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A storm in a “T” cup

Date post: 23-Feb-2016
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A storm in a “T” cup. Or how (not) to make transverse projections at the LHC. Usual geometry and momentum projection. In (1+3)d:. - PowerPoint PPT Presentation
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A storm in a “T” cup Or how (not) to make transverse projections at the LHC
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Page 1: A storm in a “T” cup

A storm in a “T” cup

Or how (not) to make transverse projections at the LHC

Page 2: A storm in a “T” cup

Usual geometry and momentum projection

What to do with time-like component of P when projecting to (1+2)d?

Various options possible & used to construct time-like component: (Here labelled “T”, “V”, “o”)Differences, pros & cons not widely appreciated.

In (1+3)d:

Page 3: A storm in a “T” cup

Option 1/3The “T” projectionMass-preserving

Page 4: A storm in a “T” cup

Option 2/3The “V” projectionSpeed preserving

After this projection the 1+2-dimensional inner product is no longer M2

However, the 1+2 dimensional speed is preserved:

Page 5: A storm in a “T” cup

Option 3/3The “o” projectionAlways massless

Page 6: A storm in a “T” cup
Page 7: A storm in a “T” cup

A graphical representation

Hierarchy easily proved to be:

Page 8: A storm in a “T” cup

Partitioning events

Reconstruct parent masses by summing (1+3) or (1+2) vectors

Page 9: A storm in a “T” cup

Operations “add” and “project” do not commute

Example:

Page 10: A storm in a “T” cup

Procedures given for constructing variables for given hypothesis

Example of fully leptonictop pair decay

Page 11: A storm in a “T” cup

How existing variables fit in ourcategorisation

Page 12: A storm in a “T” cup

What common computer libraries

offer


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