Axial resonances a$$_{1}$$(1260), b$$_{1}$$(1235) and their decays from the lattice
Abstract
The light axial-vector resonances $$a_1(1260)$$ and $$b_1(1235)$$ are explored in Nf=2 lattice QCD by simulating the corresponding scattering channels $$\rho\pi$$ and $$\omega\pi$$. Interpolating fields $$\bar{q} q$$ and $$\rho\pi$$ or $$\omega\pi$$ are used to extract the s-wave phase shifts for the first time. The $$\rho$$ and $$\omega$$ are treated as stable and we argue that this is justified in the considered energy range and for our parameters $$m_\pi\simeq 266~$$MeV and $$L\simeq 2~$$fm. We neglect other channels that would be open when using physical masses in continuum. Assuming a resonance interpretation a Breit-Wigner fit to the phase shift gives the $$a_1(1260)$$ resonance mass $$m_{a1}^{res}=1.435(53)(^{+0}_{-109})$$ GeV compared to $$m_{a1}^{exp}=1.230(40)$$ GeV. The $$a_1$$ width $$\Gamma_{a1}(s)=g^2 p/s$$ is parametrized in terms of the coupling and we obtain $$g_{a_1\rho\pi}=1.71(39)$$ GeV compared to $$g_{a_1\rho\pi}^{exp}=1.35(30)$$ GeV derived from $$\Gamma_{a1}^{exp}=425(175)$$ MeV. In the $$b_1$$ channel, we find energy levels related to $$\pi(0)\omega(0)$$ and $$b_1(1235)$$, and the lowest level is found at $$E_1 \gtrsim m_\omega+m_\pi$$ but is within uncertainty also compatible with an attractive interaction. Lastly, assuming the coupling $$g_{b_1\omega\pi}$$ extracted from the experimental width we estimate $$m_{b_1}^{res}=1.414(36)(^{+0}_{-83})$$.
- Authors:
-
- Univ. of Graz, Graz (Austria)
- Jozef Stefan Institute, Ljubljana (Slovenia)
- Fermi National Accelerator Lab. (FNAL), Batavia, IL (United States)
- Jozef Stefan Institute, Ljubljana (Slovenia); Univ. of Ljubljana, Ljubljana (Slovenia)
- Publication Date:
- Research Org.:
- Fermi National Accelerator Lab. (FNAL), Batavia, IL (United States)
- Sponsoring Org.:
- USDOE Office of Science (SC), High Energy Physics (HEP)
- OSTI Identifier:
- 1128720
- Report Number(s):
- FERMILAB-PUB-14-002-T
Journal ID: ISSN 1029-8479; arXiv eprint number arXiv:1401.2088
- Grant/Contract Number:
- AC02-07CH11359
- Resource Type:
- Accepted Manuscript
- Journal Name:
- Journal of High Energy Physics (Online)
- Additional Journal Information:
- Journal Name: Journal of High Energy Physics (Online); Journal Volume: 2014; Journal Issue: 4; Journal ID: ISSN 1029-8479
- Publisher:
- Springer Berlin
- Country of Publication:
- United States
- Language:
- English
- Subject:
- 72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS; lattice QCD; QCD
Citation Formats
Lang, C. B., Leskovec, Luka, Mohler, Daniel, and Prelovsek, Sasa. Axial resonances a$_{1}$(1260), b$_{1}$(1235) and their decays from the lattice. United States: N. p., 2014.
Web. doi:10.1007/JHEP04(2014)162.
Lang, C. B., Leskovec, Luka, Mohler, Daniel, & Prelovsek, Sasa. Axial resonances a$_{1}$(1260), b$_{1}$(1235) and their decays from the lattice. United States. https://doi.org/10.1007/JHEP04(2014)162
Lang, C. B., Leskovec, Luka, Mohler, Daniel, and Prelovsek, Sasa. Mon .
"Axial resonances a$_{1}$(1260), b$_{1}$(1235) and their decays from the lattice". United States. https://doi.org/10.1007/JHEP04(2014)162. https://www.osti.gov/servlets/purl/1128720.
@article{osti_1128720,
title = {Axial resonances a$_{1}$(1260), b$_{1}$(1235) and their decays from the lattice},
author = {Lang, C. B. and Leskovec, Luka and Mohler, Daniel and Prelovsek, Sasa},
abstractNote = {The light axial-vector resonances $a_1(1260)$ and $b_1(1235)$ are explored in Nf=2 lattice QCD by simulating the corresponding scattering channels $\rho\pi$ and $\omega\pi$. Interpolating fields $\bar{q} q$ and $\rho\pi$ or $\omega\pi$ are used to extract the s-wave phase shifts for the first time. The $\rho$ and $\omega$ are treated as stable and we argue that this is justified in the considered energy range and for our parameters $m_\pi\simeq 266~$MeV and $L\simeq 2~$fm. We neglect other channels that would be open when using physical masses in continuum. Assuming a resonance interpretation a Breit-Wigner fit to the phase shift gives the $a_1(1260)$ resonance mass $m_{a1}^{res}=1.435(53)(^{+0}_{-109})$ GeV compared to $m_{a1}^{exp}=1.230(40)$ GeV. The $a_1$ width $\Gamma_{a1}(s)=g^2 p/s$ is parametrized in terms of the coupling and we obtain $g_{a_1\rho\pi}=1.71(39)$ GeV compared to $g_{a_1\rho\pi}^{exp}=1.35(30)$ GeV derived from $\Gamma_{a1}^{exp}=425(175)$ MeV. In the $b_1$ channel, we find energy levels related to $\pi(0)\omega(0)$ and $b_1(1235)$, and the lowest level is found at $E_1 \gtrsim m_\omega+m_\pi$ but is within uncertainty also compatible with an attractive interaction. Lastly, assuming the coupling $g_{b_1\omega\pi}$ extracted from the experimental width we estimate $m_{b_1}^{res}=1.414(36)(^{+0}_{-83})$.},
doi = {10.1007/JHEP04(2014)162},
journal = {Journal of High Energy Physics (Online)},
number = 4,
volume = 2014,
place = {United States},
year = {Mon Apr 28 00:00:00 EDT 2014},
month = {Mon Apr 28 00:00:00 EDT 2014}
}
Web of Science
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