Search for magnetic monopoles with the MoEDAL forward trapping detector in 2.11 fb−1 of 13 TeV proton–proton collisions at the LHC
We update our previous search for trapped magnetic monopoles in LHC Run 2 using nearly six times more integrated luminosity and including additional models for the interpretation of the data. The MoEDAL forward trapping detector, comprising 222 kg of aluminium samples, was exposed to 2.11 fb−1 of 13...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
B. Acharya [verfasserIn] J. Alexandre [verfasserIn] S. Baines [verfasserIn] P. Benes [verfasserIn] B. Bergmann [verfasserIn] J. Bernabéu [verfasserIn] A. Bevan [verfasserIn] H. Branzas [verfasserIn] M. Campbell [verfasserIn] L. Caramete [verfasserIn] S. Cecchini [verfasserIn] M. de Montigny [verfasserIn] A. De Roeck [verfasserIn] J.R. Ellis [verfasserIn] M. Fairbairn [verfasserIn] D. Felea [verfasserIn] M. Frank [verfasserIn] D. Frekers [verfasserIn] C. Garcia [verfasserIn] J. Hays [verfasserIn] A.M. Hirt [verfasserIn] J. Janecek [verfasserIn] D.-W. Kim [verfasserIn] K. Kinoshita [verfasserIn] A. Korzenev [verfasserIn] D.H. Lacarrère [verfasserIn] S.C. Lee [verfasserIn] C. Leroy [verfasserIn] G. Levi [verfasserIn] A. Lionti [verfasserIn] J. Mamuzic [verfasserIn] A. Margiotta [verfasserIn] N. Mauri [verfasserIn] N.E. Mavromatos [verfasserIn] P. Mermod [verfasserIn] V.A. Mitsou [verfasserIn] R. Orava [verfasserIn] I. Ostrovskiy [verfasserIn] B. Parker [verfasserIn] L. Patrizii [verfasserIn] G.E. Păvălaş [verfasserIn] J.L. Pinfold [verfasserIn] V. Popa [verfasserIn] M. Pozzato [verfasserIn] S. Pospisil [verfasserIn] A. Rajantie [verfasserIn] R. Ruiz de Austri [verfasserIn] Z. Sahnoun [verfasserIn] M. Sakellariadou [verfasserIn] A. Santra [verfasserIn] S. Sarkar [verfasserIn] G. Semenoff [verfasserIn] A. Shaa [verfasserIn] G. Sirri [verfasserIn] K. Sliwa [verfasserIn] R. Soluk [verfasserIn] M. Spurio [verfasserIn] Y.N. Srivastava [verfasserIn] M. Suk [verfasserIn] J. Swain [verfasserIn] M. Tenti [verfasserIn] V. Togo [verfasserIn] J.A. Tuszyński [verfasserIn] V. Vento [verfasserIn] O. Vives [verfasserIn] Z. Vykydal [verfasserIn] A. Widom [verfasserIn] G. Willems [verfasserIn] J.H. Yoon [verfasserIn] I.S. Zgura [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2018 |
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| Übergeordnetes Werk: |
In: Physics Letters B - Elsevier, 2015, 782(2018), Seite 510-516 |
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| Übergeordnetes Werk: |
volume:782 ; year:2018 ; pages:510-516 |
| Links: |
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| DOI / URN: |
10.1016/j.physletb.2018.05.069 |
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| Katalog-ID: |
DOAJ077880986 |
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| 024 | 7 | |a 10.1016/j.physletb.2018.05.069 |2 doi | |
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| 041 | |a eng | ||
| 050 | 0 | |a QC1-999 | |
| 100 | 0 | |a B. Acharya |e verfasserin |4 aut | |
| 245 | 1 | 0 | |a Search for magnetic monopoles with the MoEDAL forward trapping detector in 2.11 fb−1 of 13 TeV proton–proton collisions at the LHC |
| 264 | 1 | |c 2018 | |
| 336 | |a Text |b txt |2 rdacontent | ||
| 337 | |a Computermedien |b c |2 rdamedia | ||
| 338 | |a Online-Ressource |b cr |2 rdacarrier | ||
| 520 | |a We update our previous search for trapped magnetic monopoles in LHC Run 2 using nearly six times more integrated luminosity and including additional models for the interpretation of the data. The MoEDAL forward trapping detector, comprising 222 kg of aluminium samples, was exposed to 2.11 fb−1 of 13 TeV proton–proton collisions near the LHCb interaction point and analysed by searching for induced persistent currents after passage through a superconducting magnetometer. Magnetic charges equal to the Dirac charge or above are excluded in all samples. The results are interpreted in Drell–Yan production models for monopoles with spins 0, 1/2 and 1: in addition to standard point-like couplings, we also consider couplings with momentum-dependent form factors. The search provides the best current laboratory constraints for monopoles with magnetic charges ranging from two to five times the Dirac charge. | ||
