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Resistive Plate Chambers (RPCs) are gaseous parallel plate avalanche detectors that implement electrodes made from a material with a high volume resistivity between 10 high 7 and 10 high 12 omega cm. Large area RPCs with 2mm single gaps operated in avalanche mode provide above 98% efficiency and a time resolution of around 1 ns up to a flux of several kHz/cm high 2. These Trigger RPCs will, as an example, equip the muon detector system of the ATLAS experiment at CERN on an area of 3650 m high 2 and with 355.000 independent read out channels. Timing RPCs with a gas gap of 0.2 to 0.3mm are widely used in multi gap configurations and provide 99% efficiency and time resolution down to 50 ps. While their performance is comparable to existing scintillator-based Time-Of-Flight (TOF) technology, Timing RPCs feature a significantly, up to an order of magnitude, lower price per channel. They will for example equip the 176 m high 2 TOF barrel of the ALICE experiment at CERN with 160.000 independent read out cells. RPCs were originally operated in streamer mode providing large signals which simplifies readout electronics and gap uniformity requirements. However, high rate applications and detector aging issues made the operation in avalanche mode popular. This was also facilitated by the development of new highly quenching C2F4H2-based gas mixtures with small contents of SF6. While the physics of streamers is difficult to study, the avalanche mode opened the possibility for a detailed simulation of the detector physics processes in RPCs. Even though RPCs were introduced in the early eighties and have been (will be) used in experiments, there are still disagreements about the explanation of several aspects of the RPC performance. The high efficiency of single gap RPCs would require a large ionization density of the used gases, which according to some authors contradicts measurements. Even in the case of a large ionization density the gas gain has to be extremely large, in order to arrive at the observed RPC efficiency. This raises other questions: A very strong space charge effect is required to explain the observed small avalanche charges around 1 pC. Doubts have been raised whether an avalanche can progress under such extreme conditions without developing into a streamer. To overcome these difficulties, other processes, like the emission of an electron from the cathode, were suggested. Moreover, the shape of measured charge spectra of single gap RPCs differs largely from what is expected from the statistics of the primary ionization and the avalanche multiplication. In this thesis we discuss the detector physics processes of RPCs, from the primary ionization and the avalanche statistics to the signal induction and the read out electronics. We present Monte-Carlo simulation procedures that implement the described processes. While the fundament of the described model and some results were already published elsewhere [1], the subject of this thesis is the implementation of the space charge effect. We present analytic formulas for the electrostatic potential of a point charge in the gas gap of an RPC. These formulas were developed in collaboration with the University of Graz [2] and were published in [3, 4]. The simulation model presented in [1] is completed by the dynamic calculation of the space charge field using these formulas. Since the gas parameters like drift velocity and the Townsend and attachment coefficients depend on the electric field, they are calculated dynamically as well. The functional dependence of these parameters on the field is obtained with the simulation programs MAGBOLTZ and IMONTE. For the primary ionization parameters, we use the values that are predicted by the program HEED. While the described procedure only simulates the longitudinal avalanche development towards the anode of the RPC, we also present more dimensional models that allow a careful study of the transverse repulsive and attractive forces of the space charge fields, and of the consequences for the avalanche propagation. We shall show that the efficiencies of single gap Timing RPCs is indeed explained by the high primary ionization density (about 9.5 /cm as predicted by HEED) and a large effective Townsend coefficient (around 113 /mm as predicted by IMONTE). We show that the space charge field reaches the same magnitude as the applied electric field in avalanches at large gas gain. This strong space charge effect effectively suppresses large values for the avalanche charges. The shape of the simulated charge spectra is very similar to the measurements. Also the simulated average charges are close to the experimental results. RPCs are operated in a strong space charge regime over a large range of applied voltage, contrary to wire chambers. We apply only standard detector physics simulations to RPCs. The performance of Timing and Trigger RPCs is well reproduced by our simulations. The results concerning the space charge effect were presented and discussed at the 'RPC 2001' workshop [5] and on the '2002 NSS/MIC' conference [6].
