Nicht gehst Du fürder mehr einher Frei durch des Volkes Mitte! Genommen ist Dir Deine Wehr Nach des Gefängniß Sitte! ...

Welsch (Projektbearbeiter): Gedicht über den unbeugsamen Freiheitswillen eines aus politischen Gründen Eingekerkerten, an die regierenden Fürsten gerichtet: "D'rum hoffet nicht, durch Eure Qual Den freien Geist zu knechten! ... Ein Schlag an's Gitter und den Stein, So muß der Funke fangen! - Und Euer Thron wird Flammen sein! Und Ihr, Ihr seid gefangen!"

(O8, O8) contribution to B¯ → Xsγγ at O(αs)

In this analysis, we present the contribution associated with the chromomagnetic dipole operator O8 to the double differential decay width dΓ/(ds1ds2) for the inclusive process B¯→Xsγγ. The kinematical variables s1 and s2 are defined as si=(pb−qi)2/m2b, where pb, q1, q2 are the momenta of b quark and two photons. This contribution (taken at tree level) is of order αs, like the recently calculated QCD corrections to the contribution of the operator O7. In order to regulate possible collinear singularities of one of the photons with the strange quark, we introduce a nonzero mass ms for the strange quark. Our results are obtained for exact ms, which we interpret as a constituent mass being varied between 400 and 600 MeV. Numerically it turns out that the effect of the (O8, O8) contribution to the branching ratio of B¯→Xsγγ does not exceed +0.1% for any kinematically allowed value of our physical cutoff parameter c, confirming the expected suppression of this contribution relative to the QCD corrections to dΓ77/(ds1ds2).

Progress in Simulations with Twisted Mass Fermions at the Physical Point

In this contribution, results from Nf = 2 lattice QCD simulations at one lattice spacing using twisted mass fermions with a clover term at the physical pion mass are presented. The mass splitting between charged and neutral pions (including the disconnected contribution) is shown to be around 20(20) MeV. Further, a first measurement using the clover twisted mass action of the average momentum fraction of the pion is given. Finally, an analysis of pseudoscalar meson masses and decay constants is presented involving linear interpolations in strange and charm quark masses. Matching to meson mass ratios allows the calculation of quark mass ratios: ms=ml = 27:63(13), mc=ml = 339:6(2:2) and mc=ms = 12:29(10). From this mass matching the quantities fK = 153:9(7:5) MeV, fD = 219(11) MeV, fDs = 255(12) MeV and MDs = 1894(93) MeV are determined without the application of finite volume or discretization artefact corrections and with errors dominated by a preliminary estimate of the lattice spacing.

Amyloid beta peptide potentiates cytokine secretion by interleukin-1 beta-activated human astrocytoma cells.

Neurodegenerative processes in Alzheimer disease (AD) are thought to be driven in part by the deposition of amyloid beta (A beta), a 39- to 43-amino acid peptide product resulting from an alternative cleavage of amyloid precursor protein. Recent descriptions of in vitro neurotoxic effects of A beta support this hypothesis and suggest toxicity might be mediated by A beta-induced neuronal calcium disregulation. In addition, it has been reported that "aging" A beta results in increased toxic potency due to peptide aggregation and formation of a beta-sheet secondary structure. In addition, A beta might also promote neuropathology indirectly by activating immune/inflammatory pathways in affected areas of the brain (e.g., cortex and hippocampus). Here we report that A beta can modulate cytokine secretion [interleukins 6 and 8 (IL-6 and IL-8)] from human astrocytoma cells (U-373 MG). Freshly prepared and aged A beta modestly stimulated IL-6 and IL-8 secretion from U-373 MG cells. However, in the presence of interleukin-1 beta (IL-1 beta), aged, but not fresh, A beta markedly potentiated (3- to 8-fold) cytokine release. In contrast, aged A beta did not potentiate substance P (NK-1)- or histamine (H1)-stimulated cytokine production. Further studies showed that IL-1 beta-induced cytokine release was potentiated by A beta-(25-35), while A beta-(1-16) was inactive. Calcium disregulation may be responsible for the effects of A beta on cytokine production, since the calcium ionophore A23187 similarly potentiated IL-1 beta-induced cytokine secretion and EGTA treatment blocked either A beta or A23187 activity. Thus, chronic neurodegeneration in AD-affected brain regions may be mediated in part by the ability of A beta to exacerbate inflammatory pathways in a conformation-dependent manner.

