rotational constant of co

Rotational spectroscopy is concerned with the measurement of the energies of transitions between quantized rotational states of molecules in the gas phase.The spectra of polar molecules can be measured in absorption or emission by microwave spectroscopy or … The rotational constant of CO is 1.931 cm1. 0000005311 00000 n H�lTˎ� ��KGj/cX�Z�t3�.�͌=J�ȐV��^;`��-��9�Ю0C��@0��PT7hw�WW�@1�L��5m��cX)��O��9��c9��(Y ~g]RDa ��S�5��+��z3��. Rotational Constant Units Choose units cm-1 (wavenumbers, reciprocal centimeters) GHz (gigahertz, 10 9 sec-1) These units are related by the c, the speed of light. 0000019495 00000 n In this video will will use the rotational constant of HI to calculate its bond length. 0000001188 00000 n ��P+��]p��=��r��o�v In addition to having pure rotational spectra diatomic molecules have rotational spectra associated with their vibrational spectra. J values up to 48 for the 2-0 band and up to â¼35 for the 3-1 and 4-2 bands were measured. Rotational constant, B This applet allows you to simulate the spectra of H , D , HD, N , O and I . trailer << /Size 126 /Info 76 0 R /Root 85 0 R /Prev 975710 /ID[<0d6e6dd1b51458f8b19a1e276886f16e>] >> startxref 0 %%EOF 85 0 obj << /Type /Catalog /Pages 75 0 R /CAPT_Info << /L [ (English US)] /D [ [ ] [ (Default)()] ] >> /FICL:Enfocus 80 0 R /AcroForm 86 0 R /Metadata 83 0 R >> endobj 86 0 obj << /Fields [ ] /DR << /Font << /ZaDb 72 0 R /Helv 73 0 R >> /Encoding << /PDFDocEncoding 74 0 R >> >> /DA (/Helv 0 Tf 0 g ) >> endobj 124 0 obj << /S 384 /V 506 /Filter /FlateDecode /Length 125 0 R >> stream The relative atomic weight C =12.00 and O … Agreement NNX16AC86A, Is ADS down? T��k�SN��\�ۅ��@f�SҦ��T�]��DG�b�@��{�mXU�f N5f��/��7@�Å�A�%IQ V&��O �6�a.��Q�G��0�y��+ 8.�KR$Y The order of magnitude differs greatly between the two with the rotational transitions having energy proportional to 1-10 cm -1 (microwave radiation) and the vibrational transitions having energy proportional to 100-3,000 cm -1 (infrared radiation). 0000001364 00000 n %PDF-1.4 %�� Jones and Gordy (13) have reported measurements for CO up to the 5 --+ 6 rotational transition. 73A, No.2, Marc h-April 1969 A Table of Rotational Constants … The rotational constants are: B0 = 1.922 521, D0 = −6.1193 × 10 −6, H 0 = 5.8 × 10 −12, αe = −0.017507, βe = 1.0 × 10 −9, γe = 1.0 × 10 −6. The problem is simple: calculate CO2 rotational constant. The rotational constants are: B0 = 1.922 521, D0 = -6.1193 Ã 10 -6, H 0 = 5.8 Ã 10 -12, Î±e = -0.017507, Î²e = 1.0 Ã 10 -9, Î³e = 1.0 Ã 10 -6. 0000006785 00000 n CO Carbon Monoxide Rotational Parameters Isotopic Species B 0 [MHz] D 0 [kHz] H 0 [Hz] µ r [u] Ref. 0000012910 00000 n The spectrum of CO has been observed using a heated absorption tube. My goal with this project was to explore It is inversely proportional to the moment of inertia of the molecule. ��LC�B��2�R'�C��*k�5�22�1j3Lo�=�n t��cr�Łi ��,,�^2�008�.�7Pc``a�b`d�b�9 ��g�:(�j`p�_�`qf��,k��*��w��l!