



Z.Kisiel, L.Pszczolkowski,
"The millimeterwave rotational spectrum of chloroacetonitrile",
J.Mol.Spectrosc. 158, 318327 (1993) 





ASF

RES



H_{2}^{35}ClCCN
ground
state,
Sreduction

ASF 
RES 


H_{2}^{37}ClCCN
ground
state,
Sreduction 









Z.Kisiel and L.Pszczolkowski,
"The millimeterwave rotational spectrum of 2chloroacrylonitrile",
J.Mol.Spectrosc. 166, 3240 (1994) 





ASF

RES



H_{2}ClCC^{35}ClCN
ground
state, as in Tables I and III

ASF

RES



H_{2}ClCC^{37}ClCN
ground
state, as in Tables II and III

ASF

RES



H_{2}ClCC^{35}ClCN
v_{10}=1, as in Table IV

ASF

RES



H_{2}ClCC^{35}ClCN
v_{11}=1 
ASF

RES



H_{2}ClCC^{35}ClCN
v_{11}=2 
ASF

RES



H_{2}ClCC^{35}ClCN
v_{15}=1 









Z.Kisiel and L.Pszczolkowski,
"Nuclear quadrupole coupling
in 2chloroacrylonitrile: inertial and principal quadrupole tensor
components for Cl and N",
J.Mol.Spectrosc. 184, 215220
(1997) 





PAR

LIN

RES


H_{2}ClCC^{35}ClCN
ground
state
hyperfine
structure, Fit II, Table 2. Note the perturbation enhanced precision in χ_{ab} for the nitrogen nucleus.

PAR

LIN

RES


H_{2}ClCC^{37}ClCN
ground
state
hyperfine
structure, Fit II, Table 2










Z.Kisiel, L.Pszczolkowski, G.Cazzoli,
and G.Cotti,
"The millimeterwave rotational spectrum and Coriolis
interaction in the two lowest excited vibrational states of CHClF_{2}",
J.Mol.Spectrosc. 173, 477487 (1995) 





PAR 
LIN

RES


CHF_{2}^{35}Cl
(v_{6}=1,v_{9}=1) Coriolis coupled pair in a two state
declaration containing only the MMW data



Notes:


A fit with
added FTIR data was published in I.Merke et al., J.Mol.Spectrosc.
173,
463476 (1995), but there were some misprints, which were corrected in
J.Mol.Spectrosc. 184, 150155 (1997) 









G.Klatt, G.Graner, S.Klee, G.Mellau,
Z.Kisiel, L.Pszczolkowski, J.L.Alonso, and J.C.Lopez,
"Analysis of the
highresolution FTIR and millimeterwave spectra of the v_{5}=1
state
of
CHF_{2}Cl",
J.Mol.Spectrosc. 178,
108112 (1996) 





PAR 
LIN

RES


CHF_{2}^{35}Cl
v_{5}=1 in a two state declaration
with the (fixed) ground state, using MMW and FTIR data.



Notes:


These files
may not be the final data as published but are fairly close to that
data set. 









Z.Kisiel, J.L.Alonso, S.Blanco,
G.Cazzoli, J.M.Colmont, G.Cotti, G.Graner, J.C.Lopez, I.Merke, and
L.Pszczolkowski,
"Spectroscopic constants for HCFC22 from rotational
and highresolution vibration spectra: CHF_{2}^{37}Cl
and ^{13}CHF_{2}^{35}Cl isotopomers",
J.Mol.Spectrosc. 184, 150155 (1997) 





ASF 
RES 


CHF_{2}^{37}Cl
ground
state

ASF 
RES 


^{13}CHF_{2}^{35}Cl
ground
state

PAR 
LIN 
RES 

CHF_{2}^{37}Cl
(v_{6}=1,v_{9}=1) Coriolis coupled pair in a three
state declaration
inclusive of the (fixed) ground state



Notes: 

Data set combining MMW and
FTIR measurements










Z.Kisiel and L.Pszczolkowski,
"The
highfrequency rotational spectrum of 1,1dichloroethylene",
Z.Naturforsch. 50A, 347351 (1995) 





ASF 
RES 


H_{2}CC^{35}Cl_{2} ground state 
ASF 
RES 


H_{2}CC^{37}Cl^{35}Cl ground state 









Z.Kisiel and L.Pszczolkowski,
"Assignment and analysis of the mmwave rotational spectrum of
trichloroethylene: observation of a new, extended b.Rband and
an overview of highJ, Rtype bands",
J.Mol.Spectrosc. 177, 125137 (1996) 





