Strong fields and recycled accelerator parts as a laboratory for fundamental physics Joerg Jaeckel † M. Ahlers *,H. Gies x, J. Redondo**, A. Ringwald **

Slides:



Advertisements
Similar presentations
Searching for Magnetic Monopoles
Advertisements

European Strategy for Particle Physics 2013 Preparatory group->Strategy group Individual town meetings Town meeting in Krakow: september 2012 Drafting.
Dark Energy and Quantum Gravity Dark Energy and Quantum Gravity Enikő Regős Enikő Regős.
"Now I am become Death, the destroyer of worlds." Robert Oppenheimer after the first test of the atomic bomb.
String theoretic QCD axions in the light of PLANCK and BICEP2 (QCD axion after BICEP2) Kiwoon KIAS, May 1, 2014 KC, K.S. Jeong and M.S. Seo, arXiv:
Why we need Lab Experiments to search for Alps Joerg Jaeckel 1 E. Masso, J. Redondo 2 F. Takahashi, A. Ringwald 1 1 DESY 2 Universitat Autonoma de Barcelona.
Physics with Single, Multi- & Di-Photons at LEP HEP2003, Aachen, July HEP2003, Aachen, July Marat Gataullin (Caltech/L3) on behalf of LEP Collaborations.
Tony Liss Saturday Physics for Everyone November 9, 2013 (With debts to Chris Quigg, Leonard Susskind, Hitoshi Murayama)
CMB Constraints on Mini-charged Particles Clare Burrage (DESY) arXiv: with J. Jaeckel, J. Redondo & A. Ringwald.
Andreas Ringwald, DESY 27 th DESY PRC Closed Session, DESY, Hamburg, 26 October 2011 Towards a comprehensive summary Physics Case for WISP Searches.
Joerg Jaeckel IPPP - University of Durham S Abel, C-S Chu, J.J., V.V. Khozehep-th/ S Abel, J J, V.V. Khoze hep-th/ Living on the Edge: Why.
Neutral Particles. Neutrons Neutrons are like neutral protons. –Mass is 1% larger –Interacts strongly Neutral charge complicates detection Neutron lifetime.
Nailing Electroweak Physics (aka Higgs Hunting) with the Next Linear Collider Bob Wilson High Energy Physics Group CSU Physics Research Evening November.
The Large Hadron Collider -Exploring a New Energy Frontier
1 Yurii Maravin, SMU/CLEO Snowmass 2001 Experimental Aspects of  physics at CLEO-c measurements of fundamental quantities, tests of weak couplings and.
J. Nielsen1 The ATLAS experiment at the Large Hadron Collider Jason Nielsen UC Santa Cruz VERTEX 2004 July 28, 2010.
The International Linear Collider Barry Barish IUPAP General Assembly Cape Town 26-Oct-05.
CERN, 21 February 2001 Egil Lillestøl, CERN & Univ. of Bergen Recorded at
Discovery of the Higgs Boson Gavin Lawes Department of Physics and Astronomy.
Geneva, October 2010 Dark Energy at Colliders? Philippe Brax, IPhT Saclay Published papers :
Science Case for / Physics Goals of ALPS-II.
CERN, January 2009 Evading the CAST bound with a chameleon Philippe Brax, IPhT Saclay.
Relic Neutrinos as a Source of Dark Energy Neal Weiner New York University IDM04 R.Fardon, D.B.Kaplan, A.E.Nelson, NW What does dark energy have to do.
My Chapter 30 Lecture.
A new era in fundamental physics Higgs: from theory to experiments André França – Baku 2013.
Robert Foot, CoEPP, University of Melbourne June Explaining galactic structure and direct detection experiments with mirror dark matter 1.
The Dark Side of the Universe What is dark matter? Who cares?
The Standard Model of Electroweak Physics Christopher T. Hill Head of Theoretical Physics Fermilab.
Axel Lindner, DESY An experimental Expedition into a new Particle Habitat at smallest Masses Cosmology Meets Particle Physics, DESY Theory Workshop, 28.
From Luigi DiLella, Summer Student Program
CMS Physics at RAL Why is gravity so much weaker than electromagnetism? (The electromagnetic force repelling two electrons is much greater than the gravitational.
Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 1 Chapter 30: Particle Physics Fundamental.
DARK MATTER CANDIDATES Cody Carr, Minh Nguyen December 9 th, 2014.
INVASIONS IN PARTICLE PHYSICS Compton Lectures Autumn 2001 Lecture 8 Dec
1 CERN, 27 January 2009A. Lindner Ultra-light Particles beyond the Standard Model: Laboratory Experiments.
ATLAS experiment at the CERN Large Hadron Collider Peter Watkins, Head of Particle Physics Group, University of Birmingham, UK
GRIDFest, CERN, October 3, New Physics at the Large Hadron Collider Jos Engelen CERN a brief introduction.
CASCADE – RF cavity experiment to search for hidden sector photons Matti Kalliokoski Lancaster University and The Cockcroft Institute On behalf of the.
Direct Detection of Supersymmetric Particles in Neutrino Telescopes Z. Chacko University of Arizona I. Albuquerque & G. Burdman.
Large extra dimensions and CAST Biljana Lakić Rudjer Bošković Institute, Zagreb Joint ILIAS-CAST-CERN Axion Training, , CERN Joint ILIAS-CAST-CERN.
EXPERIMENTAL EVIDENCE FOR THE QUARK AND STANDARD MODELS J 5.1, 5.2, 5.3, 5.4, 5.5 A particle-arly interesting presentation by LIAM HEGARTY 2012 Edited.
The Higgs Boson Observation (probably) Not just another fundamental particle… July 27, 2012Purdue QuarkNet Summer Workshop1 Matthew Jones Purdue University.
Dragan Slavkov Hajdukovic
Dark matter and hidden U(1) X (Work in progress, In collaboration with E.J. Chun & S. Scopel) Park, Jong-Chul (KIAS) August 10, 2010 Konkuk University.
LIGHT PSEUDOSCALAR BOSONS, PVLAS AND DOUBLE PULSAR J Marco Roncadelli, INFN – Pavia (Italy)
Low scale gravity black holes at LHC Enikő Regős ( CERN )
Introduction to Particle Physics I Sinéad Farrington 18 th February 2015.
Compelling Scientific Questions The International Linear Collider will answer key questions about matter, energy, space and time We now sample some of.
Any Light Particle Search II Any Light Particle Search II Axel Lindner DESY Status of ALPS DESY QED VMB, DESY, 03 November 2015.
R. Bähre 1, N. Bastidon 2, B. Döbrich 3, J. Dreyling-Eschweiler 3, S. Gharazyan 3, R. Hodajerdi 1,2,3, D. Horns 2, F. Januschek 3, E.-A. Knabbe 3, N. Kuzkova.
1 The Standard Model of Particle Physics Owen Long U. C. Riverside March 1, 2014.
Particle Detectors January 18, 2011 Kevin Stenson.
Searching for Weakly-Interacting-Slim Particles by shining light-through-a-wall Searching for Weakly-Interacting-Slim Particles by shining light-through-a-wall.
Dark Energy at Future Colliders: Testing the True Nature of Dark Energy in Black Hole Evaporations Jörg Jäckel Rencontres des Moriond March 2005 Michael.
Any Light Particle Search – ALPS II Natali Kuzkova Ph.D. student, DESY PIER PhD seminar 20 th January, 2015.
New constraints on light bosons from the high energy universe Denis WOUTERS Service de Physique des Particules Supervisor: Pierre BRUN D. Wouters and P.
Jim Sullivan.  Big Bang Theory  Dark Matter and Dark Energy  Detecting Dark Matter  Radiation and Pulse Shape Discrimination  SNOLAB  Summary.
Xenon100 collaboration gives a stringent constraint on spin-independent elastic WIMP-nucleon scattering cross section. Ton-scale detectors for direct detection.
qBOUNCE: a quantum bouncing ball gravity spectrometer
Theoretical Particle Physics Group (TPP)
G. Dattoli and F. Nguyen ENEA-FRASCATI
An interesting candidate?
Particle accelerators
Axel Lindner (DESY) Benno Willke (AEI Hanover) Herman Ten Kate (CERN)
Electromagnetism 1865: James Clerk Maxwell 1887: Heinrich Hertz
dark matter Properties stable non-relativistic non-baryonic
Searching for Magnetic Monopoles
THE GOD PARTICLE 1 Shashwat Mandal & Christian Bach 5
CMS Masterclass 2017.
Neutrino Physics with SHiP
Presentation transcript:

Strong fields and recycled accelerator parts as a laboratory for fundamental physics Joerg Jaeckel † M. Ahlers *,H. Gies x, J. Redondo**, A. Ringwald ** † IPPP Durham, x ITP Heidelberg, *CTP Oxford, **DESY

Exploring fundamental high energy physics… The direct approach: MORE POWER LHC+ILC,CLIC Detects most things within energy range E.g. may find WIMPs

But… Current maximal energy few TeV May miss very weakly interacting matter (Axions, WIMPs, WISPs…) Only indirect evidence for dark matter Man its DANGEROUS…

Recycling... Complementary approaches

Light Shining through a wall Axion-like particle search Any-light particle search Laser Detector

Photons coming through the wall! It could be Axion(-like particle)s! Coupling to two photons: a a

How many photons arrive? 1 photon per second at detector

Tiny coupling, small mass ALPS

If no detection, good bound! ALPS

WISPS X =Weakly interacting sub-eV particles Axions Massive hidden photons (without B-field) =analog -oscillations Hidden photon + minicharged particle (MCP) a a MCP

String theory: Moduli, Axions, etc. String theory needs Extra Dimensions Must compactify Shape and size deformations correspond to fields: Moduli (WISPs) and Axions Connected to the fundamental scale, here string scale `Physics case’ for WISPs strengthened

String theory likes extra gauge groups Many extra U(1)s! Candidates for WISPs

String theory likes extra matter Hidden sector matter May be light and WISPy Or WIMPy and dark matter Hidden matter

A cavity experiment

It’s a Light shining through walls clone Microwaves instead of laser Emitter cavity Detector cavity

