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E8 Gauge Theory, and a Derivation of K-Theory from M-Theory
High Energy Physics - Theory · Submitted 10 May 2000
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We analyze the detailed phase factors on the two sides and show that they agree, thereby testing M-theory/Type IIA duality as well as the K-theory formalism in an interesting way.
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The abstract, sentence by sentence
The partition function of Ramond-Ramond p-form fields in Type IIA supergravity on a ten-manifold X contains subtle phase factors that are associated with T-duality, self-duality, and the relation of the RR fields to K-theory. The analogous partition function of M-theory on X x S1 contains subtle phases that are similarly associated with E8 gauge theory. We analyze the detailed phase factors on the two sides and show that they agree, thereby testing M-theory/Type IIA duality as well as the K-theory formalism in an interesting way. We also show that certain D-brane states wrapped on nontrivial homology cycles are actually unstable, that (-1)^{F_L} symmetry in Type IIA superstring theory depends in general on a cancellation between a fermion anomaly and an anomaly of RR fields, and that Type IIA superstring theory with no wrapped branes is well-defined only on a spacetime with W_7=0.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The partition function of Ramond-Ramond p-form fields in Type IIA supergravity on a ten-manifold X contains subtle phase factors that are associated with T-duality, self-duality, and the relation of the RR fields to K-theory. | background 1.00 | 0.10 | 0.06 | asserted 0.99 |
| s1 | The analogous partition function of M-theory on X x S1 contains subtle phases that are similarly associated with E8 gauge theory. | background 0.72 | 0.26 | 0.07 | asserted 0.99 |
| s2 | We analyze the detailed phase factors on the two sides and show that they agree, thereby testing M-theory/Type IIA duality as well as the K-theory formalism in an interesting way. | contribution 0.70 | 0.96 | 0.58 | asserted 1.00 |
| s3 | We also show that certain D-brane states wrapped on nontrivial homology cycles are actually unstable, that (-1)^{F_L} symmetry in Type IIA superstring theory depends in general on a cancellation between a fermion anomaly and an anomaly of RR fields, and that Type IIA superstring theory with no wrapped branes is well-defined only on a spacetime with W_7=0. | result 0.96 | 0.92 | 0.19 | asserted 1.00 |
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The paper
Original abstract
The partition function of Ramond-Ramond p-form fields in Type IIA supergravity on a ten-manifold X contains subtle phase factors that are associated with T-duality, self-duality, and the relation of the RR fields to K-theory. The analogous partition function of M-theory on X x S1 contains subtle phases that are similarly associated with E8 gauge theory. We analyze the detailed phase factors on the two sides and show that they agree, thereby testing M-theory/Type IIA duality as well as the K-theory formalism in an interesting way. We also show that certain D-brane states wrapped on nontrivial homology cycles are actually unstable, that (-1)^{F_L} symmetry in Type IIA superstring theory depends in general on a cancellation between a fermion anomaly and an anomaly of RR fields, and that Type IIA superstring theory with no wrapped branes is well-defined only on a spacetime with W_7=0.
Human review
References
How later papers used it
60 later papers cite it
2 later papers by other authors are listed below: 1 built on it and 1 cited it as support.
Builds on it 1 of 4 papers with this label
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Derived a constraint on degree twelve Chern numbers that generalizes the constraint on degree ten Chern numbers in this paper.
M-Theory with Framed Corners and Tertiary Index Invariants (2012) · 0.96 · paraphrased: the licence does not allow quoting
Cites it as support 1 paper
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Reduced compatibility of F4 with ten-dimensional type IIA at the topological level to that of E8, which follows from this paper.
