Pure spinor

Consider a complex vector space ${\displaystyle V}$ , with either even dimension ${\displaystyle 2n}$  or odd dimension ${\displaystyle 2n+1}$ , and a nondegenerate complex scalar product ${\displaystyle Q}$ , with values ${\displaystyle Q(u,v)}$  on pairs of vectors ${\displaystyle (u,v)}$ . The Clifford algebra ${\displaystyle Cl(V,Q)}$  is the quotient of the full tensor algebra on ${\displaystyle V}$  by the ideal generated by the relations

${\displaystyle u\otimes v+v\otimes u=2Q(u,v),\quad \forall \ u,v\in V.}$ 

Spinors are modules of the Clifford algebra, and so in particular there is an action of the elements of ${\displaystyle V}$  on the space of spinors. The complex subspace ${\displaystyle V_{\psi }^{0}\subset V}$  that annihilates a given nonzero spinor ${\displaystyle \psi }$  has dimension ${\displaystyle m\leq n}$ . If ${\displaystyle m=n}$  then ${\displaystyle \psi }$  is said to be a pure spinor. In terms of stratification of spinor modules by orbits of the spin group ${\displaystyle Spin(V,Q)}$ , pure spinors correspond to the smallest orbits, which are the Shilov boundary of the stratification by the orbit types of the spinor representation on the irreducible spinor (or half-spinor) modules.

Pure spinors, defined up to projectivization, are called projective pure spinors. For ${\displaystyle \,V\,}$  of even dimension ${\displaystyle 2n}$ , the space of projective pure spinors is the homogeneous space ${\displaystyle SO(2n)/U(n)}$ ; for ${\displaystyle \,V\,}$  of odd dimension ${\displaystyle 2n+1}$ , it is ${\displaystyle SO(2n+1)/U(n)}$ .

Following Cartan^[1] and Chevalley,^[2] we may view ${\displaystyle V}$  as a direct sum

${\displaystyle V=V_{n}\oplus V_{n}^{*}\ {\text{ or }}\ V=V_{n}\oplus V_{n}^{*}\oplus \mathbf {C} ,}$ 

where ${\displaystyle V_{n}\subset V}$  is a totally isotropic subspace of dimension ${\displaystyle n}$ , and ${\displaystyle V_{n}^{*}}$  is its dual space, with scalar product defined as

${\displaystyle Q(v_{1}+w_{1},v_{2}+w_{2}):=w_{2}(v_{1})+w_{1}(v_{2}),\quad v_{1},v_{2}\in V_{n},\ w_{1},w_{2}\in V_{n}^{*},}$ 

or

${\displaystyle Q(v_{1}+w_{1}+a_{1},v_{2}+w_{2}+a_{2}):=w_{2}(v_{1})+w_{1}(v_{2})+a_{1}a_{2},\quad a_{1},a_{2}\in \mathbf {C} ,}$ 

respectively.

The Clifford algebra representation ${\displaystyle \Gamma _{X}\in \mathrm {End} (\Lambda (V_{n}))}$  as endomorphisms of the irreducible Clifford/spinor module ${\displaystyle \Lambda (V_{n})}$ , is generated by the linear elements ${\displaystyle X\in V}$ , which act as

${\displaystyle \Gamma _{v}(\psi )=v\wedge \psi \ {\text{ (wedge product) }}\ {\text{for }}v\in V_{n}\ {\text{ and }}\Gamma _{w}(\psi )=\iota (w)\psi \ {\text{ (inner product) }}{\text{for}}\ w\in V_{n}^{*},}$ 

for either ${\displaystyle V=V_{n}\oplus V_{n}^{*}}$  or ${\displaystyle V=V_{n}\oplus V_{n}^{*}\oplus \mathbf {C} }$ , and

${\displaystyle \Gamma _{a}\psi =(-1)^{p}a\ \psi ,\quad a\in \mathbf {C} ,\ \psi \in \Lambda ^{p}(V_{n}),}$ 

for ${\displaystyle V=V_{n}\oplus V_{n}^{*}\oplus \mathbf {C} }$ , when ${\displaystyle \psi }$  is homogeneous of degree ${\displaystyle p}$ .

A pure spinor ${\displaystyle \psi }$  is defined to be any element ${\displaystyle \psi \in \Lambda (V_{n})}$  that is annihilated by a maximal isotropic subspace ${\displaystyle w\subset V}$  with respect to the scalar product ${\displaystyle \,Q\,}$ . Conversely, given a maximal isotropic subspace it is possible to determine the pure spinor that annihilates it, up to multiplication by a complex number, as follows.

