Spectroscopic Research of Pt + NH3
The Search for Polyatomic Molecules
Jamie Gengler, Timothy Steimle, and Jinhai Chen
Dept. of Chemistry & Biochemistry
Arizona State University, Tempe, AZ 85287
June 21, 2005
Wavenumbers
Phot
on C
ount
s
13450 13200
Funded by U.S. Dept. of Energy
Basic Energy Sciences
Motivations / Objectives
Characterize and model spectra obtained from polyatomic products of Pt + NH3.
Other polyatomic examples:
SrNH2, SrCCH, SrNC (University of Waterloo group)
Anticipation of detecting the species PtNH or PtNH2.
Plasma Chemistry and Fluorescence Detection.
20% NH3
80% Ar
500 psi
10-6 torr
diffusion pump
10-5 torr
diffusion pump
Platinum rod (rotated by stepper motor)
20 Hz Nd:YAG
355 nm (10mJ)
CW
Titanium
sapphire
750 nm
PMT
LensOptical filter
or Monochromator
Mirror
Molecular beam
20 Hz solenoid pulsed valve
pre-ampGated photon
counter
IEEE computer
board
*
*
*
D/A computer
board
*
*(variable time delay)
Burleigh
wavemeter
RS232 serial
computer board 1
#
RS232 serial
computer board 2#
Results of Previous Work.K.Y. Jung, T.C. Steimle et al, J. Chem. Phys. 102 (2): 643-652 Jan. 8 1995.
12
3 4
Features 1 and 3 are unknown. Features 2 and 4 were assumed polyatomic in nature.
Results of Previous Work.K.Y. Jung, T.C. Steimle et al, J. Chem. Phys. 102 (2): 643-652 Jan. 8 1995.
TABLE I. The predicted ab initio properties of PtN.
State Re(Å) Te(cm-1) e(cm-1) e(D)
X2 1.774 0 821 1.956a4- 1.844 975 749 2.784A2- 1.880 3431 710 2.661b4 1.928 5554 639 2.431B2 1.955 7474 564 2.255C2(II) 1.854 11040 993D2+ 1.829 13373 893 c4 2.080 14266 459E2(III) 1.885 17578 740d4(II) 1.923 18167 806 0.649
Unpublished Results.
13440
13250
13120
Wavenumber (cm-1)
Phot
on C
ount
s
12435
Low resolution spectra of Pt + NH3.
???
13450 12400
Other reagents (CH3CN, NO, N2, …) produce no spectra!
Dispersed Fluorescence (next 2 slides)
Unpublished Results.
Angstroms7900 8100 8300 8500 8700 8900 9100
Phot
on C
ount
s
12435 cm-1 Dispersed Fluorescence
1
Laser Line
Laser Line
1
945 cm-1
This molecule is probably PtN!
Unpublished Results.
Angstroms7500 7700 7900 8100 8300 8500
Phot
on C
ount
s
13120 cm-1 Dispersed Fluorescence
Laser Line
1
1940 cm-1
This molecule is probably PtN!
Laser Line
Results of Previous Work.K.Y. Jung, T.C. Steimle et al, J. Chem. Phys. 102 (2): 643-652 Jan. 8 1995.
TABLE I. The predicted ab initio properties of PtN.
State Re(Å) Te(cm-1) e(cm-1) e(cm-1)a e(D)
X2 1.774 0 821 947 1.956a4- 1.844 975 749 2.784A2- 1.880 3431 710 2.661b4 1.928 5554 639 2.431B2 1.955 7474 564 2.255C2(II) 1.854 11040 993D2+ 1.829 13373 893 c4 2.080 14266 459E2(III) 1.885 17578 740d4(II) 1.923 18167 806 0.649
a Observed value. E.J. Friedman-Hill and R.W. Field, J. Chem. Phys. 100 (9), May 1, 1994
Unpublished Results.
Angstroms7300 7500 7700 7900 8100
Phot
on C
ount
s
13250 cm-1 Dispersed Fluorescence
Laser Line
1
23
1
2
3
Laser Line
210 cm-1
440 cm-1
650 cm-1
This molecule cannot be PtN!
Platinum Dimer.
i = Ei – E0 where Ei = e(vi + ½) + exe(vi + ½)2
e = 218 ± 21cm-1
exe = -0.2 ± 5.7cm-1
Compare these to literature values:
e = 222 cm-1
exe = 0.6 cm-1
M.D. Morse et al, J. Chem Phys., 115 (16), 7543 (2001)
Band near 13255.5 cm-1 has already been assigned as Pt2.M.D. Morse et al, J. Chem Phys., 89
(9), 5517 (1988)
Pt Pt
Unpublished Results.
