sims and scanning ion microscopy · 2020. 12. 30. · figure 3: scanning ion micrograph of (a)...
TRANSCRIPT
HAL Id: jpa-00229419https://hal.archives-ouvertes.fr/jpa-00229419
Submitted on 1 Jan 1989
HAL is a multi-disciplinary open accessarchive for the deposit and dissemination of sci-entific research documents, whether they are pub-lished or not. The documents may come fromteaching and research institutions in France orabroad, or from public or private research centers.
L’archive ouverte pluridisciplinaire HAL, estdestinée au dépôt et à la diffusion de documentsscientifiques de niveau recherche, publiés ou non,émanant des établissements d’enseignement et derecherche français ou étrangers, des laboratoirespublics ou privés.
SIMS AND SCANNING ION MICROSCOPYG. Allen, I. Brown
To cite this version:G. Allen, I. Brown. SIMS AND SCANNING ION MICROSCOPY. Journal de Physique Colloques,1989, 50 (C2), pp.C2-121-C2-125. �10.1051/jphyscol:1989221�. �jpa-00229419�
JOURNAL DE PHYSIQUE Colloque C2, supplhment au n02, Tome 50, f6vrier 1989
SIMS AND SCANNING ION MICROSCOPY
G.C. ALLEN and I.T. BROWN
Central Electricity Generating Board, Berkeley Nuclear Laboratories, Berkeley, GB-Gloucestershire GL13 9PB, Great-Britain
Resume - Un microscope a b a l l a y a g e i o n i q u e developpe aux "Berke ley -- Nuclear L a b o r a t o r i e s " du C . E . G . B . , e s t d e c r i t .
Par bombardement i o n i a u e a p a r t i r d 'une s o u r c e de g a l l i u m metal 1 i q u i d e e t a n a l y s e s c o n s e c u t i v e s des i o n s s e c o n d a i r e s e t des
e l e c t r o n s emi s , s e l on des t e c h n i q u e s c o n v e n t i o n n e l l e de s p e c t r o s c o p i e de masse e t de mic roscop ie e l e c t r o n i q u e , c e t a p p a r e i l permet d ' o b t e n i r l e s p e c t r e de masse des i o n s s e c o n d a i r e s e t de v i s u a l i s e r 1 a s u r f ace exami nee.
Des r e s u l t a t s de mic roscop ie a b a l l a y a g e a p p l i q u e e s a des e t u d e s de ma te r i aux m e t a l l i q u e s , i n o r q a n i q u e s e t o rgan ique s e r o n t p r e s e n t e s .
A b s t r a c t - A scann ing ion microscope developed a t t h e C E G B ' s
Berkeley Nuclear L a b o r a t o r i e s i s d e s c r i b e d .
By ion bombardment from a l i q u i d metal ga l l ium s o u r c e , and subsequen t a n a l y s i s of both t h e r e s u l t a n t secondary i o n s and
secondary e l e c t r o n s us ing c o n v e n t i o n a l t e c h n i q u e s of mass s p e c t r o m e t r y and e l e c t r o n microscopy, t h i s i n s t r u m e n t o f f e r s both
secondary ion mass a n a l y s i s (SIMS) and t h e f a c i l i t y f o r imaging t h e
s u r f a c e under i n v e s t i g a t i o n .
R e s u l t s from t h e a p p l i c a t i o n of t h e scann ing ion microscope t o t h e s tudy of meta l1 i c y i n o r q a n i c and o r q a n i c m a t e r i a l s a r e p r e s e n t e d .
