64 th osu international symposium on molecular spectroscopy
TRANSCRIPT
Assignment of mm- and smm-wave spectra of rare isotopologues of cyanamide and the rm
(1)
geometry of NH2CN
64th OSU International Symposium on Molecular Spectroscopy
Adam Krasnicki, Zbigniew KisielInstitute of Physics, Polish Academy of Sciences
Brenda P. Winnewisser, Manfred WinnewisserDepartment of Physics, The Ohio State University
The cyanamide molecule H2NCN
5 atoms, 9 normal modesμa = 4.3192(40) D, μc =-0.9559(33) DInversion transitions (0+-0-) due to tunnelingprotons through low potential barrier (469.12 cm-1) Previous studies by rotational spectroscopy
cmw: + ND2CN, NHDCN Millen et. al, J.Mol.Spectrosc. 8, 153 (1962)D & 15N-isototopologues Tyler et. al , J.Mol.Spectrosc. 43, 248 (1972)to 120 GHz: Johnson et. al Astrophys. J. 208, 245 (1976)srb analysis: + D & 15N Brown et. al, J.Mol.Spectrosc. 114, 257 (1985)to 500 GHz: + D Read et. al, J.Mol.Spectrosc. 115, 316 (1986)14N splitting: Brown et al., J.Mol.Spectrosc. 130, 213 (1988)FT far ir: Birk,Winnewisser, J.Mol.Spectrosc. 159, 69 (1993)ir to 980 cm-1: Moruzzi,Jabs,2Winnewisser, J.Mol.Spectrosc. 190, 353 (1998)mmw + ir 8-350 cm-1 + D Kisiel,Krasnicki,2Winnewisser, 63rd OSU, WK08, (2008)
astrophysical: Turner et al., Astrophys. J. 201, L149 (1975) Lines emission in Sgr B2
More background…
MMW spectra measured on BWO based spectrometers in Giessen and Köln118-179 GHz, 202-221 GHz, 570-650 GHzWolfgang Jabs, Giessen 1998
Transitions:
a – type: 0+→ 0+, 0-→ 0- μa=4.3192(40)Dc – type: 0+→ 0-, 0-→ 0+ μc=-0.9559(33)D
Reduced quartic-quadratic potentialV(z)=A(z4+Bz2)
z=const*mred*A-⅟2*Ф
The spectra
a – type (0+ → 0+, 0- → 0-)
c – type (0+ → 0-, 0- → 0+)
Experimental spectrum
The spectra of deuterated isotopologues of NH2CN
ND2CN NHDCN
NH2CN
aR, J” = 7, {0+, 0-}
Relative intensity:ND2CN : NHDCN : NH2CN 1 : 1 : 0.15
ND213C
N
aR, J” = 7, {0+, 0-}
The spectra of deuterated isotopologues of NH2CN
NHD13CN
NH213C
N
Relative intensity:ND2CN : NHDCN : NH2CN 1 : 1 : 0.1513C abundance 1.07%
15ND2CN
Relative intensity:ND2CN : NHDCN : NH2CN 1 : 1 : 0.1513C abundance 1.07%15N abundance 0.368%
aR, J” = 7, {0+, 0-}
The spectra of deuterated isotopologues of NH2CN
15NHDCN
NHDC15
NND2C15
N
The J = 8 ← 7 rotational transition in ND2C15N
Blue – 0+
White – 0-
15ND2CN, Ka=1, 0+ NHDCN, cQ, 0+→ 0-
The J = 8 ← 7 rotational transition in ND2C15N
Ka=5Ka=4
0+ 0- 0-0+ 2:1 alternation of statistical weights
Blue – 0+
White – 0-
The Hamiltonian
Hrot – Watsonian asymmetric rotor Hamiltonian (reduction A, represent. Ir)
H01 – interstate second order Coriolis coupling terms expressed in Reduced Axis System (H.M.Pickett, J.Chem.Phys., 1972, 56, 1715.)