| 653 | 0 | |a Physics | |
| 700 | 0 | |a J. Alexandre |e verfasserin |4 aut | |
| 700 | 0 | |a S. Baines |e verfasserin |4 aut | |
| 700 | 0 | |a P. Benes |e verfasserin |4 aut | |
| 700 | 0 | |a B. Bergmann |e verfasserin |4 aut | |
| 700 | 0 | |a J. Bernabéu |e verfasserin |4 aut | |
| 700 | 0 | |a A. Bevan |e verfasserin |4 aut | |
| 700 | 0 | |a H. Branzas |e verfasserin |4 aut | |
| 700 | 0 | |a M. Campbell |e verfasserin |4 aut | |
| 700 | 0 | |a L. Caramete |e verfasserin |4 aut | |
| 700 | 0 | |a S. Cecchini |e verfasserin |4 aut | |
| 700 | 0 | |a M. de Montigny |e verfasserin |4 aut | |
| 700 | 0 | |a A. De Roeck |e verfasserin |4 aut | |
| 700 | 0 | |a J.R. Ellis |e verfasserin |4 aut | |
| 700 | 0 | |a M. Fairbairn |e verfasserin |4 aut | |
| 700 | 0 | |a D. Felea |e verfasserin |4 aut | |
| 700 | 0 | |a M. Frank |e verfasserin |4 aut | |
| 700 | 0 | |a D. Frekers |e verfasserin |4 aut | |
| 700 | 0 | |a C. Garcia |e verfasserin |4 aut | |
| 700 | 0 | |a J. Hays |e verfasserin |4 aut | |
| 700 | 0 | |a A.M. Hirt |e verfasserin |4 aut | |
| 700 | 0 | |a J. Janecek |e verfasserin |4 aut | |
| 700 | 0 | |a D.-W. Kim |e verfasserin |4 aut | |
| 700 | 0 | |a K. Kinoshita |e verfasserin |4 aut | |
| 700 | 0 | |a A. Korzenev |e verfasserin |4 aut | |
| 700 | 0 | |a D.H. Lacarrère |e verfasserin |4 aut | |
| 700 | 0 | |a S.C. Lee |e verfasserin |4 aut | |
| 700 | 0 | |a C. Leroy |e verfasserin |4 aut | |
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| 700 | 0 | |a A. Lionti |e verfasserin |4 aut | |
| 700 | 0 | |a J. Mamuzic |e verfasserin |4 aut | |
| 700 | 0 | |a A. Margiotta |e verfasserin |4 aut | |
| 700 | 0 | |a N. Mauri |e verfasserin |4 aut | |
| 700 | 0 | |a N.E. Mavromatos |e verfasserin |4 aut | |
| 700 | 0 | |a P. Mermod |e verfasserin |4 aut | |
| 700 | 0 | |a V.A. Mitsou |e verfasserin |4 aut | |
| 700 | 0 | |a R. Orava |e verfasserin |4 aut | |
| 700 | 0 | |a I. Ostrovskiy |e verfasserin |4 aut | |
| 700 | 0 | |a B. Parker |e verfasserin |4 aut | |
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| 700 | 0 | |a M. Pozzato |e verfasserin |4 aut | |
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| 700 | 0 | |a R. Ruiz de Austri |e verfasserin |4 aut | |
| 700 | 0 | |a Z. Sahnoun |e verfasserin |4 aut | |
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10.1016/j.physletb.2018.05.069 doi (DE-627)DOAJ077880986 (DE-599)DOAJ59900f35be124f578b14ccedee993bba DE-627 ger DE-627 rakwb eng QC1-999 B. Acharya verfasserin aut Search for magnetic monopoles with the MoEDAL forward trapping detector in 2.11 fb−1 of 13 TeV proton–proton collisions at the LHC 2018 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We update our previous search for trapped magnetic monopoles in LHC Run 2 using nearly six times more integrated luminosity and including additional models for the interpretation of the data. The MoEDAL forward trapping detector, comprising 222 kg of aluminium samples, was exposed to 2.11 fb−1 of 13 TeV proton–proton collisions near the LHCb interaction point and analysed by searching for induced persistent currents after passage through a superconducting magnetometer. Magnetic charges equal to the Dirac charge or above are excluded in all samples. The results are interpreted in Drell–Yan production models for monopoles with spins 0, 1/2 and 1: in addition to standard point-like couplings, we also consider couplings with momentum-dependent form factors. The search provides the best current laboratory constraints for monopoles with magnetic charges ranging from two to five