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		<title>Odderon</title>
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		<summary type="html">&lt;p&gt;83.185.36.2: &lt;/p&gt;
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&lt;div&gt;{{Infobox particle&lt;br /&gt;
| name = Odderon&lt;br /&gt;
| image = &lt;br /&gt;
| caption = &lt;br /&gt;
| num_types = &lt;br /&gt;
| composition = Odd number of gluons&lt;br /&gt;
| statistics = &lt;br /&gt;
| group = [[Hadron]]s&lt;br /&gt;
| interaction = [[Strong interaction|Strong]]&lt;br /&gt;
| antiparticle = Self&lt;br /&gt;
| status = &lt;br /&gt;
| theorized = [[Basarab Nicolescu]] and Leszek Łukaszuk (October 1973)&amp;lt;ref name=&amp;quot;Łukaszuk &amp;amp; Nicolescu 1973&amp;quot;&amp;gt;{{cite journal |last1=Łukaszuk |first1=L. |last2=Nicolescu |first2=B. |title=A possible interpretation of pp rising total cross-sections |journal=Lettere al Nuovo Cimento |date=1 October 1973 |volume=8 |issue=7 |pages=405–413 |doi=10.1007/BF02824484 |s2cid=122981407 }}&amp;lt;/ref&amp;gt;&lt;br /&gt;
| discovered = [[Tamás Csörgő]], Tamás Novák, Roman Pasechnik, András Ster and István Szanyi&amp;lt;br&amp;gt;&lt;br /&gt;
[[DØ experiment|DØ]] and [[TOTEM experiment|TOTEM]] Collaborations&amp;lt;ref name=&amp;quot;Abazov Abbott Acharya et al 2021&amp;quot; /&amp;gt;&lt;br /&gt;
| symbol = O&lt;br /&gt;
| mass = &lt;br /&gt;
| mean_lifetime = &lt;br /&gt;
| decay_particle = &lt;br /&gt;
| electric_charge = &lt;br /&gt;
| spin = &lt;br /&gt;
| strangeness = &lt;br /&gt;
| charm = &lt;br /&gt;
| isospin = &lt;br /&gt;
| hypercharge = &lt;br /&gt;
| parity = &lt;br /&gt;
}}&lt;br /&gt;
In [[particle physics]], the &#039;&#039;&#039;odderon&#039;&#039;&#039; corresponds to an elusive family of odd-gluon states, dominated by a three-gluon state. When [[proton]]s collide elastically with other protons or with anti-protons at high energies, [[gluon]]s are exchanged. Exchanging an even number of [[gluon]]s is a crossing-even part of [[Elastic collision|elastic]] proton–proton and proton–antiproton [[scattering]], while odderon exchange (i.e. exchange of odd number of gluons) corresponds to a [[Crossing (physics)|crossing]]-odd term in the elastic [[scattering amplitude]]. In turn, the odderon&#039;s crossing-odd counterpart is the [[pomeron]].{{Clarify|date=June 2024|reason=What does &amp;quot;counterpart&amp;quot; mean here, exactly?}}&lt;br /&gt;
&lt;br /&gt;
It took about 48 years to find a definite signal of odderon exchange.&amp;lt;ref name=&amp;quot;Abazov Abbott Acharya et al 2021&amp;quot;/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Description ==&lt;br /&gt;
In [[elastic collision]]s, the total kinetic energy of the system is conserved. Thus the identity of the scattered particles is not modified, no [[excited state]]s and/or new particles are produced. The [[kinematics]] of these [[collision]]s is governed by the [[Conservation of energy|conservation]] of both [[energy]] and [[momentum]].&lt;br /&gt;
&lt;br /&gt;
Data on high-energy elastic proton–proton collisions provided by the [[TOTEM experiment|TOTEM]] Collaboration in a [[Electronvolt|teraelectronvolt]] energy range, together with data from the [[DØ experiment]] on elastic proton–antiproton collisions at the [[Tevatron]] collider were key ingredients in the discovery of the odderon-exchange. The observed characteristics of the proton–proton collisions did not match the characteristics of the proton–antiproton collisions. As a result, there is an interaction-mediating family of particles ([[Regge theory|Regge trajectory]]) that can result in such a [[Deviation (statistics)|deviation]] in the range of [[strong interaction]]s.&lt;br /&gt;
