• Aucun résultat trouvé

THE NON-CORRELATION OF X-RAY PHOTOELECTRON AND X-RAY EMISSION SPECTRA FOR TRANSITION METAL COMPOUNDS

N/A
N/A
Protected

Academic year: 2021

Partager "THE NON-CORRELATION OF X-RAY PHOTOELECTRON AND X-RAY EMISSION SPECTRA FOR TRANSITION METAL COMPOUNDS"

Copied!
5
0
0

Texte intégral

(1)

HAL Id: jpa-00227297

https://hal.archives-ouvertes.fr/jpa-00227297

Submitted on 1 Jan 1987

HAL is a multi-disciplinary open access archive for the deposit and dissemination of sci- entific research documents, whether they are pub- lished or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers.

L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d’enseignement et de recherche français ou étrangers, des laboratoires publics ou privés.

THE NON-CORRELATION OF X-RAY PHOTOELECTRON AND X-RAY EMISSION

SPECTRA FOR TRANSITION METAL COMPOUNDS

P. Mcclusky, D. Urch

To cite this version:

P. Mcclusky, D. Urch. THE NON-CORRELATION OF X-RAY PHOTOELECTRON AND X-RAY

EMISSION SPECTRA FOR TRANSITION METAL COMPOUNDS. Journal de Physique Colloques,

1987, 48 (C9), pp.C9-1013-C9-1016. �10.1051/jphyscol:19879181�. �jpa-00227297�

(2)

JOURNAL DE PHYSIQUE

Colloque C9, supplement au n012, Tome 48, decembre 1987

THE NON-CORRELATION OF X-RAY PHOTOELECTRON AND X-RAY EMISSION SPECTRA FOR TRANSITION METAL COMPOUNDS

P. McCLUSKY and D. URCH

Chemistry Department, Queen Mary College, University

of

on don, Mile End Road, GB-London El

4NS,

Great-Britain

Rb-,itmB 1 . e s &.t?'k~: i n i . t i a % s et f i n a l 5 d e s t r a n s i t i a n s

el

r c . t r o n i q r - t e s q u i p r o v o q u e I 'r?!ni. ssi an d e a r a y o n r - X (ERXI son'lz s e n r s i b l e h I ' o b s e r - v a % i o n c l i r e c l : . e p a r I. a s p e c t r o s c : o p i e p h o t . ~ l e c t r o r i j . q ~ r e . D o n c i I. f ai.tt q i r e l e s

& x p l i c : a t i i ? n s p o s t u i + e s p o u r 1s.; p h e n c ~ m & n e r 5 o b s e r v e s d a n s l a

s [ s e c t : r c ) s c n p i e p h o t o & l e c t r o n i q u e ( P E j marc:he a u s r - i d a n s l a d o n a i n e d e s r:ayoris-:< c-t v i c e - - v e r s a . E x a m i n a ' t i o n t f e s s p e c t r e s P E s e t ERZis d e s c:onlpor?&+.j. ci~.r f l ~ a r i q a r i & : ~ s Q t d ~ . riic:keI a d e m o n s t r b q u e l a c o r r e s p o n d e n c e ari.tlc:ilr!be n'e':st p a s to!..~.jol-tr-s t r - o c r - 4 e .

$ 2 3 t r d ~ t T h e i n i t i a l a n d f i n a l . s t a t e s o f a n e l e c t r o r 1 j . c t t - a n r j i t i o r i t h a t g i v e s r i s e . t o X - r a y e m i s s i o n c a r i b e o b s e r v e d d i r e c t l y b y

p h o t o e l e c t r - o n rjper:trnsc:opy. T h u s r a t i o n a l i ' ; s a ' t i o n a o f w p e c t r - a 1 f e a % u r e s p r o p a s e d f o r . p h n t c s e l . e e : t r o r i (F'E) s p e c t r o s c o p y z;hoc!Rd b e eqi.ta1 1. y v a l . i d f o r X - r a y e m i s s i o n l X E i s p e c t r o s c o p y , a n d v i c e v e r s a . R c o m p a r i s o n o f PE: a n d XE r e s u 1 . t ~ f o r .=,nfna m a n g a n e s e a n d n i c k e l c o r n p o i t n d s s h o w s {:hat . t h e a,-1.1:~ c:ipat.F_.d c : o r r - e l a t i o n i s rirr!t 4x1 w a y s f ocrnd.

