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In [[Differential geometry|differential geometry]], the '''holonomy''' of a [[Connection (mathematics)|connection]] on a smooth manifold is the extent to which [[Parallel transport|parallel transport]] around closed loops fails to preserve the geometrical data being transported.  Holonomy is a general geometrical consequence of the [[Curvature|curvature]] of the connection. For flat connections, the associated holonomy is a type of [[Monodromy|monodromy]] and is an inherently global notion.  For curved connections, holonomy has nontrivial local and global features.

Any kind of connection on a manifold gives rise, through its parallel transport maps, to some notion of holonomy.  The most common forms of holonomy are for connections possessing some kind of [[Symmetry|symmetry]].  Important examples include: holonomy of the [[Levi-Civita connection]] in [[Riemannian geometry]] (called '''Riemannian holonomy'''), holonomy of [[Connection (vector bundle)|connections]] in [[Vector bundle|vector bundle]]s, holonomy of [[Cartan connection]]s, and holonomy of [[Connection (principal bundle)|connections]] in [[Principal bundle|principal bundle]]s.  In each of these cases, the holonomy of the connection can be identified with a [[Lie group]], the '''holonomy group'''.  The holonomy of a connection is closely related to the curvature of the connection, via the ''Ambrose–Singer theorem''.

The study of Riemannian holonomy has led to a number of important developments.  Holonomy was introduced by {{harvs|txt|last=Cartan|first=Élie|year=1926}} in order to study and classify [[Symmetric space|symmetric space]]s.  It was not until much later that holonomy groups would be used to study Riemannian geometry in a more general setting. In 1952 [[Biography:Georges de Rham|Georges de Rham]] proved the ''de Rham decomposition theorem'', a principle for splitting a Riemannian manifold into a [[Cartesian product]] of Riemannian manifolds by splitting the [[Tangent bundle|tangent bundle]] into irreducible spaces under the [[Group action|action]] of the local holonomy groups.  Later, in 1953, [[Biography:Marcel Berger|Marcel Berger]] classified the possible irreducible holonomies.  The decomposition and classification of Riemannian holonomy has applications to physics and to [[Physics:String theory|string theory]].

==Definitions==

===Holonomy of a connection in a vector bundle===
Let ''E'' be a rank-''k'' [[Vector bundle|vector bundle]] over a smooth manifold ''M'', and let ∇ be a [[Connection (vector bundle)|connection]] on ''E''. Given a [[Piecewise|piecewise]] smooth [[Loop (topology)|loop]] ''γ'' : [0,1] → ''M'' based at ''x'' in ''M'', the connection defines a [[Parallel transport|parallel transport]] map ''P''<sub>''γ''</sub> : ''E<sub>x</sub>'' → ''E<sub>x</sub>'' on the fiber of ''E'' at ''x''. This map is both linear and invertible, and so defines an element of the [[General linear group|general linear group]] GL(''E<sub>x</sub>''). The '''holonomy group''' of ∇ based at ''x'' is defined as

:<math>\operatorname{Hol}_x(\nabla) = \{P_\gamma \in \mathrm{GL}(E_x) \mid \gamma \text{ is a loop based at } x\}.</math>

The '''restricted holonomy group''' based at ''x'' is the subgroup <math>\operatorname{Hol}^0_x(\nabla)</math> coming from contractible loops&nbsp;''γ''.

If ''M'' is path-connected, then the holonomy group depends on the [[Pointed space|basepoint]] ''x'' only [[Up to|up to]] [[Conjugacy class|conjugation]] in GL(''k'', '''R'''). Explicitly, if ''γ'' is a path from ''x'' to ''y'' in ''M'', then

:<math>\operatorname{Hol}_y(\nabla) = P_\gamma \operatorname{Hol}_x(\nabla) P_\gamma^{-1}.</math>

Choosing different identifications of ''E<sub>x</sub>'' with '''R'''<sup>''k''</sup> also gives conjugate subgroups. Sometimes, particularly in general or informal discussions (such as below), one may drop reference to the basepoint, with the understanding that it is defined uniquely only up to conjugation.