&lt;br /&gt;
== Discovery ==&lt;br /&gt;
The first paper on the [[Theory|theoretical]] [[prediction]] of possible odderon exchange was [[Publishing|published]] in 1973 by [[Basarab Nicolescu]] and [[Leszek Łukaszuk]].&amp;lt;ref name=&amp;quot;Łukaszuk &amp;amp; Nicolescu 1973&amp;quot;/&amp;gt; The odderon name was coined in 1975 in a paper from the same group (Joynson, D.; Leader, E.; Nicolescu, B. and Lopez, C.)&amp;lt;ref&amp;gt;{{cite journal |last1=Joynson |first1=D. |last2=Leader |first2=E. |last3=Nicolescu |first3=B. |last4=Lopez |first4=C. |title=Non-regge and hyper-regge effects in pion–nucleon charge exchange scattering at high energies |journal=Il Nuovo Cimento A |date=1 December 1975 |volume=30 |issue=3 |pages=345–384 |doi=10.1007/BF02730293 |bibcode=1975NCimA..30..345J |s2cid=124183973 }}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In December 2020, the DØ and TOTEM Collaborations made public their CERN and Fermilab approved preprint&amp;lt;ref name=&amp;quot;Abazov Abbott Acharya et al 2021&amp;quot; /&amp;gt; later published in Physical Review Letters in August 2021.&amp;lt;ref name=&amp;quot;Abazov Abbott Acharya et al 2021&amp;quot; /&amp;gt; The DØ and TOTEM extrapolated TOTEM proton–proton data in the region of the diffractive minimum and maximum from 13, 8, 7 and 2.76&amp;amp;nbsp;TeV to 1.96&amp;amp;nbsp;TeV and compared this to DØ proton–antiproton measurement at 1.96&amp;amp;nbsp;TeV in the same t-range finding an odderon significance of 3.4&amp;amp;nbsp;&#039;&#039;σ&#039;&#039;. TOTEM observed an independent odderon signal at low four-momentum transfers at 13&amp;amp;nbsp;TeV. When a partial combination of the TOTEM ρ and total cross section measurements is done at 13&amp;amp;nbsp;TeV, the combined significance ranges between 3.4 and 4.6&amp;amp;nbsp;&#039;&#039;σ&#039;&#039;  for the different models. Combining this with the 3.4&amp;amp;nbsp;&#039;&#039;σ&#039;&#039; effect on the extrapolated proton–proton differential cross-sections resulted in an at least 5.2&amp;amp;nbsp;&#039;&#039;σ&#039;&#039; statistical significance. This is the first statistically significant observation of odderon exchange effects by experimental collaborations.&amp;lt;ref name=&amp;quot;Abazov Abbott Acharya et al 2021&amp;quot; /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
A Hungarian-Swedish scaling [[analysis]] introduced a new scaling function and [[observed]], model dependently, that in a limited [[energy]] range, that includes the DØ energy of 1.96&amp;amp;nbsp;TeV and the TOTEM energies of 2.76 and 7&amp;amp;nbsp;TeV, the elastic proton–proton [[collision]]s are within the experimental uncertainties independent of the energy of the collision.&amp;lt;ref name=&amp;quot;arxiv.org&amp;quot;&amp;gt;Csörgő, T.; Novák, T.; Pasechnik, R.; Ster, A.; Szanyi, I. (23 February 2021). &amp;quot;Evidence of Odderon-exchange from scaling properties of elastic scattering at TeV energies&amp;quot;. The European Physical Journal C. 81 (2): 180 https://arxiv.org/abs/1912.11968. Bibcode:2021EPJC...81..180C. {{doi|10.1140/epjc/s10052-021-08867-6}} S2CID 209500465.