1. Intraduction

T h e m a j . r . 1 f r a t l . . t r e s t h a t %I-6? o b s e r v e d i n b o t h X - r a y p h a t o e 1 . e c : t . r - o n (XF'Sj anid X--ray erni a a i . o r i (XES) s p e c t r - o s c z o p y c a n !.\st-tal. l v b e ra.t:sor:ai. i s a d

! r s i ng o n e e l e c : t . r o n nlode1.s a s d u e l-.o g ) h o l : a e r n i s s i o n f rorn s p e c i f i c : o r l . 3 i t . a l ~ % c3r- a?: d u e t o p e r m i t t e c f a i t ? c t r o n i c t r a n i i ~ i ' t i c 3 n s ( c l i p o l e

ssl c - t i o n rl..tl. e

--

di. a g r a m l i n e s )

,

I - e s s p e ~ t i v r ? l y . C3ther p e a k s , a r e o b s e r v e c l i n bcst.ti tyl:3?+s o f s 1 : ~ e c t r - a , .iate:llitcz p e a k s , .for. w h i c h a v a r - i e t y cxf d1.f f w e n t ~ ? x p S . a n a t i . o n % h a v e b e e n a d v a n c e d . A s t h e i n i i r i a l . a n d

+

i n a l

sta.k.n!r; L n t h e X-r-ay e m i !s-;j.c~n prot::er;s (:an b e I. r i i j i v i ciual. l y ol?.;er-ved i n X--.r.ay p h o t o e l . e c ; t r o n s p e c t r o s c o p y t h e t w o t y p e r i o f s p e c % r a a r e

i n t i m a t e l y r e l a t e d . T h u s t h e r a t i o n a l :i s a t i n r i i i i (71: s a t e l l. i.te p e a k < % o b 5 ; e r v e d i n o n e w i l . 1 h a v e i m p 1 i c : a t i o n s f o r t h e o - t h e r . A c o m p a r i ? = o r l o f s a t e l l i t e s i n t h e t w o . t y p e s of s p o c % r - a s t i o u 1 . d . t i ? s r - f o r - e p r o v i . d e a chec:tr o n t h e v a l i dl. t y o.f a pi-c?(rlr:!secl m e c t i a r i i s m f n r i-.hei r f n r r r ~ a . t i o n .

1 4 , .+of-. e?:arnpl.s, a ].ow e r i e r - g y :;atel.li:t.e i + s oot3:~erveCI i 1 . 1 XPS t h a t i r s s3i cj t o b e d u s tc, 'st7al::c?-.-!rp ' t h e n r e 1 a:.:at:i o n o f t h a t e:.:c:j. t e d s t a k e s h o u l d b e o b s t ? r v a i ~ l c ? j.n XE?. C!I-.

,

i f e;.:c:harig~= z s p X il: t i n q i s ~:~o:sl:!..tlatc<ci i n XFS, a s f o r Ilni-+ 2;s C 1 . 3 , t h e n c o r r e s ; p o r ' ~ d i n g s p l ~ . t t i n g s a h o c . t l d b e o b s e r v e d i n XE13. ' h i s n o ' k e h r . i e ? f l y s!.tr-veyr; a f e w a;i t!.tat t o n s i.rl.1er.c s!.tcrh c:olF.t-.er.pr~r~dericre m i g h t b e c?:.:pec:.\:ed.

2. Experimental Procedure

'The XP s p e c t r a w e r e m e a s u r e d u5;ing a V E E8C:A 1 1 1 i l l k 1) spectrometer.

i.ts3ing AX li n: ( ! . 1 r i ~ n n r i a c l l r c 3 m a e i s e t J ) r a d i a t i o n fc-~r- e , : c i t a t . i o n . S a m p l e c i ( p a w d e r s f r o m cornmc?rci a1 sirpl?l. i e r a ) w e r e m o u n t e d e i t h e r b y bc.?:i. rig p r c + s s e d i n t o a f i n e qa1.d c o v e r e d m e s h or b y b e i n q s t r l c i t t o ? s e l % o t : a p e . A P h i l i p s PW 1410 X--.ray f l u o r s s c : e n c e s p ~ c t r o m ~ ! t e r w a s ! . ~ s e d f c s r the? XEE . i p e c t r a . E:.:ci t a t i o n w a s b y mean:; o f a 3kW s e a l e d X - r a y t i ~ / > e !SK. Cr- c3r-

Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphyscol:19879181

(3)

C9-1014 JOURNAL

DE

PHYSIQUE

Mo anode) o r , f o r l o n g wave % - - r a y s , a CER open-.-wi.ndow Elt=nt-.-l.O

gas--dischar-ge ttilne. @n adcii.k.iont~l collimator- C21 was f i t t e d t o tzontr-01 ' h o r - i r o n t . a l clivergeric:e' and ttiu:; g i v e enhanced re.;nl~.ltiuri.

