crystal structure, vibrational spectroscopy and thermal properties...
TRANSCRIPT
Crystal structure, vibrational spectroscopy and thermal properties studies of
[Cd(NH3)6](ClO4)2 and [Cd(NH3)4](ReO4)2
Kamila Wojszko
Supervisor: dr Łukasz Hetmańczyk
PRESENTATION PLAN
NERA Spectrometer
Identification of compounds
DSC examinations
Experimental and calculation vibrational spectra
Infrared absorption spectra vs. temperature
Results of neutron experiment
• Neutron powder diffraction
• Inelastic neutron scattering
NERA
a multi-purpose indirect geometry spectrometer
Fig. 1 . The scheme of NERA spectrometer http://flnp.jinr.ru/img/133/233_pv_spectrometer_NERA.jpg
1 - sample 2 - Be-filters 3 - collimators 4 - He3 detectors (INS and QNS) 5 - PG analysers (INS) 6 - single crystal analysers (QNS) 7 - detectors for high intensity diffraction 8 - detectors for high resolution diffraction 9 - spectrometer shielding 10 - Ni-coated mirror neutron guide in a vacuum tube 11 - vacuum neutron guide
10 20 30 40 50 60 70 80
0
1000
2000
3000
4000
5000
6000[Cd(NH
3)
6] (ClO
4)
2
Inte
nsit
y
2
IDENTIFICATION OF COMPOUNDS
Crystal data Cubic, F-m3m a = 11.6049 Å V = 1562.875 Å3 Z = 4 T = 293 K
Crystal data Cubic, F-43m a = 10.68857 Å V = 1221.121 Å3 Z = 4 T = 295 K
10 20 30 40 50 60 70 80
0
500
1000
1500
2000
2500
3000[Cd(NH
3)
4] (ReO
4)
2
Inte
nsit
y
2
DSC EXAMINATIONS
150 200 250 300
-8
-4
0
4
8
Sample weight = 27.4000 mg
Cooling and heating rate = 10 K/min
[Cd(NH3)
4] (ReO
4)
2
Heat
Flo
w (
mW
)
Temperature (K)
120 150 180 210 240 270 300
-4
-2
0
2
4
[Cd(NH3)
6] (ClO
4)
2
Heat
Flo
w (
mW
)
Temperature (K)
Sample weight = 8.66 mg
Cooling and heating rate = 10 K/min
133 K
132 K
VIBRATIONAL SPECTRA
0 500 1000 1500 2000 2500 3000 3500 4000
[Cd(NH3)
4](ReO
4)
2
IR A
bso
rban
ce
Wavenumber (cm-1
)
ReO4
2- calculation
[Cd(NH3)
4]
2+ calculation
0 500 1000 1500 2000 2500 3000 3500 4000
[Cd(NH3)
6](ClO
4)
2
IR a
bso
rban
ce
[Cd(NH3)
6]
2+ calculation
ClO4
2- calculation
Wavenumber (cm-1
)
1664cm-1 δas.(HNH)
1676cm-1 δas.(HNH)
IR ABSORBANCE SPECTRA
500 1000 1500 3500 4000
0.0
0.5
1.0
1.5
2.0
2.5
290 K
Wavenumber (cm-1
)
20 K
80 K
110 K
135 K
170 K
200 K
230 K
[Cd(NH3)
6](ClO
4)
2
Tc
0 100 200 300 400 500
0.0
0.5
1.0
1.5
2.0
2.5
[Cd(NH3)
6](ClO
4)
2
290 K
20 K
80 K
110 K
135 K
170 K
200 K
IR a
bso
rban
ce
Wavenumber (cm-1
)
230 K
500 1000 1500 3500 4000
0
1
2
3
4
5
[Cd(NH3)
4](ReO
4)
2
Wavenumber (cm-1
)
290 K
20 K
80 K
110 K
140 K
170 K
200 K
230 K