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In this model dependently determined domain of validity, the Hungarian-Swedish team utilized a direct data-to-data [[comparison]] and showed that energy independent scaling function of elastic proton–proton collisions is significantly different from the scaling function of elastic proton–antiproton collisions, hence providing a statistically significant [[signal]] for the exchange of the elusive odderon. The preprint of this analysis was made public in December 2019 and its final form it was published in February 2021.&amp;lt;ref name=&amp;quot;arxiv.org&amp;quot;/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This paper has been seconded in July 2021 by a theoretical paper of [[Tamás Csörgő]], and [[István Szanyi]], increasing the statistical significance of odderon [[observation]] to at least 7.08&amp;amp;nbsp;&#039;&#039;σ&#039;&#039; signal.&amp;lt;ref name=&amp;quot;Csörgő, T. 2021&amp;quot;&amp;gt;Csörgő, T.; Szanyi, I. (13 July 2021). &amp;quot;Observation of Odderon effects at LHC energies: a real extended Bialas–Bzdak model study&amp;quot;. The European Physical Journal C. 81 (7): 611. arXiv:2005.14319. Bibcode:2021EPJC...81..611C. {{doi|10.1140/epjc/s10052-021-09381-5}} S2CID 219124254.&amp;lt;/ref&amp;gt; This paper utilized a previously published theoretical model, the so-called real-extended [[Bialas-Bzdak]] model, to extrapolate not only the elastic proton–proton [[scattering]] data from the [[Large Hadron Collider|LHC]] energies to the DØ energy of 1.96&amp;amp;nbsp;TeV but also to extrapolate the elastic proton–antiproton scattering data from 0.546 and 1.96&amp;amp;nbsp;TeV to the LHC energies of 2.76&amp;amp;nbsp;TeV and 7&amp;amp;nbsp;TeV. Evaluating the proton–proton data with a model increased the [[uncertainty]] and decreased the odderon signal from proton–proton scattering data alone, but this decrease was well over-compensated with the ability of the model to evaluate theoretically the proton–antiproton scattering at the LHC energies, leading to an overall increase of the statistical significance from 6.26 to 7.08&amp;amp;nbsp;&#039;&#039;σ&#039;&#039; signal.&amp;lt;ref name=&amp;quot;Csörgő, T. 2021&amp;quot;/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Chronology of articles discovering odderon exchange ==&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!Authors&lt;br /&gt;
!Submitted for publication&lt;br /&gt;
!Accepted for publication&lt;br /&gt;
!Published&lt;br /&gt;
!Article reference&lt;br /&gt;
|-&lt;br /&gt;
|Tamás Csörgő, Tamás Novák, Roman Pasechnik, András Ster, István Szanyi &lt;br /&gt;
|[[arxiv:2004.07095v1|15 Apr 2020]]&lt;br /&gt;
|[[arxiv:2004.07095v2|11 May 2020]] &lt;br /&gt;
| 16 Jun 2020&lt;br /&gt;
|[https://www.epj-conferences.org/articles/epjconf/abs/2020/11/epjconf_ismd2019_06002/epjconf_ismd2019_06002.html EPJ Web of Conferences 235, 06002 (2020)]&lt;br /&gt;
|-&lt;br /&gt;
|Tamás Csörgő, Tamás Novák, Roman Pasechnik, András Ster, István Szanyi &lt;br /&gt;
| 29 Dec 2019&lt;br /&gt;
| 12 Jan 2021&lt;br /&gt;
| 23 Feb 2021&lt;br /&gt;
|[https://link.springer.com/article/10.1140/epjc/s10052-021-08867-6 &#039;&#039;Eur. Phys. J. C&#039;&#039; &#039;&#039;&#039;81,&#039;&#039;&#039; 180 (2021)]&lt;br /&gt;
|-&lt;br /&gt;
|Tamás Csörgő and István Szanyi&lt;br /&gt;
|[https://link.springer.com/article/10.1140/epjc/s10052-021-09381-5#citeas 6 Aug 2020] &lt;br /&gt;
