Aby bylo možné charakterizovat atmosfericky citlivé vzorky ve vysokofrekvenčním elektronovém paramagnetickém rezonančním spektrometru (z angl. high-frequency electron paramagnetic resonance spectrometer, HF-EPR), je potřebné mít vakuový transportní systém. Cílem této práce je navrhnout a vyvinout tento vakuový přepravní systém, který umožní tuto přepravu. Vakuový systém, který se skládá z mobilního vakuového kufru, držáku palety a přechodové komory, byly navrženy, sestaveny a testovány. Bylo dosaženo tlaku 4,3 10^{-10}mbar, což zajistí inertní podmínky pro transport vzorků. Byl proveden transport vzorku ze systému ultravysokého vakua (UHV) do HF-EPR spektrometru. Kontaminace testovacích vzorků byla charakterizována pomocí rentgenové fotoelektronové spektroskopie. Bylo zjištěno, že nedochází téměř k žádné detekovatelné kontaminaci, pokud je vzorek přepravován pomocí vakuovém systému méně než 16 hodin. Bylo navrženo rozšíření pro přepravu vzorků z rukavicového boxu a paletky pro grafen, ale jejich výroba dosud nebyla provedena. Vyvinutý vakuový systém je plně funkční a poskytuje alternativu ke komerčně dostupným produktům, a proto bude dále používán při zkoumání vzorků citlivých na atmosféru v laboratořích CEITEC Nano.

Nitrenes are reactive intermediates for many organic reactions, such as Curtius rearrangement. The thermo- or photochemical- decomposition of azides or isocyanates was known to generate nitrenes. We investigated the thermal chemistry of nitrene adsorbed on Cu(111) using benzyl azide (Bz-N=N=N), benzyl isocyanate (Bz-N=C=O) and phenyl isocyanate (ph-N=C=O) as precursors under ultrahigh vacuum conditions using temperature-programmed reaction/desorption (TPR/D), reflectionabsorption infrared spectroscopy (RAIRS) and X-ray photoelectron spectroscopy (XPS). Our study shows that despite of the isoelectronic functionalities (-N=N=N vs. -N=C=O) these molecules undergo different reaction pathways. For benzyl azide (Bz-N=N=N), the azido group losses N2 ,and the phenyl group migrates from nitrogen to carbon, forming surface bound H2C=N-Ph at 210 K. Eventually, H2 elimination and a carbon-to-nitrogen phenyl shift give the thermally stable ph-CN final product. XPS reveals that benzyl isocyanate (Bz-N=C=O) rearranges to form amide intermediate on the surface, which breaks into CO2, HCN and toluene at 410 K. RAIRs suggests that phenyl isocyanate (ph-N=C=O) undergoes cyclodimerization, cyclotrimerization and condensation to remove CO2 at 170 K, and phenyl group shifts from nitrogen to carbon to produce a metal bound acyl nitrene species (Ph-(C=O)-N---Cu) at 410 K.

Nitromethane is the simplest organic-nitro compound as well as the archetype of an important class of high explosive. Homogeneous nitromethane reactions have been the subject of extensive studies. Particularly the unimolecular isomerization of nitromethane to methyl nitrite is proven to be competitive with simple C-N bond (bond energy 60 kcal/mol) rupture. The activation energy for the rearrangement was measured to be 55.5 kcal/mol and methyl nitrite has a very weak CH3O-NO bond energy 42 kcal/mol lower than that for homolysis. The thermal chemistry of nitromethane on Cu(111) was studied by a combination of temperature-programmed desorption (TPD) and reflection absorption infrared spectroscopy (RAIRS) techniques. TPD spectra show that the desorption features include the physisorbed multilayer and monolayer of CH3NO2 at 150 and 190 K, respectively. The major decomposition pathway is via cleavage of O-N bond to yield a major product NO, which is characterized by m/z 30(NO+). A possible contribution from isomerization of nitromethane to methyl nitrite (CH3NO2 CH3ONO) on the surface cannot be ruled out at 278 K. In addition to isomerization, the dehydrogenation products CO and CO2 are also unveiled as part of the desorption features at 314 and 455 K, respectively. We can further prove the reactivity of nitromethane on Cu(111) at 367 K by using the deuterated form of nitromethane which reveals the corresponding desorption TPR/D signals of D2, D2O and CD4. However, we find that nitromethane also reacts by dissociating the C-H bond and the O-N bond, however, leaving the C-N bond intact. Along this reaction channel, HCN desorbs as a product above 360 K, as evidenced by a broad desorption feature of m/z 27. Dimerization of CN to C2N2 occurs at 815 K. The RAIR spectroscopy demonstrates that nitromethane is indeed adsorbed on Cu(111) at 100 K. The formation of methoxy and formyl are supported by the observation of desorption of NO at 278 K with the characteristic NO stretching mode found at 1535 cm-1. Moreover, we assign side-bonded CN and aminomethylene (HC-NH2) present on Cu(111). After the surface is annealed to 330 K, a signature band at 2173 cm-1 is assigned to terminal-bounded CN stretching mode. This band eventually fades out above 900 K consistent with the evolution of cyanogen at 815 K.

