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Search for invisible Higgs boson decays in vector boson fusion at s=13 TeV with the ATLAS detector
We report a search for Higgs bosons that are produced via vector boson fusion and subsequently decay into invisible particles. The experimental signature is an energetic jet pair with invariant mass of O(1) TeV and O(100) GeV missing transverse momentum. The analysis uses 36.1fb-1 of pp collision da...
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Published in: | Physics letters. B 2019-04, Vol.793 (C) |
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creator | Anders, J. K. Andrei, V. Argyropoulos, S. Baker, O. K. Barbero, M. Batlamous, S. Beddall, A. Benjamin, D. P. Bensinger, J. R. Berlendis, S. Black, K. M. Blunier, Dr Bocchetta, S. S. Bogavac, D. Boisvert, V. Bolz, A. E. Bossio Sola, J. D. Bressler, S. Buttar, C. M. Camincher, C. Campana, S. Chegwidden, A. Chwastowski, J. J. Diehl, E. B. Duperrin, A. Dutta, B. Eigen, G. Ferrere, D. Fleck, I. Gadatsch, S. Gavrilenko, I. L. Goblirsch-Kolb, M. Gonella, G. Guo, J. Hill, J. C. Iltzsche, F. Iwasaki, H. Ju, X. Keyes, R. A. Kilby, C. R. Kluit, P. Kotwal, A. Krumnack, N. Kulinich, Y. P. Kurth, M. G. Kvita, J. Lagouri, T. Lang, V. S. Laplace, S. Lasagni Manghi, F. Le, B. Lellouch, D. Liu, Y. Loch, P. Maier, T. Malaescu, B. Melzer, A. Mindur, B. Mistry, K. P. Morettini, P. Myska, M. Nairz, A. M. Noguchi, Y. Oda, S. Orestano, D. O'Shea, V. Pandini, C. E. Parker, K. A. Rizzi, C. Ruan, X. Salt, J. Salvatore, F. Savard, P. Schillaci, Z. M. Schioppa, E. J. Schoeffel, L. Scuri, F. Shrestha, S. Shulga, E. Siegert, F. Sjölin, J. Slovak, R. Smith, M. N. K. Stanecka, E. Taffard, A. Tanaka, R. Thomas, J. P. Trofymov, A. Tsuno, S. Valero, A. Vecchio, V. Wang, W. Whiteson, D. Wu, X. Zaitsev, A. M. Zambito, S. Zemaityte, G. Zhou, Y. Zieminska, D. Zoch, K. |
description | We report a search for Higgs bosons that are produced via vector boson fusion and subsequently decay into invisible particles. The experimental signature is an energetic jet pair with invariant mass of O(1) TeV and O(100) GeV missing transverse momentum. The analysis uses 36.1fb-1 of pp collision data at √s=13 TeV recorded by the ATLAS detector at the LHC. In the signal region the 2252 observed events are consistent with the background estimation. Assuming a 125 GeV scalar particle with Standard Model cross sections, the upper limit on the branching fraction of the Higgs boson decay into invisible particles is 0.37 at 95% confidence level where 0.28 was expected. This limit is interpreted in Higgs portal models to set bounds on the wimp–nucleon scattering cross section. We also consider invisible decays of additional scalar bosons with masses up to 3 TeV for which the upper limits on the cross section times branching fraction are in the range of 0.3-1.7 pb. |
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K. ; Barbero, M. ; Batlamous, S. ; Beddall, A. ; Benjamin, D. P. ; Bensinger, J. R. ; Berlendis, S. ; Black, K. M. ; Blunier, Dr ; Bocchetta, S. S. ; Bogavac, D. ; Boisvert, V. ; Bolz, A. E. ; Bossio Sola, J. D. ; Bressler, S. ; Buttar, C. M. ; Camincher, C. ; Campana, S. ; Chegwidden, A. ; Chwastowski, J. J. ; Diehl, E. B. ; Duperrin, A. ; Dutta, B. ; Eigen, G. ; Ferrere, D. ; Fleck, I. ; Gadatsch, S. ; Gavrilenko, I. L. ; Goblirsch-Kolb, M. ; Gonella, G. ; Guo, J. ; Hill, J. C. ; Iltzsche, F. ; Iwasaki, H. ; Ju, X. ; Keyes, R. A. ; Kilby, C. R. ; Kluit, P. ; Kotwal, A. ; Krumnack, N. ; Kulinich, Y. P. ; Kurth, M. G. ; Kvita, J. ; Lagouri, T. ; Lang, V. S. ; Laplace, S. ; Lasagni