Laser Line
1 2
3 4
Angstroms7300 7500 7700 7900 8100 8300
Phot
on C
ount
s
13440 cm-1 Dispersed Flourescence
1
2
3
4
Laser Line
445 cm-1
655 cm-1
877 cm-1
1095 cm-1
This molecule cannot be PtN!
Wavenumber (cm-1)
Phot
on C
ount
s
13440 cm-1 High Resolution
0.2 cm-1 0.2 cm-1 0.2 cm-1
13440.5013439.80
Unpublished Results.
Natural
Abundances:194Pt = 32.9%195Pt = 33.8%196Pt = 25.3%198Pt = 7.2%
198Pt
196Pt
194Pt195Pt
Unpublished Results.
Could this molecule be PtNHx?
Wavenumber (cm-1)
Phot
on C
ount
s
13500 13400
Pt + NH3
13440Pt + ND313440
Unpublished Results.
Could this molecule be PtNHx?
Wavenumber (cm-1)
Phot
on C
ount
s
13440.00 13440.25
Pt + NH3
Pt + ND3
No!!
Platinum Dinitrogen?
Pt N NrPtN rN N
2V = k1(rNN)2 + k2(rPtN)2 + k3()2
In matrix form:
|GF – | = 0Calculated nitrogen isotope shifts:
1 = 80.11 cm-1
2 = 19.47 cm-1
3 = 15.88 cm-1
Obs. frequencies (in solid Ar):
2168.5 cm-1 (1), 499.6 cm-1 (2)A. Citra et al, J. Phys. Chem. A 105, 7799 (2001)
Angstroms7300 7500 7700 7900 8100 8300
Phot
on C
ount
s
13440 cm-1 Dispersed Flourescence
445 cm-1
655 cm-1
877 cm-1
1095 cm-1
2
3
2
23
Unpublished Results.
Could this molecule be PtN2? No!!
Pt + 14NH3
Pt + 15NH3
13440.15 13440.30Wavenumber (cm-1)
Phot
on C
ount
s
Platinum Dimer.
M.D. Morse et al, J. Chem Phys., 89 (9), 5517 (1988)
Platinum Dimer.
M.D. Morse et
al, J. Chem
Phys., 115
(16), 7543
(2001)
0 42
13440 cm-1 Dispersed Fluorescence13440 cm-1
13250 cm-1
Pt2 System VIII 0-01-0
wavenumber (cm-1)13450 13200
e/ ~ 187cm-1
wavenumber (cm-1)13700 12050
M.D. Morse et
al, J. Chem
Phys., 89 (9),
5517 (1988)
Results of Previous Work.K.Y. Jung, T.C. Steimle et al, J. Chem. Phys. 102 (2): 643-652 Jan. 8 1995.
Laser wavenumber18400 1860018500
Pt2 System XVIII (00 ~ 17914 cm-1)
3-0 4-0e/ ~ 171 cm-1
Platinum Dimer Chemistry.
Pt2 (as well as PtN) spectra disappear unless NH3 is used. Why??
1) Proposed chemical chain reaction:
2Pt* + 2NH3 2PtN + 3H2
2PtN Pt2 + N2 E ~ -5.22eV
2) Proposed metal cluster 3-body collision1 facilitated by NH3
chemisorption to Pt2:
2Pt* + :NH3
Pt*Pt*
:NH3
1) Michael D. Morse, “Supersonic Beam Sources”, Experimental Methods in the Physical Sciences, 29B, 735 (1996)
2) M. Garcia-Hernandez et al, Surface Science, 430, 18 (1999)
M a ss
Ion
dete
ctor
sign
al (v
olts
)
I r
I rN
IrN (N H )3
1 8 0 2 0 0 2 2 0 2 4 0 2 6 0 2 8 0 3 00-0 .0 1 4
-0 .0 1 2
-0 .0 1 0
-0 .0 0 8
-0 .0 0 6
-0 .0 0 4
-0 .0 0 2
0 .0 0 0
0 .0 0 2
IrN (N H )3 3IrN (N H )3 2
IrN (N H )3 4
Pt*Pt*
:NH3 Pt2 + NH3* (or fragments)
Conclusions.
PtN2 in abstract is actually Pt2. First known metal dimer/cluster formation
facilitated by a reagent (NH3).
Department of Chemistry
and Biochemistry
T.M aT.Ste im le
J .C he nJ . G e ng le r
W. Virg oR.Sm ith
A. M a rtin