Harold Linnartz
Professor for
Molecular Laboratory Astrophysics |
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2009 ˇ
[92] Formation rates
of complex organics in UV irradiated CH3OH-rich ices I:
Experiments (*) ˇ
[91] Quantification of
segregation dynamics in ice mixtures (*) ˇ
[90] A
zero-gravity instrument to study low velocity collisions of fragile particles
at low temperatures (*) ˇ
[89] Rotational
analysis of the A2S+ (v=1,2) – X2P (v=0) electronic transition of 15N18O
(*) ˇ
[88] Time resolved optical spectroscopy of VUV
irradiated pyrene:H2O interstellar ice (*) ˇ
[87] Hydrogenation reactions in interstellar CO
analogues – a combined experimental / theoretical study (*) ˇ
[86] Photodesorption of ices II: H2O
and D2O (*) ˇ
[85] Photodesorption of ices I: CO, N2
and CO2 (*) ˇ
[84] Cavity ring down spectroscopy of molecular
transients (*) 2008 ˇ
[83] Deep-UV absorption and Rayleigh scattering
of N2, CH4 and SF6 (*) ˇ
[82] Laboratory
evidence for efficient water formation in interstellar ices. (*) ˇ
[81] Deep-UV absorption and Rayleigh scattering
of carbon dioxide. (*) ˇ
[80] The quasi quantum treatment of
rotationally inelastic scattering from a hard shell potential: its derivation
and practical use. (*) 2007 ˇ
[79] H-atom bombardment of CO2,
HCOOH and CH3CHO containing ices. (*) ˇ
[78] Band profiles and band strengths in mixed
H2O:CO ices. (*) ˇ
[77] Vibronic spectrum of 15N16O2
between 415 and 440 nm. (*) ˇ
[76] A
systematic study of ion and cluster ion formation in continuous supersonic
planar plasma. (*) ˇ
[75] Mid
infrared continuous wave cavity ring down spectroscopy of molecular ions
using an optical parametric oscillator. (*) ˇ
[74]
Infrared spectroscopy of HCOOH interstellar ice analogues. (*) ˇ
[73]
Photodesorption of CO ice. (*) ˇ
[72]
Desorption of CO and O2 interstellar ice analogs. (*) ˇ
[71]
Selective trace gas detection of complex molecules in a planar expansion. (*) ˇ
[70]
Effects of CO2 on H2O band profiles and band strengths
in mixed H2O:CO2 ices. (*) 2006 ˇ
[69]
Parity dependent rotational rainbows in D2-NO differential
collision cross sections. (*) ˇ
[68]
Comparative studies of O2 and N2 in pure, mixed and
layered CO ices. (*) ˇ
[67]
Quantum interference as the source of steric
asymmetry and parity propensity rules in NO-rare gas inelastic scattering. (*) ˇ
[66]
High resolution electronic study of 16O14N16O,
16O14N18O and 18O14N18O;
A rovibronic survey
covering 11800 – 14380 cm-1. (*) ˇ
[65]
Fermi interaction between the n1 and n2+4ns bands
of Ar-DN2+. (*) ˇ
[64] Temperature dependent cross
sections of O2-O2 collision induced absorption
resonances at 477 and 577 nm. (*) ˇ
[63] Preface - Special Issue Phys. Scripta on “MOLEC XV” (*). ˇ
[62] The A2B2
- X2A1 electronic transition of 15NO2:
a rovibronic survey covering 14300 - 18000 cm-1.
(*)
2005 ˇ
[61] Differential cross sections
for collisions of hexapole state-selected NO with He. (*) ˇ
[60] High resolution infrared
spectroscopy of the charge transfer complex [Ar-N2]+., a combined experimental /
theoretical study. (*) ˇ
[59] What is wrong with the steric asymmetry in atom molecule collisions.
(*)
2004 ˇ
[58] A remotely controllable
optical multi-pass system. (*) ˇ
[57] New laboratory data of a molecular
band at 4429 A. (*) ˇ
[56] Sensitive fluorescence
spectroscopy of jet cooled 15NO2. (*) ˇ
[55] Sign of the state-to-state steric asymmetry of rotationally inelastic atom-molecule
collisions. (*) ˇ
[54] Preface - Special Issue Chem.
Phys. on "Stereodynamics of Molecular
Reactions. (*) ˇ
[53] Planar plasma expansions as a
tool for high resolution molecular spectroscopy. (*) ˇ
[52] Mass spectrometric and laser
spectroscopic characterization of a supersonic planar plasma expansion. (*)
2003 ˇ
[51] High resolution electronic spectroscopy
of a non-linear carbon chain radical C6H4+.
(*)
2002 ˇ
[50] Rotationally resolved infrared
spectrum of the charge transfer complex [Ar-N2]+.
(*) ˇ
[49] Electronic gas phase spectrum
of the pentaacetylene cation.
(*) ˇ
[48] Rotationally resolved A2P
u - X2Pg electronic transition of HC4D+.
