论文标题

$ k^+k^ - $ $ $对在有效的质量区域接近$ 2M_K $

Investigation of $K^+K^-$ pairs in the effective mass region near $2m_K$

论文作者

Adeva, B., Afanasyev, L., Anania, A., Aogaki, S., Benelli, A., Brekhovskikh, V., Cechak, T., Chiba, M., Chliapnikov, P., Drijard, D., Dudarev, A., Dumitriu, D., Federicova, P., Gorin, A., Gritsay, K., Guaraldo, C., Gugiu, M., Hansroul, M., Hons, Z., Horikawa, S., Iwashita, Y., Karpukhin, V., Kluson, J., Kobayashi, M., Kruglova, L., Kulikov, A., Kulish, E., Lamberto, A., Lanaro, A., Lednicky, R., Mariñas, C., Martincik, J., Nemenov, L., Nikitin, M., Okada, K., Olchevskii, V., Pentia, M., Penzo, A., Plo, M., Prusa, P., Rappazzo, G., Vidal, A. Romero, Ryazantsev, A., Rykalin, V., Saborido, J., Schacher, J., Sidorov, A., Smolik, J., Takeutchi, F., Trojek, T., Trusov, S., Urban, T., Vrba, T., Yazkov, V., Yoshimura, Y., Zrelov, P.

论文摘要

CERN的DIRAC实验在反应$ \ rm {p}(24〜 \ rm {gev}/c)+ ni $中,粒子对$ k^+ k^ - ,π^+π^ - $ and $ p \ bar {p \ bar {p} $,配对系统中的相对动量$ q $少于100 mev/c/c。由于背景影响研究,Dirac探索了三个子样本的$ K^+K^ - $对,通过减去 - 使用飞行时间(TOF)技术获得 - 来自初始$ Q $分布的背景,其$ k^+k^ - $样本分数超过70 \%,50 \%和30 \%。首先在库仑模型中对相应的对分布及其纵向投影$ q_l $进行了分析,该模型仅考虑了库仑最终状态互动(FSI),并假定类似点样对生产。此库仑模型分析导致$ k^+k^ - $ $ $ q_l = 0.5 $ meV/c的产量增加了大约四个,而100 meV/c。为了研究强烈互动的贡献,考虑了第二个更复杂的模型,考虑到库仑FSI除了谐振$ f_0(980)$和$ a_0(980)$以及可变距离$ r^*$之间的colomb fsi外,也有生产的$ r^*$。该分析基于配对生产的三个不同参数集。对于70 \%的子样本和最佳参数,$ 3680 \ pm 370 $ $ k^+k^ - $ $ pairs被发现与$ 3900 \ pm 410 $ $ $ k^+k^ - $通过COULOMB模型提取。知道TOF削减对背景抑制的效率,评估检测到的$ k^+k^ - $对的总数约为$ 40000 \ pm 10 \%$,这与30 \%subsample的结果一致。 50 \%子样本中的$ k^+k^ - $ $对数与其他两个值的不同,大约三个标准偏差,证实了本子样本中的实验数据的可靠性较低。

The DIRAC experiment at CERN investigated in the reaction $\rm{p}(24~\rm{GeV}/c) + Ni$ the particle pairs $K^+K^-, π^+ π^-$ and $p \bar{p}$ with relative momentum $Q$ in the pair system less than 100 MeV/c. Because of background influence studies, DIRAC explored three subsamples of $K^+K^-$ pairs, obtained by subtracting -- using time-of-flight (TOF) technique -- background from initial $Q$ distributions with $K^+K^-$ sample fractions more than 70\%, 50\% and 30\%. The corresponding pair distributions in $Q$ and in its longitudinal projection $Q_L$ were analyzed first in a Coulomb model, which takes into account only Coulomb final state interaction (FSI) and assuming point-like pair production. This Coulomb model analysis leads to a $K^+K^-$ yield increase of about four at $Q_L=0.5$ MeV/c compared to 100 MeV/c. In order to study contributions from strong interaction, a second more sophisticated model was applied, considering besides Coulomb FSI also strong FSI via the resonances $f_0(980)$ and $a_0(980)$ and a variable distance $r^*$ between the produced $K$ mesons. This analysis was based on three different parameter sets for the pair production. For the 70\% subsample and with best parameters, $3680\pm 370$ $K^+K^-$ pairs was found to be compared to $3900\pm 410$ $K^+K^-$ extracted by means of the Coulomb model. Knowing the efficiency of the TOF cut for background suppression, the total number of detected $K^+K^-$ pairs was evaluated to be around $40000\pm 10\%$, which agrees with the result from the 30\% subsample. The $K^+K^-$ pair number in the 50\% subsample differs from the two other values by about three standard deviations, confirming -- as discussed in the paper -- that experimental data in this subsample is less reliable.

扫码加入交流群

加入微信交流群

微信交流群二维码

扫码加入学术交流群,获取更多资源