Some important properties of the holonomy group include:
* <math>\operatorname{Hol}^0(\nabla)</math> is a connected Lie subgroup of GL(''k'', '''R''').
* <math>\operatorname{Hol}^0(\nabla)</math> is the [[Identity component|identity component]] of <math>\operatorname{Hol}(\nabla).</math>
* If ''M'' is simply connected, then <math>\operatorname{Hol}(\nabla) = \operatorname{Hol}^0(\nabla).</math>
* ∇ is flat (i.e. has vanishing curvature) [[If and only if|if and only if]] <math>\operatorname{Hol}^0(\nabla)</math> is trivial. In this case, <math>\operatorname{Hol}(\nabla)</math> may still be nontrivial.
* There is a natural, surjective [[Group homomorphism|group homomorphism]] <math>\pi_1(M) \to \operatorname{Hol}(\nabla)/ \operatorname{Hol}^0(\nabla),</math> where <math>\pi_1(M)</math> is the [[Fundamental group|fundamental group]] of ''M'', which sends the homotopy class <math>[\gamma]</math> to the [[Coset|coset]] <math>P_{\gamma}\cdot\operatorname{Hol}^0(\nabla).</math>
===Holonomy of a connection in a principal bundle===
[[File:Principal_Bundle_Path.svg|alt=Example of a principal bundle displaying the base spacetime manifold along with its fibers. It also displays how at every point along the fiber the tangent space can be split up into a vertical subspace pointing along the fiber and a horizontal subspace orthogonal to it.|right|thumb|286x286px|A connection on a principal bundle <math>P</math> with spacetime <math>M</math> separates out the tangent space at every point <math>x_p</math> along the fiber <math>G_p</math> into a vertical subspace <math>V_p</math> and a horizontal subspace <math>H_p</math>. Curves on the spacetime are uplifted to curves in the principal bundle whose tangent vectors lie in the horizontal subspace.]]
The definition for holonomy of connections on principal bundles proceeds in parallel fashion. Let ''G'' be a [[Lie group]] and ''P'' a [[Principal bundle|principal ''G''-bundle]] over a smooth manifold ''M'' which is paracompact. Let ω be a [[Connection form|connection]] on ''P''. Given a piecewise smooth [[Loop (topology)|loop]] ''γ'' : [0,1] → ''M'' based at ''x'' in ''M'' and a point ''p'' in the fiber over ''x'', the connection defines a unique ''horizontal lift'' <math>\tilde\gamma : [0,1] \to P</math> such that <math>\tilde\gamma(0) = p.</math> The end point of the horizontal lift, <math>\tilde\gamma(1)</math>, will not generally be ''p'' but rather some other point ''p''·''g'' in the fiber over ''x''. Define an [[Equivalence relation|equivalence relation]] ~ on ''P'' by saying that ''p'' ~ ''q'' if they can be joined by a piecewise smooth horizontal path in ''P''.

The '''holonomy group''' of ω based at ''p'' is then defined as

:<math>\operatorname{Hol}_p(\omega) = \{ g \in G \mid p \sim p \cdot g\}.</math>

The '''restricted holonomy group''' based at ''p'' is the subgroup <math>\operatorname{Hol}^0_p(\omega)</math> coming from horizontal lifts of contractible loops&nbsp;''γ''.

If ''M'' and ''P'' are [[Connected space|connected]] then the holonomy group depends on the [[Pointed space|basepoint]] ''p'' only up to [[Glossary of Riemannian and metric geometry#C|conjugation]] in ''G''. Explicitly, if ''q'' is any other chosen basepoint for the holonomy, then there exists a unique ''g'' ∈ ''G'' such that ''q'' ~ ''p''·''g''. With this value of ''g'',

:<math>\operatorname{Hol}_q(\omega) = g^{-1} \operatorname{Hol}_p(\omega) g.</math>

In particular,

:<math>\operatorname{Hol}_{p\cdot g}(\omega) = g^{-1} \operatorname{Hol}_p(\omega) g,</math>

Moreover, if ''p'' ~ ''q'' then <math>\operatorname{Hol}_p(\omega) = \operatorname{Hol}_q(\omega).</math> As above, sometimes one drops reference to the basepoint of the holonomy group, with the understanding that the definition is good up to conjugation.

Some important properties of the holonomy and restricted holonomy groups include:

*<math>\operatorname{Hol}^0_p(\omega)</math> is a connected Lie subgroup of ''G''.
*<math>\operatorname{Hol}^0_p(\omega)</math> is the [[Identity component|identity component]] of <math>\operatorname{Hol}_p(\omega).</math>
*There is a natural, surjective [[Group homomorphism|group homomorphism]] <math>\pi_1 \to \operatorname{Hol}_p(\omega)/\operatorname{Hol}^0_p(\omega).</math>
*If ''M'' is simply connected then <math>\operatorname{Hol}_p(\omega) = \operatorname{Hol}^0_p(\omega).</math>
*ω is flat (i.e. has vanishing curvature) if and only if <math>\operatorname{Hol}^0_p(\omega)</math> is trivial.