(*) ˇ
[47] Cw
cavity ring down spectroscopy in a supersonic planar
plasma. (*) ˇ
[46] Depletion modulation of Ar-H2O
in a supersonic planar plasma. (*) ˇ
[45] Rotationally resolved A2P
u - X2Pg electronic transition of NC6N+.
(*)
2001 ˇ
[44] Rotationally resolved 3S -
- X3S-
electronic transition of NC5N. (*) ˇ
[43] The 3S-
- X3S- electronic transition of HC6N. (*) ˇ
[42] Vibrationally
excited state spectroscopy of radicals in a supersonic
plasma. (*) ˇ
[41] The A2S+
-- X2P transition of CF starting from highly excited vibrational
states. (*)
2000 ˇ
[40] High resolution spectroscopy
of radicals, ions and ionic complexes in the gas phase. ˇ
[39] Spectroscopic and theoretical characterisation of the v2 band of Ar-DN2+.
(*) ˇ
[38] Rotationally resolved A2Pu
<- X2Pg electronic spectrum of tetraacetylene
cation. (*) ˇ
[37] The n1 and n2
bands of Ar-HN2+; a joint theoretical/experimental
study. (*) ˇ
[36] The rotational spectra of the
HCCCNH+, NCCNH+, and CH3CNH+
ions. (*) ˇ
[35] Linear
and centro symmetric N2-Ar+-N2. (*) ˇ
[34] The 3Su-
<- X3Su- electronic spectrum of linear C4
in the gas phase. (*) ˇ
[33] Infrared high resolution
direct absorption spectroscopy of ionic complexes. (*) ˇ
[32] Gas phase electronic spectra
of carbon chain radicals compared with diffuse interstellar band
observations. (*)
1999 ˇ
[31] Rotationally resolved
electronic absorption spectra of triacetylene cation in a supersonic jet. (*) ˇ
[30] The 1Pu
<- X1Su+ electronic spectrum of C5
in the gas phase. (*) ˇ
[29] Spectroscopic and theoretical
characterization of linear centrosymmetric N2-H+-N2.
(*) ˇ
[28] Electronic ground and excited
state spectroscopy of C6H and C6D. (*) ˇ
[27] Cavity ring down spectroscopy
of carbon chain radicals. ˇ
[26] Cavity ring down spectroscopy
on radicals in a supersonic slit nozzle discharge. (*) ˇ
[25] Rotationally resolved A2P
<- X2P electronic spectrum of triacetylene
cation by frequency modulation absorption
spectroscopy. (*)
1998 ˇ
[24] Along the way to high
resolution absorption spectra of ionic complexes. ˇ
[23] The 2P <- X2P
electronic spectra of C8H and C10H in the gas phase. (*) ˇ
[22] Electronic spectroscopy of
carbon chains and relevance to astrophysics. (Faraday-link) ˇ
[21] Millimeter wave spectroscopy
in a pulsed supersonic slit nozzle discharge. (*) ˇ
[20] High resolution infrared
spectrum of the n3 band in
Ar-HCO+. (*) ˇ
[19] Tunable far-infrared
spectroscopy of 82KrD+, 84KrD+, 86KrD+
and 82KrH+. (*)
1997 ˇ
[18] Infrared absorption spectrum
of Ar-HN2+ in a supersonic slit expansion. (*) ˇ
[17] N4+,
structure and distortion. (*) ˇ
[16] The pure rotational spectrum
of 84KrH+ and 86KrH+. (*) 1996-1990 ˇ
[15] Rotationally resolved infrared
spectrum of N4+. (*) ˇ
[14] Stark effect and dipole
moments of the ammonia dimer in different vibration
rotation tunneling states. (*) 1990-1995 ˇ
[13] Het
ammoniak dimeer. ˇ
[12] The ammonia dimer: new infrared - far infrared double resonance
results. (*) ˇ
[11] The ammonia dimer; complex dynamics with a dynamical complex. ˇ
[10] Infrared and far infrared
spectroscopy on transient molecules. ˇ
[9] Tunable infrared and far
infrared direct absorption spectroscopy of molecular ions in a supersonic jet
expansion. (*) ˇ
[8] The electric dipole moment of
(NH3)2 for G:|K|=1. (*) ˇ
[7] An infrared - far infrared
double resonance study on (NH3)2 in a jet. (*) ˇ
[6] Determination of the electric
dipole moment of KrH+. (*) ˇ
[5] Microwave and submillimeter
spectroscopy of Ar-HN3 states correlating with Ar
+ NH3 (j=1,|k|=1). (*) ˇ
[4] Fragmentation by electron
impact ionization and intracluster reactions of
size selected (N2H4)n
and (OCS)n clusters. ˇ
[3] IR photodissociation
of size selected molecular clusters and their structures. ˇ
[2] Infrared photodissociation
of size selected methylamine clusters. (*) ˇ
[1] Reply to the comment on
'Electron bombardment fragmentation of size selected NH3
clusters'. (*) |
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