Low scale gravity black holes at LHC Enikő Regős ( CERN )

Slides:



Advertisements
Similar presentations
Low scale gravity black holes at LHC
Advertisements

Extra Dimensions of Space-Time String theory suffers conformal anomaly that makes theory inconsistent --> get rid of it Conformal anomaly ~ (D-26) for.
Black Holes and Particle Species Gia Dvali CERN Theory Division and New York University.
M.Savina, November 25, NPD RAS Black Hole Production at the LHC: peculiarities, problems, expectations Savina Maria JINR, Dubna.
Search for Large Extra Dimensions at the Tevatron Bob Olivier, LPNHE Paris XXXVI ème Rencontre de Moriond Mars Search for Large Extra Dimensions.
Dark Energy and Quantum Gravity Dark Energy and Quantum Gravity Enikő Regős Enikő Regős.
Physics with Single, Multi- & Di-Photons at LEP HEP2003, Aachen, July HEP2003, Aachen, July Marat Gataullin (Caltech/L3) on behalf of LEP Collaborations.
Signatures of Large eXtra Dimensions LXD-Group ITP Frankfurt Marcus Bleicher, Sabine Hossenfelder (Tucson), Stefan Hofmann (Stockholm), Lars Gerland (TelAviv),
Nuclear Physics UConn Mentor Connection Mariel Tader.
What prospects for Black Holes at the Large Hadron Collider ? How might black holes be produced at the LHC? Discussion of recent developments in their.
1 De-Chang Dai ( 戴德昌 ) SUNY at Buffalo Black holes and extra dimensions Dec. 10, 2009 NTHU Dec. 10, 2009 NTHU.
14 April, 2009C. Dallapiccola, MIT Seminar Mini Black Holes at the LHC as a Signature of Extra Dimensions Carlo Dallapiccola University of Massachusetts,
Black Holes and Extra Dimensions Jonathan Feng UC Irvine Penn State Physics Department Colloquium 30 January 2003.
Discovering Gluinos at Hadron Colliders SLAC Theory Group Jay Wacker December 5, 2008 In collaboration with: M. Lisanti, J. Alwall, M. Le.
Dark Energy and Void Evolution Dark Energy and Void Evolution Enikő Regős Enikő Regős.
New Physics from Cosmic Neutrinos: Extra Dimensions and Black Holes Jonathan Feng UC Irvine 1 st ANITA Collaboration Meeting, UCI 24 November 2002.
Black Holes and Extra Dimensions Jonathan Feng UC Irvine Harvey Mudd Colloquium 7 December 2004.
Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u.
Introduction to universal extra dimensions (UEDs) Mitsuru Kakizaki (ICRR, University of Tokyo) May 10, KEK Refs: Original idea: Appelquist, Cheng,
Extra Dimensions Primer (see S. Hossenfelder) LED in many dimensions JLH, Lillie, Rizzo hep-ph/ SUSY05 DurhamJ. Hewett.
Theoretical Particle Physics: Beyond the Standard Model Jonathan Feng UC Irvine UCI Pizza Talk 18 April 2003.
Physics with ATLAS and CMS Are there new symmetries or extra-dimensions? What is dark matter? Where does mass come from? The two big multi-purpose experiments.
Primordial BHs. 2 Main reviews and articles astro-ph/ Primordial Black Holes - Recent Developments astro-ph/ Gamma Rays from Primordial.
Paris 22/4 UED Albert De Roeck (CERN) 1 Identifying Universal Extra Dimensions at CLIC  Minimal UED model  CLIC experimentation  UED signals & Measurements.
The CMS Muon Detector Thomas Hebbeker Aachen July 2001 Searching for New Physics with High Energy Muons.
The Big Bang, the LHC and the Higgs Boson Dr Cormac O’ Raifeartaigh (WIT)
Search for dark matter candidates in events with a jet and missing transverse momentum using the ATLAS detector Pierre-Hugues Beauchemin Tufts University.
Phenomenology of bulk scalar production at the LHC A PhD oral examination A PhD oral examination By Pierre-Hugues Beauchemin.
Quintessino model and neutralino annihilation to diffuse gamma rays X.J. Bi (IHEP)
Kaluza-Klein gluon production at the LHC
My Chapter 30 Lecture.
Searching for Extra Dimensions in High Energy Cosmic Rays Work in collaboration with Alessandro Cafarella (Lecce) Theodore Tomaras (Univ. of Crete) XIII.
Colliding Hadrons as Cosmic Membranes and Possible Signatures of Lost Momentum I.Ya.Aref’eva Steklov Mathematical Institute, Moscow A topical conference.