The t e c h n i q u e s used f o r t h e examina t ion and a n a l y s i s of s o l i d s a r e many and v a r i e d b u t t h e i r development may be t r a c e d us i n q s c a n n i n g e l e c t r o n microscopy as a s t a r t i n g p o i n t . Fol lowing t h e i n t r o d u c t i o n of t h i s method came t h e d e s i r e t o de te rmine t h e chemical compos i t ion of t h e f e a t u r e s r e v e a l e d . A t f i r s t t h i s was p o s s i b l e th rough t h e a n a l y s i s of X - r a d i a t i o n produced dur ing t h e p r o c e s s of bombardment of t h e specimen w i t h t h e high energy e l e c t r o n beam, b u t two decades ago t e c h n i q u e s o f f e r i n g i n f o r m a t i o n
more r e p r e s e n t a t i v e of t h e s u r f a c e such as X-ray 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 ,
Auger e l e c t r o n s p e c t r o s c o p y (AES) and secondary ion mass s p e c t r o m e t r y (SIMS)
Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphyscol:1989221
C2-122 JOURNAL DE PHYSIQUE
were developed. Of t h e s e methods a c c e p t a n c e was gained most s lowly by t h e l a t t e r b u t mic roscop ic a n a l y s i s by SIMS has been made p o s s i b l e by t h e use of l i q u i d metal s o u r c e s t o produce t h e pr imary ion beaml. These hiqh
b r i g h t n e s s s o u r c e s pe rmi t t h e fo rma t ion of high i n t e n s i t y submicron i o n p robes and modern i n s t r u m e n t a t i o n a l l o w s t h e c o l l e c t i o n of secondary e l e c t r o n and secondary ion images which p r o v i d e s u r f a c e topography of one monolayer 2 . The Berkeley i n s t r u m e n t , shown s c h e m a t i c a l l y i n F i g u r e 1 , i s
t h e r e f o r e , a combinat ion of a microscope and a submicron a n a l y t i c a l p robe 3 .
DETECTOR r - - - *
MASS LIQUID METAL I O N GUN
VACUUM SYSTEM 25 DISPLAY D l SPLAY
COPIER / PRINTER i--i
F i g u r e 1: Schemat ic diagram of Berke ley Scanning Ion Microscope (SIM)
Typ ica l images from a number of specimens d i f f i c u l t t o examine w i t h o u t p r i o r c o a t i n g t e c h n i q u e s which mask o r modify i m p o r t a n t s u r f a c e chemical p r o p e r t i e s i n conven t iona l e l e c t r o n microscopy a r e shown i n F i g u r e s 2 and 3 .
F i g u r e 2 : Ion induced e l e c t r o n micrograph from f o o t of h o r s e f l y (Tabanus )
F i g u r e 3 : Scanning ion micrograph of ( a ) p u l v e r i s e d f u e l ash (PFA) p a r t i c l e ( b ) a r e a of p a r t i c l e a t h i g h e r m a g n i f i c a t i o n
Organic m a t e r i a l s a r e normal ly degraded i n an e l e c t r o n beam and i n s u l a t i n g samples such a s t h e PFA sample ( F i g u r e 3 ) which i s mainly
composed of s i l i c a , may be s u b j e c t t o c h a r g i n g '+. I n t h e ion microscope
however, good images w i t h a remarkable depth of f i e l d were o b t a i n e d a f t e r s e v e r a l minu tes ; presumably t h e i m p l a n t a t i o n of gal 1 ium i o n s a1 l e v i a t e s t h e
b u i l d up of s u r f a c e cha rge d u r i n g t h e bombardment p r o c e s s . Bombardment of t h e s u r f a c e w i t h i-ons n o t o n l y produces secondary
e l e c t r o n s b u t a l s o s t i m u l a t e s t h e emiss ion of secondary i o n s . I f t h e pr imary ion beam i s r a s t e r scanned ove r t h e s u r f a c e and s p e c i f i c secondary
i o n s moni tored a t each p o i n t , a chemical image can be gene ra ted : T h i s i s done by computer p r o c e s s i n q t h e d a t a t o y i e l d maps o r s p a t i a l images of t h e
secondary i o n s ana lysed which may then be r e l a t e d t o e l e c t r o n images from t h e same s u r f a c e ( F i g u r e 4 ) .