ASF 
RES 


ground state of the parent
isotopic species ^{35}Cl_{2}C=C^{35}ClH

ASF 
RES 


ground state of 1^{37}Cl^{c}trichloroethylene (c is relative to H)

ASF 
RES 


ground state of 1^{37}Cl^{t}trichloroethylene (t is relative to H) 
ASF 
RES 


ground state of 2^{37}Cltrichloroethylene 




ground state of 1^{37}Cl^{c},1^{37}Cl^{t}trichloroethylene 




ground state of 1^{37}Cl^{c},2^{37}Cltrichloroethylene 




ground state of 1^{37}Cl^{t},2^{37}Cltrichloroethylene 




v_{12}=1
of
the
parent
isotopic
species 




v_{8}=1
of
the
parent
isotopic
species 




v_{9}=1
of
the
parent
isotopic
species 




v_{9}=2
of
the
parent
isotopic
species 









Z.Kisiel, E.BialkowskaJaworska, and
L.Pszczolkowski,
"Nuclear quadrupole coupling in Cl_{2}C=CHCl
and Cl_{2}C=CH_{2}; "Evidence for systematic
differences in orientation between internuclear and field gradient axes
for terminal quadrupolar nuclei",
J.Chem.Phys. 109,
1026310272 (1998) 





PAR 
LIN 
RES 

Cl_{2}C=CHCl:
triple
^{35}Cl hyperfine coupling 
PAR 
LIN 
RES 

Cl_{2}C=CH_{2}: double ^{35}Cl hyperfine coupling 









Z.Kisiel, L.Pszczolkowski, W.Caminati,
and P.G.Favero,
"First assignment of the rotational spectrum of a
molecule containing two iodine nuclei: spectroscopic constants and
structure of CH_{2}I_{2}",
J.Chem.Phys. 105,
17781785
(1996) 





ASF 
RES 


CH_{2}I_{2}
ground state, fit to hyperfinefree transitions

PAR 
LIN

RES


CH_{2}I_{2}
ground state, fit to hyperfine components










Z.Kisiel, L.Pszczolkowski, L.B.Favero,
and W.Caminati,
"Rotational spectrum of CD_{2}I_{2} An isotopomer of the first molecule containing two
iodine nuclei investigated by microwave spectroscopy",
J.Mol.Spectrosc. 189, 283290 (1998) 





ASF 
RES 


CD_{2}I_{2}
ground state, fit to hyperfinefree transitions 
PAR

LIN

RES


CD_{2}I_{2}
ground state, fit to hyperfine components 









Z.Kisiel, E.BialkowskaJaworska,
L.Pszczolkowski,
"The <ICI bending satellites in the millimeterwave
rotational spectra of CH_{2}I_{2} and CD_{2}I_{2}",
J.Mol.Spectrosc. 199, 512 (2000) 





ASF

RES



CH_{2}I_{2}
ground state, Sreduction, as in Table 3 
ASF

RES



CH_{2}I_{2}
v_{4}=1 




CH_{2}I_{2}
v_{4}=2 




CH_{2}I_{2}
v_{4}=3 




CH_{2}I_{2}
v_{4}=4 
ASF

RES



CD_{2}I_{2}
ground state, Sreduction, as in Table 4

ASF

RES



CD_{2}I_{2}
v_{4}=1 




CD_{2}I_{2}
v_{4}=2 




CD_{2}I_{2}
v_{4}=3 




CD_{2}I_{2}
v_{4}=4 









Z.Kisiel, E.BialkowskaJaworska,
L.Pszczolkowski,
"The mmwave rotational spectrum of CBrClF_{2} (halon BCF): observation of a new Rtype band and
generalization of conditions for oblatetype band formation",
J.Mol.Spectrosc. 177, 240250 (1996) 





ASF

RES



C^{79}Br^{35}ClF_{2} ground state, Sreduction

ASF 
RES 


C^{81}Br^{35}ClF_{2} ground state, Sreduction 
ASF 
RES 


C^{79}Br^{37}ClF_{2} ground state, Sreduction 
ASF 
RES 


C^{81}Br^{37}ClF_{2} ground state, Sreduction 









Z.Kisiel, E.BialkowskaJaworska,
L.Pszczolkowski,
"The rotational spectrum of CBrClF_{2} (halon BCF); II. The lowest excited vibrational states and
nuclear quadrupole coupling tensors",
J.Mol.Spectrosc. 185, 7178 (1997) 