1 EXTRA DIMENSIONS AT FUTURE HADRON COLLIDERS G.F. Giudice CERN.
Sreerup Raychaudhuri TIFR Extra Dimensions and Collider Physics Workshop on Synergy between High Energy and High Luminosity Frontiers Tata Institute of.
Detecting GRB ν’s – an Opportunity For Observing Lorentz Invariance Violation Uri Jacob and Tsvi Piran The Hebrew University Jerusalem, Israel ν γ.
ICHEP-2002, AmsterdamG. Bernardi, LPNHE- Paris Search for Low Scale Gravity & Extra Dimensions at HERA, LEP, and the Tevatron Mini-review talk ICHEP-2002.
By Mengqing Wu XXXV Physics in Collision September 15-19, 2015 University of Warwick Dark matter searches with the ATLAS detector.
Introduction to CERN David Barney, CERN Introduction to CERN Activities Intro to particle physics Accelerators – the LHC Detectors - CMS.
Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 1 Chapter 30: Particle Physics Fundamental.
Low scale supergravity mediation in brane world scenario and hidden sector phenomenology Phys.Rev.D74:055005,2006 ( arXiv: hep-ph/ ) ACFA07 in Beijing:
Search for a Z′ boson in the dimuon channel in p-p collisions at √s = 7TeV with CMS experiment at the Large Hadron Collider Search for a Z′ boson in the.
Randall Sundrum KK Graviton at CMS
Generalized solution for RS metric and LHC phenomenology Alexander Kisselev IHEP, NRC “Kurchatov Institute”, Protvino, Russia The Third Annual Conference.
Report on LHT at the LHC ~ Some results from simulation study ~ Shigeki Matsumoto (Univ. of Toyama) 1.What kinds of LHT signals are expected, and how accurately.
22 December 2006Masters Defense Texas A&M University1 Adam Aurisano In Collaboration with Richard Arnowitt, Bhaskar Dutta, Teruki Kamon, Nikolay Kolev*,
Introduction to CERN Activities
Alternatives: Beyond SUSY Searches in CMS Dimitri Bourilkov University of Florida For the CMS Collaboration SUSY06, June 2006, Irvine, CA, USA.
The Standard Model of the elementary particles and their interactions
Don LincolnExperimental QCD and W/Z+Jet Results 1 Recent Dijet Measurements at DØ Don Lincoln Fermi National Accelerator Laboratory for the DØ Collaboration.
Randall- Sundrum Gravitons and Black Holes at the LHC Kevin Black Harvard University For the ATLAS and CMS Collaborations.
03/31/2006S. M. Lietti - UED Search at SPRACE 1 Universal Extra Dimensions Search at SPRACE S. M. Lietti DOSAR Workshop at U.T. Arlington.
STAU CLIC Ilkay Turk Cakir Turkish Atomic Energy Authority with co-authors O. Cakir, J. Ellis, Z. Kirca with the contributions from A. De Roeck,
Z’ Signals from KK Dark Matter Sabine Riemann (DESY) LCWS, Stanford, March 18-22, 2005 Outline  Universal extra dimensions (UED)  KK dark matter?  Sensitivity.
Elba -- June 7, 2006 Collaboration Meeting 1 CDF Melisa Rossi -- Udine University On behalf of the Multilepton Group CDF Collaboration Meeting.
Collider Signals of Extra Dimension Scenarios
Higgs in the Large Hadron Collider Joe Mitchell Advisor: Dr. Chung Kao.
Searches for Resonances in dilepton final states Searches for Resonances in dilepton final states PANIC th -14 th November 2008, Eilat, ISRAEL A.
Search for large extra dimensions at the Tevatron V. Krutelyov (UCSB) for CDF and D0 Collaborations DIS-2008 Conference, London April 7-11, 2008 Large.
Searching for in High Mass Dilepton Spectrum at CDF, Fermilab ADD model Drell-Yan production of a graviton of varying string scale M S = M Pl(4+n) [4]
BlackMax, a new BH generator arXiv:0711
Nick Evans University of Southampton
Sensitivity of ATLAS to Extra Dimensions
Exploration and Challenges at the Large Hadron Collider
Introduction to universal extra dimensions (UEDs)
New Physics at a TeV and the LHC – II & III
Gregorio Bernardi, LPNHE - Paris G. Bernardi, LPNHE- Paris
SUSY SEARCHES WITH ATLAS
Collider Signals of Large Extra Dimension
Presentation transcript:

Low scale gravity black holes at LHC Enikő Regős ( CERN )

Search for Extra Dimensions LHC : Quantum Gravity & Extra Dims LHC : Quantum Gravity & Extra Dims Stringy Quantum Black Holes Stringy Quantum Black Holes Low-scale Gravity Black Holes at LHC Low-scale Gravity Black Holes at LHC Comparison of Black Hole Generators Comparison of Black Hole Generators w De Roeck Gamsizkan Trocsanyi De Roeck Gamsizkan Trocsanyi

Quantum gravity and accelerator physics Obtain limits from collider experiments Obtain limits from collider experiments Graviton interference effects at Large Hadron Collider, CERN Graviton interference effects at Large Hadron Collider, CERN Decay modes of particles with mass in TeV range Decay modes of particles with mass in TeV range Hadron/lepton scatterings and Hadron/lepton scatterings and decays in extra-dimensional models decays in extra-dimensional models Black holes at LHC, CMS Black holes at LHC, CMS Limits from cosmology and astrophysics: cosmic rays and supernovae Limits from cosmology and astrophysics: cosmic rays and supernovae Particle astrophysics Particle astrophysics  Dark matter  mass of particles, Ex: Axions Ex: Axions Evidence from Evidence from observations for extra D observations for extra D  Quantum black holes: energy spectrum, depend on parameters of space times, strings

Cosmic rays and supernovae ; Cosmic rays : Nature’s free collider SN cores emit large fluxes of KK gravitons producing a cosmic background -> radiative decays : diffuse γ – ray background SN cores emit large fluxes of KK gravitons producing a cosmic background -> radiative decays : diffuse γ – ray background Cooling limit from SN 1987A neutrino burst -> bound on radius of extra dimensions Cooling limit from SN 1987A neutrino burst -> bound on radius of extra dimensions Cosmic neutrinos produce black holes, energy loss from graviton mediated interactions cannot explain cosmic ray events above a limit Cosmic neutrinos produce black holes, energy loss from graviton mediated interactions cannot explain cosmic ray events above a limit BH’s in observable collisions of elementary particles if ED BH’s in observable collisions of elementary particles if ED CR signals from mini BH’s in ED, evaporation of mini BHs CR signals from mini BH’s in ED, evaporation of mini BHs

Hierarchy problem & ED Fundamental scales in nature : Fundamental scales in nature : Planck mass : E19 GeV Planck mass : E19 GeV Electroweak scale : 240 GeV Electroweak scale : 240 GeV Supersymmetry : fundamental theory at M_Pl, Supersymmetry : fundamental theory at M_Pl, EW derived ( small #) from dynamics EW derived ( small #) from dynamics Broken ( particle mass ) : gravity mediated Broken ( particle mass ) : gravity mediated gravitino mass determines partner masses gravitino mass determines partner masses EW breaking induced by radiative corrections EW breaking induced by radiative corrections

Extra dimensions EW scale fundamental, M_Pl derived EW scale fundamental, M_Pl derived Compact ED ( radius R ) Compact ED ( radius R ) Matter confined in 4D Matter confined in 4D Gravity : propagates in all D, Gravity : propagates in all D, weak : compact space dimensions large compared to electroweak scale weak : compact space dimensions large compared to electroweak scale G = G_D / (2 π R)^ (D-4) G = G_D / (2 π R)^ (D-4)

Black holes at LHC Event generator for ED BHs : BlackMax I-II Event generator for ED BHs : BlackMax I-II Rotation, fermion splitting, brane tension Rotation, fermion splitting, brane tension Experimental signatures, particle decay Experimental signatures, particle decay CMSSW analysis CMSSW analysis Comparison with Charybdis I-II Comparison with Charybdis I-II Further models of Dvali suggest Black Hole detection even more likely Further models of Dvali suggest Black Hole detection even more likely

Distribution of black hole mass Rotating and non-rotating, 2 ED, 1-5 TeV Rotating and non-rotating, 2 ED, 1-5 TeV