Manghi, F. ; Le, B. ; Lellouch, D. ; Liu, Y. ; Loch, P. ; Maier, T. ; Malaescu, B. ; Melzer, A. ; Mindur, B. ; Mistry, K. P. ; Morettini, P. ; Myska, M. ; Nairz, A. M. ; Noguchi, Y. ; Oda, S. ; Orestano, D. ; O'Shea, V. ; Pandini, C. E. ; Parker, K. A. ; Rizzi, C. ; Ruan, X. ; Salt, J. ; Salvatore, F. ; Savard, P. ; Schillaci, Z. M. ; Schioppa, E. J. ; Schoeffel, L. ; Scuri, F. ; Shrestha, S. ; Shulga, E. ; Siegert, F. ; Sjölin, J. ; Slovak, R. ; Smith, M. N. K. ; Stanecka, E. ; Taffard, A. ; Tanaka, R. ; Thomas, J. P. ; Trofymov, A. ; Tsuno, S. ; Valero, A. ; Vecchio, V. ; Wang, W. ; Whiteson, D. ; Wu, X. ; Zaitsev, A. M. ; Zambito, S. ; Zemaityte, G. ; Zhou, Y. ; Zieminska, D. ; Zoch, K.</creator><creatorcontrib>Anders, J. K. ; Andrei, V. ; Argyropoulos, S. ; Baker, O. K. ; Barbero, M. ; Batlamous, S. ; Beddall, A. ; Benjamin, D. P. ; Bensinger, J. R. ; Berlendis, S. ; Black, K. M. ; Blunier, Dr ; Bocchetta, S. S. ; Bogavac, D. ; Boisvert, V. ; Bolz, A. E. ; Bossio Sola, J. D. ; Bressler, S. ; Buttar, C. M. ; Camincher, C. ; Campana, S. ; Chegwidden, A. ; Chwastowski, J. J. ; Diehl, E. B. ; Duperrin, A. ; Dutta, B. ; Eigen, G. ; Ferrere, D. ; Fleck, I. ; Gadatsch, S. ; Gavrilenko, I. L. ; Goblirsch-Kolb, M. ; Gonella, G. ; Guo, J. ; Hill, J. C. ; Iltzsche, F. ; Iwasaki, H. ; Ju, X. ; Keyes, R. A. ; Kilby, C. R. ; Kluit, P. ; Kotwal, A. ; Krumnack, N. ; Kulinich, Y. P. ; Kurth, M. G. ; Kvita, J. ; Lagouri, T. ; Lang, V. S. ; Laplace, S. ; Lasagni Manghi, F. ; Le, B. ; Lellouch, D. ; Liu, Y. ; Loch, P. ; Maier, T. ; Malaescu, B. ; Melzer, A. ; Mindur, B. ; Mistry, K. P. ; Morettini, P. ; Myska, M. ; Nairz, A. M. ; Noguchi, Y. ; Oda, S. ; Orestano, D. ; O'Shea, V. ; Pandini, C. E. ; Parker, K. A. ; Rizzi, C. ; Ruan, X. ; Salt, J. ; Salvatore, F. ; Savard, P. ; Schillaci, Z. M. ; Schioppa, E. J. ; Schoeffel, L. ; Scuri, F. ; Shrestha, S. ; Shulga, E. ; Siegert, F. ; Sjölin, J. ; Slovak, R. ; Smith, M. N. K. ; Stanecka, E. ; Taffard, A. ; Tanaka, R. ; Thomas, J. P. ; Trofymov, A. ; Tsuno, S. ; Valero, A. ; Vecchio, V. ; Wang, W. ; Whiteson, D. ; Wu, X. ; Zaitsev, A. M. ; Zambito, S. ; Zemaityte, G. ; Zhou, Y. ; Zieminska, D. ; Zoch, K. ; SLAC National Accelerator Laboratory (SLAC), Menlo Park, CA (United States) ; Harvard Univ., Cambridge, MA (United States) ; Lawrence Berkeley National Laboratory (LBNL), Berkeley, CA (United States) ; Univ. of Oregon, Eugene, OR (United States)</creatorcontrib><description>We report a search for Higgs bosons that are produced via vector boson fusion and subsequently decay into invisible particles. The experimental signature is an energetic jet pair with invariant mass of O(1) TeV and O(100) GeV missing transverse momentum. The analysis uses 36.1fb-1 of pp collision data at √s=13 TeV recorded by the ATLAS detector at the LHC. In the signal region the 2252 observed events are consistent with the background estimation. Assuming a 125 GeV scalar particle with Standard Model cross sections, the upper limit on the branching fraction of the Higgs boson decay into invisible particles is 0.37 at 95% confidence level where 0.28 was expected. This limit is interpreted in Higgs portal models to set bounds on the wimp–nucleon scattering cross section. We also consider invisible decays of additional scalar bosons with masses up to 3 TeV for which the upper limits on the cross section times branching fraction are in the range of 0.3-1.7 pb.