===Holonomy bundles===
Let ''M'' be a connected paracompact smooth manifold and ''P'' a principal ''G''-bundle with connection ω, as above. Let ''p'' ∈ ''P'' be an arbitrary point of the principal bundle. Let ''H''(''p'') be the set of points in ''P'' which can be joined to ''p'' by a horizontal curve. Then it can be shown that ''H''(''p''), with the evident projection map, is a principal bundle over ''M'' with structure group <math>\operatorname{Hol}_p(\omega).</math> This principal bundle is called the '''holonomy bundle''' (through ''p'') of the connection. The connection ω restricts to a connection on ''H''(''p''), since its parallel transport maps preserve ''H''(''p''). Thus ''H''(''p'') is a reduced bundle for the connection. Furthermore, since no subbundle of ''H''(''p'') is preserved by parallel transport, it is the minimal such reduction.<ref>{{harvnb|Kobayashi|Nomizu|1963|loc=§II.7}}</ref>

As with the holonomy groups, the holonomy bundle also transforms equivariantly within the ambient principal bundle ''P''. In detail, if ''q'' ∈ ''P'' is another chosen basepoint for the holonomy, then there exists a unique ''g'' ∈ ''G'' such that ''q'' ~ ''p'' ''g'' (since, by assumption, ''M'' is path-connected). Hence ''H''(''q'') = ''H''(''p'') ''g''. As a consequence, the induced connections on holonomy bundles corresponding to different choices of basepoint are compatible with one another: their parallel transport maps will differ by precisely the same element ''g''.

===Monodromy===
The holonomy bundle ''H''(''p'') is a principal bundle for <math>\operatorname{Hol}_p(\omega),</math> and so also admits an action of the restricted holonomy group <math>\operatorname{Hol}^0_p(\omega)</math> (which is a normal subgroup of the full holonomy group). The discrete group <math>\operatorname{Hol}_p(\omega)/\operatorname{Hol}^0_p(\omega)</math> is called the [[Monodromy group|monodromy group]] of the connection; it acts on the quotient bundle <math>H(p)/ \operatorname{Hol}^0_p(\omega).</math> There is a surjective homomorphism <math>\varphi: \pi_1 \to \operatorname{Hol}_p(\omega)/\operatorname{Hol}^0_p(\omega),</math> so that <math>\varphi\left(\pi_1(M)\right)</math> acts on <math>H(p)/ \operatorname{Hol}^0_p(\omega).</math> This action of the fundamental group is a '''monodromy representation''' of the fundamental group.<ref>{{harvnb|Sharpe|1997|loc=§3.7}}</ref>

===Local and infinitesimal holonomy===
If π: ''P'' → ''M'' is a principal bundle, and ω is a connection in ''P'', then the holonomy of ω can be restricted to the fibre over an open subset of ''M''. Indeed, if ''U'' is a connected open subset of ''M'', then ω restricts to give a connection in the bundle π<sup>−1</sup>''U'' over ''U''. The holonomy (resp. restricted holonomy) of this bundle will be denoted by <math>\operatorname{Hol}_p(\omega, U)</math> (resp. <math>\operatorname{Hol}^0_p(\omega, U)</math>) for each ''p'' with π(''p'') ∈ ''U''.

If ''U'' ⊂ ''V'' are two open sets containing π(''p''), then there is an evident inclusion

:<math>\operatorname{Hol}_p^0(\omega, U)\subset\operatorname{Hol}_p^0(\omega, V).</math>

The '''local holonomy group''' at a point ''p'' is defined by

:<math>\operatorname{Hol}^*(\omega) = \bigcap_{k=1}^\infty \operatorname{Hol}^0(\omega,U_k)</math>

for any family of nested connected open sets ''U''<sub>''k''</sub> with <math>\bigcap_k U_k = \pi(p)</math>.

The local holonomy group has the following properties:

# It is a connected Lie subgroup of the restricted holonomy group <math>\operatorname{Hol}^0_p(\omega).</math>
# Every point ''p'' has a neighborhood ''V'' such that <math>\operatorname{Hol}^*_p(\omega) = \operatorname{Hol}^0_p(\omega, V).</math> In particular, the local holonomy group depends only on the point ''p'', and not the choice of sequence ''U''<sub>''k''</sub> used to define it.
# The local holonomy is equivariant with respect to translation by elements of the structure group ''G'' of ''P''; i.e., <math>\operatorname{Hol}^*_{pg}(\omega) = \operatorname{Ad} \left(g^{-1}\right) \operatorname{Hol}^*_p(\omega)</math> for all ''g'' ∈ ''G''. (Note that, by property 1, the local holonomy group is a connected Lie subgroup of ''G'', so the adjoint is well-defined.)

The local holonomy group is not well-behaved as a global object. In particular, its dimension may fail to be constant. However, the following theorem holds:

: If the dimension of the local holonomy group is constant, then the local and restricted holonomy agree: <math>\operatorname{Hol}^*_p(\omega) = \operatorname{Hol}^0_p(\omega).</math>

==Ambrose–Singer theorem==
The Ambrose–Singer theorem (due to {{harvs|txt|first1=Warren|last1=Ambrose|first2=Isadore M.| last2=Singer |year=1953}}) relates the holonomy of a [[Connection (principal bundle)|connection in a principal bundle]] with the [[Curvature form|curvature form]] of the connection. To make this theorem plausible, consider the familiar case of an [[Affine connection|affine connection]] (or a connection in the tangent bundle{{snd}} the Levi-Civita connection, for example). The curvature arises when one travels around an infinitesimal parallelogram.