| 25 Jun 2021&lt;br /&gt;
| 13 Jul 2021&lt;br /&gt;
|[https://link.springer.com/article/10.1140/epjc/s10052-021-09381-5 &#039;&#039;Eur. Phys. J. C&#039;&#039; &#039;&#039;&#039;81,&#039;&#039;&#039; 611 (2021)]&lt;br /&gt;
|-&lt;br /&gt;
|D0 and TOTEM experimental collaborations&lt;br /&gt;
| 7 Dec 2020&lt;br /&gt;
| 10 Jun 2021&lt;br /&gt;
| 4 Aug 2021&lt;br /&gt;
|&#039;&#039;[https://journals.aps.org/prl/abstract/10.1103/PhysRevLett.127.062003 Phys. Rev. Lett. 127, 062003(2021)]&#039;&#039;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
* [[Glueball]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
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}}&lt;br /&gt;
&lt;br /&gt;
== Bibliography ==&lt;br /&gt;
* 1972: first proposal: Efremov, A. V.; Peschanski, R. (1972). &amp;quot;Evidence for new singularities in Regge phenomenology&amp;quot;. [[Office of Scientific and Technical Information|OSTI]] [https://www.osti.gov/biblio/4691439 4691439].&lt;br /&gt;
* 1973: first publication: Łukaszuk, L.; Nicolescu, B. (1 October 1973). &amp;quot;A possible interpretation of pp rising total cross-sections&amp;quot;. Lettere al Nuovo Cimento. 8 (7): 405–413. {{doi|10.1007/BF02824484}} S2CID 122981407.&lt;br /&gt;
* 1975: odderon named:  Joynson, D.; Leader, E.; Nicolescu, B.; Lopez, C. (1 December 1975). &amp;quot;Non-regge and hyper-regge effects in pion–nucleon charge exchange scattering at high energies&amp;quot;. Il Nuovo Cimento A. 30 (3): 345–384. Bibcode:1975NCimA..30..345J. {{doi|10.1007/BF02730293}} S2CID 124183973.&lt;br /&gt;
* 1980: odderon evolution equation from QCD: Kwieciǹski, J.; Praszałowicz, M. (11 August 1980). &amp;quot;Three gluon integral equation and odd C singlet Regge singularities in QCD&amp;quot;. Physics Letters B. 94 (3): 413–416. Bibcode:1980PhLB...94..413K. {{doi|10.1016/0370-2693(80)90909-0}}&lt;br /&gt;
* 1990: Pomeron and odderon in QCD: Lipatov, L. N. (15 November 1990). &amp;quot;Pomeron and odderon in QCD and a two dimensional conformal field theory&amp;quot;. Physics Letters B. 251 (2): 284–287. Bibcode:1990PhLB..251..284L. {{doi|10.1016/0370-2693(90)90937-2}}&lt;br /&gt;
* 1999: a new odderon intercept from QCD: Janik, R. A.; Wosiek, J. (8 February 1999). &amp;quot;A Solution of the Odderon Problem&amp;quot;. Physical Review Letters. 82(6): 1092–1095. arXiv:hep-th/9802100. Bibcode:1999PhRvL..82.1092J. {{doi|10.1103/PhysRevLett.82.1092}} S2CID 17976783.&lt;br /&gt;
* 2000: odderon from QCD with fixed coupling constant: Bartels, J.; Lipatov, L. N.; Vacca, G. P. (23 March 2000). &amp;quot;A new odderon solution in perturbative QCD&amp;quot;. Physics Letters B. 477 (1): 178–186. arXiv:hep-ph/9912423. Bibcode:2000PhLB..477..178B. {{doi|10.1016/S0370-2693(00)00221-5}} S2CID 18651924.&lt;br /&gt;
* 2003: Odderon in Quantum Chromo Dynamics: Ewerz, Carlo (17 June 2003). &amp;quot;The Odderon in Quantum Chromodynamics&amp;quot;. arXiv:hep-ph/0306137. Bibcode:2003hep.ph....6137E.&lt;br /&gt;
* 2007: Proposal to find the odderon at RHIC and at LHC: Avila, R., Gauron, P. &amp;amp; Nicolescu, B. Eur. Phys. J. C 49, 581–592 (2007).https://link.springer.com/article/10.1140/epjc/s10052-006-0074&lt;br /&gt;
* 2015: proposal to use LHC data to hunt down the odderon: Ster, András; Jenkovszky, László; Csörgő, Tamás (13 April 2015). &amp;quot;Extracting the Odderon from p p and p p scattering data&amp;quot;. Physical Review D. 91 (7): 074018. arXiv:1501.03860. {{doi|10.1103/PhysRevD.91.074018}} S2CID 118354589.&lt;br /&gt;