times the Dirac charge. Physics J. Alexandre verfasserin aut S. Baines verfasserin aut P. Benes verfasserin aut B. Bergmann verfasserin aut J. Bernabéu verfasserin aut A. Bevan verfasserin aut H. Branzas verfasserin aut M. Campbell verfasserin aut L. Caramete verfasserin aut S. Cecchini verfasserin aut M. de Montigny verfasserin aut A. De Roeck verfasserin aut J.R. Ellis verfasserin aut M. Fairbairn verfasserin aut D. Felea verfasserin aut M. Frank verfasserin aut D. Frekers verfasserin aut C. Garcia verfasserin aut J. Hays verfasserin aut A.M. Hirt verfasserin aut J. Janecek verfasserin aut D.-W. Kim verfasserin aut K. Kinoshita verfasserin aut A. Korzenev verfasserin aut D.H. Lacarrère verfasserin aut S.C. Lee verfasserin aut C. Leroy verfasserin aut G. Levi verfasserin aut A. Lionti verfasserin aut J. Mamuzic verfasserin aut A. Margiotta verfasserin aut N. Mauri verfasserin aut N.E. Mavromatos verfasserin aut P. Mermod verfasserin aut V.A. Mitsou verfasserin aut R. Orava verfasserin aut I. Ostrovskiy verfasserin aut B. Parker verfasserin aut L. Patrizii verfasserin aut G.E. Păvălaş verfasserin aut J.L. Pinfold verfasserin aut V. Popa verfasserin aut M. Pozzato verfasserin aut S. Pospisil verfasserin aut A. Rajantie verfasserin aut R. Ruiz de Austri verfasserin aut Z. Sahnoun verfasserin aut M. Sakellariadou verfasserin aut A. Santra verfasserin aut S. Sarkar verfasserin aut G. Semenoff verfasserin aut A. Shaa verfasserin aut G. Sirri verfasserin aut K. Sliwa verfasserin aut R. Soluk verfasserin aut M. Spurio verfasserin aut Y.N. Srivastava verfasserin aut M. Suk verfasserin aut J. Swain verfasserin aut M. Tenti verfasserin aut V. Togo verfasserin aut J.A. Tuszyński verfasserin aut V. Vento verfasserin aut O. Vives verfasserin aut Z. Vykydal verfasserin aut A. Widom verfasserin aut G. Willems verfasserin aut J.H. Yoon verfasserin aut I.S. Zgura verfasserin aut In Physics Letters B Elsevier, 2015 782(2018), Seite 510-516 (DE-627)266015360 (DE-600)1466612-1 18732445 nnns volume:782 year:2018 pages:510-516 https://doi.org/10.1016/j.physletb.2018.05.069 kostenfrei https://doaj.org/article/59900f35be124f578b14ccedee993bba kostenfrei http://www.sciencedirect.com/science/article/pii/S0370269318304337 kostenfrei https://doaj.org/toc/0370-2693 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2014 GBV_ILN_2025 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2064 GBV_ILN_2111 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 782 2018 510-516 |
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10.1016/j.physletb.2018.05.069 doi (DE-627)DOAJ077880986 (DE-599)DOAJ59900f35be124f578b14ccedee993bba DE-627 ger DE-627 rakwb eng QC1-999 B. Acharya verfasserin aut Search for magnetic monopoles with the MoEDAL forward trapping detector in 2.11 fb−1 of 13 TeV proton–proton collisions at the LHC 2018 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We update our previous search for trapped magnetic monopoles in LHC Run 2 using nearly six times more integrated luminosity and including additional models for the interpretation of the data. The MoEDAL forward trapping detector, comprising 222 kg of aluminium samples, was exposed to 2.11 fb−1 of 13 TeV proton–proton collisions near the LHCb interaction point and analysed by searching for induced persistent currents after passage through a superconducting magnetometer. Magnetic charges equal to the Dirac charge or above are excluded in all samples. The results are interpreted in Drell–Yan production models for monopoles with spins 0, 1/2 and 1: in addition to standard point-like couplings, we also consider couplings with momentum-dependent form factors. The search provides the best current laboratory constraints for monopoles with magnetic charges ranging from two to five times the Dirac charge. Physics J. Alexandre verfasserin aut S. Baines verfasserin aut P. Benes verfasserin aut B. Bergmann verfasserin aut J. Bernabéu verfasserin aut A. Bevan verfasserin aut H. Branzas verfasserin aut M. Campbell verfasserin aut L. Caramete verfasserin aut S. Cecchini verfasserin aut M. de Montigny verfasserin aut A. De Roeck verfasserin aut J.R. Ellis verfasserin aut M. Fairbairn verfasserin aut D. Felea verfasserin aut M. Frank verfasserin aut D. Frekers verfasserin aut C. Garcia verfasserin aut J. Hays verfasserin aut A.M. Hirt verfasserin aut J. Janecek verfasserin aut D.