The Surface Scattering Machine
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The physical and chemical processes leading to the formation of molecules in
extraterrestrial environments fascinated scientists since the first detection
of CH, CH +, and CN radicals in diffuse clouds 60 years ago.
Although more than half a century passed by, and 151 species
from molecular hydrogen (H2) to polyatomics
like the sugar glycolaldehyde (HOCH2CHO),
benzene (C 6 H 6 ), and cyanopentaacetylene
(HC11 N) have been identified so far, the enigma ‘How do these
molecules actually form under the harsh conditions in the interstellar medium
and in the hostile environments of our solar system?’ is still under
debate. The Surface Scattering Machine simulates the interaction of charged
particles (nuclei, electrons), atoms, and photons with extraterrestrial
analogue ices as can be found in our solar system (comets, Mars, Pluto, icy
satellites, Kuiper belt objects) and in cold,
molecular clouds. Although the interstellar dust component embodies only 1 % of
the mass of the interstellar medium, these predominantly silicate- and
carbonaceous-based grain nuclei play a key role in the formation of new
molecules. Deep in the interior of dense molecular clouds, grain particles
effectively shield newly synthesized molecules in the gas phase from the
destructive external galactic UV radiation field with a flux of about 108
photons cm-2 s-1 at energies > 6.2 eV. In addition,
these grains hold typical temperatures of 10 K in molecular clouds, and
molecules, radicals as well as atoms from the gas phase are accreted on grain
surfaces resulting in an icy mantle up to 0.1 um thick. Here, solid mixtures
containing H 2 O, CO, CH3OH, NH3, CH4 , H2CO, OCS, OCN-, and
CO2 were identified assigned via IR spectroscopy on interstellar
grains. The identification of formic acid (HCOOH), the HCOO - anion,
and acetaldehyde (CH3CHO) must be regarded as tentatively.

These ices are processed by the
cosmic ray induced internal UV radiation present even in the deep interior of
dense clouds and by particles of the galactic cosmic radiation field; this
leads to the formation of new molecules in the solid state. The particle
component consists of 97 - 98 % protons (p, H+ in the low energy
range of 1 - 10 MeV) and 2 - 3 % helium nuclei Since, however, typical carbon-hydrogen and carbon-carbon
bond strengths in organic molecules range between 3 and 10 eV, the cosmic ray
particles are too energetic to form stable chemical bond as implanted into the
icy mantle. But upon interaction with the solid target, each cosmic ray
particle releases its excess energy to the target atoms in successive
collisions via elastic and inelastic interactions. Here, the elastic process
transfers energy to the nuclei of the target atoms igniting knock on particles
if this amount is larger than the binding energy of the atom. MeV particles, for example, generate carbon knock on
particles with kinetic energies up to 10 keV. These
knock on particles can transfer their energy in consecutive encounters to the
target atoms resulting in a collision cascade of secondary, tertiary, etc.,
knock-on atoms. Moderated to about 1 - 10 eV - the so-called chemical energy
range - these atoms are not in thermal equilibrium with the 10 K target (hence:
non equilibrium or suprathermal particles) and can
react finally with the target molecules via elementary steps of bond insertion,
addition to double or triple bonds, or hydrogen abstraction. The power of these
suprathermal reactions to form new molecules at
temperatures even as low as 10 K is based in their ability to overcome reaction
barriers in the entrance channel easily, since suprathermal
species can impart their excess kinetic energy into the transition state of the
reaction. Even reactions endothermic at 10 K are feasible and extend the
synthetic power of this reaction class further beyond thermal processes of
diffusion controlled chemistry on interstellar grains. Those unique aspects of suprathermal reactions result in reaction rate constants
orders of magnitude larger than their thermal counterparts. These findings
engaged our interest to elucidate chemical and physical effects upon galactic
cosmic ray MeV ion interaction with frozen organic samples resulting
in the formation of new molecules in interstellar ices.

The machine consists of a stainless steel cylinder; a 12'' CF flange
serves as the lid of the chamber and holdis a
centered, differentially pumped feedthrough. This
construction enables an attached closed cycle helium refrigerator and the
target to rotate horizontally 360°. The cold finger is made of a
silver mono crystal attached to the 10K cold head. The crystal serves as a
substrate of a highly polished silver wafer. The temperature of the crystal is
sampled by a silicon diode facilitating any temperature choice between 10K and
350K with the help of a heater and a programmable temperature controller. A
magnetically suspended turbomolecular pump (

Ion beams of well-defined kinetic energy and composition are generated via electron bombardment of a precursor gas, ion extraction, focusing, and mass separation in an ion gun coupled to a Wien filter. The ion source is interfaced via four differentially pumped chambers (10-5 torr, 10-6 torr, 10 -8 torr, 10-10 torr) to the main recipient. This setup can prepare stable H+, He2+, C +, N+, O+, Si+, P+ , and S+ beams while keeping an ultrahigh vacuum of 10-11 torr in the main chamber. Note that electron beams are produced in a commercially available electron gun. The modular design of the sources makes it feasible to incorporate also a tunable photon source, a radiofrequency discharge source (H atoms), and a laser ablation source (C, N, O, S, Fe. Mg, Si, P) in future experiments. During the experiments the chemical modifications of the target are monitored on line and in situ by a FTIR spectrometer in the spectral region of 15,0000 - 400 cm-1 via absorption-reflection. The infrared beam, attenuated by the condensates and the KBr windows, is analyzed by an external, liquid nitrogen cooled mercury-cadmium-telluride detector. Species in the gas phase are detected by a quadrupole mass spectrometer in the residual gas analyzer mode. In future experiments, the detection techniques shall be upgraded and a time-of-flight mass spectrometer perpendicular to the photon or particle beam should be incorporated. Since the ice target is rotatable, operating the mass spectrometer in the time-of-flight mode gives additional information on the underlying chemical dynamics.