� �{� endstream endobj 125 0 obj 416 endobj 87 0 obj << /Type /Page /MediaBox [ 0 0 622.31946 799.67944 ] /Parent 78 0 R /CAPT_Info << /R [ 0 6664 0 5186 ] /S [ 0 3325 0 2584 ] /Rz [ 300 300 300 300 0 0 ] /SK (Accurate Rotational Constants of CO HCI_00001a)>> /Contents [ 95 0 R 101 0 R 105 0 R 109 0 R 111 0 R 117 0 R 119 0 R 121 0 R ] /Resources << /XObject << /Im3 123 0 R >> /Font << /F6 92 0 R /F14 103 0 R /F12 107 0 R /F20 88 0 R /F13 89 0 R /F16 115 0 R /F9 98 0 R /F17 97 0 R /F15 112 0 R >> /ProcSet [ /PDF /Text /ImageB ] >> /CropBox [ 56.88095 111.60342 533.94699 799.67944 ] /Rotate 0 >> endobj 88 0 obj << /Type /Font /Subtype /TrueType /BaseFont /ArialMT /FirstChar 0 /LastChar 255 /Encoding /WinAnsiEncoding /FontDescriptor 90 0 R /Widths [ 750 750 750 750 750 750 750 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667 389 389 389 389 722 722 778 778 778 778 778 570 778 722 722 722 722 722 611 556 500 500 500 500 500 500 722 444 444 444 444 444 278 278 278 278 500 556 500 500 500 500 500 549 500 556 556 556 556 500 556 500 ] >> endobj 90 0 obj << /Type /FontDescriptor /FontName /ArialMT /FontBBox [ -250 -250 1072 1000 ] /Flags 32 /CapHeight 724 /Ascent 905 /Descent 212 /StemV 80 /ItalicAngle 0 /XHeight 506 /Leading 33 /AvgWidth 441 /MaxWidth 1294 >> endobj 91 0 obj << /Type /FontDescriptor /FontName /TimesNewRomanPSMT /FontBBox [ -250 -250 1009 1000 ] /Flags 34 /CapHeight 712 /Ascent 891 /Descent 216 /StemV 73 /ItalicAngle 0 /XHeight 498 /Leading 42 /AvgWidth 401 /MaxWidth 1175 >> endobj 92 0 obj << /Type /Font /Subtype /TrueType /BaseFont /TimesNewRomanPSMT /FirstChar 0 /LastChar 255 /Encoding /WinAnsiEncoding /FontDescriptor 91 0 R /Widths [ 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 250 333 408 500 500 833 778 180 333 333 500 564 250 333 250 278 500 500 500 500 500 500 500 500 500 500 278 278 564 564 564 444 921 722 667 667 722 611 556 722 722 333 389 722 611 889 722 722 556 722 667 556 611 722 722 944 722 722 611 333 278 333 469 500 333 444 500 444 500 444 333 500 500 278 278 500 278 778 500 500 500 500 333 389 278 500 500 722 500 500 444 480 200 480 541 778 500 778 333 500 444 1000 500 500 333 1000 556 333 889 778 611 778 778 333 333 444 444 350 500 1000 333 980 389 333 722 778 444 722 250 333 500 500 500 500 200 500 333 760 276 500 564 333 760 500 400 549 300 300 333 576 453 250 333 300 310 500 750 750 750 444 722 722 722 722 722 722 889 667 611 611 611 611 333 333 333 333 722 722 722 722 722 722 722 564 722 722 722 722 722 722 556 500 444 444 444 444 444 444 667 444 444 444 444 444 278 278 278 278 500 500 500 500 500 500 500 549 500 500 500 500 500 500 500 500 ] >> endobj 93 0 obj << /Type /FontDescriptor /FontName /TimesNewRomanPS-BoldMT /FontBBox [ -250 -250 1089 1000 ] /Flags 34 /CapHeight 712 /Ascent 891 /Descent 216 /StemV 136 /ItalicAngle 0 /XHeight 498 /Leading 42 /AvgWidth 427 /MaxWidth 1273 >> endobj 94 0 obj 654 endobj 95 0 obj << /Filter /FlateDecode /Length 94 0 R >> stream The first rotational line in the rotational spectrum of CO is observed at 3.84235 cm-1. 