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WIMP Shigeki Matsumoto (Kavli IPMU) Collaborators: - PowerPoint PPT Presentation

WIMP Shigeki Matsumoto (Kavli IPMU) Collaborators: Members in IPMU WIMP PROJECT S. M., S. Mukhopadhyay, Y. L. Sming Tsai, [JHEP 1410 (2014) 155] S. Banerjee, S. M., K. Mukaida, Y. L. Sming Tsai,


  1. WIMP ダークマター探査の現状と見通し Shigeki Matsumoto (Kavli IPMU) Collaborators: Members in IPMU WIMP PROJECT S. M., S. Mukhopadhyay, Y. L. Sming Tsai, [JHEP 1410 (2014) 155] S. Banerjee, S. M., K. Mukaida, Y. L. Sming Tsai, [JHEP 16xx (2016) xxx] S. M., S. Mukhopadhyay, Y. L. Sming Tsai, [PRD94 (2016) 065034 ] 以下の WIMP に関する3つの問題に焦点を当て、講演します。 What is the current status of the WIMP scenario? How far can we cover the WIMP scenario in future? What is the leftover remaining as unexplored regions?

  2. 1/11 Dark Matter (DM) overview  What we know about DM ( ∃ DM established)  Neutrality  Stability Observations  Coldness  Abundance  DM candidate in the standard model? No DM candidate! (Even a single component pBH is excluded.)  DM seems some new particle that is not discovered yet.  Mass range of a particle DM Particle dark matter GeV 10 20 10 – 28 de Broglie length < dSph size Compton length > Schwarzschild radius ( l = 2 p /mv) ( l = 2 p /m) (r = 2m/M pl 2 )

  3. 2/11 WIMP hypothesis WIMP hypothesis Dark matter is a electromagnetically neutral and stable particle, whose abundance at present is determined by the usual decoupling mechanism. Solving the Boltzmann equation gives Boltzmann eq. tells the following behavior of n WIMP /s → W TH h 2 ~ 0.1 (1pb/< s v>) 2 W OB h 2 ~ 0.12 ± 0.0015 Decoupling (reaction vs. expansion) often plays an important role in U.  Mass range WIMP dark matter GeV 10 5 10 – 3 Particle Physicists: The mass of WIMP may have the same origin of the EWSB! Experimenters: WIMP must have some interactions with SM particles, so that there exists a lot of opportunities to detect WIMP! Which SM particle(s) does the WIMP interact with?

  4. 3/11 WIMP searches @ Colliders WIMP is expected to be directly produced at colliders, if its energy is high enough. Hadron Collider : Interaction with quarks. Lepton Collider : Interaction with leptons. @ Direct detection WIMP can be detected by observing release energy by the scattering off a nucleus. SI scattering : Int. with quarks & Higgs. SD scattering : Int. with quarks & Z boson. @ Indirect detection WIMP could be searched for by observing annihilation products produced at DM halo. Gamma ray : Int. with all the SM particles Cosmic ray : Int. with all the SM particles

  5. 4/11 Studying WIMP without prejudice Discussing WIMP without relying on any specific new physics models! [New physics viewpoint is used to support the region found in the above discussion.] Interac action Which interaction exists =? GeV/c 2 0 DM ? between WIMP and SM? WIMP Classifying WIMPs by each interaction is not useful due to the consistency of FT. ↓ Classifying WIMPs based on its quantum number is more useful for our purpose. Weak charge plays an important role!!! WIMPs can be classified into the following three categories.  WIMP has a weak charge of (almost) zero. … Singlet( -like) WIMP  WIMP has a weak charge close of (half) integer. … EWIMP  WIMP has a mixed weak charge due to EWSB. … Well -tempered WIMP Let us discuss each WIMP using the simplest example to see what kind of strategy is (expected to be) taken to detect it at present (future).

  6. 5/11 Well-tempered WIMP  The simple lest st exam ample = F Fermion onic c singlet-doubl oublet WIMP model el.  Minimal al contents ar are 1 1 0 , 2 2 ½ , 2 –½ due to an anomal aly can ancelat ation.  3 neutral al M Maj ajoran ana a an and 1 1 char arged d Dirac ac fermion on introdu duce ced. d.  Lag agran angian an as assuming Z 2 symmetry ry mak aking the WIMP s stab able is is d by [M S , M D , y 1 = ycos q , y 2 = ysin q ] ,  Par aram ameter spac ace ar are defined nding to [M 1 , m , (g’/ 𝟑 )cos b , (g’/ 𝟑 )sin b ] at corres espo pondi at the MSSM. [DM in interac actions ar are as assumed d to preser erve ve the C CP symmetry.] .]  Such a a WIMP is predic icted ed by some nat atural al SUSY scenar arios. s.  Scan anning p par aram ameter s r spa pace u e using M g MCMC CMC to clar arify the current stat atus an and fu future p prosp spect cts of th the WI WIMP, as assuming |y |y i i | ≦ 1.