This thesis presented the measurement of antideuteron and antihelium-3 production in central AuAu collisions at V SNN = 200 GeV center-of-mass energy at RHIC. The analysis is based on STAR data, about 3 x 10 high 6 events at top 10% centrality. Within the data sample a total number of about 5000 antideuterons and 193 antihelium-3 were observed in the STARTPC at mid-rapidity. The specific energy loss measurement in the TPC provides antideuteron identification only in a small momentum window, antihelium-3 however can be identified nearly background free with almost complete momentum range coverage. Following the statistical analysis of the hadronic composition at chemical freeze-out of the fireball, the antinuclei abundances were analyzed in terms of the same statistical description. Now applied to the clusterization of the fireball, the statistical analysis yields a fireball temperature of (135+-10) MeV and chemical potential of (5+-10) MeV at kinetic freeze-out. In the same way as the hadronization, the clusterization process is phase-space dominated and clusters are born into a state of maximum entropy. The large sample of observed antihelium-3 allowed for the first time in heavy-ion physics to calculate a differential multiplicity and invariant cross section as a function of transverse momentum. As expected, the collective transverse flow in the fireball flattens the shape of the transverse momentum spectrum and leads to the high inverse slope parameter of (950+-140) MeV of the antihelium-3 spectrum. With the extracted mean transverse momentum of antihelium-3, the collective flow velocity in transverse direction could be estimated. As the average thermal velocity is small compared to the mean collective flow velocity for heavy particles, the mean transverse momentum of antihelium-3 by itself constrains the flow velocity. Here, a simple ideal-gas approximation was fitted to the distribution of the mean transverse momentum as a function of particle mass and provided direct access to the kinetic freeze-out temperature and the flow velocity. A concept, which is complementary to the combined analysis of momentum spectra and two-particle HBT correlation methods commonly used to extract these parameters, and a cross check for the statistical analysis. The upper limit for the transverse collective flow velocity from the antihelium-3 measurement alone is v flow <= (0.68+-0.06)c, whereas the ideal-gas approximation yields a temperature of (130+-40) MeV and v flow = (0.46+-0.08)c. The results indicate, that the kinetic freeze-out conditions at SPS and RHIC are very similar, except for a smaller baryon chemical potential at RHIC. The simultaneous inclusive measurement of antiprotons allowed to study the cluster production in terms of the coalescence picture. With the large momentum coverage of the antihelium-3 momentum spectrum, the coalescence parameter could be calculated as a function of transverse momentum. Due to the difference between antiproton and antihelium-3 inverse slopes, increases with increasing transverse momentum - again a direct consequence of collective transverse flow. Both B2 and B3 follow the common behavior of decreasing coalescence parameters as a function of collision energy. According to the simple thermodynamic coalescence model, this indicates an increasing freeze-out volume for higher energies and is confirmed by the interpretation of the coalescence parameters in the framework of Scheibl and Heinz. Their model includes a dynamically expanding source in a quantum mechanical description of the coalescence process and expresses the coalescence parameter as a function of the homogeneity volume V hom accessible also in two-particle HBT correlation analyzes. The values for the antideuteron and antihelium-3 results agree well with the homogeneity volume from pion-pion correlations, but do not seem to follow the same transverse mass dependence. A comparison with proton-proton correlations may clarify this point and provide an important cross check for this analysis. Compared to SPS the homogeneity volume increases nearly by a factor of two. The analysis of the antinuclei emission at RHIC allowed to study the kinetic freeze-out of the created fireball. The results show, that the temperature and mean transverse velocity in the expanding system does not change significantly, when the collision energy increases by one order of magnitude. Only the source volume, i.e. the homogeneity volume, increases. That leaves open questions for the theoreticians to the details of the system evolution from the initial hot and dense phase - the initial energy density is a factor of two to three higher at RHIC than at SPS - to the final kinetic freeze-out with similar conditions. At the same time, the results are important constraints for the theoretical descriptions. The successful implementation of the Level-3 trigger system in STAR opens the door for the measurement of very rare signals. Indeed, in the coalescence physics perspective, the first observations of anti-alpha 4 He nuclei and antihypertritons 3/Delta H will come within the reach of STAR, in addition to a high statistics sample of antihelium-3.