-W. Kim verfasserin aut K. Kinoshita verfasserin aut A. Korzenev verfasserin aut D.H. Lacarrère verfasserin aut S.C. Lee verfasserin aut C. Leroy verfasserin aut G. Levi verfasserin aut A. Lionti verfasserin aut J. Mamuzic verfasserin aut A. Margiotta verfasserin aut N. Mauri verfasserin aut N.E. Mavromatos verfasserin aut P. Mermod verfasserin aut V.A. Mitsou verfasserin aut R. Orava verfasserin aut I. Ostrovskiy verfasserin aut B. Parker verfasserin aut L. Patrizii verfasserin aut G.E. Păvălaş verfasserin aut J.L. Pinfold verfasserin aut V. Popa verfasserin aut M. Pozzato verfasserin aut S. Pospisil verfasserin aut A. Rajantie verfasserin aut R. Ruiz de Austri verfasserin aut Z. Sahnoun verfasserin aut M. Sakellariadou verfasserin aut A. Santra verfasserin aut S. Sarkar verfasserin aut G. Semenoff verfasserin aut A. Shaa verfasserin aut G. Sirri verfasserin aut K. Sliwa verfasserin aut R. Soluk verfasserin aut M. Spurio verfasserin aut Y.N. Srivastava verfasserin aut M. Suk verfasserin aut J. Swain verfasserin aut M. Tenti verfasserin aut V. Togo verfasserin aut J.A. Tuszyński verfasserin aut V. Vento verfasserin aut O. Vives verfasserin aut Z. Vykydal verfasserin aut A. Widom verfasserin aut G. Willems verfasserin aut J.H. Yoon verfasserin aut I.S. Zgura verfasserin aut In Physics Letters B Elsevier, 2015 782(2018), Seite 510-516 (DE-627)266015360 (DE-600)1466612-1 18732445 nnns volume:782 year:2018 pages:510-516 https://doi.org/10.1016/j.physletb.2018.05.069 kostenfrei https://doaj.org/article/59900f35be124f578b14ccedee993bba kostenfrei http://www.sciencedirect.com/science/article/pii/S0370269318304337 kostenfrei https://doaj.org/toc/0370-2693 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2014 GBV_ILN_2025 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2064 GBV_ILN_2111 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 782 2018 510-516 |
| allfields_unstemmed |
10.1016/j.physletb.2018.05.069 doi (DE-627)DOAJ077880986 (DE-599)DOAJ59900f35be124f578b14ccedee993bba DE-627 ger DE-627 rakwb eng QC1-999 B. Acharya verfasserin aut Search for magnetic monopoles with the MoEDAL forward trapping detector in 2.11 fb−1 of 13 TeV proton–proton collisions at the LHC 2018 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We update our previous search for trapped magnetic monopoles in LHC Run 2 using nearly six times more integrated luminosity and including additional models for the interpretation of the data. The MoEDAL forward trapping detector, comprising 222 kg of aluminium samples, was exposed to 2.11 fb−1 of 13 TeV proton–proton collisions near the LHCb interaction point and analysed by searching for induced persistent currents after passage through a superconducting magnetometer. Magnetic charges equal to the Dirac charge or above are excluded in all samples. The results are interpreted in Drell–Yan production models for monopoles with spins 0, 1/2 and 1: in addition to standard point-like couplings, we also consider couplings with momentum-dependent form factors. The search provides the best current laboratory constraints for monopoles with magnetic charges ranging from two to five times the Dirac charge. Physics J. Alexandre verfasserin aut S. Baines verfasserin aut P. Benes verfasserin aut B. Bergmann verfasserin aut J. Bernabéu verfasserin aut A. Bevan verfasserin aut H. Branzas verfasserin aut M. Campbell verfasserin aut L. Caramete verfasserin aut S. Cecchini verfasserin aut M. de Montigny verfasserin aut A. De Roeck verfasserin aut J.R. Ellis verfasserin aut M. Fairbairn verfasserin aut D. Felea verfasserin aut M. Frank verfasserin aut D. Frekers verfasserin aut C. Garcia verfasserin aut J. Hays verfasserin aut A.M. Hirt verfasserin aut J. Janecek verfasserin aut D.