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1.
Using the 180 liter ITEP liquid xenon bubble chamber the time distribution of 22 Ko → 3πo decays has been studied. For the ratio ηooo of amplitudes KS → 3πo and KL → 3πo decays we found Reηooo = ?0.04 ± 0.45 and Imηooo = 0.45 ± 0.650.50. Assuming CPT invariance we obtained |ηooo|2 < 1.2 and Γ(KS → 3πo)/ Γ(KS) ? 4.3 × 10?4 at 90% confidence level.  相似文献   

2.
Results are presented on two-particle inclusive production inK + p interactions at 32 GeV/c. We study thex 1,2=x 1+x 2 dependence of invariant structure functions of (ππ)-pairs and compare them to single particle inclusive distributions in the fragmentation regions. Distributions of particles observed at Feynmanx 2 in association with various “trigger” particles or systems atx 1 in the same hemisphere are dicussed in terms of the reduced variable \(\tilde x_2 = x_2 /(1 - |x_1 |)\) . We further present absolute production rates and production ratios of π+'s and π?'s associated with π±,K s 0 , Λ, \(\bar \Lambda \) ,K *+ (890), (K s 0 π+), and (π+ π?)-triggers, and compare them with qualitative predictions of the quark recombination model. Forwardbackward correlations between (K s 0 π±), (K s 0 ,p), (Λ, π?), \((\bar \Lambda \pi ^ \pm )\) , and (p, π?) pairs are also discussed.  相似文献   

3.
Using data obtained from an exposure of the Fermilab 30-inch hydrogen bubble chamber to a 205 GeVc proton beam, we have studied K0π± correlations and the inclusive production of K1(890). Based on an analysis of the KS0π± effective mass distribution, we find a 95% confidence level upper limit of 0.22 K(890) per inelastic event. Possible systematic effects in the experimental determination of the ?0 production rate due to the Kπ correlation are discussed. Our result for K1 production at √s = 19.7 GeV is incompatible with that obtained in a recent ISR experiment at √s = 53 GeV.  相似文献   

4.
Valence quark annihilation with subsequent recombination is considered as the dominant nonscaling process contributing to lowp pion production in the proton fragmentation region at medium energies. With the aid of a Kuti-Weisskopf model for quark distribution functions the inclusive ratios π+? have been calculated and compared to data forHp→π± +anything withH±,K ?, \(\bar p\) . Each of these beam particles carries valence antiquarks. The dependence of the ratios on the Feynman variablex and their energy dependence is well reproduced.  相似文献   

5.
The reactions γp → K+ Σ± π? were studied with the SAPHIR detector using a tagged photon beam at the electron stretcher facility ELSA in Bonn. The decays Σ ? ? and Σ + +, 0 were fully reconstructed. Reaction cross-sections were measured as a function of the photon energy from threshold up to 2.6 GeV with considerably improved statistics compared to a previous bubble chamber measurement. The cross-sections rise monotonically with increasing photon energy. The two-particle mass distributions of Σ ± π ? and K + π ? show substantial production of resonant states.  相似文献   

6.
A search for the charmed baryon, Λc+, has been carried out in inclusively, measured Λ0π±π+π? and K?π±p final states with longitudinal x > 0.75 in an experiment at the CERN intersecting storage rings. An effect with invariant mass near 2.3 GeV is observed in Λ0π+π+π? with cross section times branching ratio = (2.8±1.0) μb; similar effect is observed in K?π+p with = (2.3 ± 0.3) μb. The effect is seen only in the positive charge state, in agreement with an interpretation as Λc+. However, it is pointed out that in the same experiment, the non-charmed hyperon state Σ(1385)+ also has a cross section much larger than its corresponding negative charge state Σ(1385)?.  相似文献   

7.
A precision measurement of the K S mean lifetime has been performed by comparing, in the same experimental setup, the distributions of two-pion decays of neutral kaons produced by high energy proton-beryllium interactions in two targets at a relative distance variable between 112 and 160 m. The value obtained combining the results from π+π? and π0π0 decays is τs = (0.8971 ± 0.0021) 10?10 s.  相似文献   