* 2015: Odderon in the color glass condensate: Hatta, Y.; Iancu, E.; Itakura, K.; McLerran, L. (3 October 2005). &amp;quot;Odderon in the color glass condensate&amp;quot;. Nuclear Physics A. 760 (1): 172–207. arXiv:hep-ph/0501171. Bibcode:2005NuPhA.760..172H. {{doi|10.1016/j.nuclphysa.2005.05.163}} S2CID 2880940.&lt;br /&gt;
* 2016: Measurement of elastic pp scattering at s=8s=8&amp;amp;nbsp;TeV in the Coulomb–nuclear interference region: determination of the ρρ -parameter and the total cross-section: TOTEM Collaboration; G. Antchev (Pilsen U.) et al. (Oct 3, 2016). Published in: Eur.Phys.J.C 76 (2016) 12, 661. e-Print: 1610.00603 [nucl-ex].&lt;br /&gt;
* 2017: First measurement of elastic, inelastic and total cross-section at s=13s=13&amp;amp;nbsp;TeV by TOTEM and overview of cross-section data at LHC energies: TOTEM Collaboration; G. Antchev (Sofiya, Inst. Nucl. Res.) et al. (Dec 17, 2017). Published in: Eur.Phys.J.C 79 (2019) 2, 103. e-Print: 1712.06153 [hep-ex].&lt;br /&gt;
* 2017: First determination of the ρ parameter at s=13s=13&amp;amp;nbsp;TeV: probing the existence of a colourless C-odd three-gluon compound state: TOTEM Collaboration; G. Antchev (CERN) et al. (Dec 16, 2017). Published in: Eur.Phys.J.C 79 (2019) 9, 785. e-Print: 1812.04732 [hep-ex].&lt;br /&gt;
* 2018: Elastic differential cross-section dσ/dt at s=2.76 TeVs=2.76&amp;amp;nbsp;TeV and implications on the existence of a colourless C-odd three-gluon compound state: TOTEM Collaboration, G. Antchev (Sofiya, Inst. Nucl. Res.) et al. (Dec 20, 2018). Published in: Eur.Phys.J.C 80 (2020) 2, 9. e-Print: 1812.08610 [hep-ex].&lt;br /&gt;
* 2018: Elastic differential cross-section measurement at s=13s=13&amp;amp;nbsp;TeV: TOTEM Collaboration; G. Antchev ( Sofiya, Inst. Nucl. Res.) et al. (Dec 19, 2018). Published in: Eur.Phys.J.C 79 (2019) 10, 861. e-Print: 1812.08283 [hep-ex].&lt;br /&gt;
* 2019: Odderon from real-to-imaginary ratio at zero four-momentum transfer: Martynov, E.; Tersimonov, G. (27 December 2019). &amp;quot;Ratio ρ p p p p ( s ) in Froissaron and maximal odderon approach&amp;quot;. Physical Review D. 100 (11): 114039. {{doi|10.1103/PhysRevD.100.114039}} S2CID 208139556.&lt;br /&gt;
* 2019: New physics from recent TOTEM measurements: Szanyi, István; Bence, Norbert; Jenkovszky, László (9 April 2019). &amp;quot;New physics from TOTEM&#039;s recent measurements of elastic and total cross sections&amp;quot;. Journal of Physics G: Nuclear and Particle Physics. 46 (5): 055002. arXiv:1808.03588. Bibcode:2019JPhG...46e5002S. {{doi|10.1088/1361-6471/ab1205}} S2CID 104292347.&lt;br /&gt;
* 2019: Odderon and proton-substructure from a model-independent Levy expansion: Csörgő, T.; Pasechnik, R.; Ster, A. (28 January 2019). &amp;quot;Odderon and proton substructure from a model-independent Lévy imaging of elastic pp and pp collisions&amp;quot;. The European Physical Journal C. 79 (1): 62. {{doi|10.1140/epjc/s10052-019-6588-8}} PMC 6349816. PMID 30774536.&lt;br /&gt;
* 2019: Odderon effects from the differential cross-sections at TeV energies: Martynov, Evgenij; Nicolescu, Basarab (June 2019). &amp;quot;Odderon effects in the differential cross-sections at Tevatron and LHC energies&amp;quot;. The European Physical Journal C. 79 (6): 461. arXiv:1808.08580. Bibcode:2019EPJC...79..461M. {{doi|10.1140/epjc/s10052-019-6954-6}} S2CID 119393479.&lt;br /&gt;