PAR 
LIN 
RES 

C^{79}Br^{35}ClF_{2}, (v_{9}=1,v_{5}=1)
Coriolis
coupling,
Sreduction

PAR 
LIN 
RES 

C^{81}Br^{35}ClF_{2}, (v_{9}=1,v_{5}=1)
Coriolis
coupling,
Sreduction 
PAR

LIN

RES


C^{79}Br^{35}ClF_{2}
ground state, ^{79}Br+^{35}Cl
hyperfine coupling

PAR 
LIN 
RES 

C^{81}Br^{35}ClF_{2}
ground state, ^{81}Br+^{35}Cl
hyperfine coupling 









Z.Kisiel, J.Kosarzewski, and L.Pszczolkowski,
"Nuclear
quadrupole coupling tensor of CH_{2}Cl_{2}: Comparison
of quadrupolar and structural angles in methylene halides",
Acta
Physica Polonica A. 92, 507516 (1997)






PAR

LIN

RES


CH_{2}^{35}Cl_{2}
ground state hyperfine structure in supersonic expansion










Z.Kisiel and L.Pszczolkowski,
"Millimeter wave rotational spectra of the ^{37}Cl species of
1,1,1trichloroethane",
J.Mol.Spectrosc. 181, 4855
(1997) 





ASF

RES



^{35}Cl_{2}^{37}ClCCH_{3}
ground state III.r: ASFIT could fit the more conventional III.l
so that this fit differs in the signs of the offdiagonal
centrifugal distortion constants. Current ASFIT also catches some line
duplications missed in the original data set.

PAR 
LIN 
RES 

^{35}Cl_{2}^{37}ClCCH_{3}
ground state III.l: reproduced with SPFIT after automatic conversion from ASFIT data and proper treatment of blends.

ASF

RES



^{35}Cl^{37}Cl_{2}CCH_{3}
ground state, III.r

PAR 
LIN 
RES 

^{35}Cl^{37}Cl_{2}CCH_{3}
ground state, III.l 
SYM 
RES 


^{37}Cl_{3}CCH_{3}
ground state: the data and results files for this symmetric top species are for the SYMF program










L.Dore and Z.Kisiel,
"Nuclear
quadrupole coupling in 1,1,1Trichloroethane: Inertial and principal
tensors for ^{35}Cl and ^{37}Cl",
J.Mol.Spectrosc. 189, 228234 (1998) 





PAR

LIN

RES


^{35}Cl_{3}CCH_{3}
ground state hyperfine structure 
PAR

LIN

RES


^{35}Cl_{2}^{37}ClCCH_{3}
ground state hyperfine structure










Z.Kisiel, L.Pszczolkowski, G.Cazzoli, L.Dore,
"Strong Coriolis coupling between v_{5} and v_{14} states of CH_{3}CCl_{3} studied by millimeterwave spectroscopy",
J.Mol.Spectrosc. 251, 235240 (2008) 





PAR 
LIN 
RES 

Coupling between the lowest Esymmetry and Asymmetry vibrational states in an oblate molecule using a threestate declaration










Z.Kisiel, L.Pszczolkowski, P.W.Fowler, A.C.Legon,
"Rotational spectrum of N_{2}...H^{35}Cl and N_{2}...H^{37}Cl:
electric
field gradients at the nitrogen nuclei",
Chem.Phys.Lett. 276, 202299 (1997) 





PAR 
LIN 
RES 

^{14}N_{2}...H^{35}Cl:
hyperfine
structure from three quadrupolar nuclei

CAT 




PAR 
LIN 
RES 

^{14}N_{2}...H^{37}Cl

CAT 













Z.Kisiel, L.Pszczolkowski, J.C.Lopez,
J.L.Alonso, A.Maris, and W.Caminati,
"Investigation of the rotational
spectrum of pyrimidine from 3 to 337 GHz: Molecular structure, nuclear
quadrupole coupling, and vibrational satellites",
J.Mol.Spectrosc., 195,332339(1999). 





PAR

LIN 
RES 

Ground state double
nitrogen hyperfine
structure

PAR 
LIN 
RES 

Ground state, A,I.r fit using SPFIT

ASF

RES



Ground state, A,I.r fit using ASFIT.
The two fits above allow various intercomparisons on how a given problem
is declared in these two schemes. Also note the presence of the various
subtleties concerning the listed deviations, as discussed in the cribsheet.

