### Abstract

In an earlier paper, we derived an algorithm for calculating the cross section for e^{+} +e^{-} → A + B + X, with hadrons A and B nearly back to back. The result was given in transverse position (b) space for the Fourier transform of the small angle part of the cross section. Here we discuss the structure of this result, particularly at large b, where purely perturbative calculations are not useful. We then describe how to return from b space to transverse momentum space.

Original language | English (US) |
---|---|

Pages (from-to) | 446-476 |

Number of pages | 31 |

Journal | Nuclear Physics, Section B |

Volume | 197 |

Issue number | 3 |

DOIs | |

State | Published - Apr 12 1982 |

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### All Science Journal Classification (ASJC) codes

- Nuclear and High Energy Physics

### Cite this

_{T}.

*Nuclear Physics, Section B*,

*197*(3), 446-476. https://doi.org/10.1016/0550-3213(82)90453-9

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_{T}',

*Nuclear Physics, Section B*, vol. 197, no. 3, pp. 446-476. https://doi.org/10.1016/0550-3213(82)90453-9

**Back-to-back jets : Fourier transform from b to k _{T}.** / Collins, John C.; Soper, Davison E.

Research output: Contribution to journal › Article

TY - JOUR

T1 - Back-to-back jets

T2 - Fourier transform from b to kT

AU - Collins, John C.

AU - Soper, Davison E.

PY - 1982/4/12

Y1 - 1982/4/12

N2 - In an earlier paper, we derived an algorithm for calculating the cross section for e+ +e- → A + B + X, with hadrons A and B nearly back to back. The result was given in transverse position (b) space for the Fourier transform of the small angle part of the cross section. Here we discuss the structure of this result, particularly at large b, where purely perturbative calculations are not useful. We then describe how to return from b space to transverse momentum space.

AB - In an earlier paper, we derived an algorithm for calculating the cross section for e+ +e- → A + B + X, with hadrons A and B nearly back to back. The result was given in transverse position (b) space for the Fourier transform of the small angle part of the cross section. Here we discuss the structure of this result, particularly at large b, where purely perturbative calculations are not useful. We then describe how to return from b space to transverse momentum space.

UR - http://www.scopus.com/inward/record.url?scp=27744576844&partnerID=8YFLogxK

UR - http://www.scopus.com/inward/citedby.url?scp=27744576844&partnerID=8YFLogxK

U2 - 10.1016/0550-3213(82)90453-9

DO - 10.1016/0550-3213(82)90453-9

M3 - Article

AN - SCOPUS:27744576844

VL - 197

SP - 446

EP - 476

JO - Nuclear Physics B

JF - Nuclear Physics B

SN - 0550-3213

IS - 3

ER -

_{T}. Nuclear Physics, Section B. 1982 Apr 12;197(3):446-476. https://doi.org/10.1016/0550-3213(82)90453-9