In detail, if σ: [0, 1] × [0, 1] → ''M'' is a surface in ''M'' parametrized by a pair of variables ''x'' and ''y'', then a vector ''V'' may be transported around the boundary of σ: first along (''x'', 0), then along (1, ''y''), followed by (''x'', 1) going in the negative direction, and then (0, ''y'') back to the point of origin. This is a special case of a holonomy loop: the vector ''V'' is acted upon by the holonomy group element corresponding to the lift of the boundary of σ. The curvature enters explicitly when the parallelogram is shrunk to zero, by traversing the boundary of smaller parallelograms over [0, ''x''] × [0, ''y'']. This corresponds to taking a derivative of the parallel transport maps at ''x'' = ''y'' = 0:

:<math>\frac{D}{dx}\frac{D}{dy}V - \frac{D}{dy}\frac{D}{dx}V = R\left(\frac{\partial\sigma}{\partial x}, \frac{\partial\sigma}{\partial y} \right)V</math>

where ''R'' is the [[Riemann curvature tensor|curvature tensor]].<ref>{{harvnb|Spivak|1999|p=241}}</ref> So, roughly speaking, the curvature gives the infinitesimal holonomy over a closed loop (the infinitesimal parallelogram). More formally, the curvature is the differential of the holonomy action at the identity of the holonomy group. In other words, ''R''(''X'', ''Y'') is an element of the [[Lie algebra]] of <math>\operatorname{Hol}_p(\omega).</math>

In general, consider the holonomy of a connection in a principal bundle ''P'' → ''M'' over ''P'' with structure group ''G''. Let '''g''' denote the Lie algebra of ''G'', the [[Curvature form|curvature form]] of the connection is a '''g'''-valued 2-form Ω on ''P''. The Ambrose–Singer theorem states:<ref>{{harvnb|Sternberg|1964|loc=Theorem VII.1.2}}</ref>

:The Lie algebra of <math>\operatorname{Hol}_p(\omega)</math> is spanned by all the elements of '''g''' of the form <math>\Omega_q(X,Y)</math> as ''q'' ranges over all points which can be joined to ''p'' by a horizontal curve (''q'' ~ ''p''), and ''X'' and ''Y'' are horizontal tangent vectors at ''q''.

Alternatively, the theorem can be restated in terms of the holonomy bundle:<ref>{{harvnb|Kobayashi|Nomizu|1963|loc=Volume I, §II.8}}</ref>

:The Lie algebra of <math>\operatorname{Hol}_p(\omega)</math> is the subspace of '''g''' spanned by elements of the form <math>\Omega_q(X, Y)</math> where ''q'' ∈ ''H''(''p'') and ''X'' and ''Y'' are horizontal vectors at ''q''.

==Riemannian holonomy==
The holonomy of a [[Riemannian manifold]] (''M'', ''g'') is   the holonomy group of the [[Levi-Civita connection]] on the [[Tangent bundle|tangent bundle]] to ''M''. A 'generic' ''n''-[[Dimension|dimension]]al [[Riemannian manifold]] has an [[Orthogonal group|O(''n'')]] holonomy, or SO(''n'') if it is orientable.  Manifolds whose holonomy groups are proper subgroups of O(''n'') or SO(''n'') have special properties.

One of the earliest fundamental results on Riemannian holonomy is the theorem of {{harvtxt|Borel|Lichnerowicz|1952}}, which asserts that the restricted holonomy group is a closed Lie subgroup of O(''n'').  In particular, it is compact.

===Reducible holonomy and the de Rham decomposition===
Let ''x'' ∈ ''M'' be an arbitrary point.  Then the holonomy group Hol(''M'') acts on the tangent space T<sub>x</sub>''M''.  This action may either be irreducible as a group representation, or reducible in the sense that there is a splitting of T<sub>x</sub>''M'' into orthogonal subspaces T<sub>x</sub>''M'' = T′<sub>x</sub>''M'' ⊕ T″<sub>x</sub>''M'', each of which is invariant under the action of Hol(''M'').  In the latter case, ''M'' is said to be '''reducible'''.

Suppose that ''M'' is a reducible manifold.  Allowing the point ''x'' to vary, the bundles T′''M'' and T″''M'' formed by the reduction of the tangent space at each point are smooth distributions which are integrable in the sense of Frobenius.  The [[Integral manifold|integral manifold]]s of these distributions are totally geodesic submanifolds.  So ''M'' is locally a Cartesian product ''M′'' × ''M″''.  The (local) de Rham isomorphism follows by continuing this process until a complete reduction of the tangent space is achieved:<ref>{{harvnb|Kobayashi|Nomizu|1963|loc=§IV.5}}</ref>

