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ORGANIC MASS SPECTROMETRY, VOL. 22, 186-187 (1987) OMS Letters Dear Sir : EFFECT OF METlIOD OF ION PREPARATION ON CHARGE STRIPPING MASS SPECTRA It has been clearly demonstrated that the charge stripping mass spectra of singly charged positive ions can be used to characterize gaseous ion struc- tures; in many cases such spectra provide isomer d i f ferentat ion where collision-induced dissociation mass spectra do not.’ Although it is clearly estab- lished that charge stripping mass spectra are depen- dent on the identity of the neutral collision gas,’” it is less clear what role the internal energy of the reacting i.ons plays in determining the mass spectrum observed. Bowen et a13 and McLafferty et a14 have reported that the charge stripping mass spectra of isomeric [C H 1 ions prepared by 70 eV and by 17 eV electron impact are the same, within experimental error, suggesting no effect of reactant ion internal energy on the observed spectra. Dass et a15 have observed significant differences in the charge stiippinp mass spectra 0: [C~::~I+. iozs pre- pared by charge exchange with different internal energies but have attributed these differences to isomerization reactions of the precursor ions prior to collision rather than to internal energy effects on the mass spectrum of a distinct ionic species. On the other hand, Bowers and colleagues6 have re- ported that the charge stripping mass spectra of [CH3CH2NH3]+, [ CH3NH2CH3]+ and [ CH3CH20H2]+, p r e - pared by proton transfer chemical ionization, changed with the total ion source pressure. The protonated species were formed by a strongly exothermic proton transfer reaction; with increasing source pressure the excited species should be more effectively de- +. 36 activated by collision and they attributed the ob- served spectral changes to the effect of initial internal energy and/or angular momentum on the charge stripping mass spectra. The present letter reports observations similar to those reported by Bowers et a16, but for more complex species, which show that charge stripping mass spectra of ions pre- pared by proton transfer chemical ionization depend on the method of ion preparation; we attribute these changes in spectra to the effect of initial internal energy. + + r 2 3 r +OH CH CH=CH-CH CH =C(CH )C€l 3 II CH =CH-CCH 2 1 2 3 Table 1 presents the charge stripping mass spectra of t h e [C4H70] fer chemical ionization. These spectra were ob- t a i n e d u s i n g a ZAB-2FQ mass spectrometer7 for ions of 8 keV kinetic energy using He as collision gas at an indicatcc! presxrc of 2 S 12 xbar OF. the ioniza- tion gauge located on the pumping line below the collision cell. All mass-and energy-resolving slits were full open and signals were measured in terms of relative peak heights. Results are presented for ions prepared by CH4 chemical. ionization and by i-C4HI0 chemical ionization. studied, the charge stripping mass spectra obtained for ions prepared by i-C4H10 CI show a greater abun- dance of [C4H70]’+ and a lower abundance of ions arising by multiple loss of H/H from this ion ( i e . [C4H501 and [C4H40] ) than do the spectra obtained for the same ions prepared by CH CI; the differences are well outside the reproducibility of + ions 1 to 3, prepared by proton trans- -7 For the three species 2 2+ 2+ 4 Table 1. He Charge Stripping Mass Spectra of (C H 0)’ Ions 47 % of Total Ion Signal 1 2 3 Product CH4CI i-C4H10CI CH4CI i-C4H10CI CH4CI i-C4H10CI [ C4H701 ’+ 70.922.6 85.220.2 45.6f4.7 58.820.6 38.021.6 51.2+0.7 14.720.7 18.3t0.1 27.321.3 25.7f1.1 [CGH6012+ 0.8f0.3 [ C4H401 ’+ 26.9?2.4 12.7t0.3 22.523.4 12.120.2 - 17.2t2.0 10.820.5 13.7t0.7 9.3t0.2 [ C4H501 2f 2.2t0.3 1.2t0.1 21.121.2 13.820.4 @ 1987 by John Wiley & Sons, Ltd. Received December 1986

Effect of method of ion preparation on charge stripping mass spectra

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ORGANIC MASS SPECTROMETRY, VOL. 22, 186-187 (1987)

OMS Letters

Dear S i r :