On the geometry of the supermultiplet in M-theory (2009) · 0.97 · paraphrased: the licence does not allow quoting
How the literature uses it
61 arXiv papers cite this in 153 sentences
Papers citing it · 121 sentences without a confident label
Contests it 1 paper
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Indeed, despite wideheld beliefs within the string theory community, there is as of yet no definitive mathematically rigorous argument for twisted K-theory being the right coefficients for D-brane charge: the purported derivation of [ref] is rather a consistency check on the sign of the partition function over K-theory fields—a priori many other (twisted) cohomology theories could yield the same sign rule; the arguments of [ref] are differential form computations, hence cannot capture any torsion information; and there are moreover persistent conceptual issues with the proposal that D-brane charge is classified by twisted K-theory (see for example [ref] ).
Parametrised Homotopy Theory and Gauge Enhancement · Conclusion · contest 0.77
Builds on it 4 papers
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In particular the question of extension of the $_2$ invariant $f(a+b)- f(a) -f(b)$ of [ref] becomes a question of extension on String manifolds of $MString_10 ( Z)$ rather than $MSpin(Z)$ for the Spin case, where $Z$ is $K(, 4 ) ×K(, 4)$ or $K(, 4) ∧K(, 4)$.
Anomalies of E8 gauge theory on String manifolds · Introduction · 0.90
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This results in a constraint on degree twelve Chern numbers that generalize the constraint on degree ten Chern numbers in [ref] , and gives rise to a cup product composite Chern–Simons theory.
M-Theory with Framed Corners and Tertiary Index Invariants · Introduction · 0.96
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This is the orbifold generalization of the Freed-Witten condition [ref] formulated in terms of obstruction classes in Bredon cohomology.
Ramond-Ramond Fields, Fractional Branes and Orbifold Differential K-Theory · Consistency conditions · 0.99
Uses its method or tool 3 papers
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The analysis follows that of [ref] .
Anomalies of E8 gauge theory on String manifolds · Refinement of the M-theory/IIA partition Function · 0.87
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This approach has been used in [ref] , and is the approach we will use to determine the duality anomaly of type IIB string theory.
The anomaly that was not meant IIB · Bordism groups and anomalies · 0.96
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We will analyze the first system in a way that is similar to the analysis of the latter in [ref] .
Topological aspects of the NS5-brane · Introduction · 0.80
Compares with it 6 papers
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Thus that makes a departure from the discussion of [ref] in two respects: We are looking at the phase in eleven dimensions, involving the eta invariant, instead of the phase in twelve dimensions, involving the index, and the expression is a ten-dimensional integral.
Geometry of Spin and Spin^c structures in the M-theory partition function · Introduction and Summary · 1.00
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We show that it reproduces the relevant properties of previous models, mainly [ref] , and refines them in the following ways. * All three gauge fields are dynamical (gravity, C-field, $E_8$-field), none is fixed background.
The E8 moduli 3-stack of the C-field in M-theory · Introduction · 0.83
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This allows for more general boundary conditions than those of Atiyah-Patodi-Singer (APS) [ref] used in [ref] .
Corners in M-theory · Introduction · 0.87
Cites it as support 1 paper
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Hence at the topological level, compatibility of $F_4$ with ten-dimensional type IIA is reduced to that of $E_8$, which follows from [ref] [ref] [ref] .
On the geometry of the supermultiplet in M-theory · Compatibility with ten-dimensional superstring theories · 0.97
Cites it as background 12 papers
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The DMW anomaly [ref] in the comparison of the partition functions of M-theory and type IIA string theory is given by the vanishing of the seventh integral Stiefel-Whitney class $W_7(X)$ of spacetime $X$.
Anomalies of E8 gauge theory on String manifolds · Introduction · 0.90
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We start by recalling the setting and the results that we need from [ref] .
Geometry of Spin and Spin^c structures in the M-theory partition function · The phase of M-theory in the $Spin^c$ case. · 0.98
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It has been tradition to describe the expected M-brane charge quantization via ordinary cohomology equipped with an incremental sequence of constraints (e.g. [ref] [ref] [ref] [ref] ).
M/F-Theory as Mf-Theory · Introduction · 0.97
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