  7. 6/11 Well-tempered WIMP @ Near future @ Present After LZ/PICO250 Direct detection is very powerful to explore the well-tempered WIMP! Well-tempered WIMP ← Yukawa interactions → DM-DM-h(Z) couplings The same conclusion is obtained for the most of well-tempered WIMPs, for the origin of the mixing and DM-DM-h(Z) couplings are the same. What we learn: Just waiting future big direct detection experiments!

  8. 7/11 EW charged WIMP (EWIMP)  The simple lest st exam ample = F Fermion onic c triplet-like ke WIMP MP mod model. l.  Minimal al content is 3 0 , , nam amely just o one represen entat ation.  1 neutral al M Maj ajoran ana a an and 1 1 char arged d Dirac ac fermion on introdu duce ced. d.  Lag agran angian an as assuming Z 2 symmetry ry mak aking the WIMP s stab able is is  Par aram ameter spac ace is simply defined by only o one parameter M T .  Such a a WIMP is predat ated ed by the AM AMSB (high-sca cale) scenar arios os. .  Scan anning p par aram ameter er sp spac ace is is simp imple le bec becau ause se o of on one par arame meter er.  It is possi sible le to in include higher r dimension ional al operat rators rs to ta take new w physic ics s effect cts beyond the WIMP into ac account, howeve wever, r, those do not play important roles at WIMP’s phenomenology.

  9. 8/11 EW charged WIMP (EWIMP) LHC @ Near future @ Present Favored Favored The WIMP seems difficult to be detected at DD searches in near future. [ s SI ~ 2 10 – 11 pb, and, in addition, it may be cancelled by BSM contributions. ] LHC will explore the WIMP mass region below 500GeV. Can it go more? IDD searches are promising, for the WIMP’s annihilation is enhanced!!! [The enhancement is from the Sommerfeld effect, Hisano, S.M., Nojiri, 2014.] g -ray obs. (Fermi. CTA) → IDD ( g from dSphs) ← DM dist. (PSC, PFS)

  10. 9/11 Singlet-like WIMP  The WIMP can annot in interac act wi with SM SM p par articles by al alone d due to th the SM ga gauge s symmetry a y and the Z Z 2 symmet etry, , if it is a a fermion. .  Some the other r new w par article ( s ) must be i introdu duce ced d WIMP, wh which is cal alled the m mediat ator or connecting WIMP & SM (p (portal al scenar ario).  Phenomen omenol olog ogy of the WIMP depends ds strongly on th the mediat ator. r.  When the mediat ator or is h heav avier er enough h than an t the WIMP an and the EW scal ale, the p phenom omenol olog ogy is effectively ly described bed by the E EFT, where L represe wh sents s the e typical al mas ass scal ale of t the mediat ator or.  Par aram ameter spac ace is very compl plicat ated, ed, ∃ ar around d 10 p par aram ameters. EWSB, n , & dar  The WIMP is p predat ated d in in man any BSMs of E ark sector. r.  Scan anning p par aram ameter s r spa pace u e using M g MCMC, CMC, as assuming CP invar arian ance an and th the fl flav avor blindness ss of th the WI WIMP interac action with |c i i | ≦ 1.

  11. 10/11 Singlet-like WIMP @ Near future @ Present After LZ/PICO250 Light mediator region Light mediator region Direct detection is powerful to explore the H- & Z-resonance regions. The four Fermi interactions governs the other region with L < 10m DM , [This region is not so much searched for at DD and LHC exps in near future!] LHC results → The four Fermi region ← DD (LZ, PICO250) results ↓ Leptophilic WIMP! [It is governed mainly by the interactions with leptons.]

  12. 11/11 Summary  We discussed fermionic WIMPs w/o relying on specific BSMs.  Well-tempered WIMP: Direct detection searches are (and will be) playing a very important role to explore the WIMP. What we should do is to wait for their results in the near future.  Electroweakly charged WIMP (EWIMP): It seems to be the most motivated WIMP from the particle physics viewpoint. Indirect detection searches will be the only way to explore the WIMP in near future, requiring a precision determination of WIMP distribution near by us.  Singlet-like WIMP with heavy Mediator: Because of LHC and direct detection searches, leptophilic region will remain unexplored. Experiments sensitive to WIMP-lepton interactions will be very welcome.  Singlet-like WIMP with light Mediator: Studies are now on-going by many DM people in the world, via simplified models. Among those, interesting regions are reported, such as the light WIMP in the dark sector, etc.

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