Strange and Non-Strange Particle Production in Proton—Proton Reactions at an Incident Momentum of 19 Gev/C Uno Svedin

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Strange and Non-Strange Particle Production in Proton—Proton Reactions at an Incident Momentum of 19 Gev/C Uno Svedin Strange and Non-Strange Particle Production in Proton—Proton Reactions at an Incident Momentum of 19 GeV/c Uno Svedin Stockholm 1974 Strange and Non-Strange Particle Production in Proton—Proton Reactions at an Incident Momentum of 19 GeV/c Uno Svedin Stockholm 1974 ISBN <i\ 7222 000-6 Sim.li Olfvei Stockholm 74 CONTENTS 1. The scope of this thesis 7 2. Introduction 11 3. Earlier studi^B of proton-proton reactions 17 4. Experimental procedures 18 5. Resume's of publications belonging to this thesis 21 0. Discussion on some physical items related to our investigations 31 6.1 Integrated cross sections 31 6.2 Average multiplicities 34 6.3 The charge multiplicity distribution 39 6.4 Scaling properties of momentum spectra 47 7. Summary 53 8. Acknowledgement 56 9. References 58 Tables List of figures Figures- 1. THE SCOPE OF THIS THESIS The present thesis is based on studies done within the framework of the Scandi- navian Bubble Chamber Collaboration during the years 1966-1974 and concerns different aspects of proton-proton reactions at an incident beam momentum of 19 GeV/c. The presentation is divided into three different parts I. Studies of final states involving non-strange particles. II. Studies of final states involving strange particles. III. Development of equipment. The main emphasis is on the presentation of atrange particle production results (Section II of papers). The results have not been discussed in the form of a thesis before. The sample from which the results are drawn is one of the largest presented up to this day for proton-proton reactions. In the discussion on the production of strange particles we make frequent use of the non-strange final state results. As many aspects of high energy physics do not show their significance except in a study over a wide range of initial energies, We will in the discussion (after a short introduction, a survey on the experimental procedure and resume's of the included papers), frequently make use of data from other ejqperiments, at other energies, of compilations earlier presented by,different.physisists,, (often using our data in part) and of model discussions by various 'authors. The main aim is to explain how our data and conclusions have fitted into the pattern of existing high energy physics results. In order to perform any experimental work, developments of & technical nature must take place. In Paper 111:1 the development of an on line system for measuring bubble chamber pictures is described. A part of the strange particle sample has been measured using this system. Paper 111:1 was earlier included in S-O. Holmgrens thesis [l]. Work to improve the quality of the sample is described in Paper 11:3. Publications included in this thesis are 1:1 H. Bjzfggild, E. Dahl-Jensen, K.H. Hanseji, H. Johnstad, E. Lohse, R. Mbllerud, M. Suk, L. Veje, V.J. Karimaki, K.V. Laurikainen, E. Riipinen, T. Jacobsen, S.O. Sjirensen, J, Allan, G. Blomqvist, O. Danielsson, G. Ekspong, L. Granstrom, S.O. Holmgren, S. Nilsson, B. Ronne, U. Svedin and N.K. Yamdagni: "Some features of particle multiplicities and momentum spectra in inelastic proton-proton colli- sions at 19 GeV/c."Nucl. Phys. B27, 285 (1971). II. II. 1 K. Alpgard, T. Buran, H. B^ggild, A.G. Frodesen, V.M. Haginan, K.H. Hansen, J.E. Hooper, P.O. Hulth, H. Johnstad, M. Korkea-Aho, K. Marquit, R. Moller, U. Svedin, II. Tttfte, P. Villanen and N. Yam- uatiiii: "The inclusive single-partible spectra of ff~, K and A in prolon-proton collisions at 19 GcV/c." Nucl. Phys. B57.. 77-99 (1973). II.2 K. Alpgdrd, G. Ekspong, A-G. Frodesen, V.M. Hagman, P.O. Hulih, V. Kp.rimi.ilci. A. Krogstad, L1. Svedin, P. Villanen and N.K. Yamdagni: "Strange particle cross sections in 19 GeV/c proton-proton interactions and their interpretation in the KNO framework." USIP-Rsport. 74-24 November 1974. 11:3 K. Alpg&rd, P.O. Hulth. U. Svedin and N.K. Yamdagni: Measurements of strange particle production cross sections in proton-proton reactions at 19 GeV/c incident momentum. USIP-Report 74-25, November 1S74. 11:4 The Scandinavian Bubble Chamber Collaboration and the K Coliabora- 4- tion: Factorization in the inclusive reactions pp -• A +Xand K p - A+ X. USIP-Report 74-26, November 1974. Hi. 111:1 G. Blomqvist, S.O. Holmgren, P.O. Hulth and U. Svedin: A hardware system for measurements of bubble chamber films on-line. USIP-Report 70-03, June 1970. 