atic Chapte 3: Coutig 3. The Pigeohole Piciple 3.4 Biomial Coefficiets D Patic Cha School of Compute Sciece ad Egieeig South Chia Uivesity of Techology Pigeohole Piciple Suppose that a

More information

Lecture 2: Stress. 1. Forces Surface Forces and Body Forces

Lecture 2: Stress. 1. Forces Surface Forces and Body Forces Lectue : Stess Geophysicists study pheomea such as seismicity, plate tectoics, ad the slow flow of ocks ad mieals called ceep. Oe way they study these pheomea is by ivestigatig the defomatio ad flow of

More information

On the Khovanov Homology of 2- and 3-Strand Braid Links

On the Khovanov Homology of 2- and 3-Strand Braid Links Advaces i Pue Mathematics, 06, 6, 48-49 Published Olie May 06 i SciRes http://wwwscipog/joual/apm http://ddoiog/046/apm066604 O the Khovaov Homology of - ad -Stad Baid Lis Abdul Rauf Nizami, Mobee Mui,

More information

On the Zeros of Daubechies Orthogonal and Biorthogonal Wavelets *

On the Zeros of Daubechies Orthogonal and Biorthogonal Wavelets * Applied Mathematics,, 3, 778-787 http://dx.doi.og/.436/am..376 Published Olie July (http://www.scirp.og/joual/am) O the Zeos of Daubechies Othogoal ad Biothogoal Wavelets * Jalal Kaam Faculty of Sciece

More information

2012 GCE A Level H2 Maths Solution Paper Let x,

2012 GCE A Level H2 Maths Solution Paper Let x, GCE A Level H Maths Solutio Pape. Let, y ad z be the cost of a ticet fo ude yeas, betwee ad 5 yeas, ad ove 5 yeas categoies espectively. 9 + y + 4z =. 7 + 5y + z = 8. + 4y + 5z = 58.5 Fo ude, ticet costs

More information

Generalized golden ratios and associated Pell sequences

Generalized golden ratios and associated Pell sequences Notes o Nube Theoy ad Discete Matheatics it ISSN Olie ISSN 67 87 Vol. 4 8 No. DOI:.746/td.8.4..- Geealized golde atios ad associated ell sequeces A. G. Shao ad J. V. Leyedees Waae College The Uivesity

More information

Calculation of Matrix Elements in the Foldy-Wouthuysen Representation

Calculation of Matrix Elements in the Foldy-Wouthuysen Representation Calculatio of Matix Elemets i the Foldy-Wouthuyse Repesetatio V.P. Nezamov*, A.A.Sadovoy**, A.S.Ul yaov*** RFNC-VNIIEF, Saov, Russia Abstact The pape compaes the methods used to calculate matix elemets

More information

Counting Functions and Subsets

Counting Functions and Subsets CHAPTER 1 Coutig Fuctios ad Subsets This chapte of the otes is based o Chapte 12 of PJE See PJE p144 Hee ad below, the efeeces to the PJEccles book ae give as PJE The goal of this shot chapte is to itoduce

More information

OVERVIEW OF THE COMBINATORICS FUNCTION TECHNIQUE

OVERVIEW OF THE COMBINATORICS FUNCTION TECHNIQUE OVERVIEW OF THE COMBINATORICS FUNCTION TECHNIQUE Alai J. Phaes Depatet of Physics, Medel Hall, Villaova Uivesity, Villaova, Pesylvaia, 985-699, USA, phaes@eail.villaova.edu Hek F. Aoldus Depatet of Physics

More information

THE ABCD-HANKEL TRANSFORMATION IN TWO-DIMENSIONAL FREQUENCY-DOMAIN WITH POLAR COORDINATES

THE ABCD-HANKEL TRANSFORMATION IN TWO-DIMENSIONAL FREQUENCY-DOMAIN WITH POLAR COORDINATES Jue Phys. hem. News ( 9-34 PN THE BD-HNKEL TRNSFORMTION IN TWO-DIMENSIONL FREQUENY-DOMIN WITH POLR OORDINTES M. Ibchaikh,. Belafhal * Laboatoie de Physique Moléculaie, Dépatemet de Physique, B.P, Faculté

More information

W = mgdz = mgh. We can express this potential as a function of z: V ( z) = gz. = mg k. dz dz

W = mgdz = mgh. We can express this potential as a function of z: V ( z) = gz. = mg k. dz dz Electoagetic Theoy Pof Ruiz, UNC Asheville, doctophys o YouTube Chapte M Notes Laplace's Equatio M Review of Necessay Foe Mateial The Electic Potetial Recall i you study of echaics the usefuless of the

