Journal article 838 views
Light hadron spectrum and decay constants in quenched lattice QCD
R.D. Kenway,
B.J. Pendleton,
Christopher T. Sachrajda,
D.G. Richards,
K.C. Bowler,
S.P. Booth,
D.S. Henty,
J.N. Simone
,
A.D. Simpson,
R.M. Baxter,
L. Lellouch,
H. Wittig,
C. McNeile,
Chris Allton
Physical Review D, Volume: 49, Issue: 1, Pages: 474 - 485
Swansea University Author:
Chris Allton
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DOI (Published version): 10.1103/PhysRevD.49.474
Abstract
We present results for light hadrons composed of both degenerate and non-degenerate quarks in quenched lattice QCD. We calculate masses and decay constants using 60 gauge configurations with an $O(a)$--improved fermion action at $\beta = 6.2$. Using the $\rho$ mass to set the scale, we find hadron m...
Published in: | Physical Review D |
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ISSN: | 0556-2821 |
Published: |
1994
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URI: | https://cronfa.swan.ac.uk/Record/cronfa28429 |
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<?xml version="1.0"?><rfc1807><datestamp>2016-08-08T12:43:55.7519472</datestamp><bib-version>v2</bib-version><id>28429</id><entry>2016-06-02</entry><title>Light hadron spectrum and decay constants in quenched lattice QCD</title><swanseaauthors><author><sid>de706a260fa1e1e47430693e135f41c7</sid><ORCID>0000-0003-0795-124X</ORCID><firstname>Chris</firstname><surname>Allton</surname><name>Chris Allton</name><active>true</active><ethesisStudent>false</ethesisStudent></author></swanseaauthors><date>2016-06-02</date><deptcode>SPH</deptcode><abstract>We present results for light hadrons composed of both degenerate and non-degenerate quarks in quenched lattice QCD. We calculate masses and decay constants using 60 gauge configurations with an $O(a)$--improved fermion action at $\beta = 6.2$. Using the $\rho$ mass to set the scale, we find hadron masses within two to three standard deviations of the experimental values (given in parentheses): $m_{K^*}=868\er{9}{8}$~MeV (892~MeV), $m_{\phi}=970\err{20}{10}$~MeV (1020~MeV), $m_N=820\err{90}{60}$~MeV (938~MeV), $m_\Delta=1300\errr{100}{100}$~MeV (1232~MeV) and $m_\Omega=1650\err{70}{50}$~MeV (1672~MeV). Direct comparison with experiment for decay constants is obscured by uncertainty in current renormalisations. However, for ratios of decay constants we obtain $f_K/f_\pi=1.20\er{3}{2}$ (1.22) and $f_\phi/f_\rho=1.13\er{2}{3}$ (1.22).</abstract><type>Journal Article</type><journal>Physical Review D</journal><volume>49</volume><journalNumber>1</journalNumber><paginationStart>474</paginationStart><paginationEnd>485</paginationEnd><publisher/><issnPrint>0556-2821</issnPrint><keywords/><publishedDay>31</publishedDay><publishedMonth>12</publishedMonth><publishedYear>1994</publishedYear><publishedDate>1994-12-31</publishedDate><doi>10.1103/PhysRevD.49.474</doi><url>http://inspirehep.net/record/358010</url><notes/><college>COLLEGE NANME</college><department>Physics</department><CollegeCode>COLLEGE CODE</CollegeCode><DepartmentCode>SPH</DepartmentCode><institution>Swansea University</institution><apcterm/><lastEdited>2016-08-08T12:43:55.7519472</lastEdited><Created>2016-06-02T15:05:46.9503418</Created><path><level id="1">Faculty of Science and Engineering</level><level id="2">School of Biosciences, Geography and Physics - Physics</level></path><authors><author><firstname>R.D.</firstname><surname>Kenway</surname><order>1</order></author><author><firstname>B.J.</firstname><surname>Pendleton</surname><order>2</order></author><author><firstname>Christopher T.</firstname><surname>Sachrajda</surname><order>3</order></author><author><firstname>D.G.</firstname><surname>Richards</surname><order>4</order></author><author><firstname>K.C.</firstname><surname>Bowler</surname><order>5</order></author><author><firstname>S.P.</firstname><surname>Booth</surname><order>6</order></author><author><firstname>D.S.</firstname><surname>Henty</surname><order>7</order></author><author><firstname>J.N.</firstname><surname>Simone</surname><orcid>0000-0001-8515-3337</orcid><order>8</order></author><author><firstname>A.D.</firstname><surname>Simpson</surname><order>9</order></author><author><firstname>R.M.</firstname><surname>Baxter</surname><order>10</order></author><author><firstname>L.</firstname><surname>Lellouch</surname><order>11</order></author><author><firstname>H.</firstname><surname>Wittig</surname><order>12</order></author><author><firstname>C.</firstname><surname>McNeile</surname><order>13</order></author><author><firstname>Chris</firstname><surname>Allton</surname><orcid>0000-0003-0795-124X</orcid><order>14</order></author></authors><documents/><OutputDurs/></rfc1807> |