0 100 200 300 400 5000.0
0.5
1.0
1.5
2.0
[Cd(NH3)
4](ReO
4)
2
IR a
bso
rban
ce
Wavenumber (cm-1
)
290 K
20 K
80 K
110 K
140 K
170 K
200 K
230 K
IR ABSORBANCE SPECTRA vs. TEMPERATURE
0 50 100 150 200 250 300
42
44
46
48
50
52
54
56
FW
HM
(cm
-1)
Temperature (K)
ModelNewFunction (User)
EquationP1+P2*x+P3*exp(-P4/(8.31*x))
Reduced Chi-Sqr
0.01483
Adj. R-Square 0.99921
Value Standard Error
FWHM
P1 42 0
P2 -0.00244 0.00115
P3 133.50507 6.13791
P4 5334.97718 152.27737
[Cd(NH3)6 ](ClO4)2
[Cd(NH3)4 ](ReO4)2
0 50 100 150 200 250 300
1605
1608
1611
1614
1617
1620
1623
1626
Po
siti
on
of
the
ban
d (
cm-1
)
Temperature (K)
0 50 100 150 200 250 300
1614
1616
1618
1620
1622
1624
1626
Po
siti
on
of
the
ban
d (
cm-1
)
Temperature (K)
50 100 150 200 250 300
23
24
25
26
27
28
29
30
FW
HM
(cm
-1)
Temperature (K)
NEUTRON POWDER DIFFRACTION
3 4 5 6 7 8
4000
8000
12000
16000
20000
24000
Reflex position
293 K
155 K
125 K
25 K
[Cd(NH3)
6] (ClO
4)
2
Inte
nsi
ty
dhkl
(Å)
Tc
3 4 5 6 7 8
0
4000
8000
12000
16000
20000
Reflex position
293 K
150 K
50 K
[Cd(NH3)
4] (ReO
4)
2
Inte
nsi
ty
dhkl
(Å)
INELASTIC NEUTRON SCATTERING
1 2 3 4 5 6
0
50
100
150
200
250
300
350
400[Cd(NH
3)
4] (ReO
4)
2
50 K
150 K
293 KII
NS
Int
ensi
ty (
a.u)
Incoming neutron wavelength (Å)
1 2 3 4 5 6
0
500
1000
1500
2000[Cd(NH
3)
6] (ClO
4)
2
155 K
125 K
25 K
IIN
S I
nte
nsi
ty (
a.u
)
Incoming neutron wavelength (Å)
Tc
750 600 450 300 150 0
0
15
30
45
60
75 [Cd(NH3)
4](ReO
4)
2
[Cd(NH3)
4]
2+ calculation
G (
)
Wavenumber (cm-1
)
750 600 450 300 150 0
0
1000
2000
3000
4000
5000
[Cd(NH3)
6](ClO
4)
2
[Cd(NH3)
6]
2+ calculation
G (
)
Wavenumber (cm-1
)
References
[1] I. Natkaniec, S.I. Bragin, J. Brańkowski, J. Mayer, in: U. Steigenberger, T. Brome, G. Rees, A. Soper, (Eds); Proceedings of the ICANS XII Meeting, Abingdon 1993, RAL Report 94-025, Vol. I, (1994) 89-96. [2] M.J. Frisch, G.W. Trucks, H.B. Schlegel, G.E. Scuseria, M.A. Robb, J.R. Cheeseman, J.A. Montgomery, Jr., T. Vreven, K.N. Kudin, J.C. Burant, J.M. Millam, S.S. Iyengar, J. Tomasi, V. Barone, B. Mennucci, M. Cossi, G. Scalmani, N. Rega, G.A. Petersson, H. Nakatsuji, M. Hada, M. Ehara, K. Toyota, R. Fukuda, J. Hasegawa, M. Ishida, T. Nakajima, Y. Honda, O. Kitao, H. Nakai, M. Klene, X. Li, J.E. Knox, H.P. Hratchian, J.B. Cross, V. Bakken, C. Adamo, J. Jaramillo, R. Gomperts, R.E. Stratmann, O. Yazyev, A.J. Austin, R. Cammi, C. Pomelli, J.W. Ochterski, P.Y. Ayala, K. Morokuma, G.A. Voth, P. Salvador, J.J. Dannenberg, V.G. Zakrzewski, S. Dapprich, A.D. Daniels, M.C. Strain, O. Farkas, D.K. Malick, A.D. Rabuck, K. Raghavachari, J.B. Foresman, J. V. Ortiz, Q. Cui, A.G. Baboul, S. Clifford, J. Cioslowski, B.B. Stefanov, G. Liu, A. Liashenko, P. Piskorz, I. Komaromi, R.L. Martin, D.J. Fox, T. Keith, M.A. Al-Laham, C.Y. Peng, A. Nanayakkara, M. Challacombe, P.M.W. Gill, B. Johnson, W. Chen, M.W. Wong, C. Gonzalez, and J.A. Pople, Gaussian 03, Revision D.01, Gaussian, Inc., Wallingford CT, 2004. [3] A.D.Becke, J.Chem.Phys. 98(1993)5648–5652. [4] P.J.Stephens, F.J.Devlin, C.F.Chabalowski, M.J.Frisch, J.Phys.Chem. 98 (1994) 11623–11627. [5] L.E. Roy, P.J. Hay, R.L. Martin, Revised basis sets for the LANL effective core potentials, J. Chem. Theory Comput. 4 (2008) 1029–1031. [6] K.T. Schuchardt, B.T. Didier, T. Elsethagen, L. Sun, V. Gurumoorthi, J. Chase, J. Li, T.L. Windus, Basis Set Exchange: A Community Database for Computational Sciences, J. Chem. Inf. Model. 47 (2007) 1045–1052. [7] Y. Tantirungrotechai, K. Phanasant, S. Roddecha,P. Surawatanawong, V. Sutthikhum, J. Limtrakul, J. Mol. Struct. (Theochem) 760 (2006) 189. [8] S.W. Lovesey, Theory of Neutron Scattering from Condensed Matter, Clarendon Press, Oxford, 1984. [9] A.J. Ramirez-Cuesta (2004). Comput. Phys. Comm. 157, 226–238. ACLIMAX 4.0.1, The new version of the software for analyzing and interpreting INS spectra. [10] W.J. Kazimirov, I. Natkaniec, Programme for Calculation of the Resolution Function of NERA-PR and KDSOG-M Inelastic Neutron Scattering Inverse Geometry spectrometers, Preprint P14-2003-48 JINR, Dubna, 2003. [11] C. Carabatos-Nédelec, P. Becker, J. Raman Spectrosc. 28 (1997) 663. [12] P. da R. Andrade, A.D. PasadRao, R.S. Katiyar, S.P.S. Porto, Solid St. Commun. 12 (1973) 847. [13] P da R. Andrade, S.P.S. Porto, Solid St. Commun. 13 (1973) 1249. [14] http://nuvis.jankrawczyk.pl/ [15] S. Hodorowicz, M. Ciechanowicz-Rutkowska, J. M. Janik, J. A. Janik, Phys. Stat.Sol. (a), 43 (1977) 53-57 [16] K. S. Pitzer, Zeitschrift fuer Kristallographie, Kristallgeometrie, Kristallphysik, Kristallchemie, 92 (1935) 131-135.
THANK YOU FOR YOUR ATTENTION
The infrared research was carried out with the equipment purchased thanks to the financial support of the European Regional Development Fund in the framework of the Polish Innovation Economy Operational Program (contract no. POIG.02.01.00-12-023/08).
Acknowledgments for
dr Łukasz Hetmańczyk
PL-Grid Infrastucture
ATOMIN Project