More information

SOME FINITE SIMPLE GROUPS OF LIE TYPE C n ( q) ARE UNIQUELY DETERMINED BY THEIR ELEMENT ORDERS AND THEIR ORDER

SOME FINITE SIMPLE GROUPS OF LIE TYPE C n ( q) ARE UNIQUELY DETERMINED BY THEIR ELEMENT ORDERS AND THEIR ORDER Joural of Algebra, Nuber Theory: Advaces ad Applicatios Volue, Nuber, 010, Pages 57-69 SOME FINITE SIMPLE GROUPS OF LIE TYPE C ( q) ARE UNIQUELY DETERMINED BY THEIR ELEMENT ORDERS AND THEIR ORDER School

More information

Announcements: The Rydberg formula describes. A Hydrogen-like ion is an ion that

Announcements: The Rydberg formula describes. A Hydrogen-like ion is an ion that Q: A Hydogelike io is a io that The Boh odel A) is cheically vey siila to Hydoge ios B) has the sae optical spectu as Hydoge C) has the sae ube of potos as Hydoge ) has the sae ube of electos as a Hydoge

More information

Masses and orbits of minor planets with the GAIA mission

Masses and orbits of minor planets with the GAIA mission asses ad obits of io laets with the GAIA issio Sege ouet Suevisos : F.igad D.Hestoffe PLAN Itoductio Puose of the PhD Iotace of asses The diffeet ethods to estiate these asses Descitio of close aoach Diffeet

More information

The Multivariate-t distribution and the Simes Inequality. Abstract. Sarkar (1998) showed that certain positively dependent (MTP 2 ) random variables

The Multivariate-t distribution and the Simes Inequality. Abstract. Sarkar (1998) showed that certain positively dependent (MTP 2 ) random variables The Multivaiate-t distibutio ad the Simes Iequality by Hey W. Block 1, Saat K. Saka 2, Thomas H. Savits 1 ad Jie Wag 3 Uivesity of ittsbugh 1,Temple Uivesity 2,Gad Valley State Uivesity 3 Abstact. Saka

More information

Using Difference Equations to Generalize Results for Periodic Nested Radicals

Using Difference Equations to Generalize Results for Periodic Nested Radicals Usig Diffeece Equatios to Geealize Results fo Peiodic Nested Radicals Chis Lyd Uivesity of Rhode Islad, Depatmet of Mathematics South Kigsto, Rhode Islad 2 2 2 2 2 2 2 π = + + +... Vieta (593) 2 2 2 =

More information

ON EUCLID S AND EULER S PROOF THAT THE NUMBER OF PRIMES IS INFINITE AND SOME APPLICATIONS

ON EUCLID S AND EULER S PROOF THAT THE NUMBER OF PRIMES IS INFINITE AND SOME APPLICATIONS Joual of Pue ad Alied Mathematics: Advaces ad Alicatios Volume 0 Numbe 03 Pages 5-58 ON EUCLID S AND EULER S PROOF THAT THE NUMBER OF PRIMES IS INFINITE AND SOME APPLICATIONS ALI H HAKAMI Deatmet of Mathematics

More information

INVERSE CAUCHY PROBLEMS FOR NONLINEAR FRACTIONAL PARABOLIC EQUATIONS IN HILBERT SPACE

INVERSE CAUCHY PROBLEMS FOR NONLINEAR FRACTIONAL PARABOLIC EQUATIONS IN HILBERT SPACE IJAS 6 (3 Febuay www.apapess.com/volumes/vol6issue3/ijas_6_3_.pdf INVESE CAUCH POBLEMS FO NONLINEA FACTIONAL PAABOLIC EQUATIONS IN HILBET SPACE Mahmoud M. El-Boai Faculty of Sciece Aleadia Uivesit Aleadia

More information

Electron states in a periodic potential. Assume the electrons do not interact with each other. Solve the single electron Schrodinger equation: KJ =

Electron states in a periodic potential. Assume the electrons do not interact with each other. Solve the single electron Schrodinger equation: KJ = Electo states i a peiodic potetial Assume the electos do ot iteact with each othe Solve the sigle electo Schodige equatio: 2 F h 2 + I U ( ) Ψ( ) EΨ( ). 2m HG KJ = whee U(+R)=U(), R is ay Bavais lattice

More information

REVIEW ARTICLE ABSTRACT. Interpolation of generalized Biaxisymmetric potentials. D. Kumar* G.L. `Reddy**

REVIEW ARTICLE ABSTRACT. Interpolation of generalized Biaxisymmetric potentials. D. Kumar* G.L. `Reddy** Itepolatio of Geealized Biaxisyetic potetials D Kua ad GL Reddy 9 REVIEW ARTICLE Itepolatio of geealized Biaxisyetic potetials D Kua* GL `Reddy** ABSTRACT I this pape we study the chebyshev ad itepolatio

More information

Prof. Dr. I. Nasser atomic and molecular physics -551 (T-112) February 20, 2012 Spin_orbit.doc. The Fine Structure of the Hydrogen Atom

