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Summary of The Importance of
  the Higgs Research Results by
   the CERN Scientists and Why
 the Problem is Much Harder to
     Fully Master Than What
 People Think; i.e., Spontaneous
    Symmetry Breaking For a
     Particle Lasting 10 to the
   Minus Six Power Seconds, or
               Less.

                                       Dr. Andrew Walcott Beckwith, Chongqing

                                      University Department of Physics, with
    eMOTION! REPORTS.com
                                          Research Analyst Myron D. Stokes
      74 W. Long Lake Rd.

Suite 201 Bloomfield Hills, MI          “As a professional physics researcher, I, Andrew

            48304                Beckwith, congratulate CERN on its invaluable dedication

                                 to the solution of the Higgs-boson problem. This note will
             631-909-7245(NY)
                                 not be to scold the CERN researchers but to outline the
     Email: abeckwith@uh.edu
                                 very hard work ahead as to a solution of the TOTAL Higgs-

                     7/4/2012    boson problem, which needs to be carried through in an

                                 organized manner.”
Summary of The Importance of the Higgs Research Results by the

    CERN Scientists and Why the Problem is Much Harder to Fully

     Master Than What People Think; i.e. Spontaneous Symmetry

 Breaking For a Particle Lasting 10 to the Minus Six Power Seconds,

                                            or Less.

     Dr. Andrew Beckwith, in Collaboration with Research Analyst Myron D. Stokes:




                             Artist’s Concept of Big Bang Image: Deviantart.com




As a professional physics researcher, I, Andrew Beckwith, congratulate CERN on its

invaluable dedication to the solution of the Higgs-boson problem. This note will not be to
scold the CERN researchers but to outline the very hard work ahead as to a solution of the

TOTAL Higgs-boson problem, which needs to be carried through in an organized manner.


First of all, I will review the history of the Higgs mechanism for spontaneous symmetry

breaking and what is known as to outline as to the formation of mass problem in the electro

weak case: In doing this line of inquiry, we look at the additional fourth order term added

to form a modified Lagrangian term:


                      2
        1    1 2 2 1
     L             4
           x  2
                                                                                      (1)
        2           4


    The minimum of the potential given in (1) occurs when the derivative of the potential with

respect to the scalar field  is zero, i.e.


     1 2 2 1
V         4                                                                     (2)
     2      4


Such that


    2   2   0                                                                (3)


So then the case for a minimum of the potential V , with V minimum set as when V has a non-

zero constant value for its minimum value, instead of V = 0, when one has a minimum value of

V when  2  0 , so that one has


                1/2
      2 
                                                                                (4)
       
Having   0 is a false vacuum solution, instead we work directly with (4) so that


so that instead of V== 0 ( false vacuum), we have, when (4) is for the true vacuum


V    4 4

(5)


In the case of the electro weak we substitute in


  v    x

(6)


for (1) and (2) above, obtaining


                               2
                    1       1 2 2                4 
                 L             v      v         const
                                                    3
                                                                                                (7)
                    2  x
                      
                               2
                                                     4 


Comparing (7) with the 2nd term in L as a mass term, with (1) gives us the mass term which if before the

shift we work with in (1) such that


                    2 
        v     
                     

(8)


We isolate from (7) that there is a mass term which has a value of


m  2v 2  2 2                                                                               (9)


This is spontaneous symmetry breaking. It happens all the time in physics.
The basis for symmetry breaking involves a true versus a false vacuum, in physics: Very difficult to

duplicate conditions for such arising in CERN.


Getting mass formed this way, for the Higgs formation is a fantastic feat when 106 seconds are involved.

By necessity, considering the 106 seconds involved, plus the fantastic heat involved will mean that

imprecision will be rampant. Saying that one has a particular MASS for the Higgs, considering the time

duration, 106 seconds or less, and also the heat values involved will require decades of work. Note that

Higgs himself derived these sorts of procedures and extended it to a Higgs-boson 50 years ago and to this

day he is overwhelmed by the attention given to this construct when he was a very young Graduate

student. And note the ratio values obtained by (4) will be part of the experimental considerations of the

Higgs, in terms of a true vacuum.


What Myron Stokes and others have done has been to super impose a certain subset of results 10 days ago

with the announcement of the Higgs discovery, just recently. As submitted by the Author of this

discussion, the real physics begins with (4) above as a ratio expression, and then the mass, as in (9)


Both Myron and I congratulate CERN on a magnificent technical achievement, as to beginning to delve

into the formation of mass, as given by (9). We submit though, especially in lieu of the fact that the

difference between the false and true vacuum results comes about due to (4) for the true vacuum as a ratio

result, that CERN has BEGUN to work developing a fantastic achievement in future astro-particle

physics . We do wish to point though to the fact that the authors 10 days ago, gave evidence of where to

go, and that this should be part of the general record.