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2016-08-08T12:43:55.7519472 v2 28429 2016-06-02 Light hadron spectrum and decay constants in quenched lattice QCD de706a260fa1e1e47430693e135f41c7 0000-0003-0795-124X Chris Allton Chris Allton true false 2016-06-02 SPH We present results for light hadrons composed of both degenerate and non-degenerate quarks in quenched lattice QCD. We calculate masses and decay constants using 60 gauge configurations with an $O(a)$--improved fermion action at $\beta = 6.2$. Using the $\rho$ mass to set the scale, we find hadron masses within two to three standard deviations of the experimental values (given in parentheses): $m_{K^*}=868\er{9}{8}$~MeV (892~MeV), $m_{\phi}=970\err{20}{10}$~MeV (1020~MeV), $m_N=820\err{90}{60}$~MeV (938~MeV), $m_\Delta=1300\errr{100}{100}$~MeV (1232~MeV) and $m_\Omega=1650\err{70}{50}$~MeV (1672~MeV). Direct comparison with experiment for decay constants is obscured by uncertainty in current renormalisations. However, for ratios of decay constants we obtain $f_K/f_\pi=1.20\er{3}{2}$ (1.22) and $f_\phi/f_\rho=1.13\er{2}{3}$ (1.22). Journal Article Physical Review D 49 1 474 485 0556-2821 31 12 1994 1994-12-31 10.1103/PhysRevD.49.474 http://inspirehep.net/record/358010 COLLEGE NANME Physics COLLEGE CODE SPH Swansea University 2016-08-08T12:43:55.7519472 2016-06-02T15:05:46.9503418 Faculty of Science and Engineering School of Biosciences, Geography and Physics - Physics R.D. Kenway 1 B.J. Pendleton 2 Christopher T. Sachrajda 3 D.G. Richards 4 K.C. Bowler 5 S.P. Booth 6 D.S. Henty 7 J.N. Simone 0000-0001-8515-3337 8 A.D. Simpson 9 R.M. Baxter 10 L. Lellouch 11 H. Wittig 12 C. McNeile 13 Chris Allton 0000-0003-0795-124X 14 |
title |
Light hadron spectrum and decay constants in quenched lattice QCD |
spellingShingle |
Light hadron spectrum and decay constants in quenched lattice QCD Chris Allton |
title_short |
Light hadron spectrum and decay constants in quenched lattice QCD |
title_full |
Light hadron spectrum and decay constants in quenched lattice QCD |
title_fullStr |
Light hadron spectrum and decay constants in quenched lattice QCD |
title_full_unstemmed |
Light hadron spectrum and decay constants in quenched lattice QCD |
title_sort |
Light hadron spectrum and decay constants in quenched lattice QCD |
author_id_str_mv |
de706a260fa1e1e47430693e135f41c7 |
author_id_fullname_str_mv |
de706a260fa1e1e47430693e135f41c7_***_Chris Allton |
author |
Chris Allton |
author2 |
R.D. Kenway B.J. Pendleton Christopher T. Sachrajda D.G. Richards K.C. Bowler S.P. Booth D.S. Henty J.N. Simone A.D. Simpson R.M. Baxter L. Lellouch H. Wittig C. McNeile Chris Allton |
format |
Journal article |
container_title |
Physical Review D |
container_volume |
49 |
container_issue |
1 |
container_start_page |
474 |
publishDate |
1994 |
institution |
Swansea University |
issn |
0556-2821 |
doi_str_mv |
10.1103/PhysRevD.49.474 |
college_str |
Faculty of Science and Engineering |
hierarchytype |
|
hierarchy_top_id |
facultyofscienceandengineering |
hierarchy_top_title |
Faculty of Science and Engineering |
hierarchy_parent_id |
facultyofscienceandengineering |
hierarchy_parent_title |
Faculty of Science and Engineering |
department_str |
School of Biosciences, Geography and Physics - Physics{{{_:::_}}}Faculty of Science and Engineering{{{_:::_}}}School of Biosciences, Geography and Physics - Physics |
url |
http://inspirehep.net/record/358010 |
document_store_str |
0 |
active_str |
0 |
description |
We present results for light hadrons composed of both degenerate and non-degenerate quarks in quenched lattice QCD. We calculate masses and decay constants using 60 gauge configurations with an $O(a)$--improved fermion action at $\beta = 6.2$. Using the $\rho$ mass to set the scale, we find hadron masses within two to three standard deviations of the experimental values (given in parentheses): $m_{K^*}=868\er{9}{8}$~MeV (892~MeV), $m_{\phi}=970\err{20}{10}$~MeV (1020~MeV), $m_N=820\err{90}{60}$~MeV (938~MeV), $m_\Delta=1300\errr{100}{100}$~MeV (1232~MeV) and $m_\Omega=1650\err{70}{50}$~MeV (1672~MeV). Direct comparison with experiment for decay constants is obscured by uncertainty in current renormalisations. However, for ratios of decay constants we obtain $f_K/f_\pi=1.20\er{3}{2}$ (1.22) and $f_\phi/f_\rho=1.13\er{2}{3}$ (1.22). |
published_date |
1994-12-31T03:34:34Z |
_version_ |
1763751466637459456 |
score |
11.01306 |