Not signed in (Sign In)

Not signed in

Want to take part in these discussions? Sign in if you have an account, or apply for one below

  • Sign in using OpenID

Discussion Tag Cloud

Vanilla 1.1.10 is a product of Lussumo. More Information: Documentation, Community Support.

Welcome to nForum
If you want to take part in these discussions either sign in now (if you have an account), apply for one now (if you don't).
    • CommentRowNumber1.
    • CommentAuthorUrs
    • CommentTimeJan 22nd 2016

    I have copied the nice implication flow chart from Adams’ original paper into the entry, here

    • CommentRowNumber2.
    • CommentAuthorUrs
    • CommentTimeJan 22nd 2016
    • (edited Jan 23rd 2016)

    I have been adding little bits and pieces to Hopf invariant and to Hopf invariant one.

    It occurs to me that for the quaternionic case of n=4n = 4, the Hopf-invariant-one theorem has a neat interpretation in terms of the story of M2/M5-brane charges (here):

    Namely the L L_\infty-computation which shows that the M2/M5-charge rationally lands in the base S rat 4S^4_{rat} of the rational quaternionic Hopf fibration has two natural non-rational integration: on the one hand to the actual S 4S^4, and on the other hand – more “conservatively” – to the homotopy fiber of the cup product on ordinary cohomology: hofib(B 4B 8)hofib(\mathbf{B}^4 \mathbb{Z} \stackrel{\cup}{\to} \mathbf{B}^8 \mathbb{Z}) .

    It seems plausible that the former is the genuine case to be considered for M2/M5-branes, but the latter certainly also still captures important information, and so a natural question is how the two compare.

    Drawing the evident hexagonal diagram

    S 7 ϕ S 4 * B 4 * B 8 \array{ && S^7 \\ & {}^{\mathllap{\phi}}\swarrow && \searrow \\ S^4 && && \ast \\ \downarrow && && \downarrow \\ \mathbf{B}^4 \mathbb{Z} && && \ast \\ & {}_{\mathllap{\cup}}\searrow && \swarrow \\ && \mathbf{B}^8 \mathbb{Z} }

    (with [S 4B 4]=1[S^4 \to \mathbf{B}^4 \mathbb{Z}] = 1 and with unit homotopy filling the diagram)

    we get a canonical comparison map induced:

    S 7fib(). S^7 \longrightarrow fib(\cup) \,.

    So the natural question is: is this comparison faithful? Does it for instance send unit M2-brane charge in degree-4 cohomotopy to unit M2-brane charge in the more ordinary cohomology with coefficients in fib()fib(\cup).

    Now, simply by factoring the above homotopy differently, there is a sibling of the above comparison map induced:

    cofib(ϕ)B 8. cofib(\phi) \longrightarrow \mathbf{B}^8 \mathbb{Z} \,.

    But inspection of the proof of the Hopf-invariant-one theorem shows that it says that the map that takes the class of

    S 4B 4S^4 \to \mathbf{B}^{4}\mathbb{Z}

    to the class of this sibling comparison map, indeed sends generators to generators!

    But passing back to the dual picture, this should exactly mean that our original comparison map

    S 7fib() S^7 \to fib(\cup)

    sends generators to generators. Which is what we would hope it does.

    For example, for a single black M2-brane with near-horizon geometry

    AdS 4×S 7 homotopyS 7, AdS_4 \times S^7 \simeq_{homotopy} S^7 \,,

    this says that its unit charge as measured in degree-4 cohomotopy

    S 7S 4 S^7 \to S^4

    is sent under the comparison map to unit charge in the more naive almost-ordinary cohomology

    S 7fib(). S^7 \to fib(\cup) \,.

    In conclusion, it seems that the Hopf invariant one theorem may be read as providing a further nontrivial consistency on the statement that M2/M5-brane charge is, non-rationally, in cohomotopy.

    • CommentRowNumber3.
    • CommentAuthorUrs
    • CommentTimeJan 24th 2016
    • (edited Jan 27th 2016)

    I have spelled out the possibly cryptic remark above with a few more diagrams for better illustration.