Pseudoscalar susceptibilities and quark condensates: chiral restoration and lattice screening masses

We derive the formal Ward identities relating pseudoscalar susceptibilities and quark condensates in three-flavor QCD, including consistently the 77-n' sector and the U-A(1) anomaly. These identities are verified in the low-energy realization provided by ChPT, both in the standard SU(3) framework for the octet case and combining the use of the SU(3) framework and the large-Nc expansion of QCD to account properly for the nonet sector and anomalous contributions. The analysis is performed including finite temperature corrections as well as the calculation of U(3) quark condensates and all pseudoscalar susceptibilities, which together with the full set of Ward identities, are new results of this work. Finally, the Ward identities are used to derive scaling relations for pseudoscalar masses which explain the behavior with temperature of lattice screening masses near chiral symmetry restoration.

Measurement of electrons from heavy-flavour hadron decays in p-Pb collisions at $\\sqrt{s_{NN}} = 5.02$ TeV using TPC and EMCal detectors with ALICE at LHC

Heavy-ion collisions are a powerful tool to study hot and dense QCD matter, the so-called Quark Gluon Plasma (QGP). Since heavy quarks (charm and beauty) are dominantly produced in the early stages of the collision, they experience the complete evolution of the system. Measurements of electrons from heavy-flavour hadron decay is one possible way to study the interaction of these particles with the QGP. With ALICE at LHC, electrons can be identified with high efficiency and purity. A strong suppression of heavy-flavour decay electrons has been observed at high $p_{m T}$ in Pb-Pb collisions at 2.76 TeV. Measurements in p-Pb collisions are crucial to understand cold nuclear matter effects on heavy-flavour production in heavy-ion collisions. The spectrum of electrons from the decays of hadrons containing charm and beauty was measured in p-Pb collisions at $\\sqrt = 5.02$ TeV. The heavy flavour decay electrons were measured by using the Time Projection Chamber (TPC) and the Electromagnetic Calorimeter (EMCal) detectors from ALICE in the transverse-momentum range $2 < p_ < 20$ GeV/c. The measurements were done in two different data set: minimum bias collisions and data using the EMCal trigger. The non-heavy flavour electron background was removed using an invariant mass method. The results are compatible with one ($R_ \\approx$ 1) and the cold nuclear matter effects in p-Pb collisions are small for the electrons from heavy-flavour hadron decays.

Ausgewählte kapitel der zahlentheorie...

Available on demand as hard copy or computer file from Cornell University Library.

Exotic meson decay widths using lattice quantum chromodynamics

Most experiments in particle physics are scattering experiments, the analysis of which leads to masses, scattering phases, decay widths and other properties of one or multi-particle systems. Until the advent of Lattice Quantum Chromodynamics (LQCD) it was difficult to compare experimental results on low energy hadron-hadron scattering processes to the predictions of QCD, the current theory of strong interactions. The reason being, at low energies the QCD coupling constant becomes large and the perturbation expansion for scattering; amplitudes does not converge. To overcome this, one puts the theory onto a lattice, imposes a momentum cutoff, and computes the integral numerically. For particle masses, predictions of LQCD agree with experiment, but the area of decay widths is largely unexplored. ^ LQCD provides ab initio access to unusual hadrons like exotic mesons that are predicted to contain real gluonic structure. To study decays of these type resonances the energy spectra of a two-particle decay state in a finite volume of dimension L can be related to the associated scattering phase shift δ(k) at momentum k through exact formulae derived by Lüscher. Because the spectra can be computed using numerical Monte Carlo techniques, the scattering phases can thus be determined using Lüscher's formulae, and the corresponding decay widths can be found by fitting Breit-Wigner functions. ^ Results of such a decay width calculation for an exotic hybrid( h) meson (JPC = 1-+) are presented for the decay channel h → πa 1. This calculation employed Lüscher's formulae and an approximation of LQCD called the quenched approximation. Energy spectra for the h and πa1 systems were extracted using eigenvalues of a correlation matrix, and the corresponding scattering phase shifts were determined for a discrete set of πa1 momenta. Although the number of phase shift data points was sparse, fits to a Breit-Wigner model were made, resulting in a decay width of about 60 MeV. ^

Coherent rho meson electroproduction off deuteron

QCD predicts Color Transparency (CT), which refers to nuclear medium becoming transparent to a small color neutral object produced in high momentum transfer reactions, due to reduced strong interaction. Despite several studies at BNL, SLAC, FNAL, DESY and Jefferson Lab, a definitive signal for CT still remains elusive. In this dissertation, we present the results of a new study at Jefferson Lab motivated by theoretical calculations that suggest fully exclusive measurement of coherent rho meson electroproduction off the deuteron is a favorable channel for studying CT. Vector meson production has a large cross section at high energies, and the deuteron is the best understood and simplest nuclear system. Exclusivity allows the production and propagation to be controlled separately by controlling Q 2, lf (formation length), lc (coherence length) and t. This control is important as the rapid expansion of small objects increases their interaction probability and masks CT. The CT signal is investigated in a ratio of cross sections at high t (where re-scattering is significant) to low t (where single nucleon reactions dominate). The results are presented over a Q2 range of 1 to 3 GeV2 based on the data taken with beam energy of 6 GeV.