3. R e s u l t s and D i s c u s s i o n

>-a_? K p'

--

FI:-~~s_t_-,~.~_~~~~_T~~~an.;i~tI.~lrr~ Elements

-

The K p,,,: peak o f many

f i r s t row t r a n s j . t i o n meta1.s ir; c h a r - a c t ~ e r i s a d b v l:he ur-eserice o f an a d d i t i o n a l irrw--en~+rgy feaZ:urr, K p'

.

The s e p a r a t i o n between t.tie two [peaks i s s i m i l a l - . .for- niany e?lemen%s, a h r ~ u t :I.'?: .- : l 8 e V , anif .the r - e l a t r i v e i n t . e r ~ s i . t y i::: p' : I::: @ can be rot.ighl y c o r r e i a t e d w i t h t.he nt.tmher o f t..tl-lpi3fr-e!j 3cl ei.ect:r'c?nas, a,;: leas!: for- t h e I.sr;~h'ter el.eme~-~i:c,, tFe 3, 141-1 4, Ti. 5 3 . '1"hi.s corrc.:l at.i.nn has .;i.tggested 'the e:.:planation t h a t .the

(.. .;.p:li-k:!:ing . a+: +:he K p peak i s due t i 3 an exctiange effec:.t., t h e c u t l p l i n g o f t h e two possj.bl.e e,pin s t a t e s c2.F 3p" w i t h t h a t o f tl-te 3 d electr-on.;.

i f t h i s irs sn t h e n ~j!.a.ch a ' f i n a l !skate' effec!l 51-~o!.tld be c l e a r - l y seen i n t h e X F spectrc.tm o f t h e 3p l e v e l . '3 comparI.son o f t h e appt-.opriate spec~tr-a f o r Rn'" iMnF=) i s shown i n F i q . I .

4

i i

\,,,

\. F i g u r e PIn k: @ -- 1. Manganese t:: @ '

,

f 1 u u r i de

\. i s o l i d l i n e )

*. -. /

./. .-. XPS f i l m 3p r e g i o n j

/ .. -./.'

F' (clot---dash I. i n e )

../

P h o t o n E n e r g y / e v

Good agreement I.n ener-gy i h ~ b ' i n o t i n t e r i s i % y i between t l i e X P peaks ik:i.nefiic enet-.gies) at. / 4 l h ~ ? V arid 14:54.eV w:i:th t::: p ' and t:: p i s apparent.

1-I-te c:o~npar'i?son o.F t h e C:' p .

-

i:.' s p e c t r a f o r paramagnetic Ni"'

(I'Ji i O H ) , i and dian~agnetic: Ni""' fdimethylqlyo:.:ime comp1.exi shows, F i g . 2, 1:he preser1c:e c ~ f a d i s t i n c t K p' f e a t u r e a t 825Pi -- t3254. eV. B u t e:-:aminati,c)r.~ 0.6 t h e n i c k e l I-~ydr-oxide XF q~ectr-i.tm 4 a i . l ~ ,to r e v e a l any peak a t abok.~+:. 1.2 v o l t s l e q s i < j . n e t i c energy t h a n t h e main N i '!p peal.::.

(The l:ai 1 in g t h a t i s c31rrserved for- N i :3p may be d!.!e t o shake-up, - a - f f pr-ctc:e:sii;es s i n c e l c s w energy s a t e l I. I. t e peaks

-

r e s o l v e d w i t h i n c r e a s i n g c:laril:y - a r e ?seen s.t t h e same r e 1 a t i v e p o s i t i o n , abot.ht 6.5 ev lecis l::irtet:ic energy, f o r Sp, 3rj and 2 p peaks.) It: may be n o t e d t h a t a s i i n i l a r - lack: i : ~ f c o r r e ~ p o r i i ~ c e hetween X P and Xf: s p e c t r a f o r t h e K p . peak: has been sew-I f o r i r n n compounds. Why sho!.!ld t h e e f f ccirs o f

exchange cot-tpling be more c l e a r l y and c o n s j . s t e r - i t l y seen i n X E t h a n i n :fP s p e c t r a ?