0000021648 00000 n ҽh�Y6ՒT@+��'q�Z�*��5�>F�-�� BN-�JRE��(XM�d�.��;F0�C��-�!�"D��ߛ��x%R�Y-] �QP>��+��?�Ǘ�)ߞ&d|�R|+��/d�3}�j�� 99f��@cn)�?��\k)oq'9L��!Cn�� ;��z�@xhP� ��2��(B�V��)jM�@�t�� NQmC�d�ߖ�o��o7��5BZn��;m�l��i,��xR��h��jW��W��Ͼ��vi�>��p�0�8 In general the rotational constant B 1 of a vibrationally excited state is slightly smaller than the rotational constant of the ground vibrational state B 0, because the vibration causes a … By how much does the internuclear distance change as … The vibrational constants in vacuum wave numbers are: W e = 2169.8232, W e X e = -13.2932, W e Y e = 0.01144. ; B = rotational constant, units cm-1 4. 0000015889 00000 n 1979) was used to calculate the rotational energy levels. The constant B ′′ is used to determine the internuclear distance in the ground state as in pure rotational spectroscopy . B changes based on the molecule, and for CO I found the value of B to be as listed above. The vibrational constants in vacuum wave numbers are: W e = 2169.8232, W eX e = -13.2932, W eY e= 0.01144. H��ێ�0��w�e�X��c|IX�� 0000008043 00000 n The rotational constant of the ground vibrational state B′′ and centrifugal distortion constant, D′′ can be found by least-squares fitting this difference as a function of J. tg��#��r��J�"E��̛y�!B��`B ��`Ю��(�:�v�W� ֣��jx�4c �uMi�9�S� ��G��}�� _�2�nq��X3� ��[��8�dy��I,)� ��z��#"��1� �` ��Y� endstream endobj 110 0 obj 569 endobj 111 0 obj << /Filter /FlateDecode /Length 110 0 R >> stream We present the first accurate rate coefficients for the rotational excitation of CO by H2O in the kinetic temperature range 5–100 K. The statisticalis the Boltzmann population of level j 1 k a k c at temperature T and k B is the Boltzmann constant. The rotational constant determines the distance between the rotational lines. 0000020968 00000 n There is no implementation of any of the finer points at this stage; these include nuclear spin statistics, centrifugal distortion and anharmonicity. I ( l I t JOURNAL OF RESEARCH of the National Bureau of Standards - A. 0000011427 00000 n Use, Smithsonian Using previous measurements of the 2-0 band and the results of microwave determinations a set of rotation-vibration constants was deduced. @1��P!蒖Uj 0000010495 00000 n 0000019473 00000 n We can compare the �yR�'!�?�PLk찫�N��鷂ܧ&�ꙿ�ڷ�E��=��{6��l�{�]��e�}�v��_wP�'Ňl))�|�=㎅�F��>d�1��D�� 2� endstream endobj 96 0 obj << /Type /FontDescriptor /FontName /Arial-ItalicMT /FontBBox [ -250 -250 1082 1000 ] /Flags 96 /CapHeight 724 /Ascent 905 /Descent 212 /StemV 80 /ItalicAngle 0 /XHeight 506 /Leading 33 /AvgWidth 441 /MaxWidth 1343 >> endobj 97 0 obj << /Type /Font /Subtype /TrueType /BaseFont /Arial-ItalicMT /FirstChar 0 /LastChar 255 /Encoding /WinAnsiEncoding /FontDescriptor 96 0 R /Widths [ 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 278 278 355 556 556 889 667 191 333 333 389 584 