Angular distribution of Z(0 power) bosons in Z+jet events at the square root of S = 7 TeV

For the first time, the Z0 boson angular distribution in the center-of-momentum frame is measured in proton-proton collisions at [special characters omitted] = 7 TeV at the CERN LHC. The data sample, recorded with the CMS detector, corresponds to an integrated luminosity of approximately 36 pb–1 . Events in which there is a Z0 and at least one jet, with a jet transverse momentum threshold of 20 GeV and absolute jet rapidity less than 2.4, are selected for the analysis. Only the Z0's muon decay channel is studied. Within experimental and theoretical uncertainties, the measured angular distribution is in agreement with next-to-leading order perturbative QCD predictions.

Angular distribution of prompt photons using the compact muon solenoid detector at a square root of S = 7 TeV

The study of the angular distribution of photon plus jet events in pp collisions at [special characters omitted] = 7 TeV with the Compact Muon Solenoid (CMS) detector is presented. The photon is restricted to the central region of the detector (:η: <1.4442) while the jet is allowed to be present in both central and forward regions of CMS (:η: < 2.4). Dominant backgrounds due to jets fragmenting into neutral mesons are accounted for through the use of a template method that discriminates between signal and background. The angular distribution, :η*:, is defined as the absolute value of the difference in η between the leading photon and leading jet in an event divided by two. The angular distribution ranging from 0–1.4 was examined and compared with next-to-leading order QCD predictions and was found to be in good agreement.

A Measurement of the Proton Structure Function g2p at Low Q2

Experiments at Jefferson Lab have been conducted to extract the nucleon spin-dependent structure functions over a wide kinematic range. Higher moments of these quantities provide tests of QCD sum rules and predictions of chiral perturbation theory ($\chi$PT). While precise measurements of $g_{1}^n$, $g_{2}^n$, and $g_1^p$ have been extensively performed, the data of $g_2^p$ remain scarce. Discrepancies were found between existing data related to $g_2$ and theoretical predictions. Results on the proton at large $Q^2$ show a significant deviation from the Burkhardt-Cottingham sum rule, while results for the neutron generally follow this sum rule. The next-to-leading order $\chi$PT calculations exhibit discrepancy with data on the longitudinal-transverse polarizability $\delta_{LT}^n$. Further measurements of the proton spin structure function $g_2^p$ are desired to understand these discrepancies.

Experiment E08-027 (g2p) was conducted at Jefferson Lab in experimental Hall A in 2012. Inclusive measurements were performed with polarized electron beam and a polarized ammonia target to obtain the proton spin-dependent structure function $g_2^p$ at low Q$^2$ region (0.02$<$Q$^2$$<$0.2 GeV$^2$) for the first time. The results can be used to test the Burkhardt-Cottingham sum rule, and also allow us to extract the longitudinal-transverse spin polarizability of the proton, which will provide a benchmark test of $\chi$PT calculations. This thesis will present and discuss the very preliminary results of the transverse asymmetry and the spin-dependent structure functions $g_1^p$ and $g_2^p$ from the data analysis of the g2p experiment .