PAR 
LIN 
RES 

Ground state, S,III.l fit 
ASF

RES



Satellite A, S,IIIr (note that this is NOT
III.l so that it differs in
the sign of d_{1})

ASF 
RES 


Satellite B, S,IIIr 
ASF 
RES 


Satellite C, S,IIIr 
PAR 
LIN 
RES 

13C(2) species, ground state, S, III.l 
PAR 
LIN 
RES 

13C(4) species, ground state, S, III.l

PAR 
LIN 
RES 

13C(5) species, ground state, S, III.l

PAR 
LIN 
RES 

15N species, ground state, S, III.l










Z.Kisiel, E.BialkowskaJaworska, L.Pszczolkowski, A.Milet, C.Struniewicz, R.Moszynski, J.Sadlej,
"Structure and properties of the weakly bound cluster (H_{2}O)_{2}HCl observed by rotational spectroscopy",
J.Chem.Phys., 112,57675776(2000). 





PAR 
LIN 
RES 

The W state (ground state) for the parent species

PAR 
LIN 
RES 

The S state for the parent species 
PAR 
LIN 
RES 

The W state (ground state) for the ^{37}Cl species 
PAR 
LIN 
RES 

The S state for the ^{37}Cl species 









Z.Kisiel, E.BialkowskaJaworska, L.Pszczolkowski, H.Mader,
"Ground state rotational spectrum of toluene",
J.Mol.Spectrosc., 227,109113(2004). 





ASF 
RES 


Data and results files for Fit II in Table 1










V.V.Ilyushin, Z.Kisiel, L.Pszczolkowski, H.Mader, J.T.Hougen,
"A new torsion–rotation fitting program for molecules with a sixfold barrier: Application to the microwave spectrum of toluene",
J.Mol.Spectrosc., 259,2638(2010). 





INP 
OUT 
RES 

The input, the original and the reformatted output files for the RAM36 program.










V.V.Ilyushin, E.A. Alekseev, Z.Kisiel, L.Pszczolkowski,
"HighJ rotational spectrum of toluene in m <= 3 torsional states",
J.Mol.Spectrosc., xxx, xxxx (2017). 





INP 
OUT 
RES 

The input file for the RAM36 program, the original output file and the output file reformatted with VIFORM. 









Z.Kisiel, L.Pszczolkowski, E.BialkowskaJaworska, S.B.Charnley,
"The millimeter wave rotational spectrum of pyruvic acid",
J.Mol.Spectrosc., 241,220229(2007). 





PAR 
LIN 
RES 

Data and results files for the ground state Asubstate fit using SPFIT

PAR 
LIN 
RES 

Data and results files for the ground state Esubstate fit using SPFIT 
XI 
XO 


Data and results files for joint fit of ground state A and Esubstate lines with XIAM

IN 
RES 


Data and reformatted results files for joint fit of ground state A and Esubstate lines with ERHAM 
PAR 
LIN 
RES 

Data and results files for the SPFIT fit of the Asubstate of the v24=1 state

PAR 
LIN 
RES 

Data and results files for the SPFIT fit of the Esubstate of the v24=1 state 
IN 
RES 


Data and results files for the ERHAM fit of the A and Esubstates of the v24=1 state 
PAR 
LIN 
RES 

Data and results files for the SPFIT fit of the Asubstate of the v23=1 state 
PAR 
LIN 
RES 

Data and results files for the SPFIT fit of the Esubstate of the v23=1 state 
IN 
RES 


Data and results files for the ERHAM fit of the A and Esubstates of the v23=1 state 
IN 
RES 


Data and results files for the ERHAM fit of the A and Esubstates of the v24=2 state 
PAR 
LIN 
RES 

Data and results files for the SPFIT fit of the v24=3 state 









Z.Kisiel, O.Dorosh, M.Winnewisser, M.Behnke, I.R.Medvedev,
F.C.De Lucia,
"Comprehensive analysis of the FASSST rotational spectrum of S(CN)_{2}",
J.Mol.Spectrosc., 246,3956(2007) 





ZIP




The paper is associated
with twelve supplementary tables, but for some reason only the first of
these tables made it into the J.Mol.Spectrosc. archive and the OSU
Supplementary archives. All of the intended tables are contained
in this ZIP archive.