Denote the Grassmannian of maximal isotropic (${\displaystyle n}$ -dimensional) subspaces of ${\displaystyle V}$  as ${\displaystyle \mathbf {Gr} _{n}^{0}(V,Q)}$ . The Cartan map ^[1][12][13]

${\displaystyle \mathbf {Ca} :\mathbf {Gr} _{n}^{0}(V,Q)\rightarrow \mathbf {P} (\Lambda (V_{n}))}$ 

is defined, for any element ${\displaystyle w\in \mathbf {Gr} _{n}^{0}(V,Q)}$ , with basis ${\displaystyle (X_{1},\dots ,X_{n})}$ , to have value

${\displaystyle \mathbf {Ca} (w):=\mathrm {Im} (\Gamma _{X_{1}}\cdots \Gamma _{X_{n}});}$ 

i.e. the image of ${\displaystyle \Lambda (V_{n})}$  under the endomorphism formed from taking the product of the Clifford representation endomorphisms ${\displaystyle \{\Gamma _{X_{i}}\in \mathrm {End} (\Lambda (V_{n}))\}_{i=1,\dots ,n}}$ , which is independent of the choice of basis ${\displaystyle (X_{1},\cdots ,X_{n})}$ . This is a ${\displaystyle 1}$ -dimensional subspace, due to the isotropy conditions,

${\displaystyle Q(X_{i},X_{j})=0,\quad 1\leq i,j\leq n,}$ 

which imply

${\displaystyle \Gamma _{X_{i}}\Gamma _{X_{j}}+\Gamma _{X_{j}}\Gamma _{X_{i}}=0,\quad 1\leq i,j\leq n,}$ 

and hence ${\displaystyle \mathbf {Ca} (w)}$  defines an element of the projectivization ${\displaystyle \mathbf {P} (\Lambda (V_{n}))}$  of the irreducible Clifford module ${\displaystyle \Lambda (V_{n})}$ . It follows from the isotropy conditions that, if the projective class ${\displaystyle [\psi ]}$  of a spinor ${\displaystyle \psi \in \Lambda (V_{n})}$  is in the image ${\displaystyle \mathbf {Ca} (w)}$  and ${\displaystyle X\in w}$ , then

${\displaystyle \Gamma _{X}(\psi )=0.}$ 

So any spinor ${\displaystyle \psi }$  with ${\displaystyle [\psi ]\in \mathbf {Ca} (w)}$  is annihilated, under the Clifford representation, by all elements of ${\displaystyle w}$ . Conversely, if ${\displaystyle \psi }$  is annihilated by ${\displaystyle \Gamma _{X}}$  for all ${\displaystyle X\in w}$ , then ${\displaystyle [\psi ]\in \mathbf {Ca} (w)}$ .

If ${\displaystyle V=V_{n}\oplus V_{n}^{*}}$  is even dimensional, there are two connected components in the isotropic Grassmannian ${\displaystyle \mathbf {Gr} _{n}^{0}(V,Q)}$ , which get mapped, under ${\displaystyle \mathbf {Ca} }$ , into the two half-spinor subspaces ${\displaystyle \Lambda ^{+}(V_{n}),\Lambda ^{-}(V_{n})}$  in the direct sum decomposition

${\displaystyle \Lambda (V_{n})=\Lambda ^{+}(V_{n})\oplus \Lambda ^{-}(V_{n}),}$ 

where ${\displaystyle \Lambda ^{+}(V_{n})}$  and ${\displaystyle \Lambda ^{-}(V_{n})}$  consist, respectively, of the even and odd degree elements of ${\displaystyle \Lambda ^{(}V_{n})}$  .

Define a set of bilinear forms ${\displaystyle \{\beta _{m}\}_{m=0,\dots 2n}}$  on the spinor module ${\displaystyle \Lambda (V_{n})}$ , with values in ${\displaystyle \Lambda ^{m}(V^{*})\sim \Lambda ^{m}(V)}$  (which are isomorphic via the scalar product ${\displaystyle Q}$ ), by

${\displaystyle \beta _{m}(\psi ,\phi )(X_{1},\dots ,X_{m}):=\beta _{0}(\psi ,\Gamma _{X_{1}}\cdots \Gamma _{X_{m}}\phi ),\quad {\text{for }}\psi ,\phi \in \Lambda (V_{n}),\ X_{1},\dots ,X_{m}\in V,}$ 

where, for homogeneous elements ${\displaystyle \psi \in \Lambda ^{p}(V_{n})}$ , ${\displaystyle \phi \in \Lambda ^{q}(V_{n})}$  and volume form ${\displaystyle \Omega }$  on ${\displaystyle \Lambda (V_{n})}$ ,

${\displaystyle \beta _{0}(\psi ,\phi )\,\Omega ={\begin{cases}\psi \wedge \phi \quad {\text{if }}p+q=n\\0\quad {\text{otherwise. }}\end{cases}}}$ 

As shown by Cartan,^[1] pure spinors ${\displaystyle \psi \in \Lambda (V_{n})}$  are uniquely determined by the fact that they satisfy the following set of homogeneous quadratic equations, known as the Cartan relations:^[1][12][13]

${\displaystyle \beta _{m}(\psi ,\psi )=0\quad \forall \ m\equiv n\mod (4),\quad 0\leq m<n}$ 

on the standard irreducible spinor module.

