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# Physics # High Energy Physics - Experiment

Light and Charmed Mesons in High-Energy Collisions

A deep look at meson production in energetic particle collisions.

Belle Collaboration, R. Seidl, I. Adachi, H. Aihara, T. Aushev, R. Ayad, Sw. Banerjee, K. Belous, J. Bennett, M. Bessner, B. Bhuyan, D. Biswas, D. Bodrov, M. Bračko, P. Branchini, T. E. Browder, A. Budano, M. Campajola, K. Chilikin, K. Cho, S. -K. Choi, Y. Choi, S. Choudhury, S. Das, G. De Nardo, G. De Pietro, F. Di Capua, J. Dingfelder, Z. Doležal, T. V. Dong, D. Dossett, P. Ecker, T. Ferber, B. G. Fulsom, V. Gaur, A. Giri, P. Goldenzweig, E. Graziani, Y. Guan, K. Gudkova, C. Hadjivasiliou, T. Hara, H. Hayashii, D. Herrmann, W. -S. Hou, C. -L. Hsu, K. Inami, N. Ipsita, A. Ishikawa, R. Itoh, M. Iwasaki, W. W. Jacobs, S. Jia, Y. Jin, K. K. Joo, A. B. Kaliyar, C. Kiesling, C. H. Kim, D. Y. Kim, K. -H. Kim, P. Kodyš, A. Korobov, S. Korpar, P. Križan, P. Krokovny, D. Kumar, K. Kumara, Y. -J. Kwon, T. Lam, L. K. Li, Y. B. Li, L. Li Gioi, J. Libby, D. Liventsev, Y. Ma, M. Masuda, T. Matsuda, D. Matvienko, M. Merola, K. Miyabayashi, R. Mussa, M. Nakao, A. Natochii, M. Niiyama, S. Nishida, S. Ogawa, H. Ono, G. Pakhlova, S. Pardi, J. Park, S. -H. Park, A. Passeri, S. Patra, S. Paul, T. K. Pedlar, R. Pestotnik, L. E. Piilonen, T. Podobnik, E. Prencipe, M. T. Prim, G. Russo, S. Sandilya, L. Santelj, V. Savinov, G. Schnell, C. Schwanda, Y. Seino, K. Senyo, M. E. Sevior, W. Shan, J. -G. Shiu, B. Shwartz, J. B. Singh, E. Solovieva, M. Starič, M. Sumihama, M. Takizawa, K. Tanida, F. Tenchini, T. Uglov, Y. Unno, S. Uno, Y. Usov, C. Van Hulse, A. Vinokurova, A. Vossen, M. -Z. Wang, B. D. Yabsley, W. Yan, Y. Yook, C. Z. Yuan, L. Yuan, Z. P. Zhang, V. Zhilich

― 6 min read


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Table of Contents

Let’s dive into the thrilling world of particle physics, where tiny particles play a big role! Today, we’ll talk about the production of light and charmed Mesons during some energetic collisions, where particles meet, greet, and, well, annihilate each other. We’re focusing on a specific energy level: 10.58 GeV. Yes, that’s right, GeV, which stands for giga-electronvolts. It’s a lot of energy compacted into very tiny particles!

What are Mesons Anyway?

Before we go too far, let’s chat about mesons. Imagine mesons as squishy little blobs made up of quarks (those are even tinier particles) and held together by strong forces. They come in two flavors: light (which are pretty common) and charmed (which are a bit special). Light mesons are like your everyday snack, while charmed mesons are the gourmet versions you enjoy on a special occasion.

The Belle Experiment

Now, how do we measure these mesons? Enter the Belle experiment, which is like a big camera capturing all the action in an electron-positron collider. When these two particles hit each other, they create a whole zoo of other particles, including our beloved mesons. The Belle detector collects data so scientists can study how many mesons are produced during these cosmic collisions. They recorded a massive amount of data, enough to make any scientist do a little happy dance!