</description><identifier>ISSN: 0370-2693</identifier><language>eng</language><publisher>United States: Elsevier</publisher><subject>PHYSICS OF ELEMENTARY PARTICLES AND FIELDS</subject><ispartof>Physics letters. 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The experimental signature is an energetic jet pair with invariant mass of O(1) TeV and O(100) GeV missing transverse momentum. The analysis uses 36.1fb-1 of pp collision data at √s=13 TeV recorded by the ATLAS detector at the LHC. In the signal region the 2252 observed events are consistent with the background estimation. Assuming a 125 GeV scalar particle with Standard Model cross sections, the upper limit on the branching fraction of the Higgs boson decay into invisible particles is 0.37 at 95% confidence level where 0.28 was expected. This limit is interpreted in Higgs portal models to set bounds on the wimp–nucleon scattering cross section. We also consider invisible decays of additional scalar bosons with masses up to 3 TeV for which the upper limits on the cross section times branching fraction are in the range of 0.3-1.7 pb.</description><subject>PHYSICS OF ELEMENTARY PARTICLES AND FIELDS</subject><issn>0370-2693</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><recordid>eNqNi7sKwjAYRjMoWC_v8ONeSEwvODgUUTq4tbiWNKZNpCTQP1Z8e4P6AE4Hvu-cGYkoz2m8y_Z8QZaId0opS2kWkbZSYpQaOjeCsZNB0w4KStP3CK1DZ-GmpHhhOGFS0gftO3cPNAHCAx4Yh1pd4Wm8Bq8VFPWlqELoP8GazDsxoNr8uCLb86k-lrFDbxqUJmhaOmuD3bA0T9KE8b-kN8W5Q2Q</recordid><startdate>20190415</startdate><enddate>20190415</enddate><creator>Anders, J. K.</creator><creator>Andrei, V.</creator><creator>Argyropoulos, S.</creator><creator>Baker, O. K.</creator><creator>Barbero, M.</creator><creator>Batlamous, S.</creator><creator>Beddall, A.</creator><creator>Benjamin, D. P.</creator><creator>Bensinger, J. 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M. ; Zambito, S. ; Zemaityte, G. ; Zhou, Y. ; Zieminska, D. ; Zoch, K.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-osti_scitechconnect_15745413</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><topic>PHYSICS OF ELEMENTARY PARTICLES AND FIELDS</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Anders, J. K.</creatorcontrib><creatorcontrib>Andrei, V.</creatorcontrib><creatorcontrib>Argyropoulos, S.</creatorcontrib><creatorcontrib>Baker, O. K.</creatorcontrib><creatorcontrib>Barbero, M.</creatorcontrib><creatorcontrib>Batlamous, S.</creatorcontrib><creatorcontrib>Beddall, A.</creatorcontrib><creatorcontrib>Benjamin, D. P.</creatorcontrib><creatorcontrib>Bensinger, J. R.</creatorcontrib><creatorcontrib>Berlendis, S.</creatorcontrib><creatorcontrib>Black, K. 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L.</creatorcontrib><creatorcontrib>Goblirsch-Kolb, M.</creatorcontrib><creatorcontrib>Gonella, G.</creatorcontrib><creatorcontrib>Guo, J.</creatorcontrib><creatorcontrib>Hill, J. C.</creatorcontrib><creatorcontrib>Iltzsche, F.</creatorcontrib><creatorcontrib>Iwasaki, H.</creatorcontrib><creatorcontrib>Ju, X.</creatorcontrib><creatorcontrib>Keyes, R. A.</creatorcontrib><creatorcontrib>Kilby, C. R.</creatorcontrib><creatorcontrib>Kluit, P.</creatorcontrib><creatorcontrib>Kotwal, A.</creatorcontrib><creatorcontrib>Krumnack, N.</creatorcontrib><creatorcontrib>Kulinich, Y. P.</creatorcontrib><creatorcontrib>Kurth, M. G.</creatorcontrib><creatorcontrib>Kvita, J.</creatorcontrib><creatorcontrib>Lagouri, T.