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DBI Analysis of Open String Bound States on Non-compact D-branes

DBI Analysis of Open String Bound States on Non-compact D-branes

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CHAPTER 3. SUPERSTRINGS 423.3.1 Closed stringsWe start by c<strong>on</strong>sidering the possibility thatψ + (σ, τ) = ±ψ + (σ + π, τ), (3.16)ψ − (σ, τ) = ±ψ − (σ + π, τ). (3.17)Note that these suppositi<strong>on</strong>s imply that the same relati<strong>on</strong>s also apply to the variati<strong>on</strong>sδψ ± . Furthermore, we see that if the + sign is chosen, the functi<strong>on</strong>s are periodic andare said to obey Ram<strong>on</strong>d boundary c<strong>on</strong>diti<strong>on</strong>s (R), if − is chosen they are antiperiodicand obey Neveu-Schwarz boundary c<strong>on</strong>diti<strong>on</strong>s (NS). ψ + corresp<strong>on</strong>ds to left-movers, ψ −to right-movers, and the periodicity c<strong>on</strong>diti<strong>on</strong> for them can be chosen independantly,resulting in four different possible combinati<strong>on</strong>s, namely, choosing to write them as(left-movers,right-movers), (NS,NS), (NS,R), (R,NS) and (R,R).To realize these different boundary c<strong>on</strong>diti<strong>on</strong>s, the following expansi<strong>on</strong>s can be applied:3 R left-movers: ψ + (σ, τ) = ∑ m∈˜dµ m e −2im(τ+σ) , (3.18)R right-movers: ψ − (σ, τ) = ∑ n∈d µ ne −2in(τ−σ) , (3.19)NS left-movers:ψ + (σ, τ) = ∑˜bµ r e −2ir(τ+σ) , (3.20)NS right-movers:r∈+ 1 2ψ − (σ, τ) = ∑b µ se −2is(τ−σ) . (3.21)s∈+ 12We see that the (anti)periodicity is reflected in the (half-)integer summing indices. Fromhere<strong>on</strong>, we will follow the c<strong>on</strong>venti<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> using indices (m, n) for integer numbers, and(r, s) for half-integer numbers.3.3.2 <str<strong>on</strong>g>Open</str<strong>on</strong>g> stringsWhen c<strong>on</strong>sidering open strings, the names Ram<strong>on</strong>d and Neveu-Schwarz boundary c<strong>on</strong>diti<strong>on</strong>sare still used, but they corresp<strong>on</strong>d to different c<strong>on</strong>diti<strong>on</strong>s. Nevertheless, they arevery similar, explaining the double usage.Since now the positi<strong>on</strong>s (σ = 0) and (σ = π) corresp<strong>on</strong>d to two different and a prioriunrelated positi<strong>on</strong>s <strong>on</strong> the string, the two terms in Eq. 3.15 should vanish seperately.Hence, we see that{ψ − (0, τ)δψ − (0, τ) − ψ + (0, τ)δψ + (0, τ) = 0,(3.22)ψ − (π, τ) δψ − (π, τ) − ψ + (π, τ)δψ + (π, τ) = 0.3 Almost every reference uses b and d to denote the NS and R modes respectively, except for [14] whouse b for both, and differentiate <strong>on</strong>ly by means <str<strong>on</strong>g>of</str<strong>on</strong>g> their indices (m, n) or (r, s).

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