-W. Kim verfasserin aut K. Kinoshita verfasserin aut A. Korzenev verfasserin aut D.H. Lacarrère verfasserin aut S.C. Lee verfasserin aut C. Leroy verfasserin aut G. Levi verfasserin aut A. Lionti verfasserin aut J. Mamuzic verfasserin aut A. Margiotta verfasserin aut N. Mauri verfasserin aut N.E. Mavromatos verfasserin aut P. Mermod verfasserin aut V.A. Mitsou verfasserin aut R. Orava verfasserin aut I. Ostrovskiy verfasserin aut B. Parker verfasserin aut L. Patrizii verfasserin aut G.E. Păvălaş verfasserin aut J.L. Pinfold verfasserin aut V. Popa verfasserin aut M. Pozzato verfasserin aut S. Pospisil verfasserin aut A. Rajantie verfasserin aut R. Ruiz de Austri verfasserin aut Z. Sahnoun verfasserin aut M. Sakellariadou verfasserin aut A. Santra verfasserin aut S. Sarkar verfasserin aut G. Semenoff verfasserin aut A. Shaa verfasserin aut G. Sirri verfasserin aut K. Sliwa verfasserin aut R. Soluk verfasserin aut M. Spurio verfasserin aut Y.N. Srivastava verfasserin aut M. Suk verfasserin aut J. Swain verfasserin aut M. Tenti verfasserin aut V. Togo verfasserin aut J.A. Tuszyński verfasserin aut V. Vento verfasserin aut O. Vives verfasserin aut Z. Vykydal verfasserin aut A. Widom verfasserin aut G. Willems verfasserin aut J.H. Yoon verfasserin aut I.S. Zgura verfasserin aut In Physics Letters B Elsevier, 2015 782(2018), Seite 510-516 (DE-627)266015360 (DE-600)1466612-1 18732445 nnns volume:782 year:2018 pages:510-516 https://doi.org/10.1016/j.physletb.2018.05.069 kostenfrei https://doaj.org/article/59900f35be124f578b14ccedee993bba kostenfrei http://www.sciencedirect.com/science/article/pii/S0370269318304337 kostenfrei https://doaj.org/toc/0370-2693 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2014 GBV_ILN_2025 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2064 GBV_ILN_2111 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 782 2018 510-516 |
| allfieldsGer |
10.1016/j.physletb.2018.05.069 doi (DE-627)DOAJ077880986 (DE-599)DOAJ59900f35be124f578b14ccedee993bba DE-627 ger DE-627 rakwb eng QC1-999 B. Acharya verfasserin aut Search for magnetic monopoles with the MoEDAL forward trapping detector in 2.11 fb−1 of 13 TeV proton–proton collisions at the LHC 2018 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We update our previous search for trapped magnetic monopoles in LHC Run 2 using nearly six times more integrated luminosity and including additional models for the interpretation of the data. The MoEDAL forward trapping detector, comprising 222 kg of aluminium samples, was exposed to 2.11 fb−1 of 13 TeV proton–proton collisions near the LHCb interaction point and analysed by searching for induced persistent currents after passage through a superconducting magnetometer. Magnetic charges equal to the Dirac charge or above are excluded in all samples. The results are interpreted in Drell–Yan production models for monopoles with spins 0, 1/2 and 1: in addition to standard point-like couplings, we also consider couplings with momentum-dependent form factors. The search provides the best current laboratory constraints for monopoles with magnetic charges ranging from two to five times the Dirac charge. Physics J. Alexandre verfasserin aut S. Baines verfasserin aut P. Benes verfasserin aut B. Bergmann verfasserin aut J. Bernabéu verfasserin aut A. Bevan verfasserin aut H. Branzas verfasserin aut M. Campbell verfasserin aut L. Caramete verfasserin aut S. Cecchini verfasserin aut M. de Montigny verfasserin aut A. De Roeck verfasserin aut J.R. Ellis verfasserin aut M. Fairbairn verfasserin aut D. Felea verfasserin aut M. Frank verfasserin aut D. Frekers verfasserin aut C. Garcia verfasserin aut J. Hays verfasserin aut A.M. Hirt verfasserin aut J. Janecek verfasserin aut D.