surface barrier effects in non-resonant microwave absorption by superconducting thin films of...

2
PHYSICA Phystca C 235-240 (1994) 2056-2057 North-Holland Surface barrier effects in non-resonant microwave absorption by superconducting thin films of YBa2CuaOr_a Annt Rastogi a, V.V. Snniv,tsu", M.S. Hegde b and S.V Bhat" "Departmer,t of Physics, lndmn Institute of Smm,ce, Bangalore 560 012, India t'Solid State m,d Sttuctural Chemistry Unit, Indian lnstPute of Science, BangMore 560 012, htdbt. We present an unusual tempe~atmxe dependence of h~sterests m the non ~esonant mmrowave ab~mpt~on (NRMA) mgnals trom supmconductmg thin films of YBaaCuaOr-,, We observe thaL the h3stetesis zncreuses a~th increase m t, emperatu~e tdl T~ wluch we mtmp~et as evidence fm the plesence of Bem,-L~wngston sulface bamms (BLSB) m the ~mglc clystalhne hhns i. INTRODUCTION 3. RESULTS According to Bean ~tnd Livingston [1], throe emst,~ ,t b,uner to the flux peneuatmr, a~,d al.~o to expulsioI, due to the smface x~htch keeps the flUX from pei,etratit~g n, <t supeicoI~ductmg >~tm- ple upto a field Ho lugher than I-]¢]. Konez 3 kowsk~ et a], have reported the eMstence of BLSB ~n single crystal of YBa2(.'u~Or_~ [2]. The3 ob- serve zero magnet~zatiov nt :e~c~se field ~ee I) ~tnle m fot~atd ~cep flux penetrates at a held t-lp g~eate~ thorn H,: l(ecentl\ Zuo et al [3] haxe tepo, ted the p~e.-ence of >utface b~tniel> In Nd~-,(:eu~;(ueO, ,/ \'ke ~epult here the vx,.- tence of BLSB m thin hhns of Yl3aeCuaO,_,, ob- served using the technique of NRMA [4] 2. EXPERIMENTAL Thin superconducting him> el gBa2('u307 a x~exe deposited b\ pul~ed l~tsm ablatton method [5] on Y-ZrO2 sub>t~au,. 1'he c-axt> ermined hl.ns vr'l'~, -- v:,-,x,.,'R"'W) \ k t ' i , t hdi~t( ..... ,..t h,,.ul b',, X-l.t'~ ddhact~ot~ alUt four l)~,~be ~e>i~t~xitx ltlt'd'~tll('- llleI':Lb 'lhe .NttM.\ ~_lg],M>_ ~xete te~mcled u.thg ,t B~ukm 171(2001) X-I).u~d 121'1( .tw(t~on,,t,,1 cqtupped \~tth <tn ()\told ('1"1200 hehunt thin (l\OSttdl T h e dllOt, tlUlt of tit tllAgllCtlC held ~aa-, pardllcl to the ':-<L\I'.~ ot lht' "~,mplc 'l'he & I~t:t~,It~'tl~ h':'td x~:~- ,x~cl)l ])('IV,('('II -{- ~()(i \\ll]l l(: (l 0t}kl D.)m**dul,ttluh Figure 1 shows the NRMA signals reco,_'ded at vmmus tempelattue-.. It is obsmved that the zero field h3steresls (dehned as the vmtical separatiot, between for x~ a~ d itltd 1 evel se sweep sign,d-, a' zel u field) into eases ~ ith incl ease in temper~u tn e u pro T, while the ~ign,d intensity falls dowr, A I/I c O "I- "O II. "O R ! ! I -30 0 30 Field (Gauss) lhgm,' l \I~\1 \ "~lgnal5 fol folv.<ud aml lc'X'<.'l.~(' "~vel~> ,~t ~]w held al dlfh'tc'~t tenll)Ct,o m('.~ lIl hgm(' 2 ~<' h,tx~' I)lou('d the ttollll<tllLed h~-,- tme.~l-. (dvlmv, I .~-. tlu, l,ttlo <,~ 7he :cto held I,~-,- IOle~l",tt) tho..,l~ll,~l illl~,ll~ll\) ,tg,llllml ('l" -'l )o, ,1, IlClll~ 14'lli]~t'l,ll ill, ,)~ , II,' -.lllll)i':. I'll,:' I1()1 lll,.I][zcd h\ >t('t t'..-q.-, tip I,'+t'.,,,~ q",.lJ~Hl~'llt i,~llx ,t-, ~,, ,tl>pto,ttlt 0921-4534/94/$07 00 © 1994 - Elsevmr Science R V All nghts reserved. SSDI IY)21-4534(94)01594-5

Upload: amit-rastogi

Post on 26-Jun-2016

216 views

Category:

Documents


4 download

TRANSCRIPT

PHYSICA Phystca C 235-240 (1994) 2056-2057

North-Holland

Surface barrier effects in non-resonant microwave absorption by superconducting thin films of YBa2CuaOr_a Annt Rastogi a, V.V. Snniv,tsu", M.S. Hegde b and S.V Bhat"

"Depar tmer , t of Physics, lndmn Ins t i tu te of Smm,ce, Banga lore 560 012, India

t'Solid S ta te m,d S t tuc tura l Chemis t ry Unit, Indian l n s t P u t e of Science, BangMore 560 012, htdbt.

