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SNOWMASS-ELECTROWEAK  April 2013

SNOWMASS-ELECTROWEAK April 2013

Subject:

Re: question from the Capabilities group

From:

Ashutosh Kotwal <[log in to unmask]>

Reply-To:

snowmass-electroweak Snowmass 2013 Electroweak study group <[log in to unmask]>

Date:

Wed, 24 Apr 2013 19:48:48 -0400

Content-Type:

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On Apr 24, 2013, at 7:41 PM, Jens Erler <[log in to unmask]> wrote:

> Hi Ashutosh,
> 
> yes, people talk about this (and there are some results), and in the very long run it should be possible to do this


thats good to know


> competitively.  One also needs the physical charm mass for the charm threshold,
> but this can be done on the lattice, as well.  In the moment the lattice approach is not precise enough,
> and one caveat is that it is unclear when and how to trust the error.  There are
> vigorous discussions between different lattice groups using different fermion definitions.
> Also, they would have to make it a priority (in effort and CPU), which from our perspective it certainly would be,
> but from my experience they may well think other simulations are more important.



I would put it to them as follows: what is the point of  developing a precise lattice formulation for 40 years if one precise prediction which is important cannot be obtained from it? 


regards,
Ashutosh


> Regards,
> Jens
> 
> 
> On Apr 24, 2013, at 6:26 PM, Ashutosh Kotwal wrote:
> 
>> 
>> On Apr 19, 2013, at 10:17 AM, Jens Erler <[log in to unmask]> wrote:
>> 
>>> Hi,
>>> 
>>> I also see alpha_s less of a concern.  The alpha_s value from the Z-lineshape has
>>> currently a negligible theory error, so it is especially here that I would expect great
>>> improvement.  If one then also gets alpha_s to per mille precision from event shapes,
>>> one would even gain another independent EW observable to very high precision.
>>> But one needs a plausible avenue to credibly improve Delta alpha (M_Z)
>> 
>> 
>> what about computing Delta alpha (MZ) using lattice QCD for the non-perturbative hadronic loops?
>> 
>> regards,
>> Ashutosh

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