: Let ''M'' be a simply connected Riemannian manifold,<ref>This theorem generalizes to non-simply connected manifolds, but the statement is more complicated.</ref> and T''M'' = T<sup>(0)</sup>''M'' ⊕ T<sup>(1)</sup>''M'' ⊕ ⋯ ⊕ T<sup>(''k'')</sup>''M'' be the complete reduction of the tangent bundle under the action of the holonomy group.  Suppose that T<sup>(0)</sup>''M'' consists of vectors invariant under the holonomy group (i.e., such that the holonomy representation is trivial).  Then locally ''M'' is isometric to a product
:: <math>V_0\times V_1\times \cdots\times V_k,</math>
: where ''V''<sub>0</sub> is an open set in a [[Euclidean space]], and each ''V<sub>i</sub>'' is an integral manifold for T<sup>(''i'')</sup>''M''.  Furthermore, Hol(''M'') splits as a direct product of the holonomy groups of each ''M<sub>i</sub>'', the maximal integral manifold of T<sup>(''i'')</sup> through a point.

If, moreover, ''M'' is assumed to be geodesically complete, then the theorem holds globally, and each ''M<sub>i</sub>'' is a geodesically complete manifold.<ref>{{harvnb|Kobayashi|Nomizu|1963|loc=§IV.6}}</ref>

===The Berger classification===
In 1955, M. Berger gave a complete classification of possible holonomy groups for simply connected, Riemannian manifolds which are irreducible (not locally a product space) and nonsymmetric (not locally a Riemannian symmetric space). '''Berger's list''' is as follows:
{| class="wikitable" style="margin: auto;"
! Hol(''g'') || dim(''M'') || Type of manifold || Comments
|-
| SO(''n'') || ''n'' || Orientable manifold || —
|-
| [[Unitary group|U(''n'')]] || 2''n'' || [[Kähler manifold]] || Kähler
|-
| [[Special unitary group|SU(''n'')]] || 2''n'' || [[Calabi–Yau manifold]] || Ricci-flat, Kähler
|-
| Sp(''n'') · Sp(1) || 4''n'' || [[Quaternion-Kähler manifold]] || [[Einstein manifold|Einstein]]
|-
| [[Symplectic group|Sp(''n'')]] || 4''n'' || [[Hyperkähler manifold]] || Ricci-flat, Kähler
|-
| [[G2 (mathematics)|G<sub>2</sub>]] || 7 || [[G2 manifold|G<sub>2</sub> manifold]] || Ricci-flat
|-
| [[Spin group|Spin(7)]] || 8 || Spin(7) manifold || Ricci-flat
|}
Manifolds with holonomy Sp(''n'')·Sp(1) were simultaneously studied  in 1965 by [[Biography:Edmond Bonan|Edmond Bonan]] and Vivian Yoh Kraines,
who both discovered that such manifolds would necessarily carry a parallel 4-form.

Manifolds with holonomy G<sub>2</sub> or  Spin(7) were first investigated in abstract by [[Biography:Edmond Bonan|Edmond Bonan]] in 1966, who classified  the parallel differential forms that such a manifold would carry, and showed that such a  manifold would necessarily be Ricci-flat. However, no examples such  manifolds would actually be constructed for another 30 years. 

Berger's original list also included the possibility of Spin(9) as a subgroup of SO(16). Riemannian manifolds with such holonomy were later shown independently by D. Alekseevski and Brown-Gray to be necessarily locally symmetric, i.e., locally isometric to the [[Cayley plane]] F<sub>4</sub>/Spin(9) or locally flat. See below.) It is now known that all of these possibilities occur as holonomy groups of Riemannian manifolds. The last two exceptional cases were the most difficult to find. See [[G2 manifold|G<sub>2</sub> manifold]] and Spin(7) manifold.

Note that Sp(''n'') ⊂ SU(2''n'') ⊂ U(2''n'') ⊂ SO(4''n''), so every [[Hyperkähler manifold|hyperkähler manifold]] is a [[Calabi–Yau manifold]], every [[Calabi–Yau manifold]] is a [[Kähler manifold]], and every [[Kähler manifold]] is orientable.

The strange list above was explained by Simons's proof of Berger's theorem. A simple and geometric proof of Berger's theorem was given by Carlos E. Olmos in 2005. One first shows that if a Riemannian manifold is ''not'' a locally symmetric space and the reduced holonomy acts irreducibly on the tangent space, then it acts transitively on the unit sphere. The Lie groups acting transitively on spheres are known: they consist of the list above, together with 2 extra cases: the group Spin(9) acting on '''R'''<sup>16</sup>, and the group ''T'' · Sp(''m'') acting on '''R'''<sup>4''m''</sup>. Finally one checks that the first of these two extra cases only occurs as a holonomy group for locally symmetric spaces (that are locally isomorphic to the Cayley projective plane), and the second does not occur at all as a holonomy group.