Measuring Cross Sections

One of the coolest things scientists do is measure "cross sections." Think of cross sections as a gauge of how likely something is to happen during a particle collision. In this case, it tells us how often light and charmed mesons pop out after the smash-up. Scientists took a close look at the momentum of the mesons, which is the fancy way of saying they studied how fast and in what direction the mesons were moving after the collisions.

Comparing Predictions

To see if their results made sense, the scientists compared their findings with predictions from a program called pythia. It’s like a digital crystal ball for particle collisions. Sometimes the predictions about how many mesons should appear were spot on, and sometimes they weren’t. They looked specifically at light mesons and charmed ones to understand better how quarks behave when they split into mesons.

The Role of Fragmentation Functions

Here’s where things get a little technical, but stay with me! Fragmentation functions are like secret recipes that explain how quarks turn into mesons. Since we can’t just calculate these functions using math alone, scientists need to gather data from real collisions to check how they work. This information is super useful for predicting the behavior of particles in various high-energy situations, like during cosmic events.

The Importance of Vector Mesons

One exciting part of this research is looking into vector mesons-the fancier cousins of regular mesons. They're somewhat heavier and often show interesting behaviors when created. With the right measurements, scientists hope to answer some big questions, like why and how particles decay in certain ways.

Cosmic Rays and Particle Production

Ever heard of cosmic rays? Picture them as space particles zooming around at high speeds. When they crash into Earth’s atmosphere, they create a shower of particles, including mesons. By understanding meson production, scientists can learn more about these cosmic showers, which can be useful in figuring out what’s happening beyond our world.

Event and Particle Selection Criteria

When scientists look at data, they have to make choices about which events and particles to include. Only the best candidates make the cut! They create strict guidelines to ensure they’re focusing on quality data. For instance, only looking at collisions that meet specific energy and momentum criteria helps reduce noise from irrelevant events.

Reconstruction and Efficiency

Once they select the particles, scientists use some clever tricks to reconstruct the events. It’s a bit like putting together pieces of a puzzle! They ensure everything fits together, checking their work for accuracy. They also calculate how efficiently they can detect these particles, which is crucial for making sure their measurements are reliable.

Initial-state Radiation (ISR) Corrections

Ah, the pesky ISR! This happens when energy is taken away from the particles during their initial interactions. It can skew results if not properly accounted for, so scientists carefully adjust their measurements to compensate for this.

Systematic Tests and Consistency

Before they declare their findings as gospel, scientists do a little detective work. They compare the results from different angles and check if they’re consistent across various conditions. This helps them identify any lingering uncertainties and refine their conclusions.

Displaying the Results

Finally, once all the data is in and the numbers are crunched, it’s time to show off the results. They create graphs displaying the production cross sections of different mesons and how they vary with momentum. It’s like a visual feast for other scientists-and let’s face it, who doesn’t love a good graph?

A Peek at the Data

The data from this study reveal interesting patterns in how often light and charmed mesons are produced at 10.58 GeV. The findings will help scientists improve their understanding of meson production and the underlying physics of particle collisions.

Why Does This Matter?

You might wonder, "Why should I care about tiny particles crashing together?" Well, the behavior of these mesons can tell us so much about the forces that hold our universe together. Understanding particle interactions at this level helps us explore the mysteries of the cosmos, from the building blocks of matter to the evolution of the universe itself. Plus, it’s pretty cool to think about how we’re all made of these tiny building blocks!

Conclusion

So, there you have it, folks! A whirlwind tour through the world of light and charmed mesons, the Belle experiment, and the exciting journey to measure particle production in high-energy collisions. Who knew the tiny world of particle physics could be such an engaging and amusing topic? As scientists continue their work, we can only expect more fascinating discoveries in the future. And who knows, maybe one day you’ll be telling your friends about the time you learned about mesons and cosmic collisions!