</creatorcontrib><creatorcontrib>Lang, V. S.</creatorcontrib><creatorcontrib>Laplace, S.</creatorcontrib><creatorcontrib>Lasagni Manghi, F.</creatorcontrib><creatorcontrib>Le, B.</creatorcontrib><creatorcontrib>Lellouch, D.</creatorcontrib><creatorcontrib>Liu, Y.</creatorcontrib><creatorcontrib>Loch, P.</creatorcontrib><creatorcontrib>Maier, T.</creatorcontrib><creatorcontrib>Malaescu, B.</creatorcontrib><creatorcontrib>Melzer, A.</creatorcontrib><creatorcontrib>Mindur, B.</creatorcontrib><creatorcontrib>Mistry, K. P.</creatorcontrib><creatorcontrib>Morettini, P.</creatorcontrib><creatorcontrib>Myska, M.</creatorcontrib><creatorcontrib>Nairz, A. M.</creatorcontrib><creatorcontrib>Noguchi, Y.</creatorcontrib><creatorcontrib>Oda, S.</creatorcontrib><creatorcontrib>Orestano, D.</creatorcontrib><creatorcontrib>O'Shea, V.</creatorcontrib><creatorcontrib>Pandini, C. E.</creatorcontrib><creatorcontrib>Parker, K. A.</creatorcontrib><creatorcontrib>Rizzi, C.</creatorcontrib><creatorcontrib>Ruan, X.</creatorcontrib><creatorcontrib>Salt, J.</creatorcontrib><creatorcontrib>Salvatore, F.</creatorcontrib><creatorcontrib>Savard, P.</creatorcontrib><creatorcontrib>Schillaci, Z. M.</creatorcontrib><creatorcontrib>Schioppa, E. J.</creatorcontrib><creatorcontrib>Schoeffel, L.</creatorcontrib><creatorcontrib>Scuri, F.</creatorcontrib><creatorcontrib>Shrestha, S.</creatorcontrib><creatorcontrib>Shulga, E.</creatorcontrib><creatorcontrib>Siegert, F.</creatorcontrib><creatorcontrib>Sjölin, J.</creatorcontrib><creatorcontrib>Slovak, R.</creatorcontrib><creatorcontrib>Smith, M. N. K.</creatorcontrib><creatorcontrib>Stanecka, E.</creatorcontrib><creatorcontrib>Taffard, A.</creatorcontrib><creatorcontrib>Tanaka, R.</creatorcontrib><creatorcontrib>Thomas, J. P.</creatorcontrib><creatorcontrib>Trofymov, A.</creatorcontrib><creatorcontrib>Tsuno, S.</creatorcontrib><creatorcontrib>Valero, A.</creatorcontrib><creatorcontrib>Vecchio, V.</creatorcontrib><creatorcontrib>Wang, W.</creatorcontrib><creatorcontrib>Whiteson, D.</creatorcontrib><creatorcontrib>Wu, X.</creatorcontrib><creatorcontrib>Zaitsev, A. M.</creatorcontrib><creatorcontrib>Zambito, S.</creatorcontrib><creatorcontrib>Zemaityte, G.</creatorcontrib><creatorcontrib>Zhou, Y.</creatorcontrib><creatorcontrib>Zieminska, D.</creatorcontrib><creatorcontrib>Zoch, K.</creatorcontrib><creatorcontrib>SLAC National Accelerator Laboratory (SLAC), Menlo Park, CA (United States)</creatorcontrib><creatorcontrib>Harvard Univ., Cambridge, MA (United States)</creatorcontrib><creatorcontrib>Lawrence Berkeley National Laboratory (LBNL), Berkeley, CA (United States)</creatorcontrib><creatorcontrib>Univ. of Oregon, Eugene, OR (United States)</creatorcontrib><collection>OSTI.GOV</collection><jtitle>Physics letters. B</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Anders, J. K.</au><au>Andrei, V.</au><au>Argyropoulos, S.</au><au>Baker, O. K.</au><au>Barbero, M.</au><au>Batlamous, S.</au><au>Beddall, A.</au><au>Benjamin, D. P.</au><au>Bensinger, J. R.</au><au>Berlendis, S.</au><au>Black, K. M.</au><au>Blunier, Dr</au><au>Bocchetta, S. S.</au><au>Bogavac, D.</au><au>Boisvert, V.</au><au>Bolz, A. E.</au><au>Bossio Sola, J. D.</au><au>Bressler, S.</au><au>Buttar, C. M.</au><au>Camincher, C.</au><au>Campana, S.</au><au>Chegwidden, A.</au><au>Chwastowski, J. J.</au><au>Diehl, E. B.</au><au>Duperrin, A.</au><au>Dutta, B.</au><au>Eigen, G.</au><au>Ferrere, D.</au><au>Fleck, I.</au><au>Gadatsch, S.</au><au>Gavrilenko, I. L.