Mass function Log Φ ~ M - M_min Log Φ ~ M - M_min for various models of for various models of Planck mass, ED, M_min, Planck mass, ED, M_min, rotation, brane tension rotation, brane tension

Distribution of BH color (red – blue - green) Rotating and non-rotating, 2 ED, 1-5 TeV Rotating and non-rotating, 2 ED, 1-5 TeV

Distribution of BH charge / 3q / Rotating and non-rotating, 2 ED, 1-5 TeV Rotating and non-rotating, 2 ED, 1-5 TeV

of emitted particles vs. BH mass of emitted particles vs. BH mass Rotating and non-rotating, 2 ED, 5-14 TeV Rotating and non-rotating, 2 ED, 5-14 TeV

Number of emitted particles vs. BH mass during Hawking phase Rotating and non-rotating, 2 ED, 5-14 TeV Rotating and non-rotating, 2 ED, 5-14 TeV

Number of emitted particles vs. # extra dimensions and # fermion splitting dimensions rotating and non-rotating ED = 7 rotating and non-rotating ED = 7

Number of emitted particles / BH vs. brane tension B non-rotating non-rotating ED = 2 ED = TeV 5-14 TeV Hawking phase Hawking phase M_Pl = 1 TeV M_Pl = 1 TeV

Pseudorapidity with final burst Non-rotating and rotating, 2 ED, 1-5 TeV, quarks, anti-quarks, leptons, anti-leptons Non-rotating and rotating, 2 ED, 1-5 TeV, quarks, anti-quarks, leptons, anti-leptons

Lepton transverse momentum : models Planck mass : 2 TeV Planck mass : 2 TeV ED = 3 ED = 3 5 – 14 TeV 5 – 14 TeV Minimum black hole Minimum black hole mass (non-rot) mass (non-rot) Multiplicity decreases w Planck mass Multiplicity decreases w Planck mass Energy & momentum increase Energy & momentum increase

Electrons/positrons, (anti)muons, photons : Transverse momentum & energy spectrum

Pseudorapidity : e - μ - γ Ratio of 0 < ή < 0.5 Ratio of 0 < ή < 0.5 & 0.5 < ή < 1 & 0.5 < ή < 1 distinguishes among beyond standard models distinguishes among beyond standard models All models and species All models and species have values very different from QCD have values very different from QCD

Model comparisons Further models : Planck mass : 2, 5 TeV ED = 5, 3 Minimum mass : 4, 7 TeV Vs. Standard Model top quark transv. momentum /GeV

Analysis at CMS Missing Transverse Energy : Missing Transverse Energy : graviton + neutrino : model dependent graviton + neutrino : model dependent Lepton transverse momentum : Lepton transverse momentum : easy to identify, cuts off for Standard Model easy to identify, cuts off for Standard Model Combined cuts : ή, p_T distribution Combined cuts : ή, p_T distribution

Model settings for detector which have different signature Angular cut for detector acceptance Angular cut for detector acceptance ή_lepton < 2.5 Jets, q, W, Z < 5 ή_lepton < 2.5 Jets, q, W, Z < 5 t, b t, b Implementation of generators in CMSSW Implementation of generators in CMSSW Interface BlackMax II Interface BlackMax II CMSSW : signal and SM background CMSSW : signal and SM background

Comparison of BlackMax with Charybdis BlackMax has higher multiplicity & BlackMax has higher multiplicity & lower momenta lower momenta Missing ET : Missing ET : gravitons only in BlackMax gravitons only in BlackMax BlackMax-II : gravitons in final burst too BlackMax-II : gravitons in final burst too Higher MET Higher MET Apart from cross sections good agreement Apart from cross sections good agreement Yoshino – Rychkov suppression decreases σ Yoshino – Rychkov suppression decreases σ

Multiplicity in BlackMax & Charybdis

Transverse momentum of emitted electrons

Transverse momentum of all particles

Spectrum of emitted electrons

Spectrum of emitted particles

Pseudorapidity of electrons

Pseudorapidity of emitted particles

Missing Transverse Energy with Gravitons

Further models to test at LHC : BHs in Dvali model for SM copies : BHs in Dvali model for SM copies : BH -> SM particle rates different, BH -> SM particle rates different, difference in particle decay difference in particle decay non-integer extra dimension non-integer extra dimension pT, MET pT, MET Dark Matter Dark Matter Even more likely for BHs w ADD & finding them Even more likely for BHs w ADD & finding them

Thank you for your attention !