Berger's original classification also included non-positive-definite pseudo-Riemannian metric non-locally symmetric holonomy. That list consisted of SO(''p'',''q'') of signature (''p'', ''q''), U(''p'', ''q'') and SU(''p'', ''q'') of signature (2''p'', 2''q''), Sp(''p'', ''q'') and Sp(''p'', ''q'')·Sp(1) of signature (4''p'', 4''q''), SO(''n'', '''C''') of signature (''n'', ''n''), SO(''n'', '''H''') of signature (2''n'', 2''n''), split G<sub>2</sub> of signature (4, 3), G<sub>2</sub>('''C''') of signature (7, 7), Spin(4, 3) of signature (4, 4), Spin(7, '''C''') of signature (7,7), Spin(5,4) of signature (8,8) and, lastly, Spin(9, '''C''') of signature (16,16). The split and complexified Spin(9) are necessarily locally symmetric as above and should not have been on the list. The complexified holonomies SO(''n'', '''C'''), G<sub>2</sub>('''C'''), and Spin(7,'''C''') may be realized from complexifying real analytic Riemannian manifolds. The last case, manifolds with holonomy contained in SO(''n'', '''H'''), were shown to be locally flat by R. McLean.<ref>{{citation
 | last = Bryant | first = Robert L.
 | contribution = Classical, exceptional, and exotic holonomies: a status report
 | contribution-url = https://ftp.gwdg.de/pub/misc/EMIS/journals/SC/1996/1/pdf/smf_sem-cong_1_93-165.pdf
 | isbn = 2-85629-047-7
 | mr = 1427757
 | pages = 93–165
 | publisher = Soc. Math. France, Paris
 | series = Sémin. Congr.
 | title = Actes de la Table Ronde de Géométrie Différentielle (Luminy, 1992)
 | volume = 1
 | year = 1996}}</ref>

Riemannian symmetric spaces, which are locally isometric to [[Homogeneous space|homogeneous space]]s ''G''/''H'' have local holonomy isomorphic to ''H''. These too have been [[List of simple Lie groups|completely classified]].

Finally, Berger's paper lists possible holonomy groups of manifolds with only a torsion-free [[Affine connection|affine connection]]; this is discussed below.

===Special holonomy and spinors===
Manifolds with special holonomy are characterized by the presence  of parallel [[Spinor|spinor]]s, meaning spinor fields with vanishing covariant derivative.<ref name="Lawson">{{harvnb|Lawson|Michelsohn|1989|loc=§IV.9–10}}</ref>  In particular, the following facts hold:
* Hol(ω) ⊂ ''U''(n) if and only if ''M'' admits a covariantly constant (or ''parallel'') projective pure spinor field.
* If ''M'' is a [[Spin structure|spin manifold]], then Hol(ω) ⊂ ''SU''(n) if and only if ''M'' admits at least two linearly independent  parallel pure spinor fields.  In fact, a parallel pure spinor field determines a canonical reduction of the structure group to ''SU''(''n'').
* If ''M'' is a seven-dimensional spin manifold, then ''M'' carries a non-trivial parallel spinor field if and only if the holonomy is contained in G<sub>2</sub>.
* If ''M'' is an eight-dimensional spin manifold, then ''M'' carries a non-trivial parallel spinor field if and only if the holonomy is contained in Spin(7).
<!--Anyone know of nice results specific to the hyper-Kaehler and quaternion-Kaehler holonomies?-->

The unitary and special unitary holonomies are often studied in connection with [[Physics:Twistor theory|twistor theory]],<ref>{{harvnb|Baum|Friedrich|Grunewald|Kath|1991}}</ref> as well as in the study of almost complex structures.<ref name="Lawson" />

===Applications===

====String Theory====
Riemannian manifolds with special holonomy play an important role in [[Physics:String theory|string theory]] [[Compactification|compactifications]].
<ref>{{citation | author = Gubser, S. | title = Special holonomy in string theory and M-theory | editor=Gubser S.|display-editors=etal}}
+{{citation |  title=Strings, branes and extra dimensions, TASI 2001. Lectures presented at the 2001 TASI school, Boulder, Colorado, USA, 4–29 June 2001.  | place=River Edge, NJ | publisher=World Scientific | isbn=978-981-238-788-2 | pages=197–233 | year=2004 | arxiv=hep-th/0201114 | last1=Gubser | first1=Steven S. }}.</ref>
This is because special holonomy manifolds admit [[Covariance and contravariance of vectors|covariantly]] constant (parallel) [[Spinor|spinor]]s and thus preserve some fraction of the original [[Supersymmetry|supersymmetry]]. Most important are compactifications on [[Calabi–Yau manifold]]s with SU(2) or SU(3) holonomy. Also important are compactifications on [[G2 manifold|G<sub>2</sub> manifold]]s.