These determine the image of the submanifold of maximal isotropic subspaces of the vector space ${\displaystyle V,}$  with respect to the scalar product ${\displaystyle Q}$ , under the Cartan map, which defines an embedding of the Grassmannian of isotropic subspaces of ${\displaystyle V}$  in the projectivization of the spinor module (or half-spinor module, in the even dimensional case), realizing these as projective varieties.

There are therefore, in total,

${\displaystyle \sum _{0\leq m\leq n-1 \atop m\equiv n,{\text{ mod }}4}{{\text{dim}}(V) \choose m}}$ 

Cartan relations, signifying the vanishing of the bilinear forms ${\displaystyle \beta _{m}}$  with values in the exterior spaces ${\displaystyle \,\Lambda ^{m}(V)\,}$  for ${\displaystyle m\equiv n,{\text{ mod }}4}$ , corresponding to these skew symmetric elements of the Clifford algebra. However, since the dimension of the Grassmannian of maximal isotropic subspaces of ${\displaystyle \,V\,}$  is ${\displaystyle \,{\tfrac {1}{2}}\,n(n-1)\,}$  when ${\displaystyle \,V\,}$  is of even dimension ${\displaystyle 2n}$  and ${\displaystyle \,{\tfrac {1}{2}}\,n(n+1)\,}$  when ${\displaystyle \,V\,}$  has odd dimension ${\displaystyle 2n+1}$ , and the Cartan map is an embedding of the connected components of this in the projectivization of the half-spinor modules when ${\displaystyle \,V\,}$  is of even dimension and in the irreducible spinor module if it is of odd dimension, the number of independent quadratic constraints is only

${\displaystyle 2^{n-1}-{\tfrac {1}{2}}\,n(n-1)-1}$ 

in the ${\displaystyle \,2n\,}$  dimensional case, and

${\displaystyle 2^{n}-{\tfrac {1}{2}}\,n(n+1)-1}$ 

in the ${\displaystyle \,2n+1\,}$  dimensional case.

In 6 dimensions or fewer, all spinors are pure. In 7 or 8  dimensions, there is a single pure spinor constraint. In 10 dimensions, there are 10 constraints

${\displaystyle \psi \;\Gamma _{\mu }\,\psi =0~,\quad \mu =1,\dots ,10,}$ 

where ${\displaystyle \,\Gamma _{\mu }\,}$  are the Gamma matrices that represent the vectors in ${\displaystyle \,\mathbb {C} ^{10}\,}$  that generate the Clifford algebra. However, only ${\displaystyle 5}$  of these are independent, so the variety of projectivized pure spinors for ${\displaystyle V=\mathbb {C} ^{10}}$  is ${\displaystyle 10}$  (complex) dimensional.

For ${\displaystyle d=10}$  dimensional, ${\displaystyle N=1}$  supersymmetric Yang-Mills theory, the super-ambitwistor correspondence,^[4][5] consists of an equivalence between the supersymmetric field equations and the vanishing of supercurvature along super null lines, which are of dimension ${\displaystyle (1|16)}$ , where the ${\displaystyle 16}$  Grassmannian dimensions correspond to a pure spinor. Dimensional reduction gives the corresponding results for ${\displaystyle d=6}$ , ${\displaystyle N=2}$  and ${\displaystyle d=4}$ , ${\displaystyle N=3}$  or ${\displaystyle 4}$ .

Pure spinors were introduced in string quantization by Nathan Berkovits.^[6] Nigel Hitchin^[14] introduced generalized Calabi–Yau manifolds, where the generalized complex structure is defined by a pure spinor. These spaces describe the geometry of flux compactifications in string theory.

In the approach to integrable hierarchies developed by Mikio Sato,^[15] and his students,^[16][17] equations of the hierarchy are viewed as compatibility conditions for commuting flows on an infinite dimensional Grassmannian. Under the (infinite dimensional) Cartan map, projective pure spinors are equivalent to elements of the infinite dimensional Grassmannian consisting of maximal isotropic subspaces of a Hilbert space under a suitably defined complex scalar product. They therefore serve as moduli for solutions of the BKP integrable hierarchy,^[9][10][11] parametrizing the associated BKP ${\displaystyle \tau }$ -functions, which are generating functions for the flows. Under the Cartan map correspondence, these may be expressed as infinite dimensional Fredholm Pfaffians.^[11]

• Cartan, Élie (1981) [1966]. The Theory of Spinors. Dover Publications (reprint ed.). Paris, FR: Hermann (1966). ISBN 978-0-486-64070-9.
• Chevalley, Claude (1996) [1954]. The Algebraic Theory of Spinors and Clifford Algebras (reprint ed.). Columbia University Press (1954); Springer (1996). ISBN 978-3-540-57063-9.
• Charlton, Philip. The geometry of pure spinors, with applications, PhD thesis (1997).