Inclusive production cross sections of resonances in 32 GeV/c K+p interactions

Granet, P.; Mosca, L.; Saudraix, J.; Scheuer, J.C.; Vilanova, D.; Blumenfeld, H.; Henri, Victor; Kesteman, J.; Laurent, J.; Windmolders, R.; Wolf, E. de; Tavernier, S.; Verbeure, F.; Ajinenko, I.; Chliapnikov, P.; Gerdyukov, L.; Gorbunov, P.; Perevoztchikov, V.; Rybin, A. M.; Union, France-Soviet; Collaborations, CERN-Soviet Union

doi:10.1016/0550-3213(78)90002-0

Cited by 55 publications

(12 citation statements)

References 19 publications

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“…As the signal has a tail towards larger m values, the asymmetric Crystal Ball function [73] is used for the signal description. The shape of the background is parameterised with the Granet function [74]. An unbinned extended log likelihood fit [75] is performed using the RooFit framework [76].…”

Section: Event Selection and Signal Extractionmentioning

confidence: 99%

Measurement of D ∗± meson production and determination of $F_{2}^{c\bar{c}}$ at low Q 2 in deep-inelastic scattering at HERA

Aaron¹,

Alexa²,

Andreev³

et al. 2011

Eur. Phys. J. C

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Inclusive production of D * mesons in deepinelastic ep scattering at HERA is studied in the range 5 < Q 2 < 100 GeV 2 of the photon virtuality and 0.02 < y < 0.7 of the inelasticity of the scattering process. gle and double differential cross sections are measured and the charm contribution F cc 2 to the proton structure function F 2 is determined. The results are compared to perturbative QCD predictions at next-to-leading order implementing different schemes for the charm mass treatment and with Monte Carlo models based on leading order matrix elements with parton showers.

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Section: Event Selection and Signal Extractionmentioning

confidence: 99%

Measurement of D ∗± meson production and determination of $F_{2}^{c\bar{c}}$ at low Q 2 in deep-inelastic scattering at HERA

Aaron¹,

Alexa²,

Andreev³

et al. 2011

Eur. Phys. J. C

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“…Distortions of the line shape of ρ 0 have also been observed at RHIC in p + p and peripheral Au+Au collisions [12]. Dynamical interactions with the surrounding matter [7,8,13], interference between various scattering channels [14], phase-space distortions [7,8,13,[15][16][17][18][19][20], and Bose-Einstein correlations [7,8,15,[18][19][20] are possible explanations for the apparent modification of resonance properties.…”

Section: Introductionmentioning

confidence: 95%

K(892)resonance production in Au+Au andp+pcollisions at
Adams¹,
Aggarwal²,
Ahammed³
et al. 2005
Phys. Rev. C*

161

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The short-lived K(892)* resonance provides an efficient tool to probe properties of the hot and dense medium produced in relativistic heavy-ion collisions. We report measurements of K * in √ s NN = 200 GeV Au+Au and p + p collisions reconstructed via its hadronic decay channels K(892) * 0 → Kπ and K(892)using the STAR detector at the Relativistic Heavy Ion Collider at Brookhaven National Laboratory. The K * 0 mass has been studied as a function of p T in minimum bias p + p and central Au+Au collisions. The K * p T spectra for minimum bias p + p interactions and for Au+Au collisions in different centralities are presented. The K * /K yield ratios for all centralities in Au+Au collisions are found to be significantly lower than the ratio in minimum bias p + p collisions, indicating the importance of hadronic interactions between chemical and kinetic freeze-outs. A significant nonzero K * 0 elliptic flow (v 2 ) is observed in Au+Au collisions and is compared to the K 0 S and v 2 . The nuclear modification factor of K * at intermediate p T is similar to that of K 0 S but different from . This establishes a baryon-meson effect over a mass effect in the particle production at intermediate p T

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“…The right and wrong charge m distributions are fitted simultaneously by means of an unbinned extended likelihood fit using RooFit [54] and ROOT [55]. The Crystal Ball [56] and Granet [57] probability distribution functions are used for modelling the signal and background, respectively. The fit to the total sample of selected D * candidates is shown for the right and wrong charge combinations in Fig.…”

Section: * Selectionmentioning

confidence: 99%

Measurement of $${\varvec{D^{*}}}$$ D ∗ production in diffractive deep inelastic scattering at HERA

et al. 2017

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Measurements of D * (2010) meson production in diffractive deep inelastic scattering (5 < Q 2 < 100 GeV 2 ) are presented which are based on HERA data recorded at a centre-of-mass energy √ s = 319 GeV with an integrated luminosity of 287 pb −1 . The reaction ep → eXY is studied, where the system X , containing at least one D * (2010) meson, is separated from a leading low-mass proton dissociative system Y by a large rapidity gap. The kinematics of D * candidates are reconstructed in the D * → K ππ decay channel. The measured cross sections compare favourably with next-to-leading order QCD predictions, where charm quarks are produced via boson-gluon fusion. The charm quarks are then independently fragmented to the D * mesons. The cal- † Deceased a

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Inclusive production cross sections of resonances in 32 GeV/c K+p interactions

Cited by 55 publications

References 19 publications

Measurement of D ∗± meson production and determination of $F_{2}^{c\bar{c}}$ at low Q 2 in deep-inelastic scattering at HERA

Measurement of D ∗± meson production and determination of $F_{2}^{c\bar{c}}$ at low Q 2 in deep-inelastic scattering at HERA

K(892)resonance production in Au+Au andp+pcollisions at
Adams¹,
Aggarwal²,
Ahammed³
et al. 2005
Phys. Rev. C*

Measurement of $${\varvec{D^{*}}}$$ D ∗ production in diffractive deep inelastic scattering at HERA

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Inclusive production cross sections of resonances in 32 GeV/c K+p interactions

Cited by 55 publications

References 19 publications

Measurement of D ∗± meson production and determination of $F_{2}^{c\bar{c}}$ at low Q 2 in deep-inelastic scattering at HERA

Measurement of D ∗± meson production and determination of $F_{2}^{c\bar{c}}$ at low Q 2 in deep-inelastic scattering at HERA

K(892)*resonance production in Au+Au andp+pcollisions atAdams1, Aggarwal2, Ahammed3 et al. 2005Phys. Rev. C

Measurement of $${\varvec{D^{*}}}$$ D ∗ production in diffractive deep inelastic scattering at HERA

Contact Info

Product

Resources

About

K(892)resonance production in Au+Au andp+pcollisions at
Adams¹,
Aggarwal²,
Ahammed³
et al. 2005
Phys. Rev. C*