</au><au>Goblirsch-Kolb, M.</au><au>Gonella, G.</au><au>Guo, J.</au><au>Hill, J. C.</au><au>Iltzsche, F.</au><au>Iwasaki, H.</au><au>Ju, X.</au><au>Keyes, R. A.</au><au>Kilby, C. R.</au><au>Kluit, P.</au><au>Kotwal, A.</au><au>Krumnack, N.</au><au>Kulinich, Y. P.</au><au>Kurth, M. G.</au><au>Kvita, J.</au><au>Lagouri, T.</au><au>Lang, V. S.</au><au>Laplace, S.</au><au>Lasagni Manghi, F.</au><au>Le, B.</au><au>Lellouch, D.</au><au>Liu, Y.</au><au>Loch, P.</au><au>Maier, T.</au><au>Malaescu, B.</au><au>Melzer, A.</au><au>Mindur, B.</au><au>Mistry, K. P.</au><au>Morettini, P.</au><au>Myska, M.</au><au>Nairz, A. M.</au><au>Noguchi, Y.</au><au>Oda, S.</au><au>Orestano, D.</au><au>O'Shea, V.</au><au>Pandini, C. E.</au><au>Parker, K. A.</au><au>Rizzi, C.</au><au>Ruan, X.</au><au>Salt, J.</au><au>Salvatore, F.</au><au>Savard, P.</au><au>Schillaci, Z. M.</au><au>Schioppa, E. J.</au><au>Schoeffel, L.</au><au>Scuri, F.</au><au>Shrestha, S.</au><au>Shulga, E.</au><au>Siegert, F.</au><au>Sjölin, J.</au><au>Slovak, R.</au><au>Smith, M. N. K.</au><au>Stanecka, E.</au><au>Taffard, A.</au><au>Tanaka, R.</au><au>Thomas, J. P.</au><au>Trofymov, A.</au><au>Tsuno, S.</au><au>Valero, A.</au><au>Vecchio, V.</au><au>Wang, W.</au><au>Whiteson, D.</au><au>Wu, X.</au><au>Zaitsev, A. M.</au><au>Zambito, S.</au><au>Zemaityte, G.</au><au>Zhou, Y.</au><au>Zieminska, D.</au><au>Zoch, K.</au><aucorp>SLAC National Accelerator Laboratory (SLAC), Menlo Park, CA (United States)</aucorp><aucorp>Harvard Univ., Cambridge, MA (United States)</aucorp><aucorp>Lawrence Berkeley National Laboratory (LBNL), Berkeley, CA (United States)</aucorp><aucorp>Univ. of Oregon, Eugene, OR (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Search for invisible Higgs boson decays in vector boson fusion at s=13 TeV with the ATLAS detector</atitle><jtitle>Physics letters. B</jtitle><date>2019-04-15</date><risdate>2019</risdate><volume>793</volume><issue>C</issue><issn>0370-2693</issn><abstract>We report a search for Higgs bosons that are produced via vector boson fusion and subsequently decay into invisible particles. The experimental signature is an energetic jet pair with invariant mass of O(1) TeV and O(100) GeV missing transverse momentum. The analysis uses 36.1fb-1 of pp collision data at √s=13 TeV recorded by the ATLAS detector at the LHC. In the signal region the 2252 observed events are consistent with the background estimation. Assuming a 125 GeV scalar particle with Standard Model cross sections, the upper limit on the branching fraction of the Higgs boson decay into invisible particles is 0.37 at 95% confidence level where 0.28 was expected. This limit is interpreted in Higgs portal models to set bounds on the wimp–nucleon scattering cross section. We also consider invisible decays of additional scalar bosons with masses up to 3 TeV for which the upper limits on the cross section times branching fraction are in the range of 0.3-1.7 pb.</abstract><cop>United States</cop><pub>Elsevier</pub></addata></record> |
fulltext | fulltext |
identifier | ISSN: 0370-2693 |
ispartof | Physics letters. B, 2019-04, Vol.793 (C) |
issn | 0370-2693 |
language | eng |
recordid | cdi_osti_scitechconnect_1574541 |
source | ScienceDirect Freedom Collection; ScienceDirect Journals |
subjects | PHYSICS OF ELEMENTARY PARTICLES AND FIELDS |
title | Search for invisible Higgs boson decays in vector boson fusion at s=13 TeV with the ATLAS detector |
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