Prof. Dr. I. Nasser atomic and molecular physics -551 (T-112) February 20, 2012 Spin_orbit.doc. The Fine Structure of the Hydrogen Atom Pof. D. I. Nasse atomic ad molecula physics -55 (T-) Febuay 0, 0 Spi_obit.doc The Fie Stuctue of the Hydoge Atom Whilst the pedictios of the quatum model of hydoge ae a vey good appoximatio to eality,

More information

Math 166 Week-in-Review - S. Nite 11/10/2012 Page 1 of 5 WIR #9 = 1+ r eff. , where r. is the effective interest rate, r is the annual

Math 166 Week-in-Review - S. Nite 11/10/2012 Page 1 of 5 WIR #9 = 1+ r eff. , where r. is the effective interest rate, r is the annual Math 66 Week-i-Review - S. Nite // Page of Week i Review #9 (F-F.4, 4.-4.4,.-.) Simple Iteest I = Pt, whee I is the iteest, P is the picipal, is the iteest ate, ad t is the time i yeas. P( + t), whee A

More information

Some Properties of the K-Jacobsthal Lucas Sequence

Some Properties of the K-Jacobsthal Lucas Sequence Deepia Jhala et. al. /Iteatioal Joual of Mode Scieces ad Egieeig Techology (IJMSET) ISSN 349-3755; Available at https://www.imset.com Volume Issue 3 04 pp.87-9; Some Popeties of the K-Jacobsthal Lucas

More information

Available online at ScienceDirect. Procedia Engineering 153 (2016 ) 16 23

Available online at   ScienceDirect. Procedia Engineering 153 (2016 ) 16 23 Availale olie at wwwsciecediectcom ScieceDiect Pocedia Egieeig 5 (06 6 XXV Polish Russia Slovak Semia heoetical Foudatio of Civil Egieeig Semiaalytical stuctual aalysis ased o comied applicatio of fiite

More information

Relativistic shape invariant potentials

Relativistic shape invariant potentials Relativistic shape ivaiat potetials A. D. Alhaidai Physics Depatmet, Kig Fahd Uivesity of Petoleum & Mieals, Box 5047, Dhaha 36, Saudi Aabia E-mail: haidai@mailaps.og Diac equatio fo a chaged spio i electomagetic

More information

Taylor Transformations into G 2

Taylor Transformations into G 2 Iteatioal Mathematical Foum, 5,, o. 43, - 3 Taylo Tasfomatios ito Mulatu Lemma Savaah State Uivesity Savaah, a 344, USA Lemmam@savstate.edu Abstact. Though out this pape, we assume that

More information

ELEMENTARY AND COMPOUND EVENTS PROBABILITY

ELEMENTARY AND COMPOUND EVENTS PROBABILITY Euopea Joual of Basic ad Applied Scieces Vol. 5 No., 08 ELEMENTARY AND COMPOUND EVENTS PROBABILITY William W.S. Che Depatmet of Statistics The Geoge Washigto Uivesity Washigto D.C. 003 E-mail: williamwsche@gmail.com

More information

Lecture 6: October 16, 2017

Lecture 6: October 16, 2017 Ifomatio ad Codig Theoy Autum 207 Lectue: Madhu Tulsiai Lectue 6: Octobe 6, 207 The Method of Types Fo this lectue, we will take U to be a fiite uivese U, ad use x (x, x 2,..., x to deote a sequece of

More information

(s)h(s) = K( s + 8 ) = 5 and one finite zero is located at z 1

(s)h(s) = K( s + 8 ) = 5 and one finite zero is located at z 1 ROOT LOCUS TECHNIQUE 93 should be desiged differetly to eet differet specificatios depedig o its area of applicatio. We have observed i Sectio 6.4 of Chapter 6, how the variatio of a sigle paraeter like

More information

New Sharp Lower Bounds for the First Zagreb Index

New Sharp Lower Bounds for the First Zagreb Index SCIENTIFIC PUBLICATIONS OF THE STATE UNIVERSITY OF NOVI PAZAR SER. A:APPL. MATH. INFORM. AND MECH. vol. 8, 1 (016), 11-19. New Shap Lowe Bouds fo the Fist Zageb Idex T. Masou, M. A. Rostami, E. Suesh,

More information

4. PERMUTATIONS AND COMBINATIONS

4. PERMUTATIONS AND COMBINATIONS 4. PERMUTATIONS AND COMBINATIONS PREVIOUS EAMCET BITS 1. The umbe of ways i which 13 gold cois ca be distibuted amog thee pesos such that each oe gets at least two gold cois is [EAMCET-000] 1) 3 ) 4 3)

More information

Generalized Near Rough Probability. in Topological Spaces

Generalized Near Rough Probability. in Topological Spaces It J Cotemp Math Scieces, Vol 6, 20, o 23, 099-0 Geealized Nea Rough Pobability i Topological Spaces M E Abd El-Mosef a, A M ozae a ad R A Abu-Gdaii b a Depatmet of Mathematics, Faculty of Sciece Tata

More information