====Machine Learning====
Computing the holonomy of Riemannian manifolds has been suggested as a way to learn the structure of data manifolds in [[Machine learning|machine learning]], in particular in the context of manifold learning. As the holonomy group contains information about the global structure of the data manifold, it can be used to identify how the data manifold might decompose into a product of submanifolds. The holonomy cannot be computed exactly due to finite sampling effects, but it is possible to construct a numerical approximation using ideas from [[Spectral graph theory|spectral graph theory]] similar to Vector Diffusion Maps. The resulting algorithm, the Geometric Manifold Component Estimator ({{Smallcaps|GeoManCEr}}) gives a numerical approximation to the de Rham decomposition that can be applied to real-world data.<ref>{{citation |last1=Pfau |first1=David |last2=Higgins |first2=Irina |last3=Botev |first3=Aleksandar |last4=Racanière |first4=Sébastien |title=Disentangling by Subspace Diffusion |journal=Advances in Neural Information Processing Systems |date=2020 |arxiv=2006.12982}}</ref>

==Affine holonomy==
Affine holonomy groups are the groups arising as holonomies of torsion-free [[Affine connection|affine connection]]s; those which are not Riemannian or pseudo-Riemannian holonomy groups are also known as non-metric holonomy groups. The de Rham decomposition theorem does not apply to affine holonomy groups, so a complete classification is out of reach. However, it is still natural to classify irreducible affine holonomies.

On the way to his classification of Riemannian holonomy groups, Berger developed two criteria that must be satisfied by the Lie algebra of the holonomy group of a torsion-free affine connection which is not [[Symmetric space|locally symmetric]]: one of them, known as ''Berger's first criterion'', is a consequence of the Ambrose–Singer theorem, that the curvature generates the holonomy algebra; the other, known as ''Berger's second criterion'', comes from the requirement that the connection should not be locally symmetric. Berger presented a list of groups acting irreducibly and satisfying these two criteria; this can be interpreted as a list of possibilities for irreducible affine holonomies.

Berger's list was later shown to be incomplete: further examples were found by [[Biography:Robert Bryant (mathematician)|R. Bryant]] (1991) and by Q. Chi, S. Merkulov, and L. Schwachhöfer (1996). These are sometimes known as ''exotic holonomies''. The search for examples ultimately led to a complete classification of irreducible affine holonomies by Merkulov and Schwachhöfer (1999), with Bryant (2000) showing that every group on their list occurs as an affine holonomy group.

The Merkulov–Schwachhöfer classification has been clarified considerably by a connection between the groups on the list and certain symmetric spaces, namely the [[Hermitian symmetric space|hermitian symmetric space]]s and the [[Quaternion-Kähler symmetric space|quaternion-Kähler symmetric space]]s. The relationship is particularly clear in the case of complex affine holonomies, as demonstrated by Schwachhöfer (2001).

Let ''V'' be a finite-dimensional complex vector space, let ''H'' ⊂ Aut(''V'') be an irreducible semisimple complex connected Lie subgroup and let ''K'' ⊂ ''H'' be a [[Maximal compact subgroup|maximal compact subgroup]].
# If there is an irreducible hermitian symmetric space of the form ''G''/(U(1) · ''K''), then both ''H'' and '''C'''*· ''H'' are non-symmetric irreducible affine holonomy groups, where ''V'' the tangent representation of ''K''.
# If there is an irreducible quaternion-Kähler symmetric space of the form ''G''/(Sp(1) · ''K''), then ''H'' is a non-symmetric irreducible affine holonomy groups, as is '''C'''* · ''H'' if dim ''V'' = 4. Here the complexified tangent representation of Sp(1) · ''K'' is '''C'''<sup>2</sup> ⊗ ''V'', and ''H'' preserves a complex symplectic form on ''V''.
These two families yield all non-symmetric irreducible complex affine holonomy groups apart from the following:
:<math> \begin{align}
  \mathrm{Sp}(2, \mathbf C) \cdot \mathrm{Sp}(2n, \mathbf C)
                              &\subset \mathrm{Aut}\left(\mathbf C^{2} \otimes\mathbf C^{2n}\right)\\
               G_2(\mathbf C) &\subset \mathrm{Aut}\left(\mathbf C^7\right)\\
  \mathrm{Spin}(7, \mathbf C) &\subset \mathrm{Aut}\left(\mathbf C^8\right).
\end{align}</math>

Using the classification of hermitian symmetric spaces, the first family gives the following complex affine holonomy groups:
:<math> \begin{align}
  Z_{\mathbf C} \cdot \mathrm{SL}(m, \mathbf C) \cdot \mathrm{SL}(n, \mathbf C)
                                                   &\subset \mathrm{Aut}\left(\mathbf C^m\otimes\mathbf C^n\right)\\
     Z_{\mathbf C} \cdot \mathrm{SL}(n, \mathbf C) &\subset \mathrm{Aut}\left(\Lambda^2\mathbf C^n\right)\\
     Z_{\mathbf C} \cdot \mathrm{SL}(n, \mathbf C) &\subset \mathrm{Aut}\left(S^2\mathbf C^n\right)\\
     Z_{\mathbf C} \cdot \mathrm{SO}(n, \mathbf C) &\subset \mathrm{Aut}\left(\mathbf C^n\right)\\
  Z_{\mathbf C} \cdot \mathrm{Spin}(10, \mathbf C) &\subset \mathrm{Aut}\left(\Delta_{10}^+\right) \cong \mathrm{Aut}\left(\mathbf C^{16}\right)\\
                Z_{\mathbf C} \cdot E_6(\mathbf C) &\subset \mathrm{Aut}\left(\mathbf C^{27}\right)
\end{align}</math>
where ''Z''<sub>'''C'''</sub> is either trivial, or the group '''C'''*.