We present an unusual tempe~atmxe dependence of h~sterests m the non ~esonant mmrowave ab~mpt~on (NRMA) mgnals trom supmconductmg thin films of YBaaCuaOr- , , We observe thaL the h3stetesis z n c r e u s e s a~th increase m

t, emperatu~e tdl T~ wluch we mtmp~et as evidence fm the plesence of Bem,-L~wngston sulface bamms (BLSB) m the ~mglc clystalhne hhns

i. I N T R O D U C T I O N 3 . R E S U L T S

According to Bean ~tnd Livingston [1], throe emst,~ ,t b , u n e r to the flux peneua tmr , a~,d al.~o to expulsioI, due to the smface x~htch keeps the flUX from pei,etratit~g n, <t supeicoI~ductmg >~tm- ple upto a field Ho lugher than I-]¢]. Konez 3 kowsk~ et a], have reported the eMstence of BLSB ~n single crystal of YBa2(.'u~Or_~ [2]. The3 ob- serve zero magnet~zatiov nt :e~c~se field ~ e e I) ~tnle m fo t~a td ~ c e p flux pene t ra tes at a held t-lp g~eate~ thorn H,: l(ecentl\ Zuo et al [3] haxe tepo, ted the p~e.-ence of >utface b~tniel> In N d~- , ( : e u~ ; (ue O , ,/ \'ke ~epult here the vx,.- tence of BLSB m thin hhns of Yl3aeCuaO,_,, ob- served using the technique of NRMA [4]

2. E X P E R I M E N T A L

Thin superconduc t ing him> el gBa2 ( ' u307 a x~exe deposi ted b\ pul~ed l~tsm abla t ton method [5] on Y-ZrO2 sub>t~au,. 1'he c-axt> ermined hl.ns vr'l'~, - - v:,-,x,.,'R"'W) \k t ' i , t h d i ~ t ( . . . . . ,..t h, , .ul b',, X-l . t '~

ddhact~ot~ alUt four l)~,~be ~e>i~t~xitx ltlt'd'~tll('- llleI ' :Lb

' l he .NttM.\ ~_lg],M>_ ~xete te~mcled u.thg ,t B~ukm 171(2001) X-I).u~d 121'1( .tw(t~on,,t, ,1 cqtupped \~tth <tn ( ) \ to ld ('1"1200 hehunt thin (l\OSttdl The dllOt, tlUlt of tit tllAgllCtlC held ~aa-, pardllcl to the ':-<L\I'.~ ot lht' "~,mplc 'l'he & I~t:t~,It~'tl~ h':'td x~:~- ,x~cl)l ])('IV,('('II -{- ~() ( i \ \ l l ] l l(:

(l 0t}kl D.)m**dul,ttluh

F igure 1 shows the N R M A signals reco,_'ded at v m m u s tempelat tue- . . It is obsmved tha t the zero field h3steresls (dehned as the vmtical separa t io t , be tween for x~ a~ d i t l td 1 evel se sweep sign,d-, a ' zel u field) into eases ~ ith incl ease in temper~u tn e u pro T, while the ~ign,d in tens i ty falls dowr,

A

I/I

c

O

"I- "O I I . "O

R ! ! I -30 0 30

Field (Gauss)

lhgm, ' l \ I~\1 \ "~lgnal5 fol folv.<ud aml lc'X'<.'l.~(' "~vel~> ,~t ~]w held al dlfh'tc'~t tenll)Ct,o m('.~

lIl hgm(' 2 ~<' h,tx~' I)lou('d the ttollll<tllLed h~-,- tme.~l-. (dvlmv, I .~-. tlu, l , t t lo <,~ 7he :c to held I,~-,- I O l e ~ l " , t t ) t ho . . , l~ l l ,~ l i l l l ~ , l l ~ l l \ ) , tg , l l l lml ( ' l" - ' l ) o , ,1,

I l C l l l ~ 14' l l i ]~t ' l , l l i l l , ,)~ , II, ' - . l l l l l ) i ' : . I'll,: ' I1()1 l l l , . I ] [ zcd

h \ > t ( ' t t'..-q.-, t ip I,'+t'.,,,~ q",.lJ~Hl~'llt i,~llx ,t-, ~ , , , t l>pto,ttlt