8.
Antiproton-proton annihilation at rest in a gaseous H2 target at NTP into the final state π+ π? K ± π? (K 0) with an undetectedK 0 or \(\bar K^0 \) has been investigated. We observe theE(1420) resonance in the invariant mass spectrum (K 0)miss K ± π? with massM E =1413±8 MeV/c2 and widthГ E =62 ± 16MeV/c2 and find evidence for the production of thef 1(1285). The absolute branching ratio of \(\bar p\) p → π+ π? E 0,E 0K 0 L K ± π ? at (61±6)%P wave annihilation is (3.0±0.9)·10?4 of all annihilations. The observed suppression of theE production fromP wave with respect to theS wave together with some simple selection rules suggest that the quantum numbers of theE(1420) areJ pc=0?+ and not I++.  相似文献   

9.
We have observed a radiative transition from the ψ to a state decaying into KSK±π?, with mass M = 1.44?0.015+0.01 GeV/c2 and width Γ = 0.05?0.02+0.03 GeV/c2. We tentatively identify this state as the E(1420). Assuming that this state is an isospin singlet, we have determined the branching fraction product B(ψ → γE) × B(E × KKπ) = (3.6 ± 1.4) × 10?3.  相似文献   

10.
We present single inclusive π±, π0 andK ± spectra in the forward fragmentation region (x>0.2,p T <1.5 GeV/c) as well as correlations between two charged particles. The data were recorded in an unseparated negative hadron beam at the CERN SPS using a large acceptance forward spectrometer. Our maasurements are compared in detail with several models which emphasise the role of the beam valence quarks in this production process. The connection to measurements at largep T is also investigated.  相似文献   

11.
In an experiment carried out in the CERN SPS hyperon beam, the diffractive dissociation of incidentΞ ? hyperons into ΛK ? andΞ ?π+π? final states has been observed. Several resonances are seen in the final states, including the well known Ξ(1820) which appears in both channels, and the Ξ(1680) which appears as a narrow state (M=1691.1±2.7 MeV/c2, Γ<8 MeV/c2) in the ΛK? channel and possibly also in the Ξππ channel.  相似文献   

12.
The joint production of ? mesons andπ ±,π 0,p, \(\bar p\) ,K s 0 andK ± is investigated using a sample of 600,000 inclusive ? meson events obtained in hadron Be interactions with incidentπ ±,p, \(\bar p\) andK ± beams. Evidence is presented for the joint production of ? mesons and strange particles produced with non-strange incident beams. With incidentK ± beam the number of additional strange particles is suppressed. The results are found to be in agreement with the qualitative predictions of a parton fusion model. The comparison with the Lund model for lowp T processes is fair.  相似文献   

13.
From a study of 70 000 K° decays in the CERN 2m hydrogen bubble chamber, we have estimated the rate for KS0π+π?γ for different cuts in the γ momentum. The results are in good agreement with inner bremsstrahlung on KS0π+π?. For γ momentum in the K° c.m. greater than 50 MeV/c, we obtain the branching ratio: Γ(KSπ+π?γ, k>50 MeV/c)/Γ(KSπ+π?)=(2.8. ± 0.6)×10?3. This leads to an estimate for the direct γ emission process: Γ(KSπ+π?γ direct)/Γ(KSπ+π?)=(0.3 ± 0.6) × 10?3.  相似文献   

14.
The possibility of obtaining information about the reaction γn → πon in the Δ resonance region from the reaction γd → πonp is analyzed. To this aim, the differential cross sections d3σ/dEnπn both for unpolarized particles and in case of polarized photons and deuterons as well as the asymmetry Σ for linearly-polarized photons are calculated at photon energies from 250 to 400 MeV in the diagrammatic approach. The contributions from the pole diagrams as well as one-loop diagrams both with n-p and π-N-rescattering are taken into account. The main contribution to the differential cross sections of πo photoproduction on the neutron in the quasi-free kinematics arises from the neutron pole diagram. The correction due to n-p rescattering decreases with increasing pion angle and becomes to be less than 8% at Θπ ≥ 90°. The contributions of the proton pole diagram and the one of π -N rescattering were found to be negligible. Background effects are more pronounced in the case of the asymmetry Σ. However, they are also strongly suppressed in the neutron quasi-free kinematics at photon energies above 300 MeV.  相似文献   

