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It is nevertheless possible to find such a space by enlarging the notion of space.
In
Picking different algebras then give rise to different symmetries. The Spectral Standard Model takes as input the algebra <math>A = C^{\infty}(M) \otimes A_F </math> where <math>C^{\infty}(M)</math> is the algebra of differentiable functions encoding the 4-dimensional manifold and <math>A_F = \mathbb{C} \oplus \mathbb{H} \oplus M_3(\mathbb{C})</math> is a finite dimensional algebra encoding the symmetries of the standard model.
==History==
First ideas to use
{{cite book
| last = Connes | first = Alain | author-link = Alain Connes
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</ref> The Connes-Lott model did not incorporate the gravitational field.
In 1997, [[Ali Chamseddine]] and
{{cite journal | title = The Spectral Action Principle
| last1 = Chamseddine | first1 = Ali H.
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| arxiv = hep-th/0608221
| bibcode = 2007JMP....48a2303B | s2cid = 11511575 }}
</ref> and
{{cite journal | title = Noncommutative Geometry and the standard model with neutrino mixing
| last = Connes | first = Alain
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| year = 2008
| arxiv = 0808.0534
}}</ref> excluded a Higgs mass of 158 to 175 GeV at the 95% confidence level.
{{cite web
| title = Irony
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}}</ref> In July 2012, CERN announced the discovery of the [[Higgs boson]] with a mass around 125 GeV/''c''<sup>2</sup>.
A proposal to address the problem of the Higgs mass was published by [[Ali Chamseddine]] and
<ref name="10.1007/JHEP09(2012)104"/> by taking into account a real scalar field that was already present in the model but was neglected in previous analysis.
Another solution to the Higgs mass problem was put forward by Christopher Estrada and [[Matilde Marcolli]] by studying renormalization group flow in presence of gravitational correction terms.<ref name="10.1142/S0219887813500369">
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