Ein Programm für die Parallelisierung dynamisch adaptiver Mehrgitterverfahren

In dieser Arbeit werden dynamisch adaptive Mehrgitterverfahren parallelisiert. Bei dynamisch adaptiven Mehrgitterverfahren wird ein Gebiet mit einem Gitter überdeckt, und auf diesem Gitter wird gerechnet, indem Gitterpunkte in der Umgebung herangezogen werden, um den Wert des nächsten Zeitpunktes zu bestimmen. Dann werden gröbere und feinere Gitter erzeugt und verwendet, wobei die feineren Gitter sich auf Teilgebiete konzentrieren. Diese Teilgebiete ändern sich im Verlauf der Zeit. Durch die Verwendung der zusätzlichen Gitter werden die numerischen Eigenschaften verbessert. Die Parallelisierung solcher Verfahren geschieht in der Regel durch Bisektion. In der vorliegenden Arbeit wird die Umverteilung der Gebiete realisiert, indem Mengen von einzelnen Gitterpunkten verschickt werden. Das ist ein Scheduling-Verfahren. Die Mehrgitterstrukturen sind so aufgebaut, dass fast beliebige Gitterpunktverteilungen auf den Gitterebenen vorliegen können. Die Strukturen werden einmal erzeugt, und nur bei Bedarf geändert, sodass keine Speicherallokationen während der Iterationen nötig sind. Neben dem Gitter sind zusätzliche Strukturen, wie zum Beispiel die Randstrukturen, erforderlich. Eine Struktur Farbenfeld verzeichnet, auf welchem Kern sich ein Außenrandpunkt befindet. In der parallelen adaptiven Verfeinerung werden für einzelne durch ein Entscheidungskriterium ausgewählte Gitterpunkte 5 x 5 Punktüberdeckungen vorgenommen. Dazu werden die verfügbaren Entscheidungsinformationen zur Bestimmung von komplexeren Strukturen herangezogen. Damit muss das Verfeinerungsgitter nicht komplett abgebaut und dann wieder aufgebaut werden, sondern nur die Änderungen am Gitter sind vorzunehmen. Das spart viel Berechnungszeit. Der letzte Schritt besteht darin, den Lastausgleich durchzuführen. Zunächst werden die Lasttransferwerte bestimmt, die angeben, wie viele Gitterpunkte von wo nach wo zu verschicken sind. Das geschieht mit Hilfe einer PLB genannten Methode bzw. einer Variante. PLB wurde bisher vor allem für kombinatorische Probleme eingesetzt. Dann erfolgt eine Auswahl der zu verschickenden Gitterpunkte mit einer Strategie, welche Punkte eines Kerns zu welchen Nachbarkernen transferiert werden sollen. Im letzten Schritt werden schließlich die ausgewählten Punkte migriert, wobei alle Gitterpunktstrukturen umgebaut werden und solche Informationen gepackt werden müssen, sodass ein Umbau seiner Gitterpunktstrukturen bei dem Empfänger möglich wird. Neben den Gitterpunktstrukturen müssen auch Strukturen für die parallele adaptive Verfeinerung verändert werden. Es muss ein Weiterverschicken von Gitterpunkten möglich sein, wenn über die Lastkanten in mehreren Runden Last verschickt wird. Während des Lastausgleichs wird noch Arbeit durch eine Struktur Zwischenkorrektur durchgeführt, die es ermöglicht, das Farbenfeld intakt zu halten, wenn benachbarte Gitterpunkte gleichzeitig verschickt werden.

Os efeitos nucleares em processos de produ¸c˜ao de quarkonium no Relativistic Heavy Ion Collider (RHIC) e no Large Hadron Collider (LHC)

Neste trabalho de disserta¸c˜ao, investigamos os efeitos nucleares em processos de produ¸c˜ao de quarkonium no Relativistic Heavy Ion Collider (RHIC) e no Large Hadron Collider (LHC). Para tanto, consideramos o Modelo de Evapora¸c˜ao de Cor (CEM), baseado em processos partˆonicos calculados mediante a QCD perturbativa e em intera¸c˜oes n˜ao perturbativas via troca de gl´uons suaves para a forma¸c˜ao do quarkonium. Supress˜ao de quarkonium ´e um dos sinais de forma¸c˜ao do assim chamado Plasma de Quarks e Gl´uons (QGP) em colis˜oes ultrarelativ´ısticas de ´ıons pesados. No entanto, a supress˜ao n˜ao ´e somente causada em colis˜oes n´ucleo-n´ucleo (AA) devido `a forma¸c˜ao do QGP. De fato, a supress˜ao de quarkonium tamb´em foi observada em colis˜oes pr´oton-n´ucleo (pA). A fim de separar os efeitos da mat´eria quente (devidos ao QGP) e fria (efeitos n˜ao devidos ao QGP), pode-se olhar primeiro para colis˜oes pA, onde somente efeitos de mat´eria fria desempenham um papel fundamental, e depois aplicar esses efeitos em colis˜oes AA, uma vez que parte da supress˜ao ´e devido a efeitos de mat´eria fria. No regime de altas energias, a produ¸c˜ao do quarkonium ´e fortemente dependente da distribui¸c˜ao de gl´uons nuclear, o que viabiliza uma oportunidade ´unica de estudar o comportamento de pequeno x dos gl´uons dentro do n´ucleo e, consequentemente, restringir os efeitos nucleares. Estudamos os processos nucleares utilizando distintas parametriza¸c˜oes para as distribui¸c˜oes partˆonicas nucleares. Calculamos a raz˜ao nuclear para processos pA e AA em fun¸c˜ao da vari´avel rapidez para a produ¸c˜ao de quarkonium, o que permite estimar os efeitos nucleares. Al´em disso, apresentamos uma compara¸c˜ao com os dados do RHIC para a produ¸c˜ao do m´eson J/Ψ em colis˜oes pA, demonstrando que a an´alise deste observ´avel ´e uma quest˜ao em aberto na literatura. Adicionalmente, estimamos a produ¸c˜ao de quarks pesados e quarkonium na etapa inicial e durante a fase termal de uma colis˜ao ultrarelativ´ıstica de ´ıons pesados. O objetivo deste estudo ´e estimar as distintas contribui¸c˜oes para a produ¸c˜ao e de alguns efeitos do meio nuclear.