Setup

Advantages Resonant cavity setup: Cavity in production and regeneration region Microwave cavities can have very high Q-factors~10 11 ! Sensitive to masses in the interesting  eV-meV range

Sensitive to variety of WISPs Axions Massive hidden photons (without B-field) =analog -oscillations Hidden photon + minicharged particle (MCP) a a MCP

(theoretical) Sensitivity, e.g. hidden photons Coulomb Sun/CAST BBN+CMB LSW

Wildly optimistic proposal

AC/DC Highway to minicharged particles

AC/DC (accelerator cavity/dark current) Highway to minicharged particles

Minicharged particles Minicharged particles are particles which have a small fraction of the electron electric charge Searching them tests fundamental ideas such as charge quantization May give insight into fundamental physics Hidden matter

Schwinger Pair Production Pair Production in a strong electric Field (without Laser)! Similar to tunneling: Energy of `vacuum pair‘ An -pair separated by a distance has less energy than no particles!

Acceleator cavities must be & Sensitive to

Finding the produced MCPs Effects of millicharged particles decreases with smaller Direct detection is difficult Look for macroscopic effects

Energy loss If many particles are produced we get a Macroscopic energy loss! Can be measured

Quite strong bounds! Not quite competitive with astrophysical bounds…

Nearly-direct detection... Dark Current Shining through a Wall! Minicharged particles produced in the cavity lead to a Dark Current Dark Current detection

Advantages It’s a (nearly) direct detection It detects minicharged particles without making use of the hidden photons

All parts exist! CavityCryogenic Current Comparator

Sensitivity

Conclusions

Searching new particles with recycled tools Light particles coupled to photons are “expected” in Extensions of the Standard Model, e.g. string theory We can search for them using low energy experiments with photons!! Using recycled accelerator parts! These experiments are complementary to the collisions! Test ultrasmall couplings! Many more cool experiments possible!

Crazy ideas…

13-17 July 2009 University of Durham (UK) 5th Patras Workshop on Axions, WIMPs and WISPs Organizing committee: Laura Baudis (University of Zurich) Joerg Jaeckel (IPPP/Durham University) Axel Lindner (DESY) Andreas Ringwald (DESY) Konstantin Zioutas (University of Patras) Programme: * The physics case for WIMPs, Axions, WISPs * Review of collider experiments * Signals from astrophysical sources * Direct searches for Dark Matter * Indirect laboratory searches for Axions, WISPs * Direct laboratory searches for Axions, WISPs * New theoretical developments

Conclusions Low energy experiments with photons can provide for a AC/DC can provide (nearly) direct detection of minicharged particles A `Superconducting Box’ experiment could explore the meV valley for `hidden photons’ LSW with microwave cavities can provide a highly sensitive exploration of axions, and hidden photons

Conclusions All these experiments are small scale! They explore physics at ultra high energies and could detect hidden sectors Complementary to accelerators!

Conclusions All these experiments are small scale! They explore physics at ultra high energies and could detect hidden sectors Complementary to accelerators! Please build them !

Theorists and ‘’easy’’ experiments… …lets go WISP hunting WISP

Kinetic Mixing - How to get Minicharges Two U(1)‘s „Our“ U(1) „Hidden“ U(1) Mixing Diagonalization:

Kinetic Mixing - How to get Minicharges Two U(1)‘s „Our“ U(1) „Hidden“ U(1) Mixing carries electric charge! Diagonalization:

Hidden Photons Two U(1)‘s „Our“ U(1) „Hidden“ U(1) Mixing Diagonalization:

Massive hidden photons oscillate Two U(1)‘s „Our“ U(1) „Hidden“ U(1) Mixing photon – hidden photon oscillations analog neutrino oscillations Diagonalization:

(theoretical) Sensitivity, e.g. hidden photons Coulomb Sun/CAST BBN+CMB LSW

Q-factor Energy loss will be reflected in the Cavity‘s Q-factor: We can get bounds from Superconducting Cavities reach

Searching hidden photons inside a superconducting box

Hidden Photons Extra (light) U(1) gauge bosons Standard model particles carry no (tree-level) charge under them hidden! Tests hidden sectors of standard model extensions

Massive hidden photons Hidden Photons can mix with the ordinary photon Propagation eigenstates are not identical with interaction eigenstates Photon – Hidden photon oscillations Completely analogous to neutrino oscillations

Current bounds opportunities meV valley Coulomb Sun/CAST BBN+CMB LSW

Current bounds opportunities Extra degrees of Coulomb Sun/CAST BBN+CMB LSW

Basic idea Similar to `Light shining through walls’:

Basic idea Similar to Light shining through walls: But virtual instead of real photons, Magnetic field instead of Laser Superconductor is `wall’ Superconducting shield

Setup: The box

Magnetic fields from source to detector

Advantages Measures directly the field, i.e. amplitude instead of probability Can use fields as high as 0.1 T (higher fields not shielded by most superconductors) Can detect B as low as a few T Expect sensitivity up to  » few ! (possible disadvatage: may not work for axions!)

Sensitivity: Exactly where we want it Coulomb Sun/CAST BBN+CMB LSW Could do better than astrophysics!!!