278 333 278 278 556 556 556 556 556 556 556 556 556 556 278 278 584 584 584 556 1015 667 667 722 722 667 611 778 722 278 500 667 556 833 722 778 667 778 722 667 611 722 667 944 667 667 611 278 278 278 469 556 333 556 556 500 556 556 278 556 556 222 222 500 222 833 556 556 556 556 333 500 278 556 500 722 500 500 500 334 260 334 584 750 556 750 222 556 333 1000 556 556 333 1000 667 333 1000 750 611 750 750 222 222 333 333 350 556 1000 333 1000 500 333 944 750 500 667 278 333 556 556 556 556 260 556 333 737 370 556 584 333 737 552 400 549 333 333 333 576 537 278 333 333 365 556 834 834 834 611 667 667 667 667 667 667 1000 722 667 667 667 667 278 278 278 278 722 722 778 778 778 778 778 584 778 722 722 722 722 667 667 611 556 556 556 556 556 556 889 500 556 556 556 556 278 278 278 278 556 556 556 556 556 556 556 549 611 556 556 556 556 500 556 500 ] >> endobj 98 0 obj << /Type /Font /Subtype /TrueType /BaseFont /TimesNewRomanPS-ItalicMT /FirstChar 0 /LastChar 255 /Encoding /WinAnsiEncoding /FontDescriptor 99 0 R /Widths [ 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 250 333 420 500 500 833 778 214 333 333 500 675 250 333 250 278 500 500 500 500 500 500 500 500 500 500 333 333 675 675 675 500 920 611 611 667 722 611 611 722 722 333 444 667 556 833 667 722 611 722 611 500 556 722 611 833 611 556 556 389 278 389 422 500 333 500 500 444 500 444 278 500 500 278 278 444 278 722 500 500 500 500 389 389 278 500 444 667 444 444 389 400 275 400 541 778 500 778 333 500 556 889 500 500 333 1000 500 333 944 778 556 778 778 333 333 556 556 350 500 889 333 980 389 333 667 778 389 556 250 389 500 500 500 500 275 500 333 760 276 500 675 333 760 500 400 549 300 300 333 576 523 250 333 300 310 500 750 750 750 500 611 611 611 611 611 611 889 667 611 611 611 611 333 333 333 333 722 667 722 722 722 722 722 675 722 722 722 722 722 556 611 500 500 500 500 500 500 500 667 444 444 444 444 444 278 278 278 278 500 500 500 500 500 500 500 549 500 500 500 500 500 444 500 444 ] >> endobj 99 0 obj << /Type /FontDescriptor /FontName /TimesNewRomanPS-ItalicMT /FontBBox [ -250 -250 1120 1000 ] /Flags 98 /CapHeight 712 /Ascent 891 /Descent 216 /StemV 73 /ItalicAngle 0 /XHeight 498 /Leading 42 /AvgWidth 402 /MaxWidth 1309 >> endobj 100 0 obj 572 endobj 101 0 obj << /Filter /FlateDecode /Length 100 0 R >> stream (or is it just me...), Smithsonian Privacy C O X 2 is a linear symmetric molecule (D ∞ h point group) but nuclear spins on 12 C and 16 O are both zero and means that antisymmetric rotational lines are missing. The CO rotational constant of 1.9225 cm −1 (Lovas et al. 0000003837 00000 n The rotational energy disposal of CO(b3-SIGMA+) in the Ar(P2)-P-3+CO reaction has been measured by observing CO(b3-SIGMA+-a3-PI(r)) emission in an Ar flowing afterglow. Hey! 0000010775 00000 n Using c = 299, 792.7 km/sec (1/), the values corresponding to Bo and Do are 1.922527 and 6.1342 X 10-o cm-'. 0000007042 00000 n 0000002043 00000 n Selection rules: (1) permanent dipole moment, (2) ΔJ = ± 1 only 5. �b!