( a ) ( b )
F i g u r e 4 : ( a ) Ion induced e l e c t r o n image of wear s c a r s on t h e s u r f a c e of a
s t a i n 1 e s s s t e e l sampl e . ( b ) Map of t h e O H - ion t aken from t h e same sample.
C2-124 JOURNAL DE PHYSIQUE
To demons t ra t e t h e use of t h e i n s t r u m e n t i n secondary ion mass a n a l y s i s
(SIMS) t h supe rconduc t ing compound YBa2Cu307-x has been examined 5 . The
p o s i t i v e ion spect rum from a f r e s h l y p r e p a r e d sample i s shown i n F i g u r e 5 ( a )
and may be compared w i t h t h a t from t h e same m a t e r i a l f o l l o w i n g l e n g t h y
exposure t o t h e a tmosphere F i g u r e 5 ( b ) . The p r e s e n c e of a hydroxide l a y e r
a t t h e s u r f a c e of t h e sample exposed t o a i r i s r e a d i l y a p p a r e n t . Although
t h i s l a y e r i s r e a d i l y removed by s p u t t e r i n g t h e p r e s e n c e of y t t r i u m and
barium hydrox ides cou ld p lay a s - i g n i f i c a n t r o l e i n s u r f a c e conduc t ion
behav iour .
F i g u r e 5: P o s i t i v e SIMS S p e c t r a f o r YBa2Cu307-x ( a ) F r e s h l y S i n t e r e d
( b ) Exposed t o t h e Atmosphere
The i n t e n s i t i e s of t h e v a r i o u s c l u s t e r i o n s i n t h e s p e c t r a a r e n o t
r e l a t e d t o t h e composi t ion of t h e sample. They a r e a r e s u l t of t h e
thermodynamic/chemical equi 1 i b r i a i n v o l v e d i n t h e s p u t t e r i n g p r o c e s s 5 . The
bond d i s s o c i a t i o n e n e r g i e s f o r metal o x i d e i o n s a r e p l o t t e d a g a i n s t t h e
f u n c t i o n l o g ( M O + / M + ) i n F i g u r e 6 . T h i s r e l a t i o n s h i p s u g g e s t s t h a t a s t h e
d i s s o c i a t i o n energy of t h e meta l ox ide d e c r e a s e s , t h e obse rved meta l -oxi de
peak becomes l e s s prominent .
; 2 3 L S 6 7 8 3 I O
Dlssociat~on energy 0: (M-0 ) ' (eV)
F i g u r e 6: R e l a t i o n s h i p be tween m e t a l o x i d e SIMS i n t e n s i t i e s a.nd s t a b i l i t y o f m e t a l o x i d e i o n .
ACKNOWLEDGEMENT
The w o r k was c a r r i e d o u t a t t h e B e r k e l e y N u c l e a r L a b o r a t o r i e s o f t h e
R e s e a r c h D i v i s i o n and t h e p a p e r i s p u b l i s h e d w i t h t h e p e r m i s s i o n o f t h e
C e n t r a l E l e c t r i c i t y G e n e r a t i n g Board .
REFERENCES
1 P.D. P r e w e t t , D.K. J e f f r i e s . I n s t . Phys. Con f . Ser . V o l . 54 . L i q u i d m e t a l f i e l d e m i s s i o n i o n s o u r c e s and t h e i r a p p l i c a t i o n s . I n s t i t u t e o f P h y s i c s , B r i s t o l ( 1 9 8 0 ) p 316 .
2 R. L e v i - S e t t i , J.M. B h a b a l a , Y.L. Wang. U l t r a m i c r o s c o p y (19881 , 24, 97
G.C. A l l e n , I . T . Brown. CEGB R e s e a r c h ( 1 9 8 8 ) i n p r e s s .
4 G.C. A l l e n , A.R. J o n e s , A.G. Warner . P a r t . C h a r a c t . (19861 , 3, 89 .
5 G.C. A l l e n , I . T . Brown. P h i l . Mag. L e t t e r s ( 1 9 8 8 ) i n p r e s s .