|  Types of Dark Matter | 
In General
  > s.a. content of the universe; dark matter
  [including alternatives]; dark-matter models [including particle physics].
  * 1990: Cold
    baryonic dark matter seems to be the most reasonable guess.
  * 1991: Cold dark
    matter predictions are wrong for large-scale structure
    [@ Nat(91)jan].
  * 1996: Hybrid models,
    in which galactic dark matter is most likely cold and non-exotic,
    while at the cluster level it is probably hot.
  * 2000: Large objects ruled out
    by microlensing, WIMPs are the prime candidates (s.a. "direct detection").
  * 2001: New forms
    of cold dark matter appear possible, like comet-type objects.
  * 2003: Λ-CDM (the
    CDM being possibly WIMPs and axions) appears to fit large-scale structure
    observations well; The Central Cusps and Too Many Satellites problems appear
    to be partly solved, so Angular Momentum is the main remaining CDM problem.
  * 2004: Most likely is
    Λ-CDM with WIMPs in conventional cosmology, or higher-dimensional
    sources if spacetime needs to be extended.
  * 2010: Λ-CDM with
    WIMP dark-matter particles still considered best candidate, specially
    after recent possible direct detection by CDMS.
  * 2013: M Turner,
    "Dark matter is made of something new... there is no particle in
    the Standard Model that can account for dark matter"
    [@ PhysOrg(13)feb].
  * 2014: There is a wide
    consensus that dark matter is likely to be made of supersymmetric
    particles that should be seen soon in so-called direct detection
    experiments, which have been running for several years; Particle
    physicists have cornered themselves experimentally in this sense.
  * 2016: WIMPs and axions remain the
    front-runners, but physicists are beginning to move beyond these two possibilities.
  * 2017: The idea of a hypothetical whole
    "dark sector" has been around for several years and is becoming more popular
    [@ news sci(17)mar].
  * 2018: With still no
    evidence for WIMPs axions receive more attention, and physicists are
    moving on to search for other possible particles.
  @ General references: Taoso et al JCAP(08)-a0711 [ten-point test];
    Melia IJMPD(09)-a0812 [constraints from expansion of cosmic horizon];
    Bergström NJP(09)-a0903;
    Kouvaris & Tinyakov PRD(10)-a1004,
    de Lavallaz & Fairbairn PRD(10)-a1004 [constraints from neutron stars];
    Polisensky & Ricotti PRD(11)-a1004 [constraints from Milky Way satellites];
    news pw(10)jun [evidence for two types];
    Dienes & Thomas PRD(12)-a1106 [multi-component framework];
    Barranco et al MNRAS(15)-a1301 [equation of state from rotation curves];
    Ren & He JCAP(15)-a1410 [with purely gravitational interactions].
  @ Reviews: Jetzer ap/96;
    Mikheeva ASR(03) [hybrid, cosmological models];
    Lazarides LNP(07)hp/06 [particle physics];
    Krauss ap/07-proc;
    Feng ARAA(10)-a1003 [from particle physics];
    Profumo et al a1910-ln [particle dark matter].
Hot Dark Matter
  * Idea: Made of light
    energetic particles like light neutrinos, etc; 2002, Using KamLAND
    data, Ων ≤ 0.070
    h−2.
  * Predictions: In Zel'dovich's
    hydrodynamic theory, one gets a top-down, "pancake'' picture of galaxy
    formation, start at the cluster level, with 1015
    mSun.
  * Difficulties:
    Hard pressed to reproduce correlations, but possible with early galaxy
    formation triggered by cosmic strings; Neutrinos cannot account for
    galactic halo dark matter, because of the Pauli principle.
  @ Neutrinos: Sciama Nat(90)dec,
    PRL(90);
    NS(91)mar9, p30;
    Hogan Nat(91)may;
    Primack BL(01)ap;
    Lieu ap/05/ApJL [excluded];
    Nieuwenhuizen EPL(09)-a0812 [non-relativistic];
    Paganini a1812 [τ neutrinos as cold dark matter].
  @ Sterile neutrinos: Seljak et al PRL(06)ap;
    Biermann & Munyaneza AIP(08)ap/07;
    Shaposhnikov ap/07-MGXI;
    Riemer-Sørensen & Hansen a0901 [decay, in dwarf galaxies];
    Hamann & Hasenkamp JCAP(13)-a1308;
    Abazajian PRL(14);
    Bringmann et al JCAP(14);
    news sn(20)mar [evidence against].
  @ Other fermions: Guendelman & Kaganovich gq/03 [CLEP of regular and dark fermions];
    Hannestad et al JCAP(05)ap [vs bosons];
    Boeckel & Schaffner-Bielich PRD(07)-a0707;
    Böhmer et al JHEP(10)-a1003 [non-standard spinors];
    Dürr & Fileviez PLB(14)-a1309 [fermionic field with baryon number];
    Grams et al CQG(14)-a1407 [fermions];
    Chavanis et al PRD(15)-a1410 [King model];
    Dürr et al PRD(15)-a1506 [with new gauge symmetry];
    Shelton et al PRL(15) [tests with supermassive black holes].