!b) - .. E:.:~tianc~-,_,";-el,~~$~L~~~,,g- . . .. A c l a s s i c : e:.:ample o f e:.:change s p l j . t t i r ' ~ g i n XFS i s tti3.t nf Mn"" .35 C l I f , F i g . :5. :3s* i s t h e f i n a l s t a t e i n t h e X-ray erni.s!sion proc:esaes i.. C anti I... ?-I ( 3 s a 21'; and so i f 9s' i s , indeed, s p l i t t h e n ti-11.5 s p l i t ' t i n g shoirlci be d i r e c t 1 y o b s e r v a b l e i n t h e s e X-ray : l i n e s , u n l e s s an exe8c.kl.y s:i.mi.I.ar- s p l i t t i n g i s observed f o r t h e i n i t i a l

,7 L P I , ~ ? ancl 2 ~ 3 , : ~ s t a t e s . The XP peaks t h a t c13rre~;jpond t o t h e s e s t a t e s

?:how rsoac-? d i s.l:or-iri on buh sit:', s p l i. . k t .i ng, no new peaks -6. 5 'J away. Hut 9 p l i t t i n g i. 5 r~c!t c?h~i??r-ved f o r +he blri L. P. peal:: as can be seen i n F i g . :!;. I.ic>w can 1.k h e % t ~ n t t h e r e arl*! peal.::^ i n t h e 3s X P spectrum w h i l s t

<:he I.. C XE peal.:: i s w i k h o u t an:, l.tne:.:pected featkares'?

(4)

F i g u r e 2.

N i K p

-

I( p '

XE s p e c t r a f o r Ni ( O H ) = ( s o l i d l i n e ) a n d n i c k e l d i m e t h y l - ,

g l y o e i , m e comple:.:

( d a s h e d 1 i n e ) T h e XP s p e c t r u m f o r N i

(OH)*

i n t h e N i 3 p r e g i o n i s a l s o s h o w n

i d o t - d a s h 1 i n e )

F i g u r e 9.

M a n g a n e s e f 1 r t o r i d e : Mn L L (3s 4 2 p s , ~ ) XE s p e c t r u m ( s o l i d l i n e ) a n d XP ( M n 3s r e g i o n )

( d o t - d a s h 1 i n e ) a1 i g n e d u s i n g XP d a t a f o r

P h o t o n E n e r g y / e v Mn 2pJlz

-

k i n e t i c

SF

575 560 e n e r g y 841 e V

13% 7 395 1400 f 405

K ! n . t l c E n e r g y / e v

( c ) L cx XE a n d 2 p XP s p e c t r a <NJ?- T h e n i c k e l t a XE s p e c t r u m f r o m n i c k e l h y d r o x i d e , F i g . 4 , s h o w s c o m p l e x h i g h e n e r g y s t r u c t u r e t h a t i s a b s e n t f r o m t h a t o f t h e d i m e t h y l g l y o x i m e c o m p l e x . S e p a r a t e e x p e r i m e n t s h a v e s h o w n t h a t t h e L a : 1.. p a n d L L : 1- t-j i n t e n s i t y r a t i o s a r e t h e s a m e w h i c h i n d i c a t e s t h a t t h e L a, L p s p e c t r a a r e n o t a f f e c t e d b y s e l f - a b s o r p t i o n e f f e c 1 . t ~ . T h u s , a 1 t h o u g h t h e n e a r t . h e LI r a b s o r p t i o n e d g e , t h e h i g h - e n e r g y s t r u c t u r e i s p r o b a b l y n o t d u e t o

s e l , f - - a b s o r p t i o n .

T h e i n i t i a l s t a t e o f t h e L, a t r a n s i t i o n (Zps, "PxNa) s h o w s a cle* a n d r e l a t i v e l y i n t e n s e ' s h a k e - u p ' p e a k i n t h e XP s p e c t r u m a t a b o u t 7 v o l t s l e s s i n k i n e t i c e n e r g y t h a n t h e m a i n p e a k w h i l s t o n l y a s i n g l e p e a k is o b s e r v e d i n t h e v a l e n c e b a n d c o r r e s p o n d i n g t o 3d7. I t i s t h e r f o r e i n t e r e s t i n g t o o b s e r v e , when t h e XP a n d XE s p e c t r a a r e a l i g n e d a s i n F i g . 4 , t h a t t h e ' s h a k e - u p ' s a t e l l i t e c o r r e s p o n d s t o o n e o f t h e weak p e a k s i n t . h e h i g h e n e r g y s t r u c t u r e i n t h e L cx s p e c t r u m . D o e s t h i s p e a k r e p r e s e n t t h e r e l a x a t i o n o f a ' s h a k e - - 1 . p ' s t a t e ? By c o n t r a s t t h e

d i e m t h y l g l y n x i m e c a m p l e x s h o w s n o ' s h a k e - u p ' p e a k s i n XPS a n d n o L a h i g h e n e r g y s t r u c t u r e i s s e e n e i t h e r .