15.
The NA 32 experiment at the CERN SPS has collected 38 million hadronic interactions with incident 200 GeV/c π?,K ? andp beam. Using a segmented silicon active target and a telescope of high resolution silicon microstrip counters we have selected fully reconstructedD 0K ?π+,D 0K ?π+π+π?,D +K ?π+π+,D s + K ? K +π+π+ and charge conjugate decays. The integrated cross-sections forD o,D + D *+ andD s + meson production and the dependence of the cross-section on longitudinal and transverse momentum of theD are presented.  相似文献   

16.
A high-statistics study of the π0π0-system produced in the π- p→π0π0 n reaction at 38GeV/c has been carried out at the IHEP accelerator using the GAMS-2000 multiphoton spectrometer. A partial-wave analysis which includesS, D 0, D? andD + waves has been performed in the |t|-range up to 1 (GeV/c)2. TheS */f 0(980) resonance is seen as a dip in theS-wave amplitude at small |t|. A distinct peak with a mass of 997±5MeV and a width of 48±10MeV is observed in theS-wave at |t|>0.3 (GeV/c)2. The production cross sections are measured.  相似文献   

17.
In a sample of diffractive events of high multiplicity a sharp five standard deviation signal is observed at M = 2255 MeV/c2 in the K?+ mass distribution and, although with less statistical strength, at the same mass in the Λ0π+π+π? channel. These signals are identified as being due to the decay of the charmed baryon Λ+c which is produced with a cross section times branching ratio σcB in the range 0.7?1.8 μb for the K?π+p decay and 0.3?0.7 μb for the Λ-π+π+ π? system.  相似文献   

18.
We have analyzed theK 1 0 K ± π? system in the reactions π+/pp→π+/p(K 1 0 K ± π?)p. A spin-parity analysis of theK 1 0 K ± π? system in the “4C” channel confirms the existence of the 1++ E meson which decays mainly throughK * \(\bar K\) . The data allow the presence of a 0?+ wave at a level of 14% of theE/ι signal. The production ofD andE mesons in the channels where theK 1 0 K ± π? system is produced along with a π0 or π+π? system is suppressed.  相似文献   

19.
Q-meson production is studied in the hypercharge exchange reaction π- p → (Kππ)Λ at 3.95 GeV/c by selecting events witht-Kππ)>1.2GeV2. An enhancement with a mass of 1294±10 MeV and a width of 66±15 MeV is observed in the (Kππ) mass distribution. A spin-parity analysis of the (Kππ) decay Dalitz plot shows the enhancement to be in theJ P=1+ S(K?) wave and is therefore attributed toQ 1-meson production. No evidence is found for the decayQ 1K 0ω but limited statistics allow only placing an upper limit of 30% for the decay ratioKω/K?0. TheQ 1 production cross section fort-Kππ)>1.2GeV2 is 8±1.3 μb. No evidence is found for the process π- pQ 2Λ withQ 2K *π for which the partial wave analysis gives an upper cross section limit of 2.5 μb at the 95% confidence level.  相似文献   

20.
In a experiment at the CERN SPS charged hyperon beam using incident Ξ?, we have obtained evidence for the production of two Ω* resonances decaying into Ξ?π+ K ?, with the following parameters:M 1=2251±12,Γ 1=48±20 MeV/c2, 78 ±23 events, andM 2=2284±12,Γ 2=26±23 MeV/c2 45±10 events. The first state is also observed as a 4.2σ effect in a subsample which contains an additionalK + orK 0 in the final state. Production cross sections and branching ratios to Ξ* K ? and Ξ? K * are presented.  相似文献   

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