1 / 7

Layout changes

from ATL-PHYS-2004-006. Layout changes. from ATL-PHYS-2004-006. from ATL-PHYS-2004-006. from ATL-PHYS-2004-006. fig.9 Impact parameter の正負の定義. from ATL-PHYS-2004-006. 2D b-tagging algorithm: 各 track に transverse impact の weight をつけて b である確率 wi を計算し

Télécharger la présentation

Layout changes

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. from ATL-PHYS-2004-006 Layout changes

  2. from ATL-PHYS-2004-006 from ATL-PHYS-2004-006

  3. from ATL-PHYS-2004-006 fig.9 Impact parameterの正負の定義

  4. from ATL-PHYS-2004-006 • 2D b-tagging algorithm: • 各trackにtransverse impactのweightをつけてbである確率wiを計算し • good trackのlog(wi)和を計算してjet weightする。

  5. from ATL-PHYS-2004-006 (2) 3D b-tagging: z 方向もlikelyhoodの計算に入れる。 (3) SV method : 2ndary vertexがjet中に存在するか見つける。Energy, paticle数、 invariant massなどの情報を入れる。 WH eventによるlight quark Jet rejection power計算 at e(b)=50%

  6. from ATL-PHYS-2004-006 • TDR geometryに比べDC1は • Rとmassの増加でX0.5 • 2nd layer staging-- x0.7 • Pileup, ineff, align - x0.75 • 300mm->400mm ---x0.9 とかなりdegrade • xKalmanなどaligorithmでx1.8 • 3D b-taggingx1.9 • Secondary vertex methodx2.8 この結果 150 @e(b)=60%が得られた。TDRの100@60%より良い。

  7. from ATL-PHYS-2004-006

More Related