added pointer to today’s

- Samuel Kováčik, Juraj Tekel,
*Fuzzy Onion as a Matrix Model*[arXiv:2309.00576]

added pointer to today’s

- Denjoe O’Connor, Brian P. Dolan,
*Exceptional fuzzy spaces and octonions*[arXiv:2210.14754]

added pointer to today’s

- Anwesha Chakraborty, Partha Nandi, Biswajit Chakraborty,
*A note on spectral triple with real structure on fuzzy sphere*(arXiv:2111.03012)

added pointer to today’s

- Francesco Pisacane,
*$O(D)$-equivariant fuzzy spheres*(arXiv:2002.01901)

Ah, I see. Thanks!

]]>Post the fix, you still had a mistaken $j$, but I’ve fixed that now and another typo.

]]>The first occurence of $\rho_j$ was a typo.

I have now fixed it, moved the discussion of normalizations to its own subsection *Conventions and Normalizations* and expanded a fair bit.

But maybe your comment already refers to these edits? Most equations are numbered now, please let me know which one you are looking at.

]]>Is something odd going on with $j$ and $N$ in the description of the fuzzy 2-sphere and then later in the definition of $\rho_j$?

]]>What’s the $N$-dependence of the right normalization of the integral over the unit fuzzy 2-sphere by tracing?

Is it $\tfrac{1}{\sqrt{N^2 -1}}$ or just $\tfrac{1}{N}$?

I suppose it must be the former, but some authors use the latter.

Of course it depends on what one wants to do.

I’d be inclined to argue with the cross product formula for the volume element of the ordinary 2-sphere. Identifying that cross product differential with the commutator of the fuzzy functions gives the $\tfrac{1}{\sqrt{N^2 -1}}$-factor, but now the question is why not rescale that identification.

I was hoping the answer might be in

- Francesco D’Andrea, Fedele Lizzi, Joseph CVárilly,
*Metric Properties of the Fuzzy Sphere*, Lett. Math. Phys.103 (2013), 183-205 (arXiv:1209.0108)

but if it is, I haven’t found it yet.

]]>replaced the previous graphics (showing the chord diagrams coresponding to the various shape observables on the fuzzy 2-sphere) by a slightly improved version (here). Also adjusted the text slightly, but there remains much room for improvement.

]]>added references on the fuzzy 6-sphere and higher:

Sanjaye Ramgoolam, Section 5 of:

*On spherical harmonics for fuzzy spheres in diverse dimensions*, Nucl. Phys. B610: 461-488, 2001 (arXiv:hep-th/0105006)Yusuke Kimura,

*On Higher Dimensional Fuzzy Spherical Branes*, Nucl. Phys. B664 (2003) 512-530 (arXiv:hep-th/0301055)

added the original references on the fuzzy 4-sphere:

Harald Grosse, Ctirad Klimcik, P. Presnajder,

*On Finite 4D Quantum Field Theory in Non-Commutative Geometry*, Commun. Math. Phys.180:429-438, 1996 (arXiv:hep-th/9602115)Judith Castelino, Sangmin Lee, Washington Taylor,

*Longitudinal 5-branes as 4-spheres in Matrix theory*, Nucl. Phys. B526:334-350, 1998 (arXiv:hep-th/9712105)(via D5-branes)

am adding pointers on the fuzzy 3-sphere:

The fuzzy 3-sphere was first discussed (in the context of D0-brane-systems) in

- Z. Guralnik, Sanyaje Ramgoolam,
*On the Polarization of Unstable D0-Branes into Non-Commutative Odd Spheres*, JHEP 0102:032, 2001 (arXiv:hep-th/0101001)

Discussion in the context of M2-M5-brane bound states/E-strings:

- Anirban Basu, Jeffrey Harvey,
*The M2-M5 Brane System and a Generalized Nahm’s Equation*, Nucl.Phys. B713 (2005) 136-150 (arXiv:hep-th/0412310)

added a graphics (here) illustrating how what one might call the “shape observables” on the fuzzy 2-sphere (the integrals “$\int_{S^2_N} (R^{2k})$” for any choice of fixing the ordering ambiguity of the integrand) are encoded by chord diagrams, and are in fact $\mathfrak{sl}(2)$-weight system Vassiliev invariants.

To give this a little bit of a home, I added a minimum of text around that, and in order to give that text a bit of a home I added some further text with basics on the definition of the fuzzy 2-sphere.

]]>starting a stub. Nothing here yet, but need to save.

]]>