EFFECT OF METlIOD OF I O N PREPARATION ON CHARGE STRIPPING MASS SPECTRA

It has been c l e a r l y demonstrated t h a t t h e charge

s t r i p p i n g mass s p e c t r a of s i n g l y charged p o s i t i v e

ions can be used t o c h a r a c t e r i z e gaseous ion s t r u c -

t u r e s ; i n many c a s e s such s p e c t r a p rov ide isomer

d i f f e r e n t a t ion where co l l i s ion - induced d i s s o c i a t i o n

mass s p e c t r a do n o t . ’ Although i t i s c l e a r l y e s t ab -

l i s h e d t h a t charge s t r i p p i n g mass s p e c t r a a r e depen-

dent on t h e i d e n t i t y of t h e n e u t r a l c o l l i s i o n gas,’”

i t i s l e s s c l e a r what r o l e t h e i n t e r n a l energy of

t h e r e a c t i n g i.ons p l ays i n de te rmining t h e mass

spectrum observed. Bowen et a13 and McLafferty

e t a14 have r epor t ed t h a t t h e charge s t r i p p i n g mass

s p e c t r a of i somer ic [C H 1 i ons prepared by 70 e V

and by 1 7 e V e l e c t r o n impact a r e t h e same, w i t h i n

exper imenta l e r r o r , sugges t ing no e f f e c t of r e a c t a n t

ion i n t e r n a l energy on t h e observed s p e c t r a . Dass

e t a15 have observed s i g n i f i c a n t d i f f e r e n c e s i n t h e

charge s t i i p p i n p mass s p e c t r a 0: [ C ~ : : ~ I + . i o z s p r e -

pared by charge exchange wi th d i f f e r e n t i n t e r n a l

e n e r g i e s but have a t t r i b u t e d t h e s e d i f f e r e n c e s t o

i somer i za t ion r e a c t i o n s of t h e p recu r so r i o n s p r i o r

t o c o l l i s i o n r a t h e r t han t o i n t e r n a l energy e f f e c t s

on t h e mass spectrum of a d i s t i n c t i o n i c species.

On t h e o t h e r hand, Bowers and co l l eagues6 have r e -

por ted t h a t t h e charge s t r i p p i n g mass s p e c t r a of

[CH3CH2NH3]+, [ CH3NH2CH3]+ and [ CH3CH20H2]+, pre-

pared by pro ton t r a n s f e r chemical i o n i z a t i o n , changed

wi th t h e t o t a l i on source p r e s s u r e . The pro tona ted

s p e c i e s were formed by a s t r o n g l y exothermic pro ton

t r a n s f e r r e a c t i o n ; w i th i n c r e a s i n g source p r e s s u r e

t h e exc i t ed s p e c i e s should b e more e f f e c t i v e l y de-

+. 3 6

a c t i v a t e d by c o l l i s i o n and they a t t r i b u t e d t h e ob-

se rved s p e c t r a l changes t o t h e e f f e c t of i n i t i a l

i n t e r n a l energy and/or angu la r momentum on t h e

cha rge s t r i p p i n g m a s s s p e c t r a . The p resen t l e t t e r

r e p o r t s obse rva t ions s i m i l a r t o those r epor t ed by

Bowers e t a16, bu t f o r more complex s p e c i e s , which

show t h a t cha rge s t r i p p i n g m a s s s p e c t r a of i o n s pre-

pared by p ro ton t r a n s f e r chemical i o n i z a t i o n depend

on t h e method of i on p r e p a r a t i o n ; w e a t t r i b u t e t h e s e

changes i n s p e c t r a t o t h e e f f e c t of i n i t i a l i n t e r n a l

energy.

+ + r 2 3

r +OH

CH CH=CH-CH CH =C(CH )C€l 3 II

CH =CH-CCH 2 1 2 3

Table 1 p r e s e n t s t h e charge s t r i p p i n g mass s p e c t r a of

t h e [C4H70]

f e r chemical i o n i z a t i o n . These s p e c t r a were ob-

t a i n e d u s i n g a ZAB-2FQ m a s s spec t rometer7 f o r i ons of

8 keV k i n e t i c energy us ing H e as c o l l i s i o n gas a t an

ind ica tcc! p r e s x r c of 2 S 12 xbar OF. t h e ion iza -

t i o n gauge l o c a t e d on t h e pumping l i n e below t h e

c o l l i s i o n c e l l . A l l mass-and energy-reso lv ing s l i t s

were f u l l open and s i g n a l s were measured i n te rms of

r e l a t i v e peak h e i g h t s . R e s u l t s are presented f o r

i o n s prepared by CH4 chemical. i o n i z a t i o n and by

i - C 4 H I 0 chemical i o n i z a t i o n .