�x�x��_��Lx�`$�UXrU��z��l��7u�1��io�Ck�|�A�Ŧ��pܓ ��b��p��Q�R�L��I�&�h% B0ߠ�x4��`ўbU��-� ��6��C��¼/� �`�g�^��ju�y{Aaݲb��ߛ� T��cMߝ�G�߇+��"X��N�DDq��Zg�I�䚬�J�M�\b�(��4��W��aFX�`� � �� s@4t�uqG�lԇV��36Ld��X�yQ�-'��}��b�l&��49K�Ҭ�f��]g/��)��V{��Dd�k*�̿� Astrophysical Observatory. 0000001511 00000 n 0000015139 00000 n Determining the rotational constant B enables you to calculate the bond length R. The allowed transitions for the diatomic molecule are regularly spaced at interval 2B. De ning the rotational constant as B= ~2 2 r2 1 hc = h 8ˇ2c r2, the rotational terms are simply F(J) = BJ(J+ 1): In a transition from a rotational level J00(lower level) to J0(higher level The ADS is operated by the Smithsonian Astrophysical Observatory under NASA Cooperative 0000017762 00000 n H��T�n�0��e ��$�Go�R7 �(��C��`�r�"�ZEm�~}�2��Q� H��,%��~��MW�˦��*�ꥪ��-�`�c�2�E?h�3Tj~�8�8j�c��Y%�8D�ۃ��*��[%�N(�t�# ��9��H3l��Y@I��S~��qu?_�$�Fr�"�:Y j��l��]��R�A �r��.�W�:�>��B��l�Y�.��]�b"��I"-2?��y��K~GB�%�+"i�r��Vk^?�MS�ū��U��LPI��:�6�c�zN(^�۠HZu�$*z��j��r��2=b��UOQE�3͖F��v�� A�bs��٥KP\01�x�x3��;%|�v��,��'sY?ȜdBj�YSj�M�}=`��S)f��:�U��S��|-��V��j\��$��ӛ��3��x:��V��/��:�! connection between atoms is a simple spring of constant k. The rotational energy levels then become (6) This is more usually written with two constants as (7) where the subscript e … 84 0 obj << /Linearized 1 /O 87 /H [ 1511 532 ] /L 977518 /E 94275 /N 14 /T 975720 >> endobj xref 84 42 0000000016 00000 n 0000018002 00000 n 0000016538 00000 n Calculated values for lines in the 5-3, 6-4, and 7-5 bands agree within experimental error with the results of measurement of lines in the solar spectrum. 3. Accurate Rotational Constants of CO, HCI, and HF: Spectral Standards for the 0.3- to 6-THz (10- to 200-cm-’) Region I. G. NOLT’ AND J. V. RADOSTITZ Department of Physics, University of Oregon, Eugene, Oregon 97403 40136 The rotational constant for CO is 1.9314 cm −1 and 1.6116 cm −1 in the ground and first excited vibrational states, respectively. Spacing between lines of in rotational spectra of rigid diatomic molecules is constant … 0000015161 00000 n RESULTS AND DISCUSSION 3.1. Rotational Constant and c is the speed of light and h is the Planck’s constant. 0000012932 00000 n H��Tے�@��a�J'sc.�^�hLY�]��%QH M��iX�!e�2ҧ��3��/0�?�K�E�L�1�;�,�%HP�5 0000010753 00000 n Due to this, larger and/or heavier molecules show rotational lines which are closer /��)a��#�@��d r�dv"쵱��oq޼^�^ٰ��k;h$J�Q�[��̉��.��H��ڵ5>Cދ�=��uOZ�-��$�� {��2@��]F])ݗ�~��&!