(5)

JOURNAL

DE

PHYSIQUE

F i g u r e 4 .

N i L u p e a k s f o r n i c k e l h y d r o x i d e

( s o l i d l i n e ) a n d n i c k e l d i m e t h y l -

g l y o x i m e c o m p l e x ( d a s h e d l i n e ) c o m p a r e d w i t h t h e XP s p e c t r u m f o r

N i 2p5,= r e g i o n f o r n i c k e l h y d r o x i d e ( d o t - d a s h l i n e )

845

&I ,849 i

er

/

P h o t o n ' E n a r g y / a v

-wGi

6!6 632

bp 9

b?6

$*

6?Z 6M]

K t n a t l e t n a r g y / . v

4. Concluri ons

T h e i n t e r - r e l a t i o n o f XE a n d XP s p e c t r a e n a b l e m e c h a n i s m s p r o p o s e d t o r a t i o n a l i s e t h e o c c u r a n c e o f s a t e l l i t e p e a k s i n o n e t y p e o f s p e c t r u m t o b e c r i t i c a l l y t e s t e d . N e i t h e r e l e c t r o n e x c h a n g e n o r s h a k e - u p

a p p e a r s t o g i v e e x p l a n a t i o n s t h a t c a n b e a p p l i e d c a n s i s t e n t l y t a b o t h t y p e s o f s p e c t r a , w h i c h is c u r i o u s .

Acknowledgements

T h e a u t h o r s w i s h t o t h a n k B r i t i s h G a s a n d t h e SERC who h a v e , t h r o u g h a c o - f u n d i n g s c h e m e , s u p p o r t e d a R e s e a r c h A s s i s t a n t s h i p f o r P. McC. T h e y are a l s o g r a t e f u l t o t h e R o y a l S o c i e t y , t h e C e n t r a l R e s e a r c h F u n d o f L o n d o n U n i v e r s i t y a n d t h e SERC f a r f i n a n c i a l h e l p i n t h e p u r c h a s e o f e q u i p m e n t

.

References

E l l FADLEY, C. S. P r n c . I n t . C u n f . E l e c t r o n S p e c . ( 1 9 7 1 ) 7 8 1 N o r t h - H o l ].and P u b . , C o . , A m s t e r d a m , N e t h e r l a n d s

f 2 3 HAYCOCK, D. E. a n d URCH, D. S. J. P h y s . E,, S c i . I n s t r u m . 1 5 ( 1 9 8 2 ) 40

C33 UKCH,

D.

S . a n d WEHHER, S . X - r a y S p e c t r o m . 6 (1.977) 64 C41 URCH, D. S . a n d WOOD, P. H. X - r a y S p e c t r o m . 7 (1978) 9 C 5 1 JONES, J. H. a n d URCH, D. S. A n a l y s t 108 (1983) 1 4 7 7

Références

Documents relatifs

The appearance of the long-wave intensity peaks in the alloy spectra is associated with the energy bands originated from the d-states of noble and transition

We have experimentally determined the occupied 4 f energy levels in a number of rare earth metals, namely the following ones, Nd, Sm, Eu, Gd, Dy, Er, and Yb using

- Energies of the final states involved in X-ray emission of singly ionized molecules can be obtained from photoelectron spectra.. For several small and moderately large

High resolution M,,, (3d -+ 4p) x-ray emission spectra from a k w t o n plasma were measured using a recently developed grazing-incidence reflection- grating

For this research, we constructed a high intensity field emission x-ray source used at a lower photon energy region of less than lOOkeV and using a new spectrum function

L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des

indicates that the more ionic the bond, the weaker are the satellites (Fig.2): though KF is a quite ionic solid, the satellite intensity of K Ka is weak.. We must note here that

The cartridge used was const- ructed so that most of the solid material was outside both the cyclotron diameter of the electrons and the field of view of the collimator and thus