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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

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

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Chapter 7A First Example“Le temps n’apprécie rien qui se fait sans lui...”Lambic Brewery, BrusselsWritten <strong>on</strong> a piece <str<strong>on</strong>g>of</str<strong>on</strong>g> wood patientlyhanging in the fermentati<strong>on</strong> chamber.As a way <str<strong>on</strong>g>of</str<strong>on</strong>g> getting acquainted with the problem at hand, a good place to start is toretrace the steps needed in order to obtain the results reported in [6]. In this article,a calculati<strong>on</strong> is carried out in secti<strong>on</strong> 4 ressembling the <strong>on</strong>e we will ultimately want tomake. The problem at hand is to find the spectrum <str<strong>on</strong>g>of</str<strong>on</strong>g> a D1-brane living <strong>on</strong> the cigartarget space using the small fluctuati<strong>on</strong> <str<strong>on</strong>g>DBI</str<strong>on</strong>g> analysis. We will also perform the samecomputati<strong>on</strong> for a D1-brane living <strong>on</strong> the trumpet, a case <str<strong>on</strong>g>of</str<strong>on</strong>g> interest since the D2-brane<strong>on</strong> the cigar we want to analyse came about by T-dualizing a D1-brane <strong>on</strong> the trumpet.As was menti<strong>on</strong>ed earlier, we should be careful when interpreting the results <str<strong>on</strong>g>of</str<strong>on</strong>g> thiscomputati<strong>on</strong>, since the exploding <str<strong>on</strong>g>of</str<strong>on</strong>g> the Φ field near the trumpet origin alerts us thatwe should also take into account extra perturbative terms. Nevertheless, despite this,going from the cigar to the trumpet is so easy, that this result will c<strong>on</strong>stitute a firstindicati<strong>on</strong> whether or not we are <strong>on</strong> the right track (<str<strong>on</strong>g>of</str<strong>on</strong>g> finding bound states, that is).In all the computati<strong>on</strong>s in this and the next chapter, we set α ′ = 1.7.1 D1-brane <strong>on</strong> the cigar7.1.1 Metric and acti<strong>on</strong>The cigar metric is given byds 2 = (dρ) 2 + (tanh ρ) 2 dτ 2 ; e −Φ = e −Φ 0chρ. (7.1)85

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