s t u d i e d , t h e charge s t r i p p i n g mass s p e c t r a ob ta ined

f o r i o n s prepared by i-C4H10 C I show a g r e a t e r abun-

dance of [C4H70]’+ and a lower abundance of i ons

a r i s i n g by m u l t i p l e l o s s of H / H from t h i s i on

( i e . [C4H501 and [C4H40] ) t han do t h e s p e c t r a

ob ta ined f o r t h e same i o n s prepared by CH C I ; t h e

d i f f e r e n c e s a r e w e l l o u t s i d e t h e r e p r o d u c i b i l i t y of

+ ions 1 t o 3 , p repared by pro ton t r a n s -

-7

For t h e t h r e e s p e c i e s

2 2+ 2+

4

Table 1 . H e Charge S t r i p p i n g Mass Spec t r a of (C H 0)’ Ions 4 7

% of To ta l Ion S igna l

1 2 3

Product C H 4 C I i -C4H10CI C H 4 C I i - C 4 H 1 0 C I C H 4 C I i -C4H10CI

[ C4H701 ’+ 70.922.6 85.220.2 45.6f4.7 58.820.6 38.021.6 51.2+0.7

14.720.7 18 .3 t0 .1 27.321.3 25.7f1.1 [CGH6012+ 0 .8 f0 .3

[ C4H401 ’+ 26.9?2.4 12 .7 t0 .3 22.523.4 12.120.2

- 17.2 t2 .0 10.820.5 13.7t0.7 9.3t0.2 [ C4H501 2f 2 .2 t0 .3 1 .2 t0 .1

21.121.2 13.820.4

@ 1987 by John Wiley & Sons, Ltd. Received December 1986

OMS LETTERS

t h e measuzements which a r e g i v e n i n the Table . The

s p e c t r a o b t a i n e d f o l l o w i n g CH C I are i n r e a s o n a b l e

agreement w i t h t h o s e r e p o r t e d e a r l i e r . 8 4

T h e p r o t o n a f f i n i t i e s o f the C H 0 c a r b o n y l com-

pounds have b e e n r e p o r t e d as PA(CH =CHCOCH )=826 k J

mol-', PA(CH CH=CHCHO)=824 k J mol-l and PA(CH =C(CH3)

CHO)=808 k J m o l - . compounds by [ t -C4H9] (PA(i-C4H8)=824 k J mol-' )

i n i-C4H10CI s h o u l d b e a p p r o x i m a t e l y t h e r m o n e u t r a l ,

a l t h o u g h it i s p r o b a b l e tha t n o t a l l [C4Hg]+ i o n s

are i n t h e i r ground s ta te u n d e r o u r e x p e r i m e n t a l

c o n d i t i o n s ; i n any event the e x t e n t o f e x c i t a t i o n of

t h e [C4H70] i o n s formed s h o u l d b e s m a l l . By c9n-

t ras t , p r o t o n a t i o n of t h e c a r b o n y l compounds i n

CH C I is s u b s t a n t i a l l y e x o t h e r m i c even f o r ground

s ta te r e a c t a n t i o n s (f'g(CH4)=546 k J mol-I ) and

PA(C2H4)=684 k J mo1-l

n i f i c a n t f r a c t i o n of t h i s e x o t h e r m i c i t y t o b e re-

t a i n e d by the [C4H70] i o n s formed. The s i m p l e s t

i n t e r p r e t a t i o n of the r e s u l t s is tha t a t least p a r t

of t h i s excess i n t e r n a l e n e r g y is c a r r i e d o v e r t o

the [C4H70]

p r o c e s s and r e s u l t s i n an i n c r e a s e d e x t e n t o f f r a g -

m e n t a t i o n of t h i s i o n . In s u p p o r t of t h i s i n t e r p r e -

t a t i o n w e n o t e t h a t v a r i a t i o n of t h e s o u r c e p r e s s u r e

i n the CH C I s y s t e m l e a d s t o a v a r i a t i o n i n t h e

c h a r g e s t r i p p i n g m a s s s p e c t r a a s shown i n T a b l e 2

f o r [CH CE=TUCHOH]+; w i t h i n c r e s s i n g p r e s s u r e t h e

[C4H70]

c o l l i s i o n a l l y , r e s u l t i n g i n less f r a g m e n t a t i o n f o l -

lowing c o l l i s i o n a l i o n i z a t i o n . The s p e c t r a o f T a b l e