11 2. INTRODUCTION A dominant feature of hadron collisions above a few hundred MeV/c incident momentum (17-threshold) is the creation of new particles. In proton-proton reactions at 19 GeV/c, such creations occur in « 75 % of all reactions. Fig. 1 shows this inelastic part as well as the total cross sections as a func- tion of the incident laboratory momentum for proton-proton re. 3tions. We observe that a large fraction of the total cross section involves the creation of new particles over a wide range of incident momenta. The produced particles could be of several types: ft , K , K , p, p, +-0 I , A, etc. There are certain restrictions on the production of these par- ticles in the form of conservation laws, as the conservation of charge, energy, baryon number etc. The earliest identification of an event of what we now call strange particles was reported by L, Le Prince-Kinguet in 1944 [2]. It was discovered in a cloud chamber exposed to cosmic rays. The mass of the particle was found to be 2 500 ± 50 MeV/c . Such a particle is called a K-meson today. In 1947 Rochester and Butler [3] , found two cases of "forked" (or V-like) tracks in a cloud cham- ber . One of them was interpreted as the decay of a new type of uncharged elementary particle decaying into two lighter charged ones. The mass was estimated to be of the order of 1000 electron masses. Today we know there are two types of V°-particIes called A and K°. After extensive work in many labora- tories this was definitely established by R.W. Thompson et al. [4]. Whereas the strange particles were produced copiously (a 1 %..of the ff-meson _HQ . production), they had lifetimes > 10 sec. From the production cross section it 12 was derived that the matrix element, e.g. for A production, should be of the order of one-third of that of the Yukawa interaction. Thus assuming the same mechanism which produces the V-particles also to be instrumental in their decay, —22 12 one would estimate lifetimes of the order of 10" seconds, a number of 10 smaller than the experimental one. Due to this puzzle the particles were called "strange". Pais [5] solved this difficulty by suggesting that the production of strange par- ticles occurs in pairs only. The decay and production processes thus involve different particles and cannot be simply related. Experiments in 1953 , including the first artificial production of K's at the new cosmotron at Brookhaven [6], established that the production of V s(K or A) occurs in pairs only - "associated production" [7]. This whole subject was systematized in 1953 by Gell Mann [8] and almost simul- taneously by Nakano and Nishijima [9]. They introduced a new additive quantum number, later called strangeness [10], which was postulated to be conserved in strong interactions. Particles given strangeness quantum number not equal to zero were accordingly called "strange particles". Strict conservation of "strange- ness" in strong interactions corresponds to "associated production" of V-particles. A strangeness breaking decay is not possible via strong interaction. Such a decay is however possible via weak interactions, thus giving the long life times observed. In the presently accepted classification scheme for elementary particles, based on group theoretical considerations (SU_) (introduced by Y. Ne'emanand M. Gell-Mann), the strangeness number is one of the Important classification *- properties for particles. 13 During the last years more and more interest has been shown in questions on the general dynamics of reactions (questions of duality, Regge and Pomeron ex- changes, scaling, etc.). Studies of the behaviour of strange particle3 have con- tributed to the understanding of high energy phenomena. The present thesis deals with the production of strange particles produced in proton-proton interactions at an incident momentum of 19 GeV/c. It also com- pares the production of strange particles with the production of non-strange particles also produced in 19 GeV/c pp-reactions. The experiment was performed using the CERN Proton Synchrotron (PS) giving beam momenta up to *» 28 GeV/c. In order to get a fair amount of strange particlb events we collected at the Bubble Chamber exposures (described be- low) around ra500 000 pictures. After the new generation of high energy proton accelerators came into opera- tion (at Serpukov, USSR, pT ._ up to 70 GeV/c, at NAL, Batavia, USA, p_ up to fa 400 GeV/c, at CERN ISR up to a corresponding incident momentum of« 1500 GeV/c), a set of experiments studying strange and non-strange production in proton-proton reactions have been performed. Many of these experiments have studied a small sample of pictures (a few tens,of thousands) giving large .'•-.. statistical errors. The restricted number of pictures is however somewhat compensated, what the strange purtiole production concerns, by the increasing . cross sections. ' • •'.'••' :'••'••'•'•.'". '"\: '• •••'_••, ..;:' •'.. • ' • • • • 1 ' - •'**•.• A reaction ; • A •F13Jfch.+:ch; + .";r.ch' •••+--N-VN- Vi.-. N-' .1 z • n. i .4 m 14 (A is the beam and B is the target particle, Ch .
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