  @ Other types: Cheng mp/04 [Weyl's vector boson];
    > s.a. dilaton; neutrino;
      quintessence; types of gauge
      fields [symplectic].
Cold Dark Matter
  > s.a. Axinos; axions; cmb;
  dark-matter detection; dark-matter distribution;
  graviton [massive].
  * Idea: Exotic,
    heavy particles like photinos, higgsinos, scalar neutrinos, WIMPs or
    axions, particles like the χ with a mass between 1/1000
    and 1 mp and interact with
    one another through a massive particle called a "dark photon", or things
    like small black holes, brown dwarves (MACHOs), or molecular clouds.
  * WIMPs: Weakly
    Interacting Massive Particles; The Lightest Supersymmetric Particles, that
    cannot decay because of R-parity, and interact with other matter only via
    the weak nuclear force and gravity; Thought to have a mass of about 50
    mp;
    2006, Some form of neutralino WIMP is considered the leading candidate;
    SuperWIMPS may be detected at LHC; 2016, WIMPS still not showing up in
    detectors, supersymmetry arguments for them becoming shakier.
  * MACHOs: MAssive
    Compact Halo Objects, of various possible types; 2005, According to some
    microlensing experiments, they may account for about 20% of the galactic
    dark halo, but there are not enough for them to be the main component of
    dark matter; 2015, A MACHO halo cannot be ruled out.
  * Predictions: Leads to
    bottom-up galaxy formation (start with 105
    mSun).
  * Difficulties: Has
    some difficulties with distribution of galaxies, but seems to work well
    for the Milky Way; 2003, Seems to work well on large scales, may have
    difficulties on small (subgalactic) scales.
  @ Reviews:
    Tasitsiomi IJMPD(03) [small scales];
    Baer & Tata a0805-ch [and the LHC];
    Feng in(10)-a1002, news Phys(18) [alternatives to WIMPS].
  @ WIMPs: Freese et al PRD(01)ap [detection];
    Feng et al PRL(03)hp,
    PRD(03)hp,
    PRL(06) [superWIMPs];
    Cerdeno & Green NIMB(11)-a1002-ch [detection];
    Bertone Nat(10)nov-a1011 [the upcoming moment of truth];
    Aprile et al PRL(11)-a1104
    + news pw(11)apr,
    pt(11)may [stringent limits on WIMP properties];
    Angloher et al EPJC(12)-a1109
    + news bbc(11)sep [possible events];
    Kavanagh & Green PRD(12)-a1207,
    PRL(13) [improved mass estimates];
    news sn(16)oct [still no evidence];
    Arcadi et al EPJC(18)-a1703 [rev];
    news sn(17)sep,
    sn(18)may [still no evidence];
    Queiroz a1711-conf [rev];
    > s.a. IceCube Detector.
  @ Milky Way and Local Group: Lopez-Corredoira et al
      A&A(99)ap [high-velocity clouds];
    Merrifield ASP-ap/03 [halo];
    Adamek et al PRD(19)-a1901 [not with stellar-mass primordial black holes].
  @ And galaxy structure: D'Onghia & Lake ApJ(04)ap/03;
    Combes IAU-ap/03 [Λ-CDM];
    Weinberg et al PNAS(15)-a1306-proc [small scale controversies].
  @ MACHOs and MCOs: Schunck & Mielke CQG(03) [boson stars];
    Oppenheimer et al Sci(01)ap,
    Sci-ap/01 [white dwarves];
    Evans & Belokurov ap/04-conf [end of MACHO theory];
    Metcalf & Silk PRL(07)ap/06
    + pw(07)feb [constraints];
    Zackrisson & Flynn ApJ(08)-a0809 [subdwarf stars];
    Frampton JCAP(09),
    a1003-conf [black holes];
    Novati JPCS(12)-a1201 [microlensing search];
    Griest et al PRL(13),
    news ns(14)feb,
    Belotsky et al MPLA(14)-a1410 [small black holes];
    Hawkins A&A(15)-a1503 [new look at microlensing limits];
    Zumalacárregui & Seljak PRL(18),
    Schirber Phy(18)
      [black holes, limits from lensing of supernovae and debate];
    > s.a. black-hole types and primordial;
      black holes and information [remnants].
  @ Other types:
    Soberman & Dubin ap/01 [meteoroid-like];
    Ma & Bertschinger ApJ(04)ap/03 [kinetic theory of halos];
    Ellis JPCS(06)ap/05 [study with "little bangs"];
    Froggatt & Nielsen PRL(05)
    + pw(05)dec,
    ap/05-conf [balls of different phase];
    Bell et al A&A(06)ap [molecular];
    de Vega & Sánchez MNRAS(10)-a0901 [evidence for keV-scale particles];
    Rahaman et al PLB(10) [perfect fluid];
    Jacobs et al MNRAS(15)-a1410 [macro dark matter];
    Hochberg et al PRL(14) [Strongly Interacting Massive Particles];
    Hoeneisen a1502 ["back-of-the-envelope" calculations];
    Chakraborty & SenGupta EPJC(16)-a1511 [radions];
    focus Phy(18)sep
      [no evidence for millicharged dark matter];
    Saravani a1909 [OfDM];
    > s.a. QCD effects [quark nuggets].
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