At the outset of this dissertation one might pose the question why retroflex consonants should still be of interest for phonetics and for phonological theory since ample work on this segmental class already exists. Bhat (1973) conducted a quite extensive study on retroflexion that treated the geographical spread of this class, some phonological processes its members can undergo, and the phonetic motivation for these processes. Furthermore, several phonological representations of retroflexes have been proposed in the framework of Feature Geometry, as in work by Sagey (1986), Pulleyblank (1989), Gnanadesikan (1993), and Clements (2001). Most recently, Steriade (1995, 2001) has discussed the perceptual cues of retroflexes and has argued that the distribution of these cues can account for the phonotactic restrictions on retroflexes and their assimilatory behaviour. Purely phonetically oriented studies such as Dixit (1990) and Simonsen, Moen & Cowen (2000) have shown the large articulatory variation that can be found for retroflexes and hint at the insufficiency of existing definitions.
Glide formation, a process whereby an underlying high front vowel is realized as a palatal glide, is shown to occur only in unstressed prevocalic position in German, and to be blocked by specific surface restrictions such as *ji and *“j. Traditional descriptions of glide formation (including derivational as well as Optimality theoretic approaches) refer to the syllable in order to capture its conditions. The present study illustrates that glide formation (plus the distribution of long and short tense /i/) in German can better be captured in a Functional Phonology account (Boersma 1998) which makes reference to stress instead of the syllable and thus overcomes problems of former approaches.
A common topic in recent literature on phonology is the question of whether phonological processes and segments are licensed by prosodic position or by perceptual cues. The former is the traditional view, as represented by e.g. Lombardi (1995) and Beckman (1998), and holds that segments occur in specific prosodic positions such as the coda. In a licensing by cue approach, as represented by Steriade (1995, 1999), on the other hand, segments are assumed to occur in those positions only where their perceptual cues are prominent, independent of the prosodic position. In positions where the cues are not salient, neutralization occurs.
In this article I reanalyze sibilant inventories of Slavic languages by taking into consideration acoustic, perceptive and phonological evidence. The main goal of this study is to show that perception is an important factor which determines the shape of sibilant inventories. The improvement of perceptual contrast essentially contributes to creating new sibilant inventories by (i) changing the place of articulation of the existing phonemes (ii) merging sibilants that are perceptually very close or (iii) deleting them. It has also been shown that the symbol š traditionally used in Slavic linguistics corresponds to two sounds in the IPA systemsystem: it stands for a postalveolar sibilant (ʃ) in some Slavic languages, as e.g. Bulgarian, Czech, Slovak, some Serbian and Croatian dialects, whereas in others like Polish, Russian, Lower Sorbian it functions as a retroflex (s). This discrepancy is motivated by the fact that ʃ is not optimal in terms of maintaining sufficient perceptual contrast to other sibilants such as s and ç. If ʃ occurs together with s and sj there is a considerable perceptual distance between them but if it occurs with ç in an inventory, the distance is much smaller. Therefore, the strategy most languages follow is the change from a postalveolar to a retroflex sibilant.
In this article we propose that there are two universal properties for phonological stop assibilations, namely (i) assibilations cannot be triggered by /i/ unless they are also triggered by /j/, and (ii) voiced stops cannot undergo assibilations unless voiceless ones do. The article presents typological evidence from assibilations in 45 languages supporting both (i) and (ii). It is argued that assibilations are to be captured in the Optimality Theoretic framework by ranking markedness constraints grounded in perception which penalize sequences like [ti] ahead of a faith constraint which militates against the change from /t/ to some sibilant sound. The occurring language types predicted by (i) and (ii) will be shown to involve permutations of the rankings between several different markedness constraints and the one faith constraint. The article demonstrates that there exist several logically possible assibilation types which are ruled out because they would involve illicit rankings.
In this paper we provide an account of the historical development of Polish and Russian sibilants. The arguments provided here are of theoretical interest because they show that (i) certain allophonic rules are driven by the need to keep contrasts perceptually distinct, (ii) (unconditioned) sound changes result from needs of perceptual distinctiveness, and (iii) perceptual distinctiveness can be extended to a dass of consonants, i.e. the sibilants. The analysis is cast within Dispersion Theory by providing phonetic and typological data supporting the perceptual distinctiveness claims we make.
The large majority of the isoglosses which can be established in the South Slavic dialectal area date from the time of the disintegration of Common Slavic and from more recent periods (e.g., Ivi´c 1958: 25ff). The isoglosses have often shifted in the course of the centuries, so that their original position cannot always be determined. In this study I shall concentrate upon the dialectal differences which originated before the 10th century. At that time, Slavic was still a largely uniform language, though it was certainly not completely homogeneous.