0921-4534/94/$07 00 © 1994 - Elsevmr Science R V All nghts reserved. SSDI IY)21-4534(94)01594-5

d Rastogt et al/Phystca C 235-240 (1994) 2056-2057 205"

To. The solid l ine in figure 2 is the fit to the equat ion :

Y = 6.1 e x p ( - l . 7 (7~ - T) ° ~') (1)

( / I

B z 0.5 (To_ T)1/2 3.0

Figure 2. F i t of eqn. (1) to the normal ised xeru-

cal hysteresis (see text)

appl ied field and a i tuxon near the ~mlace It varies ~ e x p - ( x / ~ ) , )~ being ~he pen,'tt,ltU,,l d e p t h and x is the d i s tance of th,xon hot, the -,m face. 2) a t t rac t ive in t e rac tmn bet~eetl the [htxolt and ~ts image. It ~anes as e x p - ( 2 l / ~ \ )

For high-T0 su p e rco n d u c to r s the pene t ra t ion d e p t h A c,. (1 - T/Tc) -°~ [6]. The, 'e lore the i,i- t e rac t ions are t e m p e r a t u r e dependent A~ A in- creases with increasing t empera tu re , the mtel- ac t ion also increases leading to an tnciease nl the hysteresis with increas ing t e m p e r a t u r e a.-, ob- served here in the case of thin siugle crystal l ine fihns of YBaeCuaOr-~.

T h e fit of equa t ion (1) to the exl>mituehtal poin ts sho~n in hgure 2 Indicate~ tile c'~'.elfll,tl cor rec tness of this approach .

A C K N O W L E D G E M E N T S T h e au thors v, ould like to thank the (?oum'll ol Scientific and Indus t l i a l l (eseatch and I)epal t- merit of Science and Technolog~ india tot hna . -

clal supl)ol t

4. D I S C U S S I O N

Nmmal ly h3 s tmesis m the NRMA signal> al ~ea due to t r app ing of fluxons. T h e f luxons enter into the sample and get pinned during incle.~suig field Usually a> the tempm~ttme increases the flux(ms get more and mine thermal enetg3. If th> tllel- mal energy is sufficient enough to ovmcome the pruning force, the re is lesa u appiug of fluxons and lesser hysteresis. T ins h.vstmesis due to bulk pru- ning leads to NR~,IA signals for froward and re- verse magne t ic h e l d . weeps at dd te l en t x,due~ of the held (lateral hysteresis). Such h3 stm e>> > ab- sent tit our sample lit the t e m p e r a t u l e tange st tid- ied i l tdlcatmg negligible bulk pinning Instead, a d isplacement of the Mgnals along the x-~t.\l> (xel- ttcal hysteresis) is observed and thin hx sire es,> hi- creases with the ihcl ease m t empe~ at ut e, The ex- planation fol thi~ uitu.',u,d beha~ tout can loe -, ,tl

ht tel I11~ of .-,ut fd.ce I)<u I lel etl('cl '., Bean and [.l\lng>to:l [1] h,~\e .-.uggc>ted that

the Ollglll of >IIch b,tlllel> lies [I1 tv.o I~.llld'~ Ol IIl- t(.'taCttOl:S 1) Iel)U[',t\e ttttel+tCtl<m I)ctx~<'<:tt tlw

R E F E R E N C E S

1 C P Bean and , I D L l \ m ~ < , m Pll~- lh'~ Left 12 (196: ) 1t

2 M l(onez.3kox~skI, l.. lhnl.<hk,_,x ~ '~,'-llll- run :rid 1" l]o}lz{~Ol- }'h\-, 1{~'~ {} 1 { ,1991~

13707 3. F. Zuo S Ktuze toex , Xiugu,mg Iitlng, .I {,

Peng and t t L. Greene , l>h~ ,, l/.¢.~ l,ett 72

(1994) 1746. -1 S V BheLt, P Gangul~, 1'\. I{.,n,aktl.hl.~n

and ( ' N 1~_ Rao a Ph3~ (' 20 (19871 1.55q 5 D ~\1 lIu&ltg, T . Venk~tte.~an ( ' ( ('han,~. I.

Nazm, X I ) \~u A Inanl at .I \[ S Ih%~h' .~ppl Ph3s Lett 5-1 (19q9) 1702

6 E J . Pakuha, R I. S.tn<l._t~,lm 1' ( ' l .~l¢lhlul +trial 11- 13 I,albOX~ ttZ. \l)pI I'll\-, I,oll ~,7 ( lq90) r)t0