Original Source

Title: Production cross sections of light and charmed mesons in $e^+e^-$ annihilation near 10.58 GeV

Abstract: We report measurements of production cross sections for $\rho^+$, $\rho^0$, $\omega$, $K^{*+}$, $K^{*0}$, $\phi$, $\eta$, $K_S^0$, $f_0(980)$, $D^+$, $D^0$, $D_s^+$, $D^{*+}$, $D^{*0}$, and $D^{*+}_s$ in $e^+e^-$ collisions at a center-of-mass energy near 10.58 GeV. The data were recorded by the Belle experiment, consisting of 571 fb$^{-1}$ at 10.58 GeV and 74 fb$^{-1}$ at 10.52 GeV. Production cross sections are extracted as a function of the fractional hadron momentum $x_p$ . The measurements are compared to {\sc pythia} Monte Carlo generator predictions with various fragmentation settings, including those that have increased fragmentation into vector mesons over pseudo-scalar mesons. The cross sections measured for light hadrons are consistent with no additional increase of vector over pseudo-scalar mesons. The charmed-meson cross sections are compared to earlier measurements -- when available -- including older Belle results, which they supersede. They are in agreement before application of an improved initial-state radiation correction procedure that causes slight changes in their \xp shapes.

Authors: Belle Collaboration, R. Seidl, I. Adachi, H. Aihara, T. Aushev, R. Ayad, Sw. Banerjee, K. Belous, J. Bennett, M. Bessner, B. Bhuyan, D. Biswas, D. Bodrov, M. Bračko, P. Branchini, T. E. Browder, A. Budano, M. Campajola, K. Chilikin, K. Cho, S. -K. Choi, Y. Choi, S. Choudhury, S. Das, G. De Nardo, G. De Pietro, F. Di Capua, J. Dingfelder, Z. Doležal, T. V. Dong, D. Dossett, P. Ecker, T. Ferber, B. G. Fulsom, V. Gaur, A. Giri, P. Goldenzweig, E. Graziani, Y. Guan, K. Gudkova, C. Hadjivasiliou, T. Hara, H. Hayashii, D. Herrmann, W. -S. Hou, C. -L. Hsu, K. Inami, N. Ipsita, A. Ishikawa, R. Itoh, M. Iwasaki, W. W. Jacobs, S. Jia, Y. Jin, K. K. Joo, A. B. Kaliyar, C. Kiesling, C. H. Kim, D. Y. Kim, K. -H. Kim, P. Kodyš, A. Korobov, S. Korpar, P. Križan, P. Krokovny, D. Kumar, K. Kumara, Y. -J. Kwon, T. Lam, L. K. Li, Y. B. Li, L. Li Gioi, J. Libby, D. Liventsev, Y. Ma, M. Masuda, T. Matsuda, D. Matvienko, M. Merola, K. Miyabayashi, R. Mussa, M. Nakao, A. Natochii, M. Niiyama, S. Nishida, S. Ogawa, H. Ono, G. Pakhlova, S. Pardi, J. Park, S. -H. Park, A. Passeri, S. Patra, S. Paul, T. K. Pedlar, R. Pestotnik, L. E. Piilonen, T. Podobnik, E. Prencipe, M. T. Prim, G. Russo, S. Sandilya, L. Santelj, V. Savinov, G. Schnell, C. Schwanda, Y. Seino, K. Senyo, M. E. Sevior, W. Shan, J. -G. Shiu, B. Shwartz, J. B. Singh, E. Solovieva, M. Starič, M. Sumihama, M. Takizawa, K. Tanida, F. Tenchini, T. Uglov, Y. Unno, S. Uno, Y. Usov, C. Van Hulse, A. Vinokurova, A. Vossen, M. -Z. Wang, B. D. Yabsley, W. Yan, Y. Yook, C. Z. Yuan, L. Yuan, Z. P. Zhang, V. Zhilich

Last Update: 2024-11-18 00:00:00

Language: English

Source URL: https://arxiv.org/abs/2411.12216

Source PDF: https://arxiv.org/pdf/2411.12216

Licence: https://creativecommons.org/licenses/by/4.0/

Changes: This summary was created with assistance from AI and may have inaccuracies. For accurate information, please refer to the original source documents linked here.

Thank you to arxiv for use of its open access interoperability.

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