Part I. Energy straggling of ^4He below 2.0 MeV in Al, Ni, Au and Pt. Part II. Studies of the Ti-W metallization system on Si

<p>Part I.</p> <p>In recent years, backscattering spectrometry has become an important tool for the analysis of thin films. An inherent limitation, though, is the loss of depth resolution due to energy straggling of the beam. To investigate this, energy straggling of ⁴He has been measured in thin films of Ni, Al, Au and Pt. Straggling is roughly proportional to square root of thickness, appears to have a slight energy dependence and generally decreases with decreasing atomic number of the adsorber. The results are compared with predictions of theory and with previous measurements. While Ni measurements are in fair agreement with Bohr's theory, Al measurements are 30% above and Au measurements are 40% below predicted values. The Au and Pt measurements give straggling values which are close to one another.</p> <p>Part II.</p> <p>MeV backscattering spectrometry and X-ray diffraction are used to investigate the behavior of sputter-deposited Ti-W mixed films on Si substrates. During vacuum anneals at temperatures near 700��C for several hours, the metallization layer reacts with the substrate. Backscattering analysis shows that the resulting compound layer is uniform in composition and contains Ti, Wand Si. The Ti:W ratio in the compound corresponds to that of the deposited metal film. X-ray analyses with Reed and Guinier cameras reveal the presence of the ternary Ti_xW_(1-x)Si₂ compound. Its composition is unaffected by oxygen contamination during annealing, but the reaction rate is affected. The rate measured on samples with about 15% oxygen contamination after annealing is linear, of the order of 0.5 �� per second at 725��C, and depends on the crystallographic orientation of the substrate and the dc bias during sputter-deposition of the Ti-W film.</p> <p>Au layers of about 1000 �� thickness were deposited onto unreacted Ti-W films on Si. When annealed at 400��C these samples underwent a color change,and SEM micrographs of the samples showed that an intricate pattern of fissures which were typically 3��m wide had evolved. Analysis by electron microprobe revealed that Au had segregated preferentially into the fissures. This result suggests that Ti-W is not a barrier to Au-Si intermixing at 400��C.</p>

A study of W boson properties with four-jet W^+W^- events at LEP

<p>In this thesis I present a study of W pair production in e⁺e^- annihilation using fully hadronic W⁺W^- events. Data collected by the L3 detector at LEP in 1996-1998, at collision center-of-mass energies between 161 and 189 GeV, was used in my analysis.</p> <p>Analysis of the total and differential W⁺W^- cross sections with the resulting sample of 1,932 W⁺W^- ��� qqqq event candidates allowed me to make precision measurements of a number of properties of the W boson. I combined my measurements with those using other W⁺W^- final states to obtain stringent constraints on the W boson's couplings to fermions, other gauge bosons, and scalar Higgs field by measuring the total e⁺e^- ��� W⁺W^- cross section and its energy dependence</p> <p>��(e⁺e^- ��� W⁺W^-) =</p> <p>{2.68^+0.98_-0.67(stat.)�� 0.14(syst.) pb, ���s = 161.34 GeV</p> <p>{12.04^+1.38_-1.29(stat.)�� 0.23(syst.) pb, ���s = 172.13 GeV</p> <p>{16.45 �� 0.67(stat.) �� 0.26(syst.) pb, ���s = 182.68 GeV</p> <p>{16.28 �� 0.38(stat.) �� 0.26(syst.) pb, ���s = 188.64 GeV</p> <p>the fraction of W bosons decaying into hadrons</p> BR(W ���qq') = 68.72 �� 0.69(stat.) �� 0.38(syst.) %, <p>invisible non-SM width of the W boson</p> ��^invisible_W less than MeV at 95% C.L., <p>the mass of the W boson</p> M_W = 80.44 �� 0.08(stat.)�� 0.06(syst.) GeV, <p>the total width of the W boson</p> ��_W = 2.18 �� 0.20(stat.)�� 0.11(syst.) GeV, <p>the anomalous triple gauge boson couplings of the W</p> <p>��g^Z₁ = 0.16^+0.13_-0.20(stat.) �� 0.11(syst.)</p> <p>��k_�� = 0.26^+0.24_-0.33(stat.) �� 0.16(syst.)</p> <p>��_�� = 0.18^+0.13_-0.20(stat.) �� 0.11(syst.)</p> <p>No significant deviations from Standard Model predictions were found in any of the measurements.</p>

