The split of index pairs into symmetric traceless

PHYSICS · Multi-part · Fermi University Physics · Particle Physics & Quantum Fields · Symmetry, groups and the quark model · Beyond the Standard Model

Symmetry and Flavour, Ch The relativistic string: action, light-cone quantisation, spectrum and D-branes

Problem

The split of index pairs into symmetric traceless, antisymmetric and trace pieces is pure counting, and it works for any number nn of transverse directions. That the closed-string states α−1Iαˉ−1J∣p⟩\alpha^I_{-1}\bar\alpha^J_{-1}|p\rangle carrying such pairs are massless is a separate fact, true in the bosonic string only at D=26D=26. ((a)) Show that the n2n^2 index pairs split into 12n(n+1)−1\tfrac12n(n+1)-1 symmetric traceless, 12n(n−1)\tfrac12n(n-1) antisymmetric and 11 trace, and that with n=D−2n=D-2 the first count equals 12D(D−3)\tfrac12D(D-3). ((b)) Evaluate the three counts for n=8n=8, the number of transverse directions if spacetime had ten dimensions. Only the counting is asked for: at D=10D=10 the bosonic states are not massless. ((c)) In the bosonic string at D=26D=26, how many massless gauge vectors does a stack of k=4k=4 coincident D-branes carry, and of which gauge group? ((d)) One of the four branes is now moved a proper distance d=0.50 fmd=0.50\,\mathrm{fm} away from the other three, which remain coincident, with string tension T0=0.20 GeV2T_0=0.20\,\mathrm{GeV^2}. State the unbroken gauge group, the number of vectors that remain massless, the number that become massive, and the common mass (in GeV\mathrm{GeV}) of the massive vectors. Use ℏc=0.1973 GeV fm\hbar c=0.1973\,\mathrm{GeV\,fm}.

Browse the problem library