�Z߯'C�I��y�o 2݅�ȥ��Z�{t��Y2O��[d/C�F�5�@�L��(� 0 �x6� endstream endobj 102 0 obj << /Type /FontDescriptor /FontName /Arial-BoldItalicMT /FontBBox [ -250 -250 1157 1000 ] /Flags 96 /CapHeight 724 /Ascent 905 /Descent 212 /StemV 153 /ItalicAngle 0 /XHeight 506 /Leading 33 /AvgWidth 479 /MaxWidth 1405 >> endobj 103 0 obj << /Type /Font /Subtype /TrueType /BaseFont /Arial-BoldItalicMT /FirstChar 0 /LastChar 255 /Encoding /WinAnsiEncoding /FontDescriptor 102 0 R /Widths [ 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 750 278 333 474 556 556 889 722 238 333 333 389 584 278 333 278 278 556 556 556 556 556 556 556 556 556 556 333 333 584 584 584 611 975 722 722 722 722 667 611 778 722 278 556 722 611 833 722 778 667 778 722 667 611 722 667 944 667 667 611 333 278 333 584 556 333 556 611 556 611 556 333 611 611 278 278 556 278 889 611 611 611 611 389 556 333 611 556 778 556 556 500 389 280 389 584 750 556 750 278 556 500 1000 556 556 333 1000 667 333 1000 750 611 750 750 278 278 500 500 350 556 1000 333 1000 556 333 944 750 500 667 278 333 556 556 556 556 280 556 333 737 370 556 584 333 737 552 400 549 333 333 333 576 556 278 333 333 365 556 834 834 834 611 722 722 722 722 722 722 1000 722 667 667 667 667 278 278 278 278 722 722 778 778 778 778 778 584 778 722 722 722 722 667 667 611 556 556 556 556 556 556 889 556 556 556 556 556 278 278 278 278 611 611 611 611 611 611 611 549 611 611 611 611 611 556 611 556 ] >> endobj 104 0 obj 626 endobj 105 0 obj << /Filter /FlateDecode /Length 104 0 R >> stream A fit of µ a, R-branch transitions of the nearly prolate asymmetric rotor H 2 CO⋯HCl (κ ≈–0.99) demonstrated that even a relatively large A 0 rotational constant can be determined with useful accuracy from such a limited set of data, provided the frequencies are of sufficient accuracy. ABSTRACT. 0000021672 00000 n 0000002021 00000 n hc is the rotational term and has the unit cm 1. 0000018250 00000 n H�b```��l��@(��р�O;��q^�O�O1lp��?gB�N�&�) 0000007795 00000 n H�lTKn�0=��D,��eP�( I know that for J=0,2,4.. it is just in ground state and for J=1,3,5..it is excited state. �M(�X�ۨ�st��9��3}?�5R�J��@��V�y�T�(��!U�%��:��}�[>��>��+,��M~M8�C�U��´��`;~��+ ��6qB@��Zo_�``��D��-p�eR�K�X;c�Aݺ�C�߱� jN�i�#��0~ɰ�]��׸�T+1ΐ� ��4��y��QC�U �g��[Ƴ,M��9�)�d�^�8fJ�{Reu#�+.��體��t�^��f{��w��/c0�57��?ƿ�ߏ��U��ǷF�{J�3��8?E�u`>�lSYMh��MCܖ l��/! ��:r$�O[s��ۡ]��PE�i��ٰ�'�K`�yc"�HYg��U� ��!W�6��l�� I have a problem. J = 0, 1, 2, …. 0000009267 00000 n 0000013902 00000 n 0000020200 00000 n 7�dd�Q�ʜ.m�qr�"k�3:�$�r|t_H]�%�yA ��C^˖\��*H��s�9:��}�j�.g��ŢpD$-*�Й@�6��*��8|��{ �=A%��P0��%�a%�4c��4� The rotational band structure for the antisymmetric vibration centred at ≈ 2349 c m − 1 (also called parallel v 3 band) has alternate lines missing, which are those having odd J. Physics and Chemistry Val. The rotational constant for CO is 1.9314 cm-1 and 1.6116 cm-1 in the ground and first excited vibrational states, respectively. 0000002620 00000 n The vibrational constants in vacuum wave numbers are: W e = 2169.8232, W e X e = -13.2932, W e Y e = 0.01144. Notice, Smithsonian Terms of The measurement and identification of one spectral line allows Calculate the rotational constant (B) and bond length of CO. The rotational constants are: B 0 = 1.922 521, D 0 = -6.1193 × 10 -6, H 0 = 5.8 × 10 -12, α e = -0.017507, β e = 1.0 × 10 -9, γ e = 1.0 × 10 -6. 