-W. Kim verfasserin aut K. Kinoshita verfasserin aut A. Korzenev verfasserin aut D.H. Lacarrère verfasserin aut S.C. Lee verfasserin aut C. Leroy verfasserin aut G. Levi verfasserin aut A. Lionti verfasserin aut J. Mamuzic verfasserin aut A. Margiotta verfasserin aut N. Mauri verfasserin aut N.E. Mavromatos verfasserin aut P. Mermod verfasserin aut V.A. Mitsou verfasserin aut R. Orava verfasserin aut I. Ostrovskiy verfasserin aut B. Parker verfasserin aut L. Patrizii verfasserin aut G.E. Păvălaş verfasserin aut J.L. Pinfold verfasserin aut V. Popa verfasserin aut M. Pozzato verfasserin aut S. Pospisil verfasserin aut A. Rajantie verfasserin aut R. Ruiz de Austri verfasserin aut Z. Sahnoun verfasserin aut M. Sakellariadou verfasserin aut A. Santra verfasserin aut S. Sarkar verfasserin aut G. Semenoff verfasserin aut A. Shaa verfasserin aut G. Sirri verfasserin aut K. Sliwa verfasserin aut R. Soluk verfasserin aut M. Spurio verfasserin aut Y.N. Srivastava verfasserin aut M. Suk verfasserin aut J. Swain verfasserin aut M. Tenti verfasserin aut V. Togo verfasserin aut J.A. Tuszyński verfasserin aut V. Vento verfasserin aut O. Vives verfasserin aut Z. Vykydal verfasserin aut A. Widom verfasserin aut G. Willems verfasserin aut J.H. Yoon verfasserin aut I.S. Zgura verfasserin aut In Physics Letters B Elsevier, 2015 782(2018), Seite 510-516 (DE-627)266015360 (DE-600)1466612-1 18732445 nnns volume:782 year:2018 pages:510-516 https://doi.org/10.1016/j.physletb.2018.05.069 kostenfrei https://doaj.org/article/59900f35be124f578b14ccedee993bba kostenfrei http://www.sciencedirect.com/science/article/pii/S0370269318304337 kostenfrei https://doaj.org/toc/0370-2693 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2014 GBV_ILN_2025 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2064 GBV_ILN_2111 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 782 2018 510-516 |
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10.1016/j.physletb.2018.05.069 doi (DE-627)DOAJ077880986 (DE-599)DOAJ59900f35be124f578b14ccedee993bba DE-627 ger DE-627 rakwb eng QC1-999 B. Acharya verfasserin aut Search for magnetic monopoles with the MoEDAL forward trapping detector in 2.11 fb−1 of 13 TeV proton–proton collisions at the LHC 2018 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We update our previous search for trapped magnetic monopoles in LHC Run 2 using nearly six times more integrated luminosity and including additional models for the interpretation of the data. The MoEDAL forward trapping detector, comprising 222 kg of aluminium samples, was exposed to 2.11 fb−1 of 13 TeV proton–proton collisions near the LHCb interaction point and analysed by searching for induced persistent currents after passage through a superconducting magnetometer. Magnetic charges equal to the Dirac charge or above are excluded in all samples. The results are interpreted in Drell–Yan production models for monopoles with spins 0, 1/2 and 1: in addition to standard point-like couplings, we also consider couplings with momentum-dependent form factors. The search provides the best current laboratory constraints for monopoles with magnetic charges ranging from two to five times the Dirac charge. Physics J. Alexandre verfasserin aut S. Baines verfasserin aut P. Benes verfasserin aut B. Bergmann verfasserin aut J. Bernabéu verfasserin aut A. Bevan verfasserin aut H. Branzas verfasserin aut M. Campbell verfasserin aut L. Caramete verfasserin aut S. Cecchini verfasserin aut M. de Montigny verfasserin aut A. De Roeck verfasserin aut J.R. Ellis verfasserin aut M. Fairbairn verfasserin aut D. Felea verfasserin aut M. Frank verfasserin aut D. Frekers verfasserin aut C. Garcia verfasserin aut J. Hays verfasserin aut A.M. Hirt verfasserin aut J. Janecek verfasserin aut D.