1 were r e c o r d e d a t the s o u r c e p r e s s u r e which gave

t h e optimum y i e l d of t h e p r o t o n a t e d s p e c i e s ; t h i s

o c c u r r e d at a s o u r c e i o n i z a t i o n gauge r e a d i n g o f

- 5 X mbar, a l t h o u g h , f rom p r e v i o u s e x p e r i e n c e

w e b e l i e v e that when these e x p e r i m e n t s were per -

formed t h e i o n i z a t i o n gauge w a s r e a d i n g low by ap-

p r o x i m a t e l y a f a c t o r of t e n .

formed by i-C4H10CI showed no dependence of t he i r

c h a r g e s t r i p p i n g m a s s s p e c t r a on s o u r c e p r e s s u r e

s i n c e t h e [C4H70]+ ions are formed i n i t i a l l y w i t h

v e r y l i t t l e e x c e s s internal energy .

the s p e c t r u m o b t a i n e d a t t h e h i g h e s t CH4 s o u r c e

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

i -C4HIOCI .

4 6

2 3

3 1 2 Thus p r o t o n a t i o n of t h e c a r P 8 n y l +

+

4

) and o n e would e x p e c t a s i g -

+

2+ i o n formed i n the c h a r g e s t r i p p i n g

4

3 i o n s are more e f f e c t i v e l y d e a c t i v a t e d

The [C4H70]+ i o n s

I n t e r e s t i n g l y

T h e p r e s e n t r e s u l t s show c l e a r l y tha t the c h a r g e

s t r i p p i n g mass s p e c t r a o f i o n s formed b y p r o t o n

t r a n s f e r c h e m i c a l i o n i z a t i o n depend on the method

of i o n f o r m a t i o n i n a manner which i s c o n s i s t e n t

w i t h an i n f l u e n c e of i n i t i a l i n t e r n a l e n e r g y on the

c h a r g e s t r i p p i n g spec t rum. Obvious ly i n s u c h

e x p e r i m e n t s one s h o u l d p r e p a r e the reactant i o n s by

the least exothermic r e a c t i o n p o s s i b l e . It is w e l l -

187

e s t a b l i s h e d ' tha t c h a r g e s t r i p p i n g u s i n g N2 or 0 2 as c o l l i s i o n g a s i m p a r t s less e n e r g y t o t h e

c h a r g e - s t r i p p e d i o n and o n e might a n t i c i p a t e t h a t

t h e e f f e c t of i n i t i a l i n t e r n a l e n e r g y would b e more

pronounced when t h e s e c o l l i s i o n g a s e s a r e u s e d . I n

t h e p r e s e n t s y s t e m s the u s e of O2 o r N2 c o l l i s i o n

g a s e s r e s u l t e d a l m o s t e n t i r e l y i n f o r m a t i o n of

[ C H 012+.

s e p a r a t e l y , o f the c h a r g e s t r i p p i n g mass s p e c t r a of

[C H ]+ i o n s we have found t h a t t h e N2 and 0

c h a r g e s t r i p p i n g mass s p e c t r a a r e more s e n s i t i v e t o

the method of i o n p r e p a r a t i o n t h a n a r e t h e He c h a r g e

s t r i p p i n g mass s p e c t r a .

However, i n s t u d i e s , t o b e r e p o r t e d 4 7

2 9 11

T a b l e 2 . E f f e c t of CH4 P r e s s u r e on Charge S t r i p p i n g

Mass S p e c t r a o f 2

% of T o t a l Ion S i g n a l

3X10-6mbar 8X10-6mbar 2 . 5X10-5mbar

[C4H701 2+ 43 .3 55.2 60.6

[ C4H601 2+ 12 .6 14 .0 15.2

[ C4H50 1 2+ 1 9 . 3 13 .8 10 .8

[ C 4 H 4 0 1 '+ 24.9 17 .O 13.4

Yours

Alex G . H a r r i s o n

Department of Chemis t ry

Un iver 5 4. t y o f Tor o n t o

T o r o n t o , O n t a r i o

Canada M5S 1 A l

R e f e r e n c e s

1.

2 .

3 .

4 .

5 .

6 .

7 .

8 .

9 .

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J.L. Holmes, Org. Mass Spect rom. , 0, 169 (1985)

R .D. Bowen, M.P. B a r r a l a s , F.P. Pagano, P . J . Todd

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( 1 980)

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C . Dass, D.A. Peake and M.L. G r o s s , Org. Mass.

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