* 2020: Proposal to search for odderon in central exclusive production at LHC: Lebiedowicz, Piotr; Nachtmann, Otto; Szczurek, Antoni (13 May 2020). &amp;quot;Searching for the odderon in p p → p p K + K − and p p → p p μ + μ − reactions in the Φ ( 1020 ) resonance region at the LHC&amp;quot;. Physical Review D. 101(9): 094012. {{doi|10.1103/PhysRevD.101.094012}} S2CID 207870047.&lt;br /&gt;
* 2020: Odderon from QCD with running coupling constant: Bartels, Jochen; Contreras, Carlos; Vacca, Gian Paolo (28 April 2020). &amp;quot;The Odderon in QCD with running coupling&amp;quot;. Journal of High Energy Physics. 2020 (4): 183. arXiv:1910.04588. Bibcode:2020JHEP...04..183B. {{doi|10.1007/JHEP04(2020)183}} S2CID 204008416.&lt;br /&gt;
* 2021: &amp;quot;Odderon Exchange from Elastic Scattering Differences between pp and pp¯ Data at 1.96&amp;amp;nbsp;TeV and from pp Forward Scattering Measurements.&amp;quot; TOTEM and DØ Collaborations • V.M. Abazov( Dubna, JINR ) et al. (4 August 2021). Published in:  Phys.Rev.Lett. 127 (2021) 6, 062003 • e-Print:  2012.03981 [hep-ex]&lt;br /&gt;
* 2021: Csörgő, T.; Novák, T.; Pasechnik, R.; Ster, A.; Szanyi, I. (23 February 2021). &amp;quot;Evidence of Odderon-exchange from scaling properties of elastic scattering at TeV energies&amp;quot;. The European Physical Journal C. 81 (2): 180 https://arxiv.org/abs/1912.11968. Bibcode:2021EPJC...81..180C. {{doi|10.1140/epjc/s10052-021-08867-6}} S2CID&lt;br /&gt;
&lt;br /&gt;
== External links ==&lt;br /&gt;
* Presentations at the 50th International Symposium on Multiparticle Dynamics:&lt;br /&gt;
** [https://indico.cern.ch/event/848680/contributions/4430297/attachments/2282695/3879781/Thursday-ChristopheRoyon.mp4 The Odderon discovery by the DØ and TOTEM collaborations], by [[Christophe Royon]] (15 July 2021).&lt;br /&gt;
** [https://indico.cern.ch/event/848680/contributions/4430734/attachments/2282841/3879785/Thursday-TamasCsorgo.mp4 Optimizing the Signal of Odderon], by Tamás Csörgő (15 July 2021).&lt;br /&gt;
* [https://youtube.com/watch?v=yHBO3zcB3V4 Discovery of the Odderon: from Theory to the Experimental Results by TOTEM/D0], by Yuri Kovchegov (28 April 2021) at CTEQ Webinar.&lt;br /&gt;
* [https://medium.com/@georgina.zsori/an-odd-interview-about-the-odderon-4bd080402518 An odd interview about the odderon], article by Georgina Anna Zsóri, interviewing Tamás Csörgő (February 2022).&lt;br /&gt;
* [https://medium.com/@georgina.zsori/interview-with-the-research-group-that-discovered-odderon-2c02adbb7852 Interview with the research group that discovered the odderon], article by Georgina Anna Zsóri, interviewing Tamás Csörgő, Tamás Novák, András Ster, István Szanyi and Roman Pasechnik (February 2022).&lt;br /&gt;
* [https://archive.gyongyos.uni-mate.hu/en/odd-discovery-odderon Odd Discovery of the Odderon]. [[Hungarian University of Agriculture and Life Sciences]] press release by Dovicsin-Péntek Csilla, Cseri-Gódor Kitti (8 March 2021).&lt;br /&gt;
* [https://cerncourier.com/a/odderon-discovered/ Odderon discovered]. CERN press release by Matthew Chalmers (ed.) (9 March 2021).&lt;br /&gt;
&lt;br /&gt;
[[Category:Bosons]]&lt;br /&gt;
[[Category:Gluons]]&lt;br /&gt;
[[Category:Hadrons]]&lt;br /&gt;
[[Category:2019 in science]]&lt;br /&gt;
[[Category:Hungarian inventions]]&lt;/div&gt;</summary>
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