Using the classification of quaternion-Kähler symmetric spaces, the second family gives the following complex symplectic holonomy groups:
:<math> \begin{align}
  \mathrm{Sp}(2, \mathbf C) \cdot \mathrm{SO}(n, \mathbf C) &\subset \mathrm{Aut}\left(\mathbf C^2\otimes\mathbf C^n\right)\\
        (Z_{\mathbf C}\,\cdot)\, \mathrm{Sp}(2n, \mathbf C) &\subset \mathrm{Aut}\left(\mathbf C^{2n}\right)\\
               Z_{\mathbf C} \cdot\mathrm{SL}(2, \mathbf C) &\subset \mathrm{Aut}\left(S^3\mathbf C^2\right)\\
                                  \mathrm{Sp}(6, \mathbf C) &\subset \mathrm{Aut}\left(\Lambda^3_0\mathbf C^6\right)\cong \mathrm{Aut}\left(\mathbf C^{14}\right)\\
                                  \mathrm{SL}(6, \mathbf C) &\subset \mathrm{Aut}\left(\Lambda^3\mathbf C^6\right)\\
                               \mathrm{Spin}(12, \mathbf C) &\subset \mathrm{Aut}\left(\Delta_{12}^+\right) \cong \mathrm{Aut}\left(\mathbf C^{32}\right)\\
                                             E_7(\mathbf C) &\subset \mathrm{Aut}\left(\mathbf C^{56}\right)\\
\end{align}</math>
(In the second row, ''Z''<sub>'''C'''</sub> must be trivial unless ''n'' = 2.)

From these lists, an analogue of Simons's result that Riemannian holonomy groups act transitively on spheres may be observed: the complex holonomy representations are all [[Prehomogeneous vector space|prehomogeneous vector space]]s. A conceptual proof of this fact is not known.

The classification of irreducible real affine holonomies can be obtained from a careful analysis, using the lists above and the fact that real affine holonomies complexify to complex ones.

==Etymology==
There is a similar word, "[[Holomorphic function|holomorphic]]", that was introduced by two of Cauchy's students, Briot (1817&ndash;1882) and Bouquet (1819&ndash;1895), and derives from the Greek ὅλος (''holos'') meaning "entire", and μορφή (''morphē'') meaning "form" or "appearance".<ref>{{harvnb|Markushevich|2005}}</ref>
The etymology of "holonomy" shares the first part with "holomorphic" (''holos''). About the second part:
{{quote|"It is remarkably hard to find the etymology of holonomic (or holonomy) on the web. I found the following (thanks to John Conway of Princeton):
'' 'I believe it was first used by Poinsot in his analysis of the motion of a rigid body. In this theory, a system is called "holonomic" if, in a certain sense, one can recover global information from local information, so the meaning "entire-law" is quite appropriate. The rolling of a ball on a table is non-holonomic, because one rolling along different paths to the same point can put it into different orientations.'' ''However, it is perhaps a bit too simplistic to say that "holonomy" means "entire-law". The "nom" root has many intertwined meanings in Greek, and perhaps more often refers to "counting". It comes from the same Indo-European root as our word "number."'' ' "|S.&nbsp;Golwala|<ref>{{harvnb|Golwala|2007|pages=65&ndash;66}}</ref>}}
See νόμος (''nomos'') and -nomy.

Despite its etymology, having "holonomy" does not mean having "entire-law". Instead, having "nontrivial holonomy" means "''failing'' to have entire-law". The case of having an "entire-law" would be called having "trivial holonomy". In this way, "holonomy" somehow means the same as "anholonomy" or "nonholonomy".

The original meaning of "holonomy" as "having an entire-law" is only preserved in classical mechanics, where a "[[Holonomic system|holonomic system]]" is a mechanical system whose constraints have an entire law.

==See also==

*[[Physics:Wilson loop|Wilson loop]]
*[[Physics:Thomas precession|Thomas precession]]
*[[Curvature]]
*[[Integrable system]]
*[[Physics:Geometric phase|Geometric phase]]
*[[Nonholonomic system]]

==Notes==
{{reflist|2}}

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==Further reading==
* [https://wayback.archive-it.org/all/20080528181257/http://page.mi.fu-berlin.de/~fwitt/LiteratureMSH.pdf Literature about manifolds of special holonomy], a bibliography by Frederik Witt.

{{curvature}}

[[Category:Differential geometry]]
[[Category:Connection (mathematics)]]
[[Category:Curvature (mathematics)]]

{{Sourceattribution|Holonomy}}