{"id":980,"date":"2023-06-29T20:10:37","date_gmt":"2023-06-30T01:10:37","guid":{"rendered":"http:\/\/www.fruechtetheory.com\/blog\/?p=980"},"modified":"2023-06-29T20:11:45","modified_gmt":"2023-06-30T01:11:45","slug":"vector-bosons-and-other-fleeting-field-particles","status":"publish","type":"post","link":"https:\/\/www.fruechtetheory.com\/blog\/2023\/06\/29\/vector-bosons-and-other-fleeting-field-particles\/","title":{"rendered":"Vector Bosons and Other Fleeting Field Particles"},"content":{"rendered":"\n<p class=\"wp-block-paragraph\">In the case of \u201c \u2018intermediate vector bosons\u2019: the charged bosons W<sup>+<\/sup> and W<sup>&#8211; <\/sup>\u201c ([1], pg. 363), it is possible that they may be Coulomb field inductors. Since it takes many gravitons to make up an inductor, it is reasonable to measure \u201cM<sub>W<\/sub> = 80.40 GeV\u201d at a test setup sensor.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">When two positive inductors meet head on in the open gamma ray field, they annihilate each other. The same is true for two negative inductors. If two inductors of the same charge annihilate at a sensor, the mass may be higher, as in \u201cM<sub>Z<\/sub> = 91.19 MeV\u201d, which may be the \u201cneutral Z<sup>0<\/sup> boson\u201d. Some extra gravitons may get into the act here, and since the vector summation of the gamma ray field is in the Z direction, this boson is appropriately named.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">It is not being said that all field particles are due to the Coulomb field, just some of them. The time these particles exist is \u201c\u0127 \/mc<sup>2<\/sup>\u201c ([2], pg. 654). Mandl and Shaw allude that \u201csome quantity in the vacuum is non-vanishing\u201d ([1], pg. 404). It has been known since 2005 that the vacuum is not really a vacuum.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">As far as J representing charged mass, Ryder mentions \u201cThe source J(t) plays a role analogous to that of an electromagnetic current, which acts as a source of the electromagnetic field.\u201d ([3], pg. 175).<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Reference: <a href=\"https:\/\/www.fruechtetheory.com\/blog\/2023\/03\/17\/nuclear-ideals\/\">https:\/\/www.fruechtetheory.com\/blog\/2023\/03\/17\/nuclear-ideals\/<\/a><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">The \u201crenormalized charge e<sub>r<\/sub>\u201d ([1], pg. 336) and \u201crenormalized mass m<sub>r<\/sub>\u201d can be thought of as the charge and mass of the electron immediately after a spin flip at the end of an atomic orbital arc. Somewhere in the middle of an electron orbital arc these are called \u201c \u2018running mass\u2019 and \u2018running charge\u2019 \u201c.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Zee says that \u201cfree quarks have not been observed\u201d ([4], pg. 377), though with the quark coincidence, something with the same energy has been observed with the gamma ray telescopes.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">[1] Madl, Franz and Shaw, Graham, \u201cQuantum Field Theory\u201d, John Wiley and Sons, Ltd., 2011<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">[2] Krane, Kenneth S., \u201cIntroductory Nuclear Physics\u201d, c. 1988, John Wiley &amp; Sons, Inc.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">[3] Ryder, Lewis H., \u201cQuantum Field Theory, Second Edition\u201d, Cambridge University Press, 1996<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">[4] Zee, Anthony, \u201cQuantum Field Theory in a Nutshell\u201d, Princeton University Press, 2010<\/p>\n","protected":false},"excerpt":{"rendered":"<p>In the case of \u201c \u2018intermediate vector bosons\u2019: the charged bosons W+ and W&#8211; \u201c ([1], pg. 363), it is possible that they may be Coulomb field inductors. Since it takes many gravitons to make up an inductor, it is reasonable to measure \u201cMW = 80.40 GeV\u201d at a test setup sensor. When two positive [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[16],"tags":[],"class_list":["post-980","post","type-post","status-publish","format-standard","hentry","category-quantum-field-theory"],"_links":{"self":[{"href":"https:\/\/www.fruechtetheory.com\/blog\/wp-json\/wp\/v2\/posts\/980","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.fruechtetheory.com\/blog\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.fruechtetheory.com\/blog\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.fruechtetheory.com\/blog\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.fruechtetheory.com\/blog\/wp-json\/wp\/v2\/comments?post=980"}],"version-history":[{"count":1,"href":"https:\/\/www.fruechtetheory.com\/blog\/wp-json\/wp\/v2\/posts\/980\/revisions"}],"predecessor-version":[{"id":981,"href":"https:\/\/www.fruechtetheory.com\/blog\/wp-json\/wp\/v2\/posts\/980\/revisions\/981"}],"wp:attachment":[{"href":"https:\/\/www.fruechtetheory.com\/blog\/wp-json\/wp\/v2\/media?parent=980"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.fruechtetheory.com\/blog\/wp-json\/wp\/v2\/categories?post=980"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.fruechtetheory.com\/blog\/wp-json\/wp\/v2\/tags?post=980"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}