ASF 
RES 


S(CN)_{2}:
ground
state 
ASF 
RES 


S(CN)_{2}:
v_{4}=1 
ASF 
RES 


S(CN)_{2}:
v_{4}=2 
PAR 
LIN 
RES 

S(CN)_{2}:
triad of interacting states (v_{8}=1),
(v_{9}=1), (v_{4}=3) 
PAR 
LIN 
RES 

S(CN)_{2}:
tetrad of interacting states (v_{8}=1,v_{4}=1), (v_{9}=1,v_{4}=1), (v_{4}=4), (v_{3}=1) 
ASF 
RES 


S(CN)_{2}:
v_{4}=5 
ASF 
RES 


S(CN)_{2}:
v_{7}=1 
ASF 
RES 


S(CN)_{2}:
(v_{7}=1, v_{4}=1) 
ASF 
RES 


^{34}S(CN)_{2}:
ground
state 
ASF 
RES 


S(^{13}CN)(CN):
ground
state 
ASF 
RES 


S(C^{15}N)(CN): ground state 









Z.Kisiel, M.Winewisser, B.P.Winnewisser, F.C.De Lucia, D.W.Tokaryk, B.E.Billinghurst,
"FarInfrared Spectrum of S(CN)_{2} Measured with Synchrotron Radiation: Global Analysis of the Available HighResolution Spectroscopic Data",
J.Phys.Chem. A, 117,1381513824(2013) 





PAR 
LIN 
RES 

Global fit of FASSST purerotation and synchrotron vibrationrotation data for 13 vibrational states










Z.Kisiel, L.Pszczolkowski, B.J.Drouin, C.S.Brauer, S.Yu, J.C.Pearson,
"The rotational spectrum of acrylonitrile up to 1.67 THz",
J.Mol.Spectrosc. 258, 2634 (2009) 





PAR 
LIN 
RES 

H_{2}CCHCN: effective single state Sreduction fit for the ground state (the .PAR file also contains the Areduction constants)

PAR

LIN

RES


H_{2}CCHCN: effective single state Sreduction fit for the v_{11}=1 state (the .PAR file also contains the Areduction constants)

PAR

LIN

RES


H_{2}CCHCN: coupled Areduction fit for the (ground)↔(v_{11}=1) state (the .PAR file also contains the Sreduction constants)

PAR

LIN

RES


H_{2}^{13}CCHCN: Sreduction fit for the ground state

PAR 
LIN 
RES 

H_{2}C^{13}CHCN: Sreduction fit for the ground state

PAR 
LIN 
RES 

H_{2}CCH^{13}CN: Sreduction fit for the ground state 
PAR 
LIN 
RES 

H_{2}CCHC^{15}N: Sreduction fit for the ground state 









A.Krasnicki, Z.Kisiel, B.J.Drouin, J.C.Pearson,
"Terahertz spectroscopy of isotopic acrylonitrile",
J.Mol.Struct. 1006, 2027 (2011) 





PAR 
LIN 
RES 

H_{2}^{13}CCHCN: coupled fit for the (ground state)↔(v_{11}=1) dyad of states 
PAR 
LIN 
RES 

H_{2}CCH^{13}CN: coupled fit for the (ground state)↔(v_{11}=1) dyad of states 
PAR 
LIN 
RES 

H_{2}CCHC^{15}N: coupled fit for the (ground state)↔(v_{11}=1) dyad of states 
PAR 
LIN 
RES 

H_{2}CCDCN: coupled fit for the (ground state)↔(v_{11}=1) dyad of states 
PAR 
LIN 
RES 

H_{2}^{13}C^{13}CHCN ground state

PAR 
LIN 
RES 

H_{2}^{13}CCH^{13}CN ground state 
PAR 
LIN 
RES 

H_{2}C^{13}CH^{13}CN ground state 
PAR 
LIN 
RES 

H_{2}^{13}CCHC^{15}N ground state 
PAR 
LIN 
RES 

H_{2}C^{13}CHC^{15}N ground state 
PAR 
LIN 
RES 

H_{2}CCH^{13}C^{15}N ground state 









Z.Kisiel, L.Pszczolkowski, B.J.Drouin, C.S.Brauer, S.Yu, J.C.Pearson, I.R.Medvedev, S.Fortman, C.Neese,
"Broadband rotational spectroscopy of acrylonitrile: Vibrational energies from perturbations",
J.Mol.Spectrosc. 280, 134144 (2012) 





PAR 
LIN 
RES 

H_{2}CCHCN: coupled fit of the (ground state)↔(v_{11}=1)↔(v_{15}=1)↔(v_{11}=2) tetrad of states