0000013638 00000 n 0000011681 00000 n Molecular spectroscopists define the rotational constant B which has which as units of energy. - the rotational constant (B) is small For large molecules the rotational levels are closer than for small molecules. → From rotational spectra we can obtain some … 0000005562 00000 n See section I.F.4 to change rotational constant units A B C reference comment 0.39021 1966Herzberg Calculated rotational constants for CO 2 (Carbon dioxide). 0000007063 00000 n 0000020990 00000 n 0000005070 00000 n O/L�ew`@G��:�n�r�.�b�*��W�[�B��;Ӣ8�X̢ I have values for J (ground state and excited state), with those grades I have to calculate rotational constant. We will follow three steps in doing this calculation. The rotational-vibrational spectrum of gaseous CO is shown below: High Resolution FTIR Spectrum of CO Q1: 0.07 0.06 0.05 Relative intensity 0.04 0.03 0.02 0.01 0.00 2240 2220 2160 2140 2120 2100 2200 2180 Wavenumbers a) . NIST / TRC Web Thermo Tables, professional edition (thermophysical and thermochemical data) By how much does the intern clear distance change as a result of this transition? Evaluate the rotational partition function (without approximation) at temperature T=10 K by direct summation over the first 10 terms and compare the obtained value with partition function �6tS��i�xn�m��O� �v��t;�O�� )�㽊�\��))ߊ,M";� W�?� endstream endobj 106 0 obj << /Type /FontDescriptor /FontName /TimesNewRomanPS-BoldItalicMT /FontBBox [ -250 -250 1206 1000 ] /Flags 98 /CapHeight 712 /Ascent 891 /Descent 216 /StemV 131 /ItalicAngle 0 /XHeight 498 /Leading 42 /AvgWidth 412 /MaxWidth 1390 >> endobj 107 0 obj << /Type /Font /Subtype /TrueType /BaseFont /TimesNewRomanPS-BoldItalicMT /FirstChar 0 /LastChar 255 /Encoding /WinAnsiEncoding /FontDescriptor 106 0 R /Widths [ 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 778 250 389 555 500 500 833 778 278 333 333 500 570 250 333 250 278 500 500 500 500 500 500 500 500 500 500 333 333 570 570 570 500 832 667 667 667 722 667 667 722 778 389 500 667 611 889 722 722 611 722 667 556 611 722 667 889 667 611 611 333 278 333 570 500 333 500 500 444 500 444 333 500 556 278 278 500 278 778 556 500 500 500 389 389 278 556 444 667 500 444 389 348 220 348 570 778 500 778 333 500 500 1000 500 500 333 1000 556 333 944 778 611 778 778 333 333 500 500 350 500 1000 333 1000 389 333 722 778 389 611 250 389 500 500 500 500 220 500 333 747 266 500 606 333 747 500 400 549 300 300 333 576 500 250 333 300 300 500 750 750 750 500 667 667 667 667 667 667 944 667 667 667 667 667 389 389 389 389 722 722 722 722 722 722 722 570 722 722 722 722 722 611 611 500 500 500 500 500 500 500 722 444 444 444 444 444 278 278 278 278 500 556 500 500 500 500 500 549 500 556 556 556 556 444 500 444 ] >> endobj 108 0 obj 626 endobj 109 0 obj << /Filter /FlateDecode /Length 108 0 R >> stream The 5 -- + 6 rotational transition vibrational spectra we can obtain …... 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