|  Holography in Field Theory | 
In General
  > s.a. boundaries; duality in field theory;
  Holographic Screen; physics [visions].
  * Idea: The holographic
    principle is an idea proposed by 't Hooft in 1993, according to which
    (i) The true degrees of freedom inside a region are enumerated on its
    surface–like a literal interpretation of Plato's cave allegory–, with
    (ii) An information density ρinfo
    ≤ 1 bit /lP2; It
    relies on the validity of the holographic entropy bound; The issue is,
    what is the mechanism behind it?
  * Motivation: It provides
    a more economic description of nature than local quantum field theory,
    having fewer degrees of freedom.
  * Weak, "Kinematic":
    The entropy inside a region is bounded by the area of its boundary; The
    number of degrees of freedom inside a volume (including gravity) is
    bounded by the area of the boundary (screen) enclosing this volume.
  * Strong, "Dynamic":
    The dynamics of a system in a volume is described by a system living on
    the boundary; The degrees of freedom live on the boundary and describe
    the physics inside the volume completely.
  > Online resources:
    see Wikipedia page.
Examples, Phenomenology
  > s.a. AdS-cft correspondence [including dS-cft];
  entropy bound and quantum
  entropy; holography in gravitation and cosmology.
  * Development: First hints
    with black-hole thermodynamics (Hawking's area theorem, and Bekenstein's
    entropy), and attempts at more general area-based entropy bounds such as
Smatter ≤ A / 4G\(\hbar\)c3 ,
    which fails in strong-gravity, large-curvature situations, and is
    replaced by the covariant one; 't Hooft's and Susskind's idea of the world
    as a hologram, which seemed to be realized in quantum field theory, from
    examples of theories with AdS-cft correspondence (didn't work in general);
    Persistent ideas of importance in quantum gravity.
  * de Alfaro et al:
    A correspondence between the generating functional for the Green functions
    of a Euclidean quantum field theory in D dimensions and the Gibbs
    average for classical statistical mechanics in D+1 dimensions.
  * In M-theory: We are
    on the boundary, and we can probe the bulk dynamics; In 2+1 dimensions, it
    is satisfied by open and flat models, not closed ones.
  * Experiments: Craig
    Hogan developed the Holometer, a pair of interferometers at Fermilab
    with which one might detect "holographic noise" in the form of spacelike
    correlations between the interferometer signals; 2015, The experiment
    hasn't seen any evidence, but no general analysis of what types of
    theories the experiment can and cannot test is available.
  @ General references: Ogushi & Sasaki PTP(05)ht/04 [in Einstein-Gauss-Bonnet gravity];
    Midodashvili ht/06 [in higher dimensions];
    Wolf et al PRL(08) [for lattice model in thermal equilibrium];
    Dvali et al PRD(16)-a1511 [Stückelberg formulation];
    Jokela & Pönni a2007 [statistical approach].
  @ Condensed-matter physics: Mefford & Horowitz PRD(14)-a1406 [holographic insulator];
    Zaanen et al 16;
    > s.a. gauge-gravity duality.
  @ Fermilab Holometer:
    news NBC(14)aug;
    Chou et al PRL(16)-a1512
    + Hossenfelder blog(15)dec
    + news sci(15)dec [results];
    Chou et al CQG+(17);
    Hogan & Kwon CQG(18)-a1711 [exotic cross-correlations and emergent spacetime].
  > Related topics:
    see complexity; composite models;
    condensed matter; knot
    invariants; phase transitions; QCD.
References
  > s.a. cosmological constant; Large-Number
  Hypothesis; quantum gravity; renormalization group.
  @ Reviews:
    Bigatti & Susskind ht/00-ln;
    Smolin NPB(01)ht/00;
    't Hooft ht/00;
    Bousso RMP(02)ht;
    Bekenstein SA(03)aug;
    Banks IJMPA(10)-a1004-conf [and phenomenology – cosmological constant and supersymmetry];
    article vox(15)jun;
    Luminet IRS-a1602 [critical review];
    Baggioli a1908-ln.
  @ General references: 't Hooft in(88),
    gq/93-in;
    Susskind JMP(95)ht/94;
    Corley & Jacobson PRD(96)gq;
    Dawid PLB(99)gq/98;
    Schroer ht/01;
    Arcioni et al ht/06-fs [discussions with 't Hooft];
    Kay & Larkin PRD(08)-a0708;
    Osborne et al PRL(10)-a1005;
    Krishnan a1011-ln [quantum field theory and black-hole physics];
    Marolf CQG(14)-a1308 [without strings];
    blog sn(14)sep;
    McInnes & Ong NPB(15)-a1504 [consistency conditions];
    Zapata a1704-GRF [and gauge];
    Xiao a1710
      [microscopic theory with holographic degrees of freedom];
    Donnelly a1806
      [reconstructing a single-particle quantum state from the metric at spatial infinity].
  @ General spacetimes: Bonelli PLB(99)ht/98;
    Bousso JHEP(99)ht,
    CQG(00)ht/99-conf;
    Tavakol & Ellis PLB(99)ht;
    Riegler a1609-PhD [2+1 non-AdS spacetimes];
    Nomura et al PRD(17)-a1611 [without asymptotic regions].
  @ Interpretations: Dance qp/04 [in terms of observations].
  @ Counterexamples, alternatives: Pinzul & Stern JHEP(01)ht [non-commutative Chern-Simons];
    Botta Cantcheff & Nogales IJMPA(06)gq/05 [statistics].
  @ Related topics:
    Álvarez & Gómez NPB(99)ht/98,
    ht/98-fs [renormalization group, c-theorem];
    Minic PLB(98)ht [and uncertainty];
    Dzhunushaliev IJMPD(00)gq/99 [event horizons];
    Ivanov & Volovich Ent(01)gq/99 [entropy bound];
    Bose & Mazumdar gq/99 [quantum];
    van de Bruck gq/00 [and stochastic quantization];
    Zois RPMP(05)ht/03 [and Deligne conjecture];
    Bousso JHEP(04)ht [and quantum mechanics];
    Hubeny et al JHEP(05)ht [and causal structure];
    Miao a2009 [codimension-2 holography].
 main page
  – abbreviations
  – journals – comments
  – other sites – acknowledgements
  send feedback and suggestions to bombelli at olemiss.edu – modified 28 may 2021