> On 28 May 2019, at 16:15, Lawrence Crowell <[email protected]> 
> wrote:
> 
> 
> On Tuesday, May 28, 2019 at 6:47:41 AM UTC-5, Bruno Marchal wrote:
> 
>> On 27 May 2019, at 14:32, Lawrence Crowell <[email protected] 
>> <javascript:>> wrote:
>> 
>> On Monday, May 27, 2019 at 6:41:39 AM UTC-5, Bruno Marchal wrote:
>> 
>>> On 24 May 2019, at 02:26, Lawrence Crowell <[email protected] <>> 
>>> wrote:
>>> 
>>> On Thursday, May 23, 2019 at 11:03:49 AM UTC-5, howardmarks wrote:
>>> Good point on the "Higgs" Boson. Especially when the discoverer said what 
>>> he said. The experiments at CERN, Fermi Lab, etc. were run with the 
>>> standard model in mind. They defined the "evidence" they expected a Higgs 
>>> boson to manifest in residue particles, and, when they found, amongst the 
>>> subatomic and atomic debris, a particle near the characteristics they 
>>> expected, they called it a "hit".  There is only indirect evidence. We 
>>> can't directly observe picometer objects moving at close to the speed of 
>>> light. We know few things, like the mass to charge ratio and approx kinetic 
>>> energy...  
>>> Cheers!
>>> 
>>> My area is physics, and have written on the connection between spacetime or 
>>> gravitation with particle physics. Cosmin wanted to see the Higgs boson, 
>>> and that is about it. It may be disappointing, but the particle only last 
>>> about 10^{-25} seconds on a path 10^{-15}cm long. So we detect this field 
>>> by the particles it decays into. Since it requires a lot of energy the 
>>> machine is large, the detectors are large and it is a major undertaking. I 
>>> don't have Higgs particles in my pocket.
>> 
>> Really? How does your handkerchief get a mass? 
>> 
>> Bruno
>> 
>> 
>> The mass of particle is due to the coupling of three of the Goldstone bosons 
>> in the two doublets. The Higgs particle detected does not couple to 
>> anything, so again I do not have a Higgs boson.
>> 
>> The two doublets (H^+, H^-) and (H^0, h) for the charged weak currents and 
>> the neutral weak currents couple as
>> 
>> W^± + H^± → WH^±
>> 
>> Z^0 + H^0 → ZH^0
>> 
>> where the condensate physics of the Higgs Goldstone bosons on the left 
>> results in the charge and neutral currents on the left that have mass. The 
>> weak interaction currents on the left have transverse field components, but 
>> since they are massive there is no longitudinal field component. On the 
>> right however the weak interaction field components have longitudinal 
>> fields, where the degree of freedom of the Higgs Goldstone bosons are 
>> transferred into these longitudinal components. A lot of physics is about 
>> counting degrees of freedom.
>> 
>> There are the Yukawa Lagrangians L_y ~ g_yψ-bar Hψ that give small masses to 
>> quarks and leptons. For low mass particles this is a few MeV, say the 
>> electron and ud quarks. It is tiny for neutrinos, which actually leads to 
>> big questions, and it approaches the mass of the Higgs particle for the top 
>> quark. However, most mass is in baryons due not to the Higgs condensate but 
>> due to the the self-confinement of the QCD interaction. 
>> 
>> So the Higgs particle measured by the LHC is this loner particle h, which in 
>> this theory does not couple to anything. One could imagine a theory where 
>> this does couple to the photon, which would break the U(1) symmetry of 
>> quantum electrodynamics (QED). However, in standard EW physics that does not 
>> happen. Curiously though, superconductivity is a case where QED is symmetry 
>> broken, and there have been proposals for saying this lone Higgs particle 
>> defines condensate states in the vacuum that are responsible for U(1) 
>> breaking of QED and superconductivity. Yet, if this particle is produced at 
>> high energy it rapidly decays into two Zs, a W++ and W^- or two photons. 
>> These diphoton decays, which the Zs and Ws decay into as well, are the 
>> target of LHC Higgs detection.
> 
> 
> I was a bit joking, now <I will have to mediate all this. May naïve idea was 
> that the Higgs boson was needed to give mass to the particles, and so is 
> present everywhere there is some mass. You seem to contradict that idea, but 
> I will have to dig deeper n this issue. Thanks for trying, anyway.
> 
> Bruno 
> 
> 
> There is a bit of an illusion that the Higgs particle gives all the mass of 
> the universe. It gives mass to the weak interaction currents, or the W and Z 
> bosons. It also gives mass to the T-quiark which has a mass slightly smaller 
> than the Higgs boson. It only gives a small amount of mass to stable 
> particles around us. Most of the mass around us come from the mass-gap 
> induced by the anti-screening or self-interacting properties of the QCD 
> bosons. This is then 98% or more the mass of a proton. 

OK. And of the neutron, I guess. 

Then for the mass of the universe, we need to understand dark matter, also.

Bruno



> 
> LC
>  
> 
> 
>> 
>> LC
>> 
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