-W. Kim verfasserin aut K. Kinoshita verfasserin aut A. Korzenev verfasserin aut D.H. Lacarrère verfasserin aut S.C. Lee verfasserin aut C. Leroy verfasserin aut G. Levi verfasserin aut A. Lionti verfasserin aut J. Mamuzic verfasserin aut A. Margiotta verfasserin aut N. Mauri verfasserin aut N.E. Mavromatos verfasserin aut P. Mermod verfasserin aut V.A. Mitsou verfasserin aut R. Orava verfasserin aut I. Ostrovskiy verfasserin aut B. Parker verfasserin aut L. Patrizii verfasserin aut G.E. Păvălaş verfasserin aut J.L. Pinfold verfasserin aut V. Popa verfasserin aut M. Pozzato verfasserin aut S. Pospisil verfasserin aut A. Rajantie verfasserin aut R. Ruiz de Austri verfasserin aut Z. Sahnoun verfasserin aut M. Sakellariadou verfasserin aut A. Santra verfasserin aut S. Sarkar verfasserin aut G. Semenoff verfasserin aut A. Shaa verfasserin aut G. Sirri verfasserin aut K. Sliwa verfasserin aut R. Soluk verfasserin aut M. Spurio verfasserin aut Y.N. Srivastava verfasserin aut M. Suk verfasserin aut J. Swain verfasserin aut M. Tenti verfasserin aut V. Togo verfasserin aut J.A. Tuszyński verfasserin aut V. Vento verfasserin aut O. Vives verfasserin aut Z. Vykydal verfasserin aut A. Widom verfasserin aut G. Willems verfasserin aut J.H. Yoon verfasserin aut I.S. Zgura verfasserin aut In Physics Letters B Elsevier, 2015 782(2018), Seite 510-516 (DE-627)266015360 (DE-600)1466612-1 18732445 nnns volume:782 year:2018 pages:510-516 https://doi.org/10.1016/j.physletb.2018.05.069 kostenfrei https://doaj.org/article/59900f35be124f578b14ccedee993bba kostenfrei http://www.sciencedirect.com/science/article/pii/S0370269318304337 kostenfrei https://doaj.org/toc/0370-2693 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2014 GBV_ILN_2025 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2064 GBV_ILN_2111 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 782 2018 510-516 |
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B. Acharya @@aut@@ J. Alexandre @@aut@@ S. Baines @@aut@@ P. Benes @@aut@@ B. Bergmann @@aut@@ J. Bernabéu @@aut@@ A. Bevan @@aut@@ H. Branzas @@aut@@ M. Campbell @@aut@@ L. Caramete @@aut@@ S. Cecchini @@aut@@ M. de Montigny @@aut@@ A. De Roeck @@aut@@ J.R. Ellis @@aut@@ M. Fairbairn @@aut@@ D. Felea @@aut@@ M. Frank @@aut@@ D. Frekers @@aut@@ C. Garcia @@aut@@ J. Hays @@aut@@ A.M. Hirt @@aut@@ J. Janecek @@aut@@ D.-W. Kim @@aut@@ K. Kinoshita @@aut@@ A. Korzenev @@aut@@ D.H. Lacarrère @@aut@@ S.C. Lee @@aut@@ C. Leroy @@aut@@ G. Levi @@aut@@ A. Lionti @@aut@@ J. Mamuzic @@aut@@ A. Margiotta @@aut@@ N. Mauri @@aut@@ N.E. Mavromatos @@aut@@ P. Mermod @@aut@@ V.A. Mitsou @@aut@@ R. Orava @@aut@@ I. Ostrovskiy @@aut@@ B. Parker @@aut@@ L. Patrizii @@aut@@ G.E. Păvălaş @@aut@@ J.L. Pinfold @@aut@@ V. Popa @@aut@@ M. Pozzato @@aut@@ S. Pospisil @@aut@@ A. Rajantie @@aut@@ R. Ruiz de Austri @@aut@@ Z. Sahnoun @@aut@@ M. Sakellariadou @@aut@@ A. Santra @@aut@@ S. Sarkar @@aut@@ G. Semenoff @@aut@@ A. Shaa @@aut@@ G. Sirri @@aut@@ K. Sliwa @@aut@@ R. Soluk @@aut@@ M. Spurio @@aut@@ Y.N. Srivastava @@aut@@ M. Suk @@aut@@ J. Swain @@aut@@ M. Tenti @@aut@@ V. Togo @@aut@@ J.A. Tuszyński @@aut@@ V. Vento @@aut@@ O. Vives @@aut@@ Z. Vykydal @@aut@@ A. Widom @@aut@@ G. Willems @@aut@@ J.H. Yoon @@aut@@ I.S. Zgura @@aut@@ |
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B. Acharya J. Alexandre S. Baines P. Benes B. Bergmann J. Bernabéu A. Bevan H. Branzas M. Campbell L. Caramete S. Cecchini M. de Montigny A. De Roeck J.R. Ellis M. Fairbairn D. Felea M. Frank D. Frekers C. Garcia J. Hays A.M. Hirt J. Janecek D.-W. Kim K. Kinoshita A. Korzenev D.H. Lacarrère S.C. Lee C. Leroy G. Levi A. Lionti J. Mamuzic A. Margiotta N. Mauri N.E. Mavromatos P. Mermod V.A. Mitsou R. Orava I. Ostrovskiy B. Parker L. Patrizii G.E. Păvălaş J.L. Pinfold V. Popa M. Pozzato S. Pospisil A. Rajantie R. Ruiz de Austri Z. Sahnoun M. Sakellariadou A. Santra S. Sarkar G. Semenoff A. Shaa G. Sirri K. Sliwa R. Soluk M. Spurio Y.N. Srivastava M. Suk J. Swain M. Tenti V. Togo J.A. Tuszyński V. Vento O. Vives Z. Vykydal A. Widom G. Willems J.H. Yoon I.S. Zgura |