Andrew Beckwith, Myron D. Stokes – 4 July, 2012
Postulated Big Bang Expansion Image: Wikipedia




Related and relevant papers to this discussion:


http://asimov52.files.wordpress.com/2011/09/sanmarino-a-beckwith5a-sept2st.pdf


http://www.slideshare.net/GHHLLC2/kk-graviton-redojuly52012


http://www.slideshare.net/GHHLLC2/hadronic1z-1

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HIGGS-BOSON? Dr. Andrew Beckwith, in Collaboration with Research Analyst Myron D. Stokes: Summary of The Importance of the Higgs Research Results by the CERN Scientists and Why the Problem is Much Harder to Fully Master Th

  • 1. Summary of The Importance of the Higgs Research Results by the CERN Scientists and Why the Problem is Much Harder to Fully Master Than What People Think; i.e., Spontaneous Symmetry Breaking For a Particle Lasting 10 to the Minus Six Power Seconds, or Less. Dr. Andrew Walcott Beckwith, Chongqing University Department of Physics, with eMOTION! REPORTS.com Research Analyst Myron D. Stokes 74 W. Long Lake Rd. Suite 201 Bloomfield Hills, MI “As a professional physics researcher, I, Andrew 48304 Beckwith, congratulate CERN on its invaluable dedication to the solution of the Higgs-boson problem. This note will 631-909-7245(NY) not be to scold the CERN researchers but to outline the Email: abeckwith@uh.edu very hard work ahead as to a solution of the TOTAL Higgs- 7/4/2012 boson problem, which needs to be carried through in an organized manner.”
  • 2. Summary of The Importance of the Higgs Research Results by the CERN Scientists and Why the Problem is Much Harder to Fully Master Than What People Think; i.e. Spontaneous Symmetry Breaking For a Particle Lasting 10 to the Minus Six Power Seconds, or Less. Dr. Andrew Beckwith, in Collaboration with Research Analyst Myron D. Stokes: Artist’s Concept of Big Bang Image: Deviantart.com As a professional physics researcher, I, Andrew Beckwith, congratulate CERN on its invaluable dedication to the solution of the Higgs-boson problem. This note will not be to
  • 3. scold the CERN researchers but to outline the very hard work ahead as to a solution of the TOTAL Higgs-boson problem, which needs to be carried through in an organized manner. First of all, I will review the history of the Higgs mechanism for spontaneous symmetry breaking and what is known as to outline as to the formation of mass problem in the electro weak case: In doing this line of inquiry, we look at the additional fourth order term added to form a modified Lagrangian term: 2 1    1 2 2 1 L        4  x  2 (1) 2    4 The minimum of the potential given in (1) occurs when the derivative of the potential with respect to the scalar field  is zero, i.e. 1 2 2 1 V     4 (2) 2 4 Such that     2   2   0 (3) So then the case for a minimum of the potential V , with V minimum set as when V has a non- zero constant value for its minimum value, instead of V = 0, when one has a minimum value of V when  2  0 , so that one has 1/2  2      (4)   
  • 4. Having   0 is a false vacuum solution, instead we work directly with (4) so that so that instead of V== 0 ( false vacuum), we have, when (4) is for the true vacuum V    4 4 (5) In the case of the electro weak we substitute in   v    x (6) for (1) and (2) above, obtaining 2 1    1 2 2   4  L       v      v    const 3 (7) 2  x   2    4  Comparing (7) with the 2nd term in L as a mass term, with (1) gives us the mass term which if before the shift we work with in (1) such that  2    v         (8) We isolate from (7) that there is a mass term which has a value of m  2v 2  2 2 (9) This is spontaneous symmetry breaking. It happens all the time in physics.
  • 5. The basis for symmetry breaking involves a true versus a false vacuum, in physics: Very difficult to duplicate conditions for such arising in CERN. Getting mass formed this way, for the Higgs formation is a fantastic feat when 106 seconds are involved. By necessity, considering the 106 seconds involved, plus the fantastic heat involved will mean that imprecision will be rampant. Saying that one has a particular MASS for the Higgs, considering the time duration, 106 seconds or less, and also the heat values involved will require decades of work. Note that Higgs himself derived these sorts of procedures and extended it to a Higgs-boson 50 years ago and to this day he is overwhelmed by the attention given to this construct when he was a very young Graduate student. And note the ratio values obtained by (4) will be part of the experimental considerations of the Higgs, in terms of a true vacuum. What Myron Stokes and others have done has been to super impose a certain subset of results 10 days ago with the announcement of the Higgs discovery, just recently. As submitted by the Author of this discussion, the real physics begins with (4) above as a ratio expression, and then the mass, as in (9) Both Myron and I congratulate CERN on a magnificent technical achievement, as to beginning to delve into the formation of mass, as given by (9). We submit though, especially in lieu of the fact that the difference between the false and true vacuum results comes about due to (4) for the true vacuum as a ratio result, that CERN has BEGUN to work developing a fantastic achievement in future astro-particle physics . We do wish to point though to the fact that the authors 10 days ago, gave evidence of where to go, and that this should be part of the general record. Andrew Beckwith, Myron D. Stokes – 4 July, 2012
  • 6. Postulated Big Bang Expansion Image: Wikipedia Related and relevant papers to this discussion: http://asimov52.files.wordpress.com/2011/09/sanmarino-a-beckwith5a-sept2st.pdf http://www.slideshare.net/GHHLLC2/kk-graviton-redojuly52012 http://www.slideshare.net/GHHLLC2/hadronic1z-1