A.Lopez, B.Tercero, Z.Kisiel, A.M.
Daly, C. Bermudez, H. Calcutt, N. Marcelino, S. Viti, B.J. Drouin, I.R.
Medvedev, C. F. Neese, L. Pszczołkowski, J. L. Alonso, J. Cernicharo,
"Laboratory characterization and astrophysical detection of
vibrationally excited states of vinyl cyanide in OrionKL",
Astronomy & Astrophysics 572, A44 (2014)






PAR 
LIN 
RES 

H_{2}CCHCN: coupled fit for the (v_{10}=1)↔(v_{11}=1,v_{15}=1) dyad of states

PAR 
LIN 
RES 

coupled fit for the (v_{15}=2)↔(v_{14}=1)↔(v_{11}=3) triad of states

PAR 
LIN 
RES 

coupled fit for the (v_{10}=1,v_{11}=1)↔(v_{11}=2,v_{15}=1) dyad of states

PAR 
LIN 
RES 

single state effective fit for the v_{9}=1 state

PAR 
LIN 
RES 

single state effective fit for the v_{11}=4 state










A.Krasnicki, Z.Kisiel, W.Jabs, B.P.Winnewisser, M.Winnewisser,
"Analysis of the mm and submmwave rotational spectra of isotopic cyanamide: New isotopologues and molecular geometry",
J.Mol.Spectrosc. 267, 144149 (2011) 





PAR 
LIN 
RES 

D_{2}N^{13}CN: coupled fit of 0^{+} and 0^{} transitions

PAR 
LIN 
RES 

D_{2}^{15}NCN: coupled fit of 0^{+} and 0^{} transitions 
PAR 
LIN 
RES 

D_{2}NC^{15}N: coupled fit of 0^{+} and 0^{} transitions 
PAR 
LIN 
RES 

HDN^{13}CN: coupled fit of 0^{+} and 0^{} transitions 
PAR 
LIN 
RES 

HD^{15}NCN: coupled fit of 0^{+} and 0^{} transitions 
PAR 
LIN 
RES 

HDNC^{15}N: coupled fit of 0^{+} and 0^{} transitions 
PAR 
LIN 
RES 

H_{2}N^{13}CN: coupled fit of 0^{+} and 0^{} transitions 
PAR 
LIN 
RES 

H_{2}^{15}NCN: coupled fit of 0^{+} and 0^{} transitions 
PAR 
LIN 
RES 

H_{2}NC^{15}N: coupled fit of 0^{+} and 0^{} transitions 
PAR 
LIN 
RES 

H_{2}^{15}NC^{15}N: coupled fit of 0^{+} and 0^{} transitions 

STF 
RES 

The data and results for determination of the r_{e}^{SE} geometry of cyanamide with the STRFIT program










Z.Kisiel, A.Krasnicki, W.Jabs, E.Herbst, B.P.Winnewisser, M.Winnewisser,
"Rotation and RotationVibration Spectroscopy of the 0^{+}0^{} Inversion Doublet in Deuterated Cyanamide",
J.Phys.Chem. A. 117, 98899898 (2013)






PAR 
LIN 
RES 

D_{2}NCN: Fit to microwave and infrared data truncated at K_{a}=15 
CAT 
INT

INP


D_{2}NCN: Room temperature linelist limited to J=80 and K_{a}=15 and the files necessary for its generation (before use rename the batch input file for the filtering program CATFIL to just catfil.inp)






PAR 
LIN 
RES 

HDNCN: Fit to microwave and infrared data truncated at K_{a}=10 
CAT 
INT

INP


HDNCN: Room temperature linelist limited to J=50 and K_{a}=10 and the files necessary for its generation (before use rename the batch input file for the filtering program CATFIL to just catfil.inp) 





PAR 
LIN 
RES 

H_{2}NCN: Fit to microwave and infrared data truncated at K_{a}=6

CAT 
INT

INP


H_{2}NCN: Room temperature linelist limited to J=70 and K_{a}=6 and the files necessary for its generation (before use rename the batch input file for the filtering program CATFIL to just catfil.inp) 









Z.Kisiel, J. Kosarzewski,
"Identification of Trace 2Chloropropene with a New Chirped Pulse Microwave Spectrometer",
Acta.Physica Polonica A. 131, 311317 (2017)






PAR 
LIN 
RES 

The global fit of chirped pulse FTMW, waveguide FTMW, and MMW data

NOTE 



Notes on the fit