A low temperature scanning tunneling microscope (LTSTM) was built that we could use in an ultra high vacuum (UHV) system. The scanning tunneling microscope (STM) was tested on an existing 3He cryostat and calibrated at room, liquid nitrogen and helium temperatures. We analyzed the operational electronic and vibration noises and made some effective improvements. To demonstrate the capabilities of the STM, we obtained atomically resolved images of the Au (111) and graphite surfaces. In addition, we showed that the stable tunneling junctions can be formed between the Pt/Ir tip and a superconducting thin film PbBi. We observed the atomic corrugation on Au (111) and measured the height of the atomic steps to be approximately2.53Å, which agrees with published values. In our images of the graphite surface, we found both the β atoms triangular structure, as well as the complete α-β hexagonal unit cell, using the same tip and the same bias voltage of 0.2V. The successful observation of the hidden α atoms of graphite is encouraging in regards to the possibility of imaging other materials with atomic resolution using our STM. We also demonstrated that stable tunneling junctions can be formed at various temperatures. To demonstrate this, the superconducting current-voltage and differential conductance-voltage characteristics of a PbBi film were measured from 1.1K to 9K From this data, the temperature dependent energy gap of the superconductor was shown to be consistent with the predictions of the Bardeen, Cooper, and Schrieffer (BCS) theory.

Two most useful families of copper CVD precursors that have been utilized widely are the Cu(I) and Cu(II) £]-diketone complexes. The Cu(II)precursors require the use of an external reducing agent such as hydrogen to deposit copper films, i.e. CuII(£]-diketonate)2 + H2 ¡÷ Cu0+2 £]-diketonate. The Cu(I) precursors deposit pure copper films without the use of an external agent via a disproportionation reaction that produces a Cu(II)£]-diketonate in conjunction with other organic byproducts, i.e. 2CuI(£]-diketonate)L ¡÷ Cu0+ CuII(£]-diketonate)2+2L where L is a typical Lewis base neutral ligand. However, Do those ligands resulting from the dissociation of the precursors simply desorb intact from the substrate or the growing films, or react further on the surface? To understand the surface chemistry of these ligands may provide better knowledge for designing more superior precursors and improvement of fabrication processes. Cu(hfac)(VTMS) and Cu(hfac)(MHY) are the most promising Cu(I) precursors, as shown in Scheme 1.1. Here we report studies on the chemistry of VTMS, MHY and hfacH on a Cu(111) surface. It should be noted that the hfacH is the simplest molecule containing the hfac, so we use it as a reference for £]-diketonate ligand. The Cu(111) single crystal was used to mimic the reactivity of these ligands on a growing Cu film during copper CVD. In situ analysis of ligand surface chemistry is carried out by TPD/R (temperature-programmed desorption/reaction) and RAIRS (reflection adsorption infrared spectroscopy) to elucidate plausible reaction mechanisms by which ligands decompose and eventually lead to impurity incorporation into the growing films, and to suggest means of minimizing such reactions.

We investigated the reactivity and bonding of perfluoroethyl groups (C2F5) on Cu(111) under ultra high vacuum conditions. Perfluoroethyl moieties bonded to the surface were generated by the dissociative adsorption of perfluoroethyl iodide. Temperature-programmed reaction/desorption (TPR/D) and reflection- adsorption infrared spectroscopy (RAIRS) revealed abounding reaction pathways, and a variety of intermediates were either identified or inferred. The major desorption products, hexafluoro-2-butyne and hexafluorocyclobutene, were detected at 360K and 440K, and some octafluorobutene was observed at 320K at higher coverages, implicating that two fluorine atoms were abstracted step-by-step from the C2F5 on Cu(111). Two sets of signature IR bands were recognized. One set (2054cm-1, 1409cm-1, 1210cm-1) was found to correlate with the surface-bound trifluorovinyl moieties which were also confirmed by directly generating this species from trifluorovinyl iodide. The other set of vibrational features (1322cm-1, 1224cm-1, 950cm-1) presumably implied the trifluoro- ethylidyne intermediate on the surface. Hence, C2F5(ad) underwent the £\-F and £]-F elimination reactions in sequence to yield trifluorovinyl which eventually led to hexafluoro-2-butyne. The alternative route was that C2F5(ad) proceeded via the £\-F elimination reaction twice to render trifluoroethylidyne which ultimately resulted in hexafluorocyclobutene. To our knowledge, the occurrence of the sequential £\-F and£]-F elimination pathway, or the double £\-F elimination reaction has never been observed in any single system.