Isotope shift measurements using k x-rays in Sn, Sm, and W

<p>Electronic K��l x-ray isotope shifts have been measured for Sn 116-124, Sm 148-154, W 182-184, W 184-186, and W 182-186 using a curved crystal Cauchois spectrometer. The analysis of the measurements has included the electrostatic volume effect, screening by the transition electron as well as the non-transition electrons, normal and specific mass shifts, dynamical nuclear qudrupole polarization, and a radiative correction effect of the electron magnetic moment in the nuclear charge radii are obtained. Where other experimental data are available, the agreement with the present measurements is satisfactory. Comparisons with several nuclear model predictions yield only partial agreement. </p>

Nuclear hyperfine interactions in W^(182), W^(183), and Pt^(195) as studies by the Mossbauer effect

<p>The M��ssbauer technique has been used to study the nuclear hyperfine interactions and lifetimes in W¹⁸² (2⁺ state) and W¹⁸³ (3/2^- and 5/2^- states) with the following results: g(5/2^-)/g(2⁺) = 1.40 �� 0.04; g(3/2^- = -0.07 �� 0.07; Q(5/2^-)/Q(2⁺) = 0.94 �� 0.04; T_1/2(3/2^-) = 0.184 �� 0.005 nsec; T_1/2(5/2^-) >�� 0.7 nsec. These quantities are discussed in terms of a rotation-particle interaction in W¹⁸³ due to Coriolis coupling. From the measured quantities and additional information on ��-ray transition intensities magnetic single-particle matrix elements are derived. It is inferred from these that the two effective g-factors, resulting from the Nilsson-model calculation of the single-particle matrix elements for the spin operators ��_z and ��₊, are not equal, consistent with a proposal of Bochnacki and Ogaza.</p> <p>The internal magnetic fields at the tungsten nucleus were determined for substitutional solid solutions of tungsten in iron, cobalt, and nickel. With g(2⁺) = 0.24 the results are: |H_eff(W-Fe)| = 715 �� 10 kG; |H_eff(W-Co)| = 360 �� 10 kG; |H_eff(W-Ni)| = 90 �� 25 kG. The electric field gradients at the tungsten nucleus were determined for WS₂ and WO₃. With Q(2⁺) = -1.81b the results are: for WS₂, eq = -(1.86 �� 0.05) 10¹⁸ V/cm²; for WO₃, eq = (1.54 �� 0.04) 10¹⁸ V/cm² and �� = 0.63 �� 0.02.</p> <p>The 5/2^- state of Pt¹⁹⁵ has also been studied with the M��ssbauer technique, and the g-factor of this state has been determined to be -0.41 �� 0.03. The following magnetic fields at the Pt nucleus were found: in an Fe lattice, 1.19 �� 0.04 MG; in a Co lattice, 0.86 �� 0.03 MG; and in a Ni lattice, 0.36 �� 0.04 MG. Isomeric shifts have been detected in a number of compounds and alloys and have been interpreted to imply that the mean square radius of the Pt¹⁹⁵ nucleus in the first-excited state is smaller than in the ground state. </p>

The Riesz space structure of an Abelian W*-algebra

<p>Let M be an Abelian W*-algebra of operators on a Hilbert space <i>H</i>. Let M₀ be the set of all linear, closed, densely defined transformations in <i>H</i> which commute with every unitary operator in the commutant M��� of M. A well known result of R. Pallu de Barriere states that if �� is a normal positive linear functional on M, then �� is of the form T ��� (Tx, x) for some x in <i>H</i>, where T is in M. An elementary proof of this result is given, using only those properties which are consequences of the fact that ReM is a Dedekind complete Riesz space with plenty of normal integrals. The techniques used lead to a natural construction of the class M₀, and an elementary proof is given of the fact that a positive self-adjoint transformation in M₀ has a unique positive square root in M₀. It is then shown that when the algebraic operations are suitably defined, then M₀ becomes a commutative algebra. If ReM₀ denotes the set of all self-adjoint elements of M₀, then it is proved that ReM₀ is Dedekind complete, universally complete Riesz spaces which contains ReM as an order dense ideal. A generalization of the result of R. Pallu de la Barriere is obtained for the Riesz space ReM₀ which characterizes the normal integrals on the order dense ideals of ReM₀. It is then shown that ReM₀ may be identified with the extended order dual of ReM, and that ReM₀ is perfect in the extended sense. </p> <p>Some secondary questions related to the Riesz space ReM are also studied. In particular it is shown that ReM is a perfect Riesz space, and that every integral is normal under the assumption that every decomposition of the identity operator has non-measurable cardinal. The presence of atoms in ReM is examined briefly, and it is shown that ReM is finite dimensional if and only if every order bounded linear functional on ReM is a normal integral.</p>