H01 = (Fca + FcaJ P 2 + Fca
K Pz 2 + …) (Pc Pa + Pa Pc ) +
(Fbc + FbcJ P 2 + Fbc
K Pz 2 + …) (Pb Pc + Pc Pb )
H(0)rot + ΔE
H01
H01
H(1)rot
0+
0-
Simultaneous fit of
data for 0+ and 0- states with SPFIT of
H.M. Pickett
Fbc term used only for the HDNCN species
The fitted constants for ND2C15N
+ similar results for NH2
13CN, NHD13CN,ND2
13CN, NHDC15N,15ND2CN, 15NHDCN
E = 494551.901(27) MHz
Fca = 267.6102(19) MHz
For ND2CN
The 0+- 0- splitting as a test for correct assignment
ΔEisot.- ΔEND2CN ND213CN ND2C15N 15ND2CN
obs. / cm-1 0.022 -0.011 -0.633
calc./ cm-1 0.049 -0.064 -0.771
ΔE(0- - 0+) ND2CN
obs. / cm-1 16.4965304(9)
calc./ cm-1 15.387
ΔE(0- - 0+) NHDCN
obs. / cm-1 32.089281(4)
calc./ cm-1 31.062
ΔEisot.- ΔENHDCN NHD13CN NHDC15N 15NHDCN
obs. / cm-1 0.029 -0.001 -0.780
calc./ cm-1 0.062 -0.082 -0.986
ΔE(0- - 0+) NH2CN
obs. / cm-1 49.567984(4)
calc./ cm-1 49.567
ΔEisot.- ΔENH2CN NH213CN
obs. / cm-1 0.062
calc./ cm-1 0.069
Results from obtained by using the reduced quartic-quadratic potential
V(z)=A(z4+Bz2)and program ANHARM
A, B parameters scaled for isotopic species based on reduced mass for inversion
motion in cyanamide
Experimental r0, rm(1) and rm
(1L) geometries of cyanamide
r0 rm(1) rm
(1L)
r(N─H) /Å 1.0032(12) 1.0189(23) 1.0152(27)
r(N─C) 1.3445(57) 1.3448(17) 1.3434(17)
r(C≡N) 1.1632(59) 1.1650(18) 1.1641(17)
(HNH) /° 116.26(23) 112.32(24) 111.79(31)
(NCN) [180.0] [180.0] [180.0]
Φ 35.47(60) 41.67(90) 43.05(70)
ca /u1/2*Å -0.0550(93) -0.121(30)
cb-0.0194(11) -0.0146(24)
cc[0.0] [0.0]
δH0.028(12)
σfit / uÅ2 0.01545 0.00462 0.00431
Comparison of geometries of cyanamide
rm(1L)
this workMP2/aug-cc-pVTZ
this workaveraged rs str. Tyler et.al JMS ’72
semirigid benderBrown et.al JMS ’88
r(N─H) /Å 1.0152(27) 1.0096 1.001(15) [0.9994]
r(N─C) 1.3434(17) 1.3450 1.346(5) 1.3301(5)
r(C≡N) 1.1641(17) 1.1724 1.160(5) [1.1645]
(HNH) /° 111.79(31) 111.93 113(2) 120.78(46)
(NCN) [180.0] 176.65 [180] [175]
Φ 43.05(70) 44.74 38(1) 45.03(20)
• The mmw and smm rotational spectra of 7 rare isotopic species of cyanamide have been assigned , up to Ka=7 and J”=34 (ca 200 lines for each species).
• Spectroscopic information on 15ND2CN, ND2C15N has been considerably improved.
• The spectra of NH213CN, NHD13CN, ND2
13CN, 15NHDCN, NHDC15N have been assigned for the first time.
• The structure of cyanamide has been derived.
• We hope that further progress in understanding of the cyanamide geometry will come from semi-experimental equilibrium structure .
Conclusions
Acknowledgments
We are indebted to Wolfgang Jabs (Giessen) who recorded all of the spectra used in this work.
We are grateful to Ewa Bialkowska-Jaworska (Warszawa) for help with ab initio calculations.