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search for magnetic monopoles with the moedal forward trapping detector in 2.11 fb−1 of 13 tev proton–proton collisions at the lhc |
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Search for magnetic monopoles with the MoEDAL forward trapping detector in 2.11 fb−1 of 13 TeV proton–proton collisions at the LHC |
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We update our previous search for trapped magnetic monopoles in LHC Run 2 using nearly six times more integrated luminosity and including additional models for the interpretation of the data. The MoEDAL forward trapping detector, comprising 222 kg of aluminium samples, was exposed to 2.11 fb−1 of 13 TeV proton–proton collisions near the LHCb interaction point and analysed by searching for induced persistent currents after passage through a superconducting magnetometer. Magnetic charges equal to the Dirac charge or above are excluded in all samples. The results are interpreted in Drell–Yan production models for monopoles with spins 0, 1/2 and 1: in addition to standard point-like couplings, we also consider couplings with momentum-dependent form factors. The search provides the best current laboratory constraints for monopoles with magnetic charges ranging from two to five times the Dirac charge. |
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We update our previous search for trapped magnetic monopoles in LHC Run 2 using nearly six times more integrated luminosity and including additional models for the interpretation of the data. The MoEDAL forward trapping detector, comprising 222 kg of aluminium samples, was exposed to 2.11 fb−1 of 13 TeV proton–proton collisions near the LHCb interaction point and analysed by searching for induced persistent currents after passage through a superconducting magnetometer. Magnetic charges equal to the Dirac charge or above are excluded in all samples. The results are interpreted in Drell–Yan production models for monopoles with spins 0, 1/2 and 1: in addition to standard point-like couplings, we also consider couplings with momentum-dependent form factors. The search provides the best current laboratory constraints for monopoles with magnetic charges ranging from two to five times the Dirac charge. |
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We update our previous search for trapped magnetic monopoles in LHC Run 2 using nearly six times more integrated luminosity and including additional models for the interpretation of the data. The MoEDAL forward trapping detector, comprising 222 kg of aluminium samples, was exposed to 2.11 fb−1 of 13 TeV proton–proton collisions near the LHCb interaction point and analysed by searching for induced persistent currents after passage through a superconducting magnetometer. Magnetic charges equal to the Dirac charge or above are excluded in all samples. The results are interpreted in Drell–Yan production models for monopoles with spins 0, 1/2 and 1: in addition to standard point-like couplings, we also consider couplings with momentum-dependent form factors. The search provides the best current laboratory constraints for monopoles with magnetic charges ranging from two to five times the Dirac charge. |
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Search for magnetic monopoles with the MoEDAL forward trapping detector in 2.11 fb−1 of 13 TeV proton–proton collisions at the LHC |
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10.1016/j.physletb.2018.05.069 |
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2024-07-03T14:41:41.331Z |
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| score |
7.3991594 |