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        <title>Les Houches 2013:groups:sm</title>
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            <title>Les Houches</title>
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            <title>2013:groups:sm:blha</title>
            <link>https://phystev.cnrs.fr/wiki/2013:groups:sm:blha?rev=1376379206&amp;do=diff</link>
            <description>BLHA Page

a) An update on this is in the make. 

The details are in the new version of the draft:

updated write-up

Suggested C/C++ and Fortran declarations  (API) for the runtime interface.

Comments:

Concerning full SM corrections, they can be accommodated by the interface (possibly split into several contributions) if CouplingPower QCD, CouplingPower QED and CorrectionType can be specified on per-process basis.$\sin^2\theta_w$</description>
            <author>anonymous@undisclosed.example.com (Anonymous)</author>
        <category>2013:groups:sm</category>
            <pubDate>Tue, 13 Aug 2013 09:33:26 +0000</pubDate>
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        <item>
            <title>2013:groups:sm:cutsobservables</title>
            <link>https://phystev.cnrs.fr/wiki/2013:groups:sm:cutsobservables?rev=1370796989&amp;do=diff</link>
            <description>Zeroth order info

	* we said to generate W-&gt;munu, but we will not be making any kinematic cuts on the W decay products; for simplicity we could just generate W+, correct? Similarly, we will not be making cuts on the Higgs decay products, for all energies, correct?</description>
            <author>anonymous@undisclosed.example.com (Anonymous)</author>
        <category>2013:groups:sm</category>
            <pubDate>Sun, 09 Jun 2013 18:56:29 +0000</pubDate>
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        <item>
            <title>2013:groups:sm:nnlowishlist</title>
            <link>https://phystev.cnrs.fr/wiki/2013:groups:sm:nnlowishlist?rev=1371022767&amp;do=diff</link>
            <description>NNLO QCD and NLO EW Les Houches Wishlist

Wishlist part 1 - Higgs (V=W,Z)
 Process  known                            desired              motivation  H      d\sigma @ NNLO QCD 
d\sigma @ NLO EW  
finite quark mass effects @ NLO       d\sigma @ NNNLO QCD + NLO EW</description>
            <author>anonymous@undisclosed.example.com (Anonymous)</author>
        <category>2013:groups:sm</category>
            <pubDate>Wed, 12 Jun 2013 09:39:27 +0000</pubDate>
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        <item>
            <title>2013:groups:sm:snowmass</title>
            <link>https://phystev.cnrs.fr/wiki/2013:groups:sm:snowmass?rev=1368645575&amp;do=diff</link>
            <description>Coordination with Snowmass

Coordination with Snowmass: QCD Issues

A link to a list of issues and topics set for Snowmass, brought to us by the LH-Snowmass coordinator pdf file

Coordination with Snowmass: QCD mini Workshop at Fermilab, 31 Jan 2013

There will be a 1-day mini-workshop at Fermilab on Jan. 31 dealing with some of the QCD issues relevant for the LHC and beyond. In particular, this meeting will concentrate
on:</description>
            <author>anonymous@undisclosed.example.com (Anonymous)</author>
        <category>2013:groups:sm</category>
            <pubDate>Wed, 15 May 2013 21:19:35 +0000</pubDate>
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        <item>
            <title>2013:groups:sm:start</title>
            <link>https://phystev.cnrs.fr/wiki/2013:groups:sm:start?rev=1370968784&amp;do=diff</link>
            <description>SM: Loops, Multi-legs, Jets

List of Topics

 1)      PDFs

a)      impact of LHC data, current and future

	*   -how well do we know PDFs at high x-&gt;implications for new physics
									*                   -how Gaussian are high x PDF uncertainties, i.e. what would it take to believe a high mass excess</description>
            <author>anonymous@undisclosed.example.com (Anonymous)</author>
        <category>2013:groups:sm</category>